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710.0453 | Higher-spin Gauge and Trace Anomalies in Two-dimensional Backgrounds | Two-dimensional quantum fields in electric and gravitational backgrounds can
be described by conformal field theories, and hence all the physical
(covariant) quantities can be written in terms of the corresponding holomorphic
quantities. In this paper, we first derive relations between covariant and
holomorphic forms... | hep-th gr-qc | twodimensional quantum fields in electric and gravitational backgrounds can be described by conformal field theories and hence all the physical covariant quantities can be written in terms of the corresponding holomorphic quantities in this paper we first derive relations between covariant and holomorphic forms of high... | [['twodimensional', 'quantum', 'fields', 'in', 'electric', 'and', 'gravitational', 'backgrounds', 'can', 'be', 'described', 'by', 'conformal', 'field', 'theories', 'and', 'hence', 'all', 'the', 'physical', 'covariant', 'quantities', 'can', 'be', 'written', 'in', 'terms', 'of', 'the', 'corresponding', 'holomorphic', 'qu... | [-0.13002230587881058, 0.18781170836221214, -0.05424882337154651, 0.10755731519285208, -0.0682082270716571, -0.06837050268553536, -0.052305265051968905, 0.30609511105682363, -0.19829006265023386, -0.2995239790338515, 0.06006383956462907, -0.26684871536086907, -0.17552999938065608, 0.18960438127396628, -0.03067761240527... |
710.0454 | Search for two photon exchange from $e^+ +e^-\to p+\bar p +\gamma$ data | We look for asymmetries in the angular distributions of events from recent
data on $e^+ +e^-\to p +\bar p +\gamma$ from BABAR collaboration. From first
principles, as the C-invariance of the electromagnetic interaction and the
crossing symmetry, the presence of two-photon exchange would create a forward
backward asym... | hep-ph | we look for asymmetries in the angular distributions of events from recent data on e eto p bar p gamma from babar collaboration from first principles as the cinvariance of the electromagnetic interaction and the crossing symmetry the presence of twophoton exchange would create a forward backward asymmetry in the data t... | [['we', 'look', 'for', 'asymmetries', 'in', 'the', 'angular', 'distributions', 'of', 'events', 'from', 'recent', 'data', 'on', 'e', 'eto', 'p', 'bar', 'p', 'gamma', 'from', 'babar', 'collaboration', 'from', 'first', 'principles', 'as', 'the', 'cinvariance', 'of', 'the', 'electromagnetic', 'interaction', 'and', 'the', '... | [-0.13540113009512425, 0.12421988385648002, -0.11268719292059541, 0.091077552087605, -0.05352824314311147, -0.07501980759343133, 0.06995774522796273, 0.3400594164729118, -0.22585668970644474, -0.2967116208560765, 0.0039389234045520425, -0.33528408474475146, -0.01589564163982868, 0.18522604536917062, 0.03896000162325799... |
710.0455 | Adjoint zero-modes as a tool to understand the Yang-Mills vacuum | The use of adjoint (quasi) zero-modes of the Dirac operator to probe the
Yangs-Mills vacuum has been recently advocated by Gonzalez-Arroyo and Kirchner.
The construction relies on the use of the super-symmetric zero mode which, for
classical configurations, provides a direct estimate of the gauge action
density. In t... | hep-lat | the use of adjoint quasi zeromodes of the dirac operator to probe the yangsmills vacuum has been recently advocated by gonzalezarroyo and kirchner the construction relies on the use of the supersymmetric zero mode which for classical configurations provides a direct estimate of the gauge action density in the lattice i... | [['the', 'use', 'of', 'adjoint', 'quasi', 'zeromodes', 'of', 'the', 'dirac', 'operator', 'to', 'probe', 'the', 'yangsmills', 'vacuum', 'has', 'been', 'recently', 'advocated', 'by', 'gonzalezarroyo', 'and', 'kirchner', 'the', 'construction', 'relies', 'on', 'the', 'use', 'of', 'the', 'supersymmetric', 'zero', 'mode', 'w... | [-0.12717680914426913, 0.17026642506963083, -0.12231660257433698, 0.07249226929878899, -0.047103202676798184, -0.07832598355546426, 0.06081726006755417, 0.3293929526718396, -0.21836956389237908, -0.2579815168289489, 0.10444118775259913, -0.2596269575748174, -0.14217132340699404, 0.14763478987446066, -0.0316139218316340... |
710.0456 | Hawking Radiation via Higher-spin Gauge Anomalies | We give a higher-spin generalization of the anomaly method for the Hawking
radiation from black holes. In the paper arXiv:0710.0453 higher-spin
generalizations of the gauge (and gravitational) anomalies in d=2 were
obtained. By applying these anomalies to black hole physics, we derive the
higher moments of the Hawkin... | hep-th gr-qc | we give a higherspin generalization of the anomaly method for the hawking radiation from black holes in the paper arxiv07100453 higherspin generalizations of the gauge and gravitational anomalies in d2 were obtained by applying these anomalies to black hole physics we derive the higher moments of the hawking fluxes we ... | [['we', 'give', 'a', 'higherspin', 'generalization', 'of', 'the', 'anomaly', 'method', 'for', 'the', 'hawking', 'radiation', 'from', 'black', 'holes', 'in', 'the', 'paper', 'arxiv07100453', 'higherspin', 'generalizations', 'of', 'the', 'gauge', 'and', 'gravitational', 'anomalies', 'in', 'd2', 'were', 'obtained', 'by', ... | [-0.09649601475232178, 0.11785745876471675, -0.07624084975326523, 0.16423222534025886, -0.10426126710242695, -0.09261491790502555, 0.005703302649115878, 0.24465737482976346, -0.12255513827346029, -0.3285436781330241, 0.07249978091937327, -0.32381392642855644, -0.1905831480842261, 0.16920532478714392, -0.068926082362258... |
710.0457 | Conditional observability versus self-duality in a schematic model | In a simple PT-symmetric model we demonstrate that and how the violation of a
reflection symmetry $E_j=-E_{N+1-j}$ of the spectrum (called "self-duality" by
Dunne and Shifman) is connected with the loss of the simplicity of the shape of
the boundary of the domain D of parameters where the Hamiltonian H is
quasi-Hermi... | quant-ph | in a simple ptsymmetric model we demonstrate that and how the violation of a reflection symmetry e_je_n1j of the spectrum called selfduality by dunne and shifman is connected with the loss of the simplicity of the shape of the boundary of the domain d of parameters where the hamiltonian h is quasihermitian ie where all... | [['in', 'a', 'simple', 'ptsymmetric', 'model', 'we', 'demonstrate', 'that', 'and', 'how', 'the', 'violation', 'of', 'a', 'reflection', 'symmetry', 'e_je_n1j', 'of', 'the', 'spectrum', 'called', 'selfduality', 'by', 'dunne', 'and', 'shifman', 'is', 'connected', 'with', 'the', 'loss', 'of', 'the', 'simplicity', 'of', 'th... | [-0.13612539696870213, 0.13347534336528535, -0.05131703755676241, 0.007929060675235371, -0.08164709532570283, -0.1355771350879538, -0.009993785848225452, 0.33965472321389084, -0.2318419109067043, -0.25643173352641574, 0.09080927733576588, -0.26375826216160747, -0.16597008949019393, 0.12248899322175776, -0.0251455112672... |
710.0458 | An alternative heavy Higgs mass limit | After commenting on the present value of the Higgs particle mass from
radiative corrections, we explore the phenomenological implications of an
alternative, non-perturbative renormalization of the scalar sector where the
mass of the Higgs particle does not represent a measure of observable
interactions at the Higgs m... | hep-ph | after commenting on the present value of the higgs particle mass from radiative corrections we explore the phenomenological implications of an alternative nonperturbative renormalization of the scalar sector where the mass of the higgs particle does not represent a measure of observable interactions at the higgs mass s... | [['after', 'commenting', 'on', 'the', 'present', 'value', 'of', 'the', 'higgs', 'particle', 'mass', 'from', 'radiative', 'corrections', 'we', 'explore', 'the', 'phenomenological', 'implications', 'of', 'an', 'alternative', 'nonperturbative', 'renormalization', 'of', 'the', 'scalar', 'sector', 'where', 'the', 'mass', 'o... | [-0.06318320490286819, 0.27889698595660906, -0.09280066250440931, 0.18840760384919122, -0.07679994538027261, -0.1824845830410985, 0.006104343174956739, 0.3143870464126979, -0.18518964120053819, -0.3126356295975191, 0.03947806052165106, -0.24624431543052197, 0.008430073463491032, 0.14939197815256194, 0.04396689723112753... |
710.0459 | Statistical properties of agent-based market area model | One dimensional stylized model taking into account spatial activity of firms
with uniformly distributed customers is proposed. The spatial selling area of
each firm is defined by a short interval cut out from selling space (large
interval). In this representation, the firm size is directly associated with
the size of... | q-fin.GN physics.comp-ph physics.soc-ph | one dimensional stylized model taking into account spatial activity of firms with uniformly distributed customers is proposed the spatial selling area of each firm is defined by a short interval cut out from selling space large interval in this representation the firm size is directly associated with the size of its se... | [['one', 'dimensional', 'stylized', 'model', 'taking', 'into', 'account', 'spatial', 'activity', 'of', 'firms', 'with', 'uniformly', 'distributed', 'customers', 'is', 'proposed', 'the', 'spatial', 'selling', 'area', 'of', 'each', 'firm', 'is', 'defined', 'by', 'a', 'short', 'interval', 'cut', 'out', 'from', 'selling', ... | [-0.11111116124163956, 0.11557446499291348, -0.04568700212666331, 0.07294948504159661, -0.07631998631165503, -0.12995014473642796, 0.11233530309663652, 0.3586136580601156, -0.30401631457450456, -0.2793020179897088, 0.10806592163703188, -0.30824130463528715, -0.028782353076241808, 0.14430226009117428, -0.057843632147685... |
710.046 | Convergence of simple random walks on random discrete trees to Brownian
motion on the continuum random tree | In this article it is shown that the Brownian motion on the continuum random
tree is the scaling limit of the simple random walks on any family of discrete
$n$-vertex ordered graph trees whose search-depth functions converge to the
Brownian excursion as $n\to\infty$. We prove both a quenched version (for
typical real... | math.PR | in this article it is shown that the brownian motion on the continuum random tree is the scaling limit of the simple random walks on any family of discrete nvertex ordered graph trees whose searchdepth functions converge to the brownian excursion as ntoinfty we prove both a quenched version for typical realisations of ... | [['in', 'this', 'article', 'it', 'is', 'shown', 'that', 'the', 'brownian', 'motion', 'on', 'the', 'continuum', 'random', 'tree', 'is', 'the', 'scaling', 'limit', 'of', 'the', 'simple', 'random', 'walks', 'on', 'any', 'family', 'of', 'discrete', 'nvertex', 'ordered', 'graph', 'trees', 'whose', 'searchdepth', 'functions'... | [-0.07755786231562938, 0.19314781308174733, -0.08476823123325546, 0.0655458385777426, -0.012836264739216296, -0.0411496546609116, 0.08400610536360902, 0.3780621575259426, -0.2742858380655345, -0.22630143107980796, 0.12679517723154277, -0.27019725292537017, -0.1458676675425785, 0.17600780921344905, -0.08854241046536061,... |
710.0461 | Momentum of an electromagnetic wave in dielectric media | Almost a hundred years ago, two different expressions were proposed for the
energy--momentum tensor of an electromagnetic wave in a dielectric. Minkowski's
tensor predicted an increase in the linear momentum of the wave on entering a
dielectric medium, whereas Abraham's tensor predicted its decrease. Theoretical
argu... | physics.class-ph physics.optics | almost a hundred years ago two different expressions were proposed for the energymomentum tensor of an electromagnetic wave in a dielectric minkowskis tensor predicted an increase in the linear momentum of the wave on entering a dielectric medium whereas abrahams tensor predicted its decrease theoretical arguments were... | [['almost', 'a', 'hundred', 'years', 'ago', 'two', 'different', 'expressions', 'were', 'proposed', 'for', 'the', 'energymomentum', 'tensor', 'of', 'an', 'electromagnetic', 'wave', 'in', 'a', 'dielectric', 'minkowskis', 'tensor', 'predicted', 'an', 'increase', 'in', 'the', 'linear', 'momentum', 'of', 'the', 'wave', 'on'... | [-0.14045806205709355, 0.14207552592420683, -0.09061046674118176, 0.05614531651575613, -0.14199386907975886, -0.10462392814835156, -0.04694161172614309, 0.3731902803691638, -0.19961121486877645, -0.26663875829923406, 0.08648832572519884, -0.2892699138606553, -0.15461055012224437, 0.14137302866609364, 0.0295839700131462... |
710.0462 | B_K with dynamical overlap fermions | We report on a calculation of $B_K$ with two-flavor dynamical overlap
fermions on a $16^3 \times 32$ lattice at $a\sim 0.12$ fm. The results are
compared with the PQChPT prediction of quark mass dependence. The systematic
errors due to finite volume effects and fixing topology are discussed.
| hep-lat | we report on a calculation of b_k with twoflavor dynamical overlap fermions on a 163 times 32 lattice at asim 012 fm the results are compared with the pqchpt prediction of quark mass dependence the systematic errors due to finite volume effects and fixing topology are discussed | [['we', 'report', 'on', 'a', 'calculation', 'of', 'b_k', 'with', 'twoflavor', 'dynamical', 'overlap', 'fermions', 'on', 'a', '163', 'times', '32', 'lattice', 'at', 'asim', '012', 'fm', 'the', 'results', 'are', 'compared', 'with', 'the', 'pqchpt', 'prediction', 'of', 'quark', 'mass', 'dependence', 'the', 'systematic', '... | [-0.1410476249107655, 0.27302726032212377, -0.04898861093704212, 0.046308534566630075, 0.017099458100076053, -0.02808208903545474, 0.1574320050867948, 0.39447266703590433, -0.1036560670175451, -0.2865424860278739, 0.1152534760098825, -0.35378148666325404, -0.007877949937345816, 0.09354223174221338, -0.00213930052903262... |
710.0463 | Ground-state phase diagram and magnetic properties of a tetramerized
spin-1/2 J_1-J_2 model: BEC of bound magnons and absence of the transverse
magnetization | We study the ground state and the magnetization process of a spin-1/2
$J_1$-$J_2$ model with a plaquette structure by using various methods. For
small inter-plaquette interaction, this model is expected to have a spin-gap
and we computed the first- and the second excitation energies. If the gap of
the lowest excitati... | cond-mat.str-el | we study the ground state and the magnetization process of a spin12 j_1j_2 model with a plaquette structure by using various methods for small interplaquette interaction this model is expected to have a spingap and we computed the first and the second excitation energies if the gap of the lowest excitation closes the c... | [['we', 'study', 'the', 'ground', 'state', 'and', 'the', 'magnetization', 'process', 'of', 'a', 'spin12', 'j_1j_2', 'model', 'with', 'a', 'plaquette', 'structure', 'by', 'using', 'various', 'methods', 'for', 'small', 'interplaquette', 'interaction', 'this', 'model', 'is', 'expected', 'to', 'have', 'a', 'spingap', 'and'... | [-0.19244414788623979, 0.2563377028285766, -0.04072795203431515, 0.0960145668009175, -0.04799117924830051, -0.12324629507009995, 0.07602699344674617, 0.35304914309449914, -0.24656407471523625, -0.2832791202265254, 0.011199066789568923, -0.3034477900690253, -0.11187540929553644, 0.10794983394282912, 0.12891735871609464,... |
710.0464 | Human proofs of identities by Osburn and Schneider | Osburn and Schneider derived several combinatorial identities involving
harmonic numbers using the computer programm Sigma. Here, they are derived by
partial fraction decomposition and creative telescoping.
| math.CO | osburn and schneider derived several combinatorial identities involving harmonic numbers using the computer programm sigma here they are derived by partial fraction decomposition and creative telescoping | [['osburn', 'and', 'schneider', 'derived', 'several', 'combinatorial', 'identities', 'involving', 'harmonic', 'numbers', 'using', 'the', 'computer', 'programm', 'sigma', 'here', 'they', 'are', 'derived', 'by', 'partial', 'fraction', 'decomposition', 'and', 'creative', 'telescoping']] | [-0.10027110318724926, 0.07088463237652412, -0.08405995214931093, 0.12631966847066695, -0.17809740690371165, -0.1264083618298173, 0.03189606198038046, 0.2802894556393417, -0.33517415534991485, -0.3306011012397133, 0.1231732946068335, -0.23863959255126807, -0.22879577671679166, 0.2932834355876996, -0.05346520393728637, ... |
710.0465 | The Loudest Event Statistic: General Formulation, Properties and
Applications | The use of the loudest observed event to generate statistical statements
about rate and strength has become standard in searches for gravitational waves
from compact binaries and pulsars. The Bayesian formulation of the method is
generalized in this paper to allow for uncertainties both in the background
estimate and... | gr-qc | the use of the loudest observed event to generate statistical statements about rate and strength has become standard in searches for gravitational waves from compact binaries and pulsars the bayesian formulation of the method is generalized in this paper to allow for uncertainties both in the background estimate and in... | [['the', 'use', 'of', 'the', 'loudest', 'observed', 'event', 'to', 'generate', 'statistical', 'statements', 'about', 'rate', 'and', 'strength', 'has', 'become', 'standard', 'in', 'searches', 'for', 'gravitational', 'waves', 'from', 'compact', 'binaries', 'and', 'pulsars', 'the', 'bayesian', 'formulation', 'of', 'the', ... | [-0.061923152427278604, 0.07984282734474758, -0.09006734691166247, 0.10001685489148188, -0.07445020503722705, -0.06369512104787506, 0.07593219905751399, 0.341783910516936, -0.22579697606583626, -0.32744115036912264, 0.1244933271377634, -0.28384601796905584, -0.12069622644339688, 0.28491716059282995, -0.0016919920812002... |
710.0466 | Measurement of beta in B decays to charm and charmonium in BABAR | In this article we will review recent BABAR measurements of Unitarity
Triangle angle beta in B meson decays to charm and charmonium.
| hep-ex | in this article we will review recent babar measurements of unitarity triangle angle beta in b meson decays to charm and charmonium | [['in', 'this', 'article', 'we', 'will', 'review', 'recent', 'babar', 'measurements', 'of', 'unitarity', 'triangle', 'angle', 'beta', 'in', 'b', 'meson', 'decays', 'to', 'charm', 'and', 'charmonium']] | [-0.07364773733372038, 0.3240206209011376, -0.09489089950114828, 0.07766415159196847, -0.12798975865271958, -0.18647603275762362, 0.17171121010323986, 0.3082230675288222, -0.18026911196383563, -0.09733619777993723, -0.0980682714143768, -0.4634618710049174, 0.0045923881910064, 0.06234621188857339, 0.009688965552909807, ... |
710.0467 | Inelastically generated solitons and anti-solitons in the perturbed KdV
equation | Under the effect of common perturbations, the multiple-soliton solution of
the KdV equation is transformed into a sum of an elastic and a first-order
inelastic component. The elastic component is a perturbation series, identical
in structure to the perturbed single-soliton solution. It preserves the
soliton-scatterin... | nlin.PS | under the effect of common perturbations the multiplesoliton solution of the kdv equation is transformed into a sum of an elastic and a firstorder inelastic component the elastic component is a perturbation series identical in structure to the perturbed singlesoliton solution it preserves the solitonscattering picture ... | [['under', 'the', 'effect', 'of', 'common', 'perturbations', 'the', 'multiplesoliton', 'solution', 'of', 'the', 'kdv', 'equation', 'is', 'transformed', 'into', 'a', 'sum', 'of', 'an', 'elastic', 'and', 'a', 'firstorder', 'inelastic', 'component', 'the', 'elastic', 'component', 'is', 'a', 'perturbation', 'series', 'iden... | [-0.20423010448743215, 0.1350282664645273, -0.13144000353634186, 0.06799824234906413, -0.07339969502183898, -0.0958482603670965, -0.09027920027488265, 0.3208911531529893, -0.3197039945543497, -0.15514508932400708, 0.05092236240951066, -0.3632935422590409, -0.14520419761003261, 0.12653054263517688, 0.08622514140717256, ... |
710.0468 | Elements of Group Theory | \noindent 1. Generalities\hfil\break 2. Lie groups and Lie
algebras\hfil\break
3. The unitary groups\hfil\break
4. Representations of the SU(n) groups (and of their algebras)\hfil\break
5. The tensor method for unitary groups, and\hb the permutation
group\hfil\break
6. Relativistic invariance. The Lorentz gro... | hep-ph | noindent 1 generalitieshfilbreak 2 lie groups and lie algebrashfilbreak 3 the unitary groupshfilbreak 4 representations of the sun groups and of their algebrashfilbreak 5 the tensor method for unitary groups andhb the permutation grouphfilbreak 6 relativistic invariance the lorentz grouphfilbreak 7 general representati... | [['noindent', '1', 'generalitieshfilbreak', '2', 'lie', 'groups', 'and', 'lie', 'algebrashfilbreak', '3', 'the', 'unitary', 'groupshfilbreak', '4', 'representations', 'of', 'the', 'sun', 'groups', 'and', 'of', 'their', 'algebrashfilbreak', '5', 'the', 'tensor', 'method', 'for', 'unitary', 'groups', 'andhb', 'the', 'per... | [-0.14423805274642432, 0.21853760964213273, -0.06968562794403017, 0.10827778843350899, -0.027507046094307534, -0.12635650877387095, -0.02813478026730128, 0.36673794037256485, -0.26691292302730757, -0.3260390672546167, 0.11616906793549275, -0.2273275006849032, -0.0973042297320297, 0.10338569098773102, 0.0104073303250166... |
710.0469 | Microscopic thickness determination of thin graphite films formed on SiC
from quantized oscillation in reflectivity of low-energy electrons | Low-energy electron microscopy (LEEM) was used to measure the reflectivity of
low-energy electrons from graphitized SiC(0001). The reflectivity shows
distinct quantized oscillations as a function of the electron energy and
graphite thickness. Conduction bands in thin graphite films form discrete
energy levels whose w... | cond-mat.mtrl-sci | lowenergy electron microscopy leem was used to measure the reflectivity of lowenergy electrons from graphitized sic0001 the reflectivity shows distinct quantized oscillations as a function of the electron energy and graphite thickness conduction bands in thin graphite films form discrete energy levels whose wave vector... | [['lowenergy', 'electron', 'microscopy', 'leem', 'was', 'used', 'to', 'measure', 'the', 'reflectivity', 'of', 'lowenergy', 'electrons', 'from', 'graphitized', 'sic0001', 'the', 'reflectivity', 'shows', 'distinct', 'quantized', 'oscillations', 'as', 'a', 'function', 'of', 'the', 'electron', 'energy', 'and', 'graphite', ... | [-0.09825087326698669, 0.22840710111898324, -0.07198425136174601, 0.012334106377058543, -0.008303596241639392, -0.14773066191632062, 0.10308382292750688, 0.45349541428213075, -0.3152175280680456, -0.31744563136950577, -0.08647482496303607, -0.38852199248158104, -0.09624106847303043, 0.16239544820031243, 0.0350585912750... |
710.047 | A minimal set of generators for the ring of multisymmetric functions | The purpose of this article is to give, for any commutative ring A, an
explicit minimal set of generators for the ring of multisymmetric functions
TS^d_A(A[x_1,...,x_r]) as an A-algebra. In characteristic zero, i.e. when A is
an algebra over the rational numbers, a minimal set of generators has been
known since the 1... | math.AC math.AG | the purpose of this article is to give for any commutative ring a an explicit minimal set of generators for the ring of multisymmetric functions tsd_aax_1x_r as an aalgebra in characteristic zero ie when a is an algebra over the rational numbers a minimal set of generators has been known since the 19th century a rather... | [['the', 'purpose', 'of', 'this', 'article', 'is', 'to', 'give', 'for', 'any', 'commutative', 'ring', 'a', 'an', 'explicit', 'minimal', 'set', 'of', 'generators', 'for', 'the', 'ring', 'of', 'multisymmetric', 'functions', 'tsd_aax_1x_r', 'as', 'an', 'aalgebra', 'in', 'characteristic', 'zero', 'ie', 'when', 'a', 'is', '... | [-0.1393255682295545, 0.08590209511021385, -0.06923317838153069, 0.049620991803091416, -0.08654312145440503, -0.10909984034406854, -0.019197358710176134, 0.2945052209121988, -0.2574776446526038, -0.2624599395636865, 0.11017068941517674, -0.23948016832582653, -0.13785817575185222, 0.25721796913483636, -0.121598835389298... |
710.0471 | Non-perturbative improvement of nHYP smeared Wilson fermions | Using Schroedinger functional techniques, we determine the coefficient of the
clover term necessary for non-perturbative O(a) improvement of hypercubic
smeared Wilson fermions on a quenched plaquette action background. Unlike for
unsmeared Wilson fermions, the resulting clover coefficients are close to the
tree-level... | hep-lat | using schroedinger functional techniques we determine the coefficient of the clover term necessary for nonperturbative oa improvement of hypercubic smeared wilson fermions on a quenched plaquette action background unlike for unsmeared wilson fermions the resulting clover coefficients are close to the treelevel value ev... | [['using', 'schroedinger', 'functional', 'techniques', 'we', 'determine', 'the', 'coefficient', 'of', 'the', 'clover', 'term', 'necessary', 'for', 'nonperturbative', 'oa', 'improvement', 'of', 'hypercubic', 'smeared', 'wilson', 'fermions', 'on', 'a', 'quenched', 'plaquette', 'action', 'background', 'unlike', 'for', 'un... | [-0.14565721486431005, 0.24890186057300934, -0.06675721900259603, 0.08306656310807413, -0.02985041595495014, -0.1453038214274974, 0.09319087559593592, 0.417343787292936, -0.09883658353016893, -0.26455370081004814, 0.08234717343836578, -0.30953109214332564, -0.07870036423373133, 0.09906638088399794, 0.015238499630298188... |
710.0472 | Ernst equation and spheroidal coordinates with a cosmological constant
term | We discuss solution generating techniques treating stationary and axially
symmetric metrics in the presence of a cosmological constant. Using the
recently found extended form of Ernst's complex equation, which takes into
account the cosmological constant term, we propose an extension of spheroidal
coordinates adapted... | gr-qc hep-th | we discuss solution generating techniques treating stationary and axially symmetric metrics in the presence of a cosmological constant using the recently found extended form of ernsts complex equation which takes into account the cosmological constant term we propose an extension of spheroidal coordinates adapted to as... | [['we', 'discuss', 'solution', 'generating', 'techniques', 'treating', 'stationary', 'and', 'axially', 'symmetric', 'metrics', 'in', 'the', 'presence', 'of', 'a', 'cosmological', 'constant', 'using', 'the', 'recently', 'found', 'extended', 'form', 'of', 'ernsts', 'complex', 'equation', 'which', 'takes', 'into', 'accoun... | [-0.1584785120561719, 0.09804641676128086, -0.08041453036324432, 0.08468445506878197, -0.08553197664829591, -0.1820673697666886, -0.04806680739857257, 0.3420086643037697, -0.18826523621488983, -0.24391813206796845, 0.08556409753873595, -0.22916429189499468, -0.14683583061366032, 0.09804827742433796, -0.0152959299720047... |
710.0473 | Reply to 'Difficulty in the Fermi-Liquid-Based Theory for the In-Plane
Magnetic Anisotropy in Untwinned High-$T_c$ Superconductors' | A Reply to the Comment by Hou-Jun Zhao and Jun Li
| cond-mat.supr-con cond-mat.str-el | a reply to the comment by houjun zhao and jun li | [['a', 'reply', 'to', 'the', 'comment', 'by', 'houjun', 'zhao', 'and', 'jun', 'li']] | [-0.08158231005072594, 0.0883157230913639, 0.018560294667258857, -0.019534672424197198, -0.1480669157579541, -0.1963637144770473, 0.2610956639051437, 0.19838393446989358, -0.10118430033326149, -0.3721160177141428, 0.0032664118334650993, -0.3602406833320856, -0.22424337826669216, 0.019931719452142716, -0.287891402747482... |
710.0474 | Fractional dynamical systems defined on fractional jet bundle and
applications in economics | Using Caputo fractional derivative of order $\alpha $ we build the fractional
jet bundle of order $\alpha $ and its main geometrical structures. Defined on
that bundle, some fractional dynamical systems with applications to economics
are studied.
| math.DS math.DG | using caputo fractional derivative of order alpha we build the fractional jet bundle of order alpha and its main geometrical structures defined on that bundle some fractional dynamical systems with applications to economics are studied | [['using', 'caputo', 'fractional', 'derivative', 'of', 'order', 'alpha', 'we', 'build', 'the', 'fractional', 'jet', 'bundle', 'of', 'order', 'alpha', 'and', 'its', 'main', 'geometrical', 'structures', 'defined', 'on', 'that', 'bundle', 'some', 'fractional', 'dynamical', 'systems', 'with', 'applications', 'to', 'economi... | [-0.18513690478035383, 0.04167835821530649, -0.027194398012943564, 0.07726505143301828, -0.17685124331286975, -0.099683593296712, -0.057759497953312734, 0.40472033087696346, -0.2983159466513566, -0.285547821862357, 0.14880384878654565, -0.2507160145789385, -0.17998932301998138, 0.16750868346009937, -0.09854466659682137... |
710.0475 | DFT-based calculation of Coulomb blockade in molecular junction | Quantum transport through single molecules is very sensitive to the strength
of the molecule-electrode contact. When a molecular junction weakly coupled to
external electrodes, charging effects do play an important role (Coulomb
blockade regime). In this regime, the non-equilibrium Green function is usually
substitut... | cond-mat.mes-hall cond-mat.mtrl-sci | quantum transport through single molecules is very sensitive to the strength of the moleculeelectrode contact when a molecular junction weakly coupled to external electrodes charging effects do play an important role coulomb blockade regime in this regime the nonequilibrium green function is usually substituted with ma... | [['quantum', 'transport', 'through', 'single', 'molecules', 'is', 'very', 'sensitive', 'to', 'the', 'strength', 'of', 'the', 'moleculeelectrode', 'contact', 'when', 'a', 'molecular', 'junction', 'weakly', 'coupled', 'to', 'external', 'electrodes', 'charging', 'effects', 'do', 'play', 'an', 'important', 'role', 'coulomb... | [-0.11285276323266275, 0.10501569597870408, -0.10456156431439709, 0.03592112508902973, -0.004167641376199676, -0.18058152545362394, 0.07013337298524269, 0.33865580245429744, -0.21684299559986336, -0.2913257219954163, -0.09504563044360344, -0.27828597089817336, -0.19718318725341655, 0.17461888233929582, -0.0153837507848... |
710.0476 | Vortex topology and the continuum limit of lattice gauge theories | We study the stability of Z_2 topological vortex excitations in d+1
dimensional SU(2) Yang-Mills theory on the lattice at T=0. This is found to
depend on d and on the coupling considered. We discuss the connection with
lattice artifacts causing bulk transitions in the beta_A-beta_F plane and draw
some conclusions reg... | hep-lat | we study the stability of z_2 topological vortex excitations in d1 dimensional su2 yangmills theory on the lattice at t0 this is found to depend on d and on the coupling considered we discuss the connection with lattice artifacts causing bulk transitions in the beta_abeta_f plane and draw some conclusions regarding the... | [['we', 'study', 'the', 'stability', 'of', 'z_2', 'topological', 'vortex', 'excitations', 'in', 'd1', 'dimensional', 'su2', 'yangmills', 'theory', 'on', 'the', 'lattice', 'at', 't0', 'this', 'is', 'found', 'to', 'depend', 'on', 'd', 'and', 'on', 'the', 'coupling', 'considered', 'we', 'discuss', 'the', 'connection', 'wi... | [-0.17094181579471165, 0.184952544015167, -0.06782319547242618, 0.041802112911162634, -0.0268553668034396, -0.10519382555503398, 0.08149245733511634, 0.3676071111112833, -0.18188167997037194, -0.1927795217572046, 0.12651514893514104, -0.3067894550206672, -0.13967406455776654, 0.0683219205820933, -0.008260769528403347, ... |
710.0477 | Gravitational time delay of light for various models of modified gravity | We reexamined the gravitational time delay of light, allowing for various
models of modified gravity. We clarify the dependence of the time delay (and
induced frequency shift) on modified gravity models and investigate how to
distinguish those models, when light propagates in static spherically symmetric
spacetimes. ... | gr-qc astro-ph hep-th | we reexamined the gravitational time delay of light allowing for various models of modified gravity we clarify the dependence of the time delay and induced frequency shift on modified gravity models and investigate how to distinguish those models when light propagates in static spherically symmetric spacetimes thus exp... | [['we', 'reexamined', 'the', 'gravitational', 'time', 'delay', 'of', 'light', 'allowing', 'for', 'various', 'models', 'of', 'modified', 'gravity', 'we', 'clarify', 'the', 'dependence', 'of', 'the', 'time', 'delay', 'and', 'induced', 'frequency', 'shift', 'on', 'modified', 'gravity', 'models', 'and', 'investigate', 'how... | [-0.13438386856088122, 0.19107846712301435, -0.10967142290476324, 0.11227971144896735, -0.0790229389615553, -0.18099994869829206, -0.0014651460070653182, 0.3683374561614504, -0.23551996093929597, -0.33314640989747685, 0.062434651052554774, -0.26266613798706157, -0.11182720740448292, 0.2333153006314349, -0.0267456038977... |
710.0478 | Nonperturbative approach to the quantum Hall bilayer | We develop a nonperturbative approach to the quantum Hall bilayer (QHB) at
\nu=1 using trial wave functions. We predict phases of the QHB for arbitrary
distance d and, our approach, in a dual picture, naturally introduces a new
kind of quasiparticles - neutral fermions. Neutral fermion is a composite of
two merons of... | cond-mat.mes-hall cond-mat.str-el | we develop a nonperturbative approach to the quantum hall bilayer qhb at nu1 using trial wave functions we predict phases of the qhb for arbitrary distance d and our approach in a dual picture naturally introduces a new kind of quasiparticles neutral fermions neutral fermion is a composite of two merons of the same vor... | [['we', 'develop', 'a', 'nonperturbative', 'approach', 'to', 'the', 'quantum', 'hall', 'bilayer', 'qhb', 'at', 'nu1', 'using', 'trial', 'wave', 'functions', 'we', 'predict', 'phases', 'of', 'the', 'qhb', 'for', 'arbitrary', 'distance', 'd', 'and', 'our', 'approach', 'in', 'a', 'dual', 'picture', 'naturally', 'introduce... | [-0.2065392362997885, 0.28146542894956506, -0.08139556163186386, 0.063748199788551, -0.002344499184945776, -0.18107195507296048, 0.064252142630559, 0.29027427526659505, -0.22330412855609114, -0.22841986895177016, -0.03516924607784007, -0.2971072178986517, -0.10102741308450984, 0.08626359625227133, 0.04675428576583553, ... |
710.0479 | Determination of the micromagnetic parameters in (Ga,Mn)As using domain
theory | The magnetic domain structure and magnetic properties of a ferromagnetic
(Ga,Mn)As epilayer with perpendicular magnetic easy-axis are investigated. We
show that, despite strong hysteresis, domain theory at thermodynamical
equilibrium can be used to determine the micromagnetic parameters. Combining
magneto-optical Ker... | cond-mat.mtrl-sci | the magnetic domain structure and magnetic properties of a ferromagnetic gamnas epilayer with perpendicular magnetic easyaxis are investigated we show that despite strong hysteresis domain theory at thermodynamical equilibrium can be used to determine the micromagnetic parameters combining magnetooptical kerr microscop... | [['the', 'magnetic', 'domain', 'structure', 'and', 'magnetic', 'properties', 'of', 'a', 'ferromagnetic', 'gamnas', 'epilayer', 'with', 'perpendicular', 'magnetic', 'easyaxis', 'are', 'investigated', 'we', 'show', 'that', 'despite', 'strong', 'hysteresis', 'domain', 'theory', 'at', 'thermodynamical', 'equilibrium', 'can... | [-0.16315771501695553, 0.19416238084067028, -0.024025629468999065, 0.02140919267517197, -0.14797347406396172, -0.11617853593818106, 0.039517798739265406, 0.4649130048864818, -0.3114270849132931, -0.2828226964920759, 0.03511996622514594, -0.24413395782032019, -0.03644741594197822, 0.2060779251854171, 0.11410943016532686... |
710.048 | Smearing and filtering methods in lattice QCD - a quantitative
comparison | We systematically compare three filtering methods used to extract topological
excitations from lattice gauge configurations, namely smearing, Laplace
filtering and the filtered fermionic topological charge (with chirally improved
fermions). Each of these techniques introduces ambiguities, like its parameter
dependenc... | hep-lat | we systematically compare three filtering methods used to extract topological excitations from lattice gauge configurations namely smearing laplace filtering and the filtered fermionic topological charge with chirally improved fermions each of these techniques introduces ambiguities like its parameter dependence we sho... | [['we', 'systematically', 'compare', 'three', 'filtering', 'methods', 'used', 'to', 'extract', 'topological', 'excitations', 'from', 'lattice', 'gauge', 'configurations', 'namely', 'smearing', 'laplace', 'filtering', 'and', 'the', 'filtered', 'fermionic', 'topological', 'charge', 'with', 'chirally', 'improved', 'fermio... | [-0.11179100731599399, 0.179708818917127, -0.11811742785291492, 0.09939594734036787, -0.07734203959857537, -0.15471668332677588, 0.044531990302361504, 0.43476388741030614, -0.2790656273189763, -0.31234650944613596, 0.03764441247965971, -0.28894129932053725, -0.15936569387982177, 0.15797994972672313, -0.0097229870840568... |
710.0481 | Confinement: $G_2$ group case | The gauge group being centreless, $G_2$ gauge theory is a good laboratory for
studying the role of the centre of the group for colour confinement in
Yang-Mills gauge theories. In this paper, we investigate $G_2$ pure gauge
theory at finite temperature on the lattice. By studying the finite size
scaling of the plaquet... | hep-lat | the gauge group being centreless g_2 gauge theory is a good laboratory for studying the role of the centre of the group for colour confinement in yangmills gauge theories in this paper we investigate g_2 pure gauge theory at finite temperature on the lattice by studying the finite size scaling of the plaquette the poly... | [['the', 'gauge', 'group', 'being', 'centreless', 'g_2', 'gauge', 'theory', 'is', 'a', 'good', 'laboratory', 'for', 'studying', 'the', 'role', 'of', 'the', 'centre', 'of', 'the', 'group', 'for', 'colour', 'confinement', 'in', 'yangmills', 'gauge', 'theories', 'in', 'this', 'paper', 'we', 'investigate', 'g_2', 'pure', '... | [-0.15946002501602236, 0.25095761350454077, -0.12368519319417445, 0.08942743590787837, -0.04120311068468972, -0.08977380276314523, 0.05361071361204315, 0.40246204009990355, -0.13160029169368118, -0.22581500463971965, 0.06738522581903165, -0.2608602142549659, -0.12290983091745722, 0.07968028280884028, 0.0290803904988263... |
710.0482 | Conserving GW scheme for nonequilibrium quantum transport in molecular
contacts | We give a detailed presentation of our recent scheme to include correlation
effects in molecular transport calculations using the GW approximation within
the non-equilibrium Keldysh formalism. We restrict the GW self-energy to the
central region, and describe the leads by density functional theory (DFT). A
minimal ba... | cond-mat.mtrl-sci cond-mat.mes-hall | we give a detailed presentation of our recent scheme to include correlation effects in molecular transport calculations using the gw approximation within the nonequilibrium keldysh formalism we restrict the gw selfenergy to the central region and describe the leads by density functional theory dft a minimal basis of ma... | [['we', 'give', 'a', 'detailed', 'presentation', 'of', 'our', 'recent', 'scheme', 'to', 'include', 'correlation', 'effects', 'in', 'molecular', 'transport', 'calculations', 'using', 'the', 'gw', 'approximation', 'within', 'the', 'nonequilibrium', 'keldysh', 'formalism', 'we', 'restrict', 'the', 'gw', 'selfenergy', 'to'... | [-0.13003267457845555, 0.08258015751179253, -0.0831616741154249, 0.12478720329665138, 0.004113069635391105, -0.10438913972884939, 0.07999758090310231, 0.3563029365481302, -0.23316930351664492, -0.2798121237530978, -0.025195226774309975, -0.2876573186934509, -0.1508379116921947, 0.15558934908793226, 0.022712324684937158... |
710.0483 | Reduction for constrained variational problems on 3D null curves | We consider the optimal control problem for null curves in de Sitter 3-space
defined by a functional which is linear in the curvature of the trajectory. We
show how techniques based on the method of moving frames and exterior
differential systems, coupled with the reduction procedure for systems with a
Lie group of s... | math.DG math-ph math.MP | we consider the optimal control problem for null curves in de sitter 3space defined by a functional which is linear in the curvature of the trajectory we show how techniques based on the method of moving frames and exterior differential systems coupled with the reduction procedure for systems with a lie group of symmet... | [['we', 'consider', 'the', 'optimal', 'control', 'problem', 'for', 'null', 'curves', 'in', 'de', 'sitter', '3space', 'defined', 'by', 'a', 'functional', 'which', 'is', 'linear', 'in', 'the', 'curvature', 'of', 'the', 'trajectory', 'we', 'show', 'how', 'techniques', 'based', 'on', 'the', 'method', 'of', 'moving', 'frame... | [-0.18652569751783804, 0.035691355115960575, -0.11797536586134418, 0.046597345110746355, -0.06462444577718506, -0.09480274807208695, -0.005797261786348237, 0.3358618367991939, -0.255203250543894, -0.2786066690208139, 0.13793418501547813, -0.260757463543701, -0.1857839082053082, 0.23593837425515457, -0.10103877694220156... |
710.0484 | AGN feedback from Jet-ISM/IGM interactions | We study the propagation of relativistic jets originating from AGNs within
the Interstellar/Intergalactic Medium of their host galaxies, and use it to
build a model for the suppression of stellar formation within the expanding
cocoon.
| astro-ph | we study the propagation of relativistic jets originating from agns within the interstellarintergalactic medium of their host galaxies and use it to build a model for the suppression of stellar formation within the expanding cocoon | [['we', 'study', 'the', 'propagation', 'of', 'relativistic', 'jets', 'originating', 'from', 'agns', 'within', 'the', 'interstellarintergalactic', 'medium', 'of', 'their', 'host', 'galaxies', 'and', 'use', 'it', 'to', 'build', 'a', 'model', 'for', 'the', 'suppression', 'of', 'stellar', 'formation', 'within', 'the', 'exp... | [-0.03217906164271491, 0.11134922489789979, -0.08763045083199228, 0.13708140110330921, -0.08083864290799414, 0.01196377414411732, 0.03864116157804217, 0.4243334272876382, -0.18858009661946978, -0.32516725100576876, 0.013383421182100261, -0.2730119021875518, -0.005582392934177603, 0.12480166340912027, 0.0689090860874525... |
710.0485 | Prediction with expert advice for the Brier game | We show that the Brier game of prediction is mixable and find the optimal
learning rate and substitution function for it. The resulting prediction
algorithm is applied to predict results of football and tennis matches. The
theoretical performance guarantee turns out to be rather tight on these data
sets, especially i... | cs.LG | we show that the brier game of prediction is mixable and find the optimal learning rate and substitution function for it the resulting prediction algorithm is applied to predict results of football and tennis matches the theoretical performance guarantee turns out to be rather tight on these data sets especially in the... | [['we', 'show', 'that', 'the', 'brier', 'game', 'of', 'prediction', 'is', 'mixable', 'and', 'find', 'the', 'optimal', 'learning', 'rate', 'and', 'substitution', 'function', 'for', 'it', 'the', 'resulting', 'prediction', 'algorithm', 'is', 'applied', 'to', 'predict', 'results', 'of', 'football', 'and', 'tennis', 'matche... | [-0.05429954102886367, -0.01906083161958446, -0.115512484313636, 0.12933153086499768, -0.06174596445240333, -0.1301213089392473, 0.13784833025124113, 0.4176181898278705, -0.23364036583925707, -0.3307838641912124, 0.10322605603634995, -0.3248795841078637, -0.18624828037632218, 0.22932996348304263, -0.11880356411181264, ... |
710.0486 | Phase-Space Coalescence for heavy and light quarks at RHIC | We review the application and successes of a phase-space coalescence plus
fragmentation model that has been applied for hadronization at RHIC. The
physical concept is discussed together with the practical implementation. The
robustness of main predictions is reviewed together with several open issues
like relevance o... | nucl-th | we review the application and successes of a phasespace coalescence plus fragmentation model that has been applied for hadronization at rhic the physical concept is discussed together with the practical implementation the robustness of main predictions is reviewed together with several open issues like relevance of thr... | [['we', 'review', 'the', 'application', 'and', 'successes', 'of', 'a', 'phasespace', 'coalescence', 'plus', 'fragmentation', 'model', 'that', 'has', 'been', 'applied', 'for', 'hadronization', 'at', 'rhic', 'the', 'physical', 'concept', 'is', 'discussed', 'together', 'with', 'the', 'practical', 'implementation', 'the', ... | [-0.08091213501253981, 0.1832109637742425, -0.10741993503783036, 0.11724012893952292, -0.046093100796879075, -0.08803946577173508, -0.011605735730241847, 0.31676532088974374, -0.18701748961559783, -0.24424289416573527, 0.06734669581630531, -0.30330332291576967, -0.054659653587243805, 0.15085652850878736, 0.042719156044... |
710.0487 | Lattice supersymmetry in 1D with two supercharges | A consistent formulation of a fully supersymmetric theory on the lattice has
been a long standing challenge. In recent years there has been a renewed
interest on this problem with different approaches. At the basis of the
formulation we present in the following there is the Dirac-Kahler twisting
procedure, which was ... | hep-lat | a consistent formulation of a fully supersymmetric theory on the lattice has been a long standing challenge in recent years there has been a renewed interest on this problem with different approaches at the basis of the formulation we present in the following there is the dirackahler twisting procedure which was propos... | [['a', 'consistent', 'formulation', 'of', 'a', 'fully', 'supersymmetric', 'theory', 'on', 'the', 'lattice', 'has', 'been', 'a', 'long', 'standing', 'challenge', 'in', 'recent', 'years', 'there', 'has', 'been', 'a', 'renewed', 'interest', 'on', 'this', 'problem', 'with', 'different', 'approaches', 'at', 'the', 'basis', ... | [-0.0884363177861762, 0.09875364722846416, -0.07140368575135758, 0.040061817474939955, -0.029586331743369068, -0.13055917512004575, -0.022406332932102185, 0.37139591635407315, -0.19943938676969727, -0.24434305305349763, 0.11151219779234109, -0.25246529884137, -0.18281778197843526, 0.16569859134809425, -0.06579638760118... |
710.0488 | On the ratio of string tensions in the 3D Z_4 lattice gauge theory | It was recently pointed out that simple scaling properties of Polyakov
correlation functions of gauge systems in the confining phase suggest that the
ratios of k-string tensions in the low temperature region is constant up to
terms of order T^3. Here we argue that, at least in a three-dimensional Z_4
gauge model, the... | hep-lat hep-th | it was recently pointed out that simple scaling properties of polyakov correlation functions of gauge systems in the confining phase suggest that the ratios of kstring tensions in the low temperature region is constant up to terms of order t3 here we argue that at least in a threedimensional z_4 gauge model the above r... | [['it', 'was', 'recently', 'pointed', 'out', 'that', 'simple', 'scaling', 'properties', 'of', 'polyakov', 'correlation', 'functions', 'of', 'gauge', 'systems', 'in', 'the', 'confining', 'phase', 'suggest', 'that', 'the', 'ratios', 'of', 'kstring', 'tensions', 'in', 'the', 'low', 'temperature', 'region', 'is', 'constant... | [-0.14243263073149137, 0.19907894809284699, -0.07220137770006356, 0.0400041154413581, 0.010027236923633609, -0.11750672055738202, 0.0387419829009256, 0.37662842017986503, -0.19485325267305598, -0.26494884317313944, 0.07753844177932478, -0.2872798074774134, -0.15659215833390286, 0.13533145642577438, 0.027414379216679663... |
710.0489 | P- and D-wave spin-orbit splittings in heavy-light mesons | This is a summary of a detailed study of heavy-light meson excited state
energies. Our lattice measurements include both radial and orbital excitations.
Particular attention is paid to the spin-orbit splittings, to see which one of
the states (for a given angular momentum L) has the lower energy. In nature the
closes... | hep-lat | this is a summary of a detailed study of heavylight meson excited state energies our lattice measurements include both radial and orbital excitations particular attention is paid to the spinorbit splittings to see which one of the states for a given angular momentum l has the lower energy in nature the closest equivale... | [['this', 'is', 'a', 'summary', 'of', 'a', 'detailed', 'study', 'of', 'heavylight', 'meson', 'excited', 'state', 'energies', 'our', 'lattice', 'measurements', 'include', 'both', 'radial', 'and', 'orbital', 'excitations', 'particular', 'attention', 'is', 'paid', 'to', 'the', 'spinorbit', 'splittings', 'to', 'see', 'whic... | [-0.12901629701299572, 0.19765551824486632, -0.08302036290934801, 0.094587467060874, -0.09928824401449883, -0.1310528395590426, 0.08116102018447101, 0.33518659708828763, -0.17201999816294203, -0.2371738145994986, -0.0029206019090274454, -0.30032720798696794, -0.00964363372413677, 0.12035102708179546, 0.0537655777030292... |
710.049 | Dynamics of galactic nuclei: Mass segregation and collisions | Massive black holes (MBHs) with a mass below ~ 1e7 Msun are likely to reside
at the centre of dense stellar nuclei shaped by 2-body relaxation, close
interactions with the MBH and direct collisions. In this contribution, we
stress the role of mass segregation of stellar-mass black holes into the
innermost tenths of a... | astro-ph | massive black holes mbhs with a mass below 1e7 msun are likely to reside at the centre of dense stellar nuclei shaped by 2body relaxation close interactions with the mbh and direct collisions in this contribution we stress the role of mass segregation of stellarmass black holes into the innermost tenths of a parsec and... | [['massive', 'black', 'holes', 'mbhs', 'with', 'a', 'mass', 'below', '1e7', 'msun', 'are', 'likely', 'to', 'reside', 'at', 'the', 'centre', 'of', 'dense', 'stellar', 'nuclei', 'shaped', 'by', '2body', 'relaxation', 'close', 'interactions', 'with', 'the', 'mbh', 'and', 'direct', 'collisions', 'in', 'this', 'contribution... | [-0.08862386042705904, 0.18126921681687236, -0.03370515092720803, 0.15744807049841023, -0.04608934730267487, 0.012799931176675435, 0.02845096847233482, 0.328125674635745, -0.14538571574032688, -0.3660952110703175, -0.01715628176073854, -0.36734441581826943, 0.050381715063196726, 0.15412180778236154, 0.00397623798403984... |
710.0491 | Analysis of Linear Difference Schemes in the Sparse Grid Combination
Technique | Sparse grids are tailored to the approximation of smooth high-dimensional
functions. On a $d$-dimensional tensor product space, the number of grid points
is $N = \mathcal O(h^{-1} |\log h|^{d-1})$, where $h$ is a mesh parameter. The
so-called combination technique, based on hierarchical decomposition and
extrapolatio... | math.NA | sparse grids are tailored to the approximation of smooth highdimensional functions on a ddimensional tensor product space the number of grid points is n mathcal oh1 log hd1 where h is a mesh parameter the socalled combination technique based on hierarchical decomposition and extrapolation requires specific multivariate... | [['sparse', 'grids', 'are', 'tailored', 'to', 'the', 'approximation', 'of', 'smooth', 'highdimensional', 'functions', 'on', 'a', 'ddimensional', 'tensor', 'product', 'space', 'the', 'number', 'of', 'grid', 'points', 'is', 'n', 'mathcal', 'oh1', 'log', 'hd1', 'where', 'h', 'is', 'a', 'mesh', 'parameter', 'the', 'socalle... | [-0.1142100007891075, 0.011891497788415188, -0.04939590095493354, 0.06132986384092651, -0.06056471743310491, -0.13578957417702073, 0.05809573755240101, 0.3520736197671412, -0.2668350537658849, -0.2780362851550116, 0.1588391063095626, -0.2513045418043539, -0.0943155601363335, 0.21048433296719418, -0.09609712271036155, 0... |
710.0492 | On the second Paneitz-Branson invariant | We define the second Paneitz-Branson operator on a compact Einsteinian
manifold of dimension $n\geq 5$ and we give sufficient conditions that make it
attained.
| math.DG math.AP | we define the second paneitzbranson operator on a compact einsteinian manifold of dimension ngeq 5 and we give sufficient conditions that make it attained | [['we', 'define', 'the', 'second', 'paneitzbranson', 'operator', 'on', 'a', 'compact', 'einsteinian', 'manifold', 'of', 'dimension', 'ngeq', '5', 'and', 'we', 'give', 'sufficient', 'conditions', 'that', 'make', 'it', 'attained']] | [-0.17499312463526925, 0.08266060970102747, -0.08023592080765714, 0.11679952552852531, -0.1052104136615526, -0.2085785103457359, -0.007589941398085405, 0.3724696758436039, -0.1643184502609074, -0.21932811083388515, 0.17126957819952318, -0.19115466608976325, -0.18079949117964134, 0.16878533634978035, -0.1237213173493122... |
710.0493 | Planar trees, free nonassociative algebras, invariants, and elliptic
integrals | We consider absolutely free nonassociative algebras and, more generally,
absolutely free algebras with (maybe infinitely) many multilinear operations.
Such algebras are described in terms of labeled reduced planar rooted trees.
This allows to apply combinatorial techniques to study their Hilbert series and
the asympt... | math.RA math.CO | we consider absolutely free nonassociative algebras and more generally absolutely free algebras with maybe infinitely many multilinear operations such algebras are described in terms of labeled reduced planar rooted trees this allows to apply combinatorial techniques to study their hilbert series and the asymptotics of... | [['we', 'consider', 'absolutely', 'free', 'nonassociative', 'algebras', 'and', 'more', 'generally', 'absolutely', 'free', 'algebras', 'with', 'maybe', 'infinitely', 'many', 'multilinear', 'operations', 'such', 'algebras', 'are', 'described', 'in', 'terms', 'of', 'labeled', 'reduced', 'planar', 'rooted', 'trees', 'this'... | [-0.18063889422747134, 0.1296286576255052, -0.07658062930805264, 0.08668776784885537, -0.06721997642544685, -0.09808039445154093, -0.0426469382657497, 0.36335648928803427, -0.36341572665367966, -0.20045943501991806, 0.14565870028541045, -0.271133026278996, -0.12575161789923353, 0.24106344718624045, -0.11772676591450969... |
710.0494 | The z=0.8 precursors of today's bulges | We study the color structure of disk galaxies in the Groth strip at redshifts
0.1<z<1.2. Our aim is to test formation models in which bulges form
before/after the disk. We find smooth color distributions with gentle outward
blueing across the galaxy image: bulges are not distinctly redder than their
disks; and bulge ... | astro-ph | we study the color structure of disk galaxies in the groth strip at redshifts 01z12 our aim is to test formation models in which bulges form beforeafter the disk we find smooth color distributions with gentle outward blueing across the galaxy image bulges are not distinctly redder than their disks and bulge colors stro... | [['we', 'study', 'the', 'color', 'structure', 'of', 'disk', 'galaxies', 'in', 'the', 'groth', 'strip', 'at', 'redshifts', '01z12', 'our', 'aim', 'is', 'to', 'test', 'formation', 'models', 'in', 'which', 'bulges', 'form', 'beforeafter', 'the', 'disk', 'we', 'find', 'smooth', 'color', 'distributions', 'with', 'gentle', '... | [-0.02619998847755293, 0.11396959434496239, -0.14213988772050168, 0.14763445149971327, -0.06999759913111726, -0.0651244535149696, -0.03444528074081366, 0.5084438485714297, -0.10991508808607857, -0.3410088425075325, 0.022252123735961506, -0.2998659293865785, -0.005028409217872346, 0.14367146262084135, -0.121136707762586... |
710.0495 | Lineshape distortion in a nonlinear auto-oscillator near generation
threshold: Application to spin-torque nano-oscillators | The lineshape in an auto-oscillator with a large nonlinear frequency shift in
the presence of thermal noise is calculated. Near the generation threshold,
this lineshape becomes strongly non-Lorentzian, broadened, and asymmetric. A
Lorentzian lineshape is recovered far below and far above threshold, which
suggests tha... | cond-mat.mtrl-sci | the lineshape in an autooscillator with a large nonlinear frequency shift in the presence of thermal noise is calculated near the generation threshold this lineshape becomes strongly nonlorentzian broadened and asymmetric a lorentzian lineshape is recovered far below and far above threshold which suggests that lineshap... | [['the', 'lineshape', 'in', 'an', 'autooscillator', 'with', 'a', 'large', 'nonlinear', 'frequency', 'shift', 'in', 'the', 'presence', 'of', 'thermal', 'noise', 'is', 'calculated', 'near', 'the', 'generation', 'threshold', 'this', 'lineshape', 'becomes', 'strongly', 'nonlorentzian', 'broadened', 'and', 'asymmetric', 'a'... | [-0.15967244979487183, 0.16861916399027585, -0.06357054792426746, 0.07471627081223928, -0.07267459766829715, -0.15586594648330526, 0.00349200058639433, 0.36916213277179527, -0.2555295465349713, -0.24119522107545943, 0.015126437643844196, -0.2897242057301542, -0.16993268032777398, 0.2029314347104553, -0.0013313834856757... |
710.0496 | Microscopic mechanisms of spin-dependent electric polarization in 3d
oxides | We address a systematic microscopic theory of spin-dependent electric
polarization in 3d oxides starting with a generic three-site two-hole cluster.
A perturbation scheme realistic for 3d oxides is applied which implies the
quenching of orbital moments by low-symmetry crystal field, strong intra-atomic
correlations, ... | cond-mat.str-el cond-mat.mtrl-sci | we address a systematic microscopic theory of spindependent electric polarization in 3d oxides starting with a generic threesite twohole cluster a perturbation scheme realistic for 3d oxides is applied which implies the quenching of orbital moments by lowsymmetry crystal field strong intraatomic correlations the dptran... | [['we', 'address', 'a', 'systematic', 'microscopic', 'theory', 'of', 'spindependent', 'electric', 'polarization', 'in', '3d', 'oxides', 'starting', 'with', 'a', 'generic', 'threesite', 'twohole', 'cluster', 'a', 'perturbation', 'scheme', 'realistic', 'for', '3d', 'oxides', 'is', 'applied', 'which', 'implies', 'the', 'q... | [-0.1894153224860432, 0.18628514190332163, -0.008424777008271475, 0.09605917591926567, -0.07024216149404323, -0.10326431494661802, 0.011534878171280214, 0.3484126307914476, -0.2771423295744956, -0.28326512059103026, -0.05179061780754048, -0.299623232160648, -0.10784210003376436, 0.10670341876931756, 0.0708556127392774,... |
710.0497 | A Joint Search for Gravitational Wave Bursts with AURIGA and LIGO | The first simultaneous operation of the AURIGA detector and the LIGO
observatory was an opportunity to explore real data, joint analysis methods
between two very different types of gravitational wave detectors: resonant bars
and interferometers. This paper describes a coincident gravitational wave burst
search, where... | gr-qc | the first simultaneous operation of the auriga detector and the ligo observatory was an opportunity to explore real data joint analysis methods between two very different types of gravitational wave detectors resonant bars and interferometers this paper describes a coincident gravitational wave burst search where data ... | [['the', 'first', 'simultaneous', 'operation', 'of', 'the', 'auriga', 'detector', 'and', 'the', 'ligo', 'observatory', 'was', 'an', 'opportunity', 'to', 'explore', 'real', 'data', 'joint', 'analysis', 'methods', 'between', 'two', 'very', 'different', 'types', 'of', 'gravitational', 'wave', 'detectors', 'resonant', 'bar... | [-0.13874083505471319, 0.0811149362435249, -0.042625300601244934, 0.08577127321483782, -0.05435154524048112, -0.06721369240695582, 0.06463974606393824, 0.3635460125831758, -0.21235981339391338, -0.3554242830702065, 0.0932496449419765, -0.3219452806649738, -0.11522478677229397, 0.22871132933616226, 0.006050326408655275,... |
710.0498 | Screening at finite temperature and density | We present lattice QCD results on heavy quark free energies, extract from its
temperature dependence entropy and internal energy contributions, and discuss
the onset of medium effects that lead to screening of static quark-antiquark
sources in a thermal medium. Most results are obtained in (2+1)-flavour QCD on
a line... | hep-lat hep-ph | we present lattice qcd results on heavy quark free energies extract from its temperature dependence entropy and internal energy contributions and discuss the onset of medium effects that lead to screening of static quarkantiquark sources in a thermal medium most results are obtained in 21flavour qcd on a line of consta... | [['we', 'present', 'lattice', 'qcd', 'results', 'on', 'heavy', 'quark', 'free', 'energies', 'extract', 'from', 'its', 'temperature', 'dependence', 'entropy', 'and', 'internal', 'energy', 'contributions', 'and', 'discuss', 'the', 'onset', 'of', 'medium', 'effects', 'that', 'lead', 'to', 'screening', 'of', 'static', 'qua... | [-0.044846058319101934, 0.2137382067355913, -0.12107159153164662, 0.07507937085651553, -0.03949536118157131, -0.034273429072855674, 0.08316985884148474, 0.36475874631444816, -0.1391538695357836, -0.2723390829086918, 0.045876357297547465, -0.324984253278559, -0.036389190463598856, 0.13903780840337276, 0.0836028325150615... |
710.0499 | A silicate disk in the heart of the Ant | We aim at getting high spatial resolution information on the dusty core of
bipolar planetary nebulae to directly constrain the shaping process. Methods:
We present observations of the dusty core of the extreme bipolar planetary
nebula Menzel 3 (Mz 3, Hen 2-154, the Ant) taken with the mid-infrared
interferometer MIDI... | astro-ph | we aim at getting high spatial resolution information on the dusty core of bipolar planetary nebulae to directly constrain the shaping process methods we present observations of the dusty core of the extreme bipolar planetary nebula menzel 3 mz 3 hen 2154 the ant taken with the midinfrared interferometer midivlti and t... | [['we', 'aim', 'at', 'getting', 'high', 'spatial', 'resolution', 'information', 'on', 'the', 'dusty', 'core', 'of', 'bipolar', 'planetary', 'nebulae', 'to', 'directly', 'constrain', 'the', 'shaping', 'process', 'methods', 'we', 'present', 'observations', 'of', 'the', 'dusty', 'core', 'of', 'the', 'extreme', 'bipolar', ... | [-0.11026775392457702, 0.11054106083454758, -0.07294888940095058, 0.029793992892134483, -0.06378271598324953, -0.09417658894946623, 0.002809379815194264, 0.4202996167283997, -0.21075446810123052, -0.3487756836750843, 0.0873286672226452, -0.2519456376444619, -0.035392096892596696, 0.15150483598743725, -0.040741790270538... |
710.05 | Infrared problem and spatially local observables in electrodynamics | An algebra previously proposed as an asymptotic field structure in
electrodynamics is considered in respect of localization properties of fields.
Fields are 'spatially local' -- localized in regions resulting as unions of two
intersecting (solid) lightcones: a future- and a past-lightcone. This
localization remains i... | hep-th math-ph math.MP | an algebra previously proposed as an asymptotic field structure in electrodynamics is considered in respect of localization properties of fields fields are spatially local localized in regions resulting as unions of two intersecting solid lightcones a future and a pastlightcone this localization remains in concord with... | [['an', 'algebra', 'previously', 'proposed', 'as', 'an', 'asymptotic', 'field', 'structure', 'in', 'electrodynamics', 'is', 'considered', 'in', 'respect', 'of', 'localization', 'properties', 'of', 'fields', 'fields', 'are', 'spatially', 'local', 'localized', 'in', 'regions', 'resulting', 'as', 'unions', 'of', 'two', 'i... | [-0.15301358622188369, 0.1435809653089319, -0.07185142676556303, 0.061684791280347255, -0.04562354709212017, -0.08656883659842675, -0.04087785207941848, 0.35098934793714637, -0.27524062076343164, -0.24295134289923714, 0.09221256081320306, -0.2644836521877717, -0.1149973938421857, 0.17916001558494105, -0.044177997817275... |
710.0501 | Form factors of boundary fields for A(2)-affine Toda field theory | In this paper we carry out the boundary form factor program for the
A(2)-affine Toda field theory at the self-dual point. The latter is an
integrable model consisting of a pair of particles which are conjugated to each
other and possessing two bound states resulting from the scattering processes 1
+1 -> 2 and 2+2-> 1... | hep-th | in this paper we carry out the boundary form factor program for the a2affine toda field theory at the selfdual point the latter is an integrable model consisting of a pair of particles which are conjugated to each other and possessing two bound states resulting from the scattering processes 1 1 2 and 22 1 we obtain sol... | [['in', 'this', 'paper', 'we', 'carry', 'out', 'the', 'boundary', 'form', 'factor', 'program', 'for', 'the', 'a2affine', 'toda', 'field', 'theory', 'at', 'the', 'selfdual', 'point', 'the', 'latter', 'is', 'an', 'integrable', 'model', 'consisting', 'of', 'a', 'pair', 'of', 'particles', 'which', 'are', 'conjugated', 'to'... | [-0.1172597111417697, 0.13270975354299971, -0.04280320801772177, 0.044476664080642735, -0.0342133614861478, -0.15070826444201746, -0.016912057124472295, 0.2877854710480628, -0.25831884938793687, -0.298135265822594, 0.11478672431907258, -0.29995142563890953, -0.1302175157237798, 0.19216255938473087, 0.03738591644124916,... |
710.0502 | Dynamical resonances and SSF singularities for a magnetic Schroedinger
operator | We consider the Hamiltonian $H$ of a 3D spinless non-relativistic quantum
particle subject to parallel constant magnetic and non-constant electric field.
The operator $H$ has infinitely many eigenvalues of infinite multiplicity
embedded in its continuous spectrum. We perturb $H$ by appropriate scalar
potentials $V$ a... | math.SP | we consider the hamiltonian h of a 3d spinless nonrelativistic quantum particle subject to parallel constant magnetic and nonconstant electric field the operator h has infinitely many eigenvalues of infinite multiplicity embedded in its continuous spectrum we perturb h by appropriate scalar potentials v and investigate... | [['we', 'consider', 'the', 'hamiltonian', 'h', 'of', 'a', '3d', 'spinless', 'nonrelativistic', 'quantum', 'particle', 'subject', 'to', 'parallel', 'constant', 'magnetic', 'and', 'nonconstant', 'electric', 'field', 'the', 'operator', 'h', 'has', 'infinitely', 'many', 'eigenvalues', 'of', 'infinite', 'multiplicity', 'emb... | [-0.15461110182480725, 0.1475222374714053, -0.06522719535793786, 0.06745447922491608, -0.05378089828914261, -0.141871483127914, 0.02231589832383561, 0.3543444568287054, -0.26014993935780917, -0.2381806470462776, 0.06977447579863597, -0.28102723589128725, -0.08968606495221898, 0.12906523278997317, 0.007603596339903806, ... |
710.0503 | Unified Approach to the Large-Signal and High-Frequency Theory of
$p-n$-Junctions | Spectral approach to the charge carrier transport in $p-n$-junctions has
allowed us to revise the theoretical results relating to large signal operation
of the junction to make them valid for both the low and high frequencies
ranges. The spectral composition of the external circuit current includes both
the DC and AC... | cond-mat.mtrl-sci | spectral approach to the charge carrier transport in pnjunctions has allowed us to revise the theoretical results relating to large signal operation of the junction to make them valid for both the low and high frequencies ranges the spectral composition of the external circuit current includes both the dc and ac compon... | [['spectral', 'approach', 'to', 'the', 'charge', 'carrier', 'transport', 'in', 'pnjunctions', 'has', 'allowed', 'us', 'to', 'revise', 'the', 'theoretical', 'results', 'relating', 'to', 'large', 'signal', 'operation', 'of', 'the', 'junction', 'to', 'make', 'them', 'valid', 'for', 'both', 'the', 'low', 'and', 'high', 'fr... | [-0.11812128307621764, 0.09810738339007873, -0.07489524154883365, 0.021083682817002028, -0.09382378593613597, -0.12242630296184318, 0.0615025794492913, 0.3665116765900798, -0.2362264252956147, -0.300850464079691, 0.04122573360598282, -0.2547478429001311, -0.06381029969324237, 0.22053387993541748, 0.004078618963451489, ... |
710.0504 | Wilson Loop in Classical Lattice Gauge Theory and the Thermal Width of
Heavy Quarkonium | We present an estimate for the imaginary part of the recently introduced
finite temperature real-time static potential. It can be extracted from the
time evolution of the Wilson loop in classical lattice gauge theory. The
real-time static potential determines, through a Schroedinger-type equation and
a subsequent Fou... | hep-lat | we present an estimate for the imaginary part of the recently introduced finite temperature realtime static potential it can be extracted from the time evolution of the wilson loop in classical lattice gauge theory the realtime static potential determines through a schroedingertype equation and a subsequent fouriertran... | [['we', 'present', 'an', 'estimate', 'for', 'the', 'imaginary', 'part', 'of', 'the', 'recently', 'introduced', 'finite', 'temperature', 'realtime', 'static', 'potential', 'it', 'can', 'be', 'extracted', 'from', 'the', 'time', 'evolution', 'of', 'the', 'wilson', 'loop', 'in', 'classical', 'lattice', 'gauge', 'theory', '... | [-0.0800907511917082, 0.12696510334596192, -0.16525169142960816, 0.07590571332765722, -0.03544949032312752, -0.07696710585150868, 0.03837662578249971, 0.3565122874603532, -0.22693471730975756, -0.24587884753000464, 0.09965077692364481, -0.2818814191710332, -0.130030231676787, 0.16693766013687028, 0.03233075402034768, 0... |
710.0505 | 1/N Expansion of the 2D CP^{N-1} Model on Non(anti)commutative
Superspace | We study UV properties of the two-dimensional supersymmetric CP^{N-1} model
on non(anti)commutative superspace. We show that the deformed model has the
same UV property as the ordinary model in the leading order of 1/N and the
deformation give rise to UV divergence which cannot be dealt with in the
next-to-leading or... | hep-th | we study uv properties of the twodimensional supersymmetric cpn1 model on nonanticommutative superspace we show that the deformed model has the same uv property as the ordinary model in the leading order of 1n and the deformation give rise to uv divergence which cannot be dealt with in the nexttoleading order | [['we', 'study', 'uv', 'properties', 'of', 'the', 'twodimensional', 'supersymmetric', 'cpn1', 'model', 'on', 'nonanticommutative', 'superspace', 'we', 'show', 'that', 'the', 'deformed', 'model', 'has', 'the', 'same', 'uv', 'property', 'as', 'the', 'ordinary', 'model', 'in', 'the', 'leading', 'order', 'of', '1n', 'and',... | [-0.037285746254313454, 0.11781177001718718, -0.09156359689166912, 0.06556905714723353, -0.05021213442803575, -0.09464450590670682, -0.08670485743249838, 0.3873589653163575, -0.20490175510685033, -0.24311016771781185, 0.06920137651300487, -0.30822927311349374, -0.1778539832896338, 0.08374708169587673, -0.07337425957218... |
710.0506 | Spitzer View of Lyman Break Galaxies | Using a combination of deep MID-IR observations obtained by IRAC, MIPS and
IRS on board Spitzer we investigate the MID-IR properties of Lyman Break
Galaxies (LBGs) at z~3, establish a better understanding of their nature and
attempt a complete characterisation of the population. With deep mid-infrared
and optical obs... | astro-ph | using a combination of deep midir observations obtained by irac mips and irs on board spitzer we investigate the midir properties of lyman break galaxies lbgs at z3 establish a better understanding of their nature and attempt a complete characterisation of the population with deep midinfrared and optical observations o... | [['using', 'a', 'combination', 'of', 'deep', 'midir', 'observations', 'obtained', 'by', 'irac', 'mips', 'and', 'irs', 'on', 'board', 'spitzer', 'we', 'investigate', 'the', 'midir', 'properties', 'of', 'lyman', 'break', 'galaxies', 'lbgs', 'at', 'z3', 'establish', 'a', 'better', 'understanding', 'of', 'their', 'nature',... | [0.017718556084636055, 0.06010492435243356, -0.07969598959103545, 0.1062721225171827, -0.09132503540164269, -0.04178787652266825, 0.08038848399570803, 0.5236207604067536, -0.11985018084325441, -0.378392932550391, 0.01667988245636679, -0.322762014828168, -0.03714200777296976, 0.12902670635644095, -0.030829076612050213, ... |
710.0507 | Results related to generalizations of Hilbert's non-immersibility
theorem for the hyperbolic plane | We discuss generalizations of the well-known theorem of Hilbert that there is
no complete isometric immersion of the hyperbolic plane into Euclidean 3-space.
We show that this problem is expressed very naturally as the question of the
existence of certain homotheties of reflective submanifolds of a symmetric
space. A... | math.DG | we discuss generalizations of the wellknown theorem of hilbert that there is no complete isometric immersion of the hyperbolic plane into euclidean 3space we show that this problem is expressed very naturally as the question of the existence of certain homotheties of reflective submanifolds of a symmetric space as such... | [['we', 'discuss', 'generalizations', 'of', 'the', 'wellknown', 'theorem', 'of', 'hilbert', 'that', 'there', 'is', 'no', 'complete', 'isometric', 'immersion', 'of', 'the', 'hyperbolic', 'plane', 'into', 'euclidean', '3space', 'we', 'show', 'that', 'this', 'problem', 'is', 'expressed', 'very', 'naturally', 'as', 'the', ... | [-0.16612324369612685, 0.09469423149924049, -0.041096350269843686, 0.11590828239974199, -0.11852247001264583, -0.12191974092980451, -0.023643060619096188, 0.38827752795557235, -0.27006697235452576, -0.2181243825250545, 0.11845755243980834, -0.28500461403393385, -0.16600798965064864, 0.18834000310215, -0.155404724621665... |
710.0508 | Structured variable selection in support vector machines | When applying the support vector machine (SVM) to high-dimensional
classification problems, we often impose a sparse structure in the SVM to
eliminate the influences of the irrelevant predictors. The lasso and other
variable selection techniques have been successfully used in the SVM to perform
automatic variable sel... | stat.ML math.ST stat.TH | when applying the support vector machine svm to highdimensional classification problems we often impose a sparse structure in the svm to eliminate the influences of the irrelevant predictors the lasso and other variable selection techniques have been successfully used in the svm to perform automatic variable selection ... | [['when', 'applying', 'the', 'support', 'vector', 'machine', 'svm', 'to', 'highdimensional', 'classification', 'problems', 'we', 'often', 'impose', 'a', 'sparse', 'structure', 'in', 'the', 'svm', 'to', 'eliminate', 'the', 'influences', 'of', 'the', 'irrelevant', 'predictors', 'the', 'lasso', 'and', 'other', 'variable',... | [-0.025801548535716447, -0.009711344568238607, -0.11334564233217023, 0.11403986890960083, -0.1721666456433013, -0.19428247662361564, 0.07336360917999592, 0.41246889709659357, -0.3359535702883138, -0.28839523783101995, 0.13616251018510073, -0.21884122063798428, -0.17935312531349779, 0.1288813459114845, -0.14055444616892... |
710.0509 | Techniques on mesh generation for the brain shift simulation | Neurosurgery interventions involve complex tracking systems because a tissue
deformation takesplace. The neuronavigation system relies only on preoperative
images. In order to overcome the soft tissue deformations and guarantee the
accuracy of the navigation a biomechanical model can be used during surgery to
simulat... | physics.med-ph | neurosurgery interventions involve complex tracking systems because a tissue deformation takesplace the neuronavigation system relies only on preoperative images in order to overcome the soft tissue deformations and guarantee the accuracy of the navigation a biomechanical model can be used during surgery to simulate th... | [['neurosurgery', 'interventions', 'involve', 'complex', 'tracking', 'systems', 'because', 'a', 'tissue', 'deformation', 'takesplace', 'the', 'neuronavigation', 'system', 'relies', 'only', 'on', 'preoperative', 'images', 'in', 'order', 'to', 'overcome', 'the', 'soft', 'tissue', 'deformations', 'and', 'guarantee', 'the'... | [-0.053356069321744144, 0.0380176997151284, -0.0736874588765204, 0.039739452122685176, -0.06627638819627464, -0.11279721627943218, 0.023999614759813995, 0.383664301559329, -0.2547793970210478, -0.3085892208572477, 0.15887219637748784, -0.23582515860907732, -0.18185903226258232, 0.2018297134200111, -0.16630243696738034,... |
710.051 | Q-adic Transform revisited | We present an algorithm to perform a simultaneous modular reduction of
several residues. This algorithm is applied fast modular polynomial
multiplication. The idea is to convert the $X$-adic representation of modular
polynomials, with $X$ an indeterminate, to a $q$-adic representation where $q$
is an integer larger t... | cs.SC | we present an algorithm to perform a simultaneous modular reduction of several residues this algorithm is applied fast modular polynomial multiplication the idea is to convert the xadic representation of modular polynomials with x an indeterminate to a qadic representation where q is an integer larger than the field ch... | [['we', 'present', 'an', 'algorithm', 'to', 'perform', 'a', 'simultaneous', 'modular', 'reduction', 'of', 'several', 'residues', 'this', 'algorithm', 'is', 'applied', 'fast', 'modular', 'polynomial', 'multiplication', 'the', 'idea', 'is', 'to', 'convert', 'the', 'xadic', 'representation', 'of', 'modular', 'polynomials'... | [-0.1408898036898913, 0.09919259373826414, -0.1210902046597173, 0.0509393403207346, -0.09586648333566726, -0.12731116765726966, 0.047445014472522425, 0.3416739751069628, -0.3591260150709051, -0.27397379352536105, 0.1052820440150586, -0.22705790333112152, -0.16206746977664768, 0.2245866056062704, -0.08268075174460492, 0... |
710.0511 | Constraints on exact Lagrangians in cotangent bundles of manifolds
fibred over the circle | We give topological obstructions to the existence of a closed exact
Lagrangian submanifold in the cotangent bundle of a closed manifold M which is
the total space of a fibration over the circle. For instance we show that the
fundamental group of such a Lagrangian submanifold cannot be the free product
of two non-triv... | math.SG math.DG | we give topological obstructions to the existence of a closed exact lagrangian submanifold in the cotangent bundle of a closed manifold m which is the total space of a fibration over the circle for instance we show that the fundamental group of such a lagrangian submanifold cannot be the free product of two nontrivial ... | [['we', 'give', 'topological', 'obstructions', 'to', 'the', 'existence', 'of', 'a', 'closed', 'exact', 'lagrangian', 'submanifold', 'in', 'the', 'cotangent', 'bundle', 'of', 'a', 'closed', 'manifold', 'm', 'which', 'is', 'the', 'total', 'space', 'of', 'a', 'fibration', 'over', 'the', 'circle', 'for', 'instance', 'we', ... | [-0.2588628786817239, 0.10988671102066651, -0.09661048628320848, 0.06552063511184382, -0.10821614305224315, -0.0641467739701455, 0.012580984956182447, 0.32959175880216524, -0.2734911976681079, -0.28721832152869964, 0.08821871047437099, -0.24677139683339147, -0.15335132248331734, 0.19980308395971394, -0.1014320300029659... |
710.0512 | Strong coupling expansion for Yang-Mills theory at finite temperature | Euclidean strong coupling expansion of the partition function is applied to
lattice Yang-Mills theory at finite temperature, i.e. for lattices with a
compactified temporal direction. The expansions have a finite radius of
convergence and thus are valid only for $\beta<\beta_c$, where $\beta_c$
denotes the nearest sin... | hep-lat | euclidean strong coupling expansion of the partition function is applied to lattice yangmills theory at finite temperature ie for lattices with a compactified temporal direction the expansions have a finite radius of convergence and thus are valid only for betabeta_c where beta_c denotes the nearest singularity of the ... | [['euclidean', 'strong', 'coupling', 'expansion', 'of', 'the', 'partition', 'function', 'is', 'applied', 'to', 'lattice', 'yangmills', 'theory', 'at', 'finite', 'temperature', 'ie', 'for', 'lattices', 'with', 'a', 'compactified', 'temporal', 'direction', 'the', 'expansions', 'have', 'a', 'finite', 'radius', 'of', 'conv... | [-0.08593251954910859, 0.21872532035316303, -0.07849446810238685, 0.08632866210124727, -0.019129238303018308, -0.08326869633917038, 0.05921662632014583, 0.3711647460477252, -0.24840631155044926, -0.2857614659248308, 0.09189001954473497, -0.28329614306373213, -0.04652461197353356, 0.17186312437964565, 0.0788916235718109... |
710.0513 | Heisenberg model of the high-energy hadron collision in terms of chiral
fields | Properties of chiral Born-Infeld Theory proposed as the model for shock-wave
fireball production in the hadron-hadron collisions was studied. The role of
the shock-waves in the multi-particle production was discussed.
| hep-ph | properties of chiral borninfeld theory proposed as the model for shockwave fireball production in the hadronhadron collisions was studied the role of the shockwaves in the multiparticle production was discussed | [['properties', 'of', 'chiral', 'borninfeld', 'theory', 'proposed', 'as', 'the', 'model', 'for', 'shockwave', 'fireball', 'production', 'in', 'the', 'hadronhadron', 'collisions', 'was', 'studied', 'the', 'role', 'of', 'the', 'shockwaves', 'in', 'the', 'multiparticle', 'production', 'was', 'discussed']] | [-0.07973351168135802, 0.19673713451872268, -0.15377975311130285, 0.1626617354961733, 0.03416393200556437, -0.017370195624729, -0.16909105540641273, 0.29680810316155354, -0.1569811273055772, -0.1988120815406243, -0.04575922716564188, -0.33718514973297714, -0.06327026523649693, 0.1142524403752759, 0.07049218316872914, 0... |
710.0514 | Miller's instability, microchaos and the short-term evolution of
initially nearby orbits | We study the phase-space behaviour of nearby trajectories in integrable
potentials. We show that the separation of nearby orbits initially diverges
very fast, mimicking a nearly exponential behaviour, while at late times it
grows linearly. This initial exponential phase, known as Miller's instability,
is commonly fou... | astro-ph | we study the phasespace behaviour of nearby trajectories in integrable potentials we show that the separation of nearby orbits initially diverges very fast mimicking a nearly exponential behaviour while at late times it grows linearly this initial exponential phase known as millers instability is commonly found in nbod... | [['we', 'study', 'the', 'phasespace', 'behaviour', 'of', 'nearby', 'trajectories', 'in', 'integrable', 'potentials', 'we', 'show', 'that', 'the', 'separation', 'of', 'nearby', 'orbits', 'initially', 'diverges', 'very', 'fast', 'mimicking', 'a', 'nearly', 'exponential', 'behaviour', 'while', 'at', 'late', 'times', 'it',... | [-0.18153756639609733, 0.13609206427492956, -0.1777706010932369, 0.09313819546784674, -0.014131700402746599, -0.07719030035659671, -0.03654666702218708, 0.3441292889061428, -0.2627531903485457, -0.26393688233968404, 0.07582678438408212, -0.24364833416128975, -0.18378894687408492, 0.18473198331360305, -0.062301666823969... |
710.0515 | Poynting's theorem and energy conservation in the propagation of light
in bounded media | Starting from the Maxwell-Lorentz equations, Poynting's theorem is
reconsidered. The energy flux vector is introduced as S_e=(E x B)/mu_0 instead
of E x H, because only by this choice the energy dissipation can be related to
the balance of the kinetic energy of the matter subsystem. Conservation of the
total energy a... | cond-mat.str-el physics.optics | starting from the maxwelllorentz equations poyntings theorem is reconsidered the energy flux vector is introduced as s_ee x bmu_0 instead of e x h because only by this choice the energy dissipation can be related to the balance of the kinetic energy of the matter subsystem conservation of the total energy as the sum of... | [['starting', 'from', 'the', 'maxwelllorentz', 'equations', 'poyntings', 'theorem', 'is', 'reconsidered', 'the', 'energy', 'flux', 'vector', 'is', 'introduced', 'as', 's_ee', 'x', 'bmu_0', 'instead', 'of', 'e', 'x', 'h', 'because', 'only', 'by', 'this', 'choice', 'the', 'energy', 'dissipation', 'can', 'be', 'related', ... | [-0.13016049060554777, 0.15814208564947227, -0.08337846489157527, 0.0953370628720482, -0.08015312603674829, -0.10804260234747615, 0.020711984325732503, 0.3229979071233954, -0.27680524328191364, -0.3389730321110359, 0.08893679743715828, -0.2502471650152334, -0.07604180318968637, 0.16332073392030516, -0.02302570813668093... |
710.0516 | Essential curves in handlebodies and topological contractions | If $X$ is a compact set, a {\it topological contraction} is a self-embedding
$f$ such that the intersection of the successive images $f^k(X)$, $k>0$,
consists of one point. In dimension 3, we prove that there are smooth
topological contractions of the handlebodies of genus $\geq 2$ whose image is
essential. Our proof... | math.GT | if x is a compact set a it topological contraction is a selfembedding f such that the intersection of the successive images fkx k0 consists of one point in dimension 3 we prove that there are smooth topological contractions of the handlebodies of genus geq 2 whose image is essential our proof is based on an easy criter... | [['if', 'x', 'is', 'a', 'compact', 'set', 'a', 'it', 'topological', 'contraction', 'is', 'a', 'selfembedding', 'f', 'such', 'that', 'the', 'intersection', 'of', 'the', 'successive', 'images', 'fkx', 'k0', 'consists', 'of', 'one', 'point', 'in', 'dimension', '3', 'we', 'prove', 'that', 'there', 'are', 'smooth', 'topolog... | [-0.19453911609290278, 0.09410581619822016, -0.13301467498326125, 0.04328792997608509, -0.06850748229087056, -0.16218424406970905, 0.005727197627386297, 0.3735952285762109, -0.260389517800992, -0.17101015947649584, 0.12194360584116486, -0.2705683767357293, -0.17523625041084254, 0.22703252908061533, -0.12229289854739737... |
710.0517 | The notion of persistence applied to breathers in thermal equilibrium | We study the thermal equilibrium of nonlinear Klein-Gordon chains at the
limit of small coupling (anticontinuum limit). We show that the persistence
distribution associated to the local energy density is a useful tool to study
the statistical distribution of so-called thermal breathers, mainly when the
equilibrium is... | cond-mat.stat-mech | we study the thermal equilibrium of nonlinear kleingordon chains at the limit of small coupling anticontinuum limit we show that the persistence distribution associated to the local energy density is a useful tool to study the statistical distribution of socalled thermal breathers mainly when the equilibrium is charact... | [['we', 'study', 'the', 'thermal', 'equilibrium', 'of', 'nonlinear', 'kleingordon', 'chains', 'at', 'the', 'limit', 'of', 'small', 'coupling', 'anticontinuum', 'limit', 'we', 'show', 'that', 'the', 'persistence', 'distribution', 'associated', 'to', 'the', 'local', 'energy', 'density', 'is', 'a', 'useful', 'tool', 'to',... | [-0.1489966452049854, 0.163461624449369, -0.11501753708072657, 0.1083925098998022, -0.044716488284015116, -0.12144093335474898, 0.03038177115611432, 0.36522770571153634, -0.2766472664317929, -0.23319777111904133, 0.10137745439099935, -0.3067213453621222, -0.12860819299536563, 0.17036160437902748, 0.029414587758869033, ... |
710.0518 | Self-directed growth of AlGaAs core-shell nanowires for visible light
applications | Al(0.37)Ga(0.63)As nanowires (NWs) were grown in a molecular beam epitaxy
system on GaAs(111)B substrates. Micro-photoluminescence measurements and
energy dispersive X-ray spectroscopy indicated a core-shell structure and Al
composition gradient along the NW axis, producing a potential minimum for
carrier confinement... | cond-mat.mtrl-sci | al037ga063as nanowires nws were grown in a molecular beam epitaxy system on gaas111b substrates microphotoluminescence measurements and energy dispersive xray spectroscopy indicated a coreshell structure and al composition gradient along the nw axis producing a potential minimum for carrier confinement the coreshell st... | [['al037ga063as', 'nanowires', 'nws', 'were', 'grown', 'in', 'a', 'molecular', 'beam', 'epitaxy', 'system', 'on', 'gaas111b', 'substrates', 'microphotoluminescence', 'measurements', 'and', 'energy', 'dispersive', 'xray', 'spectroscopy', 'indicated', 'a', 'coreshell', 'structure', 'and', 'al', 'composition', 'gradient',... | [-0.13453038376434867, 0.1753275506760411, -0.05811361142369951, -0.04656595072371821, 0.014231072064360669, -0.1392365724073145, 0.047676170694416965, 0.5341131405880803, -0.27755045540759277, -0.33420258609513787, -0.015121279406794828, -0.28738473102065, -0.08314309185691948, 0.19365391218713646, 0.08925501745322655... |
710.0519 | Differential Invariants of Conformal and Projective Surfaces | We show that, for both the conformal and projective groups, all the
differential invariants of a generic surface in three-dimensional space can be
written as combinations of the invariant derivatives of a single differential
invariant. The proof is based on the equivariant method of moving frames.
| math.DG math-ph math.MP | we show that for both the conformal and projective groups all the differential invariants of a generic surface in threedimensional space can be written as combinations of the invariant derivatives of a single differential invariant the proof is based on the equivariant method of moving frames | [['we', 'show', 'that', 'for', 'both', 'the', 'conformal', 'and', 'projective', 'groups', 'all', 'the', 'differential', 'invariants', 'of', 'a', 'generic', 'surface', 'in', 'threedimensional', 'space', 'can', 'be', 'written', 'as', 'combinations', 'of', 'the', 'invariant', 'derivatives', 'of', 'a', 'single', 'different... | [-0.17460250955722903, 0.06471098232609422, -0.12219206112153504, 0.05607572861228381, -0.06677212032651447, -0.09733618607582606, -0.06453445227626893, 0.3222196981837244, -0.29662882099333016, -0.2620868943631649, 0.11700216896639651, -0.23795809564383133, -0.17429336863974837, 0.23112216033041477, -0.090443181122005... |
710.052 | Mining the Local Volume | After recent systematic optical, IR, and HI surveys, the total number of
known galaxies within 10 Mpc has increased from 179 to 550. About half this
Local Volume (LV) sample is now been imaged with HST, yielding the galaxy
distances with an accuracy of about 8%. For the majority of the LV galaxies we
currently have H... | astro-ph | after recent systematic optical ir and hi surveys the total number of known galaxies within 10 mpc has increased from 179 to 550 about half this local volume lv sample is now been imaged with hst yielding the galaxy distances with an accuracy of about 8 for the majority of the lv galaxies we currently have halpha fluxe... | [['after', 'recent', 'systematic', 'optical', 'ir', 'and', 'hi', 'surveys', 'the', 'total', 'number', 'of', 'known', 'galaxies', 'within', '10', 'mpc', 'has', 'increased', 'from', '179', 'to', '550', 'about', 'half', 'this', 'local', 'volume', 'lv', 'sample', 'is', 'now', 'been', 'imaged', 'with', 'hst', 'yielding', 't... | [-0.06609113326522748, 0.08425389920255937, -0.04999768743039788, 0.0836970837780501, -0.07679044863561521, -0.0078109846198679625, 0.03201906772934505, 0.36278557594160776, -0.151289797612038, -0.38599168975409626, 0.07745682870012682, -0.2913568895410847, 0.0022141175545953417, 0.20812213563964374, -0.003707613560647... |
710.0521 | Kinetic Equationins in the Theory of Normal Fermi Liquid | On the bases of the improved approximation for the spectral function of
one-particle states the Landau-Silin kinetic equations for the normal Fermi
liquids of neutral and electrically charged particles are shown to be valid at
finite temperature above the temperature of superfluid transition.
| cond-mat.stat-mech | on the bases of the improved approximation for the spectral function of oneparticle states the landausilin kinetic equations for the normal fermi liquids of neutral and electrically charged particles are shown to be valid at finite temperature above the temperature of superfluid transition | [['on', 'the', 'bases', 'of', 'the', 'improved', 'approximation', 'for', 'the', 'spectral', 'function', 'of', 'oneparticle', 'states', 'the', 'landausilin', 'kinetic', 'equations', 'for', 'the', 'normal', 'fermi', 'liquids', 'of', 'neutral', 'and', 'electrically', 'charged', 'particles', 'are', 'shown', 'to', 'be', 'va... | [-0.09682556397963835, 0.28977422012276083, -0.06717693590190868, 0.08149986070862343, 0.059465715742864925, -0.12459526453600374, 0.05396840158243512, 0.30166585622138753, -0.2065675700473231, -0.2536939991594747, -0.015351745202530956, -0.31928213603448036, 0.004704110627604085, 0.14511196577358385, 0.087963614677793... |
710.0522 | Localization and delocalization of ultracold bosonic atoms in finite
optical lattices | We study bosonic atoms in small optical lattices by exact diagonalization and
observe a striking similarity to the superfluid to Mott insulator transition in
macroscopic systems. The momentum distribution, the formation of an energy gap,
and the pair correlation function show only a weak size dependence. For
noncomme... | cond-mat.other | we study bosonic atoms in small optical lattices by exact diagonalization and observe a striking similarity to the superfluid to mott insulator transition in macroscopic systems the momentum distribution the formation of an energy gap and the pair correlation function show only a weak size dependence for noncommensurat... | [['we', 'study', 'bosonic', 'atoms', 'in', 'small', 'optical', 'lattices', 'by', 'exact', 'diagonalization', 'and', 'observe', 'a', 'striking', 'similarity', 'to', 'the', 'superfluid', 'to', 'mott', 'insulator', 'transition', 'in', 'macroscopic', 'systems', 'the', 'momentum', 'distribution', 'the', 'formation', 'of', '... | [-0.18783574026236508, 0.21552619348965002, -0.06380870488244406, 0.10434845093256259, -0.01454542424936006, -0.1347152095763607, 0.09256345931777453, 0.39430879488428855, -0.25140463862508694, -0.2537536888502221, 0.008851284043556278, -0.31202709269610807, -0.13512194128905206, 0.07584074279293418, 0.0616786534937613... |
710.0523 | Fluctuation theorem applied to Dictyostelium discoideum system | In this paper, we analyze the electrotactic movement of Dictyostelium
discoideum from the viewpoint of non-equilibrium statistical mechanics. Because
we can observe fluctuating behavior of cellular trajectories, we analyze the
probability distribution of the trajectories with the aid of the fluctuation
theorem. Recen... | q-bio.CB cond-mat.soft cond-mat.stat-mech | in this paper we analyze the electrotactic movement of dictyostelium discoideum from the viewpoint of nonequilibrium statistical mechanics because we can observe fluctuating behavior of cellular trajectories we analyze the probability distribution of the trajectories with the aid of the fluctuation theorem recently the... | [['in', 'this', 'paper', 'we', 'analyze', 'the', 'electrotactic', 'movement', 'of', 'dictyostelium', 'discoideum', 'from', 'the', 'viewpoint', 'of', 'nonequilibrium', 'statistical', 'mechanics', 'because', 'we', 'can', 'observe', 'fluctuating', 'behavior', 'of', 'cellular', 'trajectories', 'we', 'analyze', 'the', 'prob... | [-0.11655805136736792, 0.11606562221250324, -0.1885859223936374, 0.10004018948529847, -0.030581685662683513, -0.0994082491034297, 0.05518307146525735, 0.32190160339491236, -0.2975210553569788, -0.2524646458267752, 0.06555390913962145, -0.2478602725012159, -0.2176766323822516, 0.19767617869904455, -0.09358478827764177, ... |
710.0524 | Raman spectra of unfilled and filled carbon nanotubes: Theory | The Raman spectra of two G-bands and a radial breathing mode (RBM) of
unfilled and filled single-wall semiconducting and metallic carbon nanotubes
have been investigated theoretically, in the presence of electron-phonon and
phonon-phonon interactions. Excitation of low frequency optical plasmons in the
metallic nanot... | cond-mat.other | the raman spectra of two gbands and a radial breathing mode rbm of unfilled and filled singlewall semiconducting and metallic carbon nanotubes have been investigated theoretically in the presence of electronphonon and phononphonon interactions excitation of low frequency optical plasmons in the metallic nanotube is res... | [['the', 'raman', 'spectra', 'of', 'two', 'gbands', 'and', 'a', 'radial', 'breathing', 'mode', 'rbm', 'of', 'unfilled', 'and', 'filled', 'singlewall', 'semiconducting', 'and', 'metallic', 'carbon', 'nanotubes', 'have', 'been', 'investigated', 'theoretically', 'in', 'the', 'presence', 'of', 'electronphonon', 'and', 'pho... | [-0.08654177107382566, 0.18549816402862365, -0.02002250580324991, 0.008474237001999946, -0.03002058527864782, -0.19449709793719064, 0.08937810054048896, 0.512369281006977, -0.22739435290984278, -0.24518938045283514, 0.003077346510586462, -0.3344938085979915, -0.11274099423234085, 0.17120030841116593, 0.0274395451897622... |
710.0525 | Hunting long-lived gluinos at the Pierre Auger Observatory | Eventual signals of split sypersymmetry in cosmic ray physics are analyzed in
detail. The study focusses particularly on quasi-stable colorless R-hadrons
originating through confinement of long-lived gluinos (with quarks,
anti-quarks, and gluons) produced in pp collisions at astrophysical sources.
Because of parton d... | hep-ph | eventual signals of split sypersymmetry in cosmic ray physics are analyzed in detail the study focusses particularly on quasistable colorless rhadrons originating through confinement of longlived gluinos with quarks antiquarks and gluons produced in pp collisions at astrophysical sources because of parton density requi... | [['eventual', 'signals', 'of', 'split', 'sypersymmetry', 'in', 'cosmic', 'ray', 'physics', 'are', 'analyzed', 'in', 'detail', 'the', 'study', 'focusses', 'particularly', 'on', 'quasistable', 'colorless', 'rhadrons', 'originating', 'through', 'confinement', 'of', 'longlived', 'gluinos', 'with', 'quarks', 'antiquarks', '... | [-0.037389561265953025, 0.3289468159032224, -0.09859450440487748, 0.2195337841626983, -0.028491011943738414, -0.04497312230853153, -0.01820915860838532, 0.3790408740648941, -0.17930665381275462, -0.3473858942161314, -0.03142188279962741, -0.3352017788796352, 0.06547388385793886, 0.17763115884150443, 0.05289951868870723... |
710.0526 | H^\pm W^\mp production in the MSSM at the LHC | We investigate the viability of observing charged Higgs bosons (H^\pm)
produced in association with W bosons at the CERN Large Hadron Collider, using
the leptonic decay H^+ -> tau^+ nu_tau and hadronic W decay, within the Minimal
Supersymmetric Standard Model. Performing a parton level study we show how the
irreducib... | hep-ph | we investigate the viability of observing charged higgs bosons hpm produced in association with w bosons at the cern large hadron collider using the leptonic decay h tau nu_tau and hadronic w decay within the minimal supersymmetric standard model performing a parton level study we show how the irreducible standard mode... | [['we', 'investigate', 'the', 'viability', 'of', 'observing', 'charged', 'higgs', 'bosons', 'hpm', 'produced', 'in', 'association', 'with', 'w', 'bosons', 'at', 'the', 'cern', 'large', 'hadron', 'collider', 'using', 'the', 'leptonic', 'decay', 'h', 'tau', 'nu_tau', 'and', 'hadronic', 'w', 'decay', 'within', 'the', 'min... | [-0.03341828616301915, 0.30224745753561943, -0.024282220949805002, 0.17149219995864282, -0.030580221788912284, -0.23324428188114812, 0.05761751165704393, 0.3209317098542048, -0.2372116634065694, -0.2443949189945692, 0.006850852631032467, -0.26804619265447666, 0.05776189536242405, 0.11092436837782038, 0.1093554656197339... |
710.0527 | The ANTARES detector: background sources and effects on detector
performance | The ANTARES Collaboration is deploying a large neutrino detector at a depth
of 2475 m in the Mediterranean Sea, 40 km off shore from La Seyne-sur-Mer in
South France. The construction of this 12-line detector with 75 phototubes per
line will be completed early 2008. Data taking has begun since April 2005 with
an inst... | astro-ph | the antares collaboration is deploying a large neutrino detector at a depth of 2475 m in the mediterranean sea 40 km off shore from la seynesurmer in south france the construction of this 12line detector with 75 phototubes per line will be completed early 2008 data taking has begun since april 2005 with an instrumentat... | [['the', 'antares', 'collaboration', 'is', 'deploying', 'a', 'large', 'neutrino', 'detector', 'at', 'a', 'depth', 'of', '2475', 'm', 'in', 'the', 'mediterranean', 'sea', '40', 'km', 'off', 'shore', 'from', 'la', 'seynesurmer', 'in', 'south', 'france', 'the', 'construction', 'of', 'this', '12line', 'detector', 'with', '... | [-0.056380430309889984, 0.22238355511866617, -0.03767495544579549, 0.07807359719374336, -0.0453883133112238, -0.1023851139166464, 0.022056422097524866, 0.34915374950147593, -0.17490516448011384, -0.41172584511626226, 0.12991784958061403, -0.3471929682003788, -0.041649620094073886, 0.22302867594736223, -0.07163679548300... |
710.0528 | On the interaction between sharing and linearity | In the analysis of logic programs, abstract domains for detecting sharing and
linearity information are widely used. Devising abstract unification algorithms
for such domains has proved to be rather hard. At the moment, the available
algorithms are correct but not optimal, i.e., they cannot fully exploit the
informat... | cs.PL cs.LO | in the analysis of logic programs abstract domains for detecting sharing and linearity information are widely used devising abstract unification algorithms for such domains has proved to be rather hard at the moment the available algorithms are correct but not optimal ie they cannot fully exploit the information convey... | [['in', 'the', 'analysis', 'of', 'logic', 'programs', 'abstract', 'domains', 'for', 'detecting', 'sharing', 'and', 'linearity', 'information', 'are', 'widely', 'used', 'devising', 'abstract', 'unification', 'algorithms', 'for', 'such', 'domains', 'has', 'proved', 'to', 'be', 'rather', 'hard', 'at', 'the', 'moment', 'th... | [-0.08816135999295512, 0.038322861545020716, -0.10850713753898163, 0.16225297695127666, -0.15752399562588834, -0.17004866163770202, 0.046262765831852445, 0.3893437442719005, -0.33547799769730774, -0.31532762651331725, 0.13750285771748166, -0.1988395092979772, -0.11711054000261356, 0.1836907237448031, -0.122999016317044... |
710.0529 | Cu-Au type orderings in the staggered quadrupolar region of the fcc
Blume Emery Griffiths model | The spin-1 Ising (BEG) model has been simulated using a cellular automaton
(CA) algorithm improved from the Creutz cellular automaton (CCA) for a
face-centered cubic (fcc) lattice. The ground state diagram ($k$, $d$) of the
fcc BEG model has ferromagnetic ($F$), quadrupolar ($Q$) and staggered
quadrupolar ($SQ$) orde... | cond-mat.stat-mech | the spin1 ising beg model has been simulated using a cellular automaton ca algorithm improved from the creutz cellular automaton cca for a facecentered cubic fcc lattice the ground state diagram k d of the fcc beg model has ferromagnetic f quadrupolar q and staggered quadrupolar sq ordering regions the simulations have... | [['the', 'spin1', 'ising', 'beg', 'model', 'has', 'been', 'simulated', 'using', 'a', 'cellular', 'automaton', 'ca', 'algorithm', 'improved', 'from', 'the', 'creutz', 'cellular', 'automaton', 'cca', 'for', 'a', 'facecentered', 'cubic', 'fcc', 'lattice', 'the', 'ground', 'state', 'diagram', 'k', 'd', 'of', 'the', 'fcc', ... | [-0.169464698971843, 0.20280508239488673, -0.013471043403815785, 0.028345095318391782, -0.009664532207294341, -0.1861436875161091, 0.0719278721702755, 0.4193223005656255, -0.2002125213161931, -0.24942125380039215, 0.029964529300416144, -0.31153937302734874, -0.07262888434556646, 0.07613710919234884, 0.15171720940617572... |
710.053 | Parametrizing the lepton mixing matrix in terms of deviations from
tri-bimaximal mixing | We propose a parametrization of the lepton mixing matrix in terms of an
expansion in powers of the deviations of the reactor, solar and atmospheric
mixing angles from their tri-bimaximal values. We show that unitarity triangles
and neutrino oscillation formulae have a very compact form when expressed in
this parametr... | hep-ph | we propose a parametrization of the lepton mixing matrix in terms of an expansion in powers of the deviations of the reactor solar and atmospheric mixing angles from their tribimaximal values we show that unitarity triangles and neutrino oscillation formulae have a very compact form when expressed in this parametrizati... | [['we', 'propose', 'a', 'parametrization', 'of', 'the', 'lepton', 'mixing', 'matrix', 'in', 'terms', 'of', 'an', 'expansion', 'in', 'powers', 'of', 'the', 'deviations', 'of', 'the', 'reactor', 'solar', 'and', 'atmospheric', 'mixing', 'angles', 'from', 'their', 'tribimaximal', 'values', 'we', 'show', 'that', 'unitarity'... | [-0.061478505725972354, 0.2422418761334934, -0.04834504886576445, 0.12998550329910646, -0.07281031133145979, -0.1132722825715595, 0.07111679076558293, 0.3145496294935151, -0.282965674360126, -0.3167388512946592, 0.06433658359461639, -0.2677450944844744, -0.13942762041962384, 0.19856959018893172, -0.022482294566228543, ... |
710.0531 | The Problem of Localization in Networks of Randomly Deployed Nodes:
Asymptotic and Finite Analysis, and Thresholds | We derive the probability that a randomly chosen NL-node over $S$ gets
localized as a function of a variety of parameters. Then, we derive the
probability that the whole network of NL-nodes over $S$ gets localized. In
connection with the asymptotic thresholds, we show the presence of asymptotic
thresholds on the netw... | cs.DM cs.IT cs.NI math.IT | we derive the probability that a randomly chosen nlnode over s gets localized as a function of a variety of parameters then we derive the probability that the whole network of nlnodes over s gets localized in connection with the asymptotic thresholds we show the presence of asymptotic thresholds on the network localiza... | [['we', 'derive', 'the', 'probability', 'that', 'a', 'randomly', 'chosen', 'nlnode', 'over', 's', 'gets', 'localized', 'as', 'a', 'function', 'of', 'a', 'variety', 'of', 'parameters', 'then', 'we', 'derive', 'the', 'probability', 'that', 'the', 'whole', 'network', 'of', 'nlnodes', 'over', 's', 'gets', 'localized', 'in'... | [-0.18573264943352863, 0.16160262118999477, -0.03229917284924129, 0.04015187504795256, 0.010840019823549546, -0.10866886247204591, 0.0899846262572818, 0.345207066490468, -0.29665715122046843, -0.2755451515406268, 0.10472411198592553, -0.26766774485091843, -0.14843598387701668, 0.11866017655558782, -0.038861553235719465... |
710.0532 | Harmonic oscillator model for current- and field-driven magnetic
vortices | In experiments the distinction between spin-torque and Oersted-field driven
magnetization dynamics is still an open problem. Here, the gyroscopic motion of
current- and field-driven magnetic vortices in small thin-film elements is
investigated by analytical calculations and by numerical simulations. It is
found that ... | cond-mat.other | in experiments the distinction between spintorque and oerstedfield driven magnetization dynamics is still an open problem here the gyroscopic motion of current and fielddriven magnetic vortices in small thinfilm elements is investigated by analytical calculations and by numerical simulations it is found that for small ... | [['in', 'experiments', 'the', 'distinction', 'between', 'spintorque', 'and', 'oerstedfield', 'driven', 'magnetization', 'dynamics', 'is', 'still', 'an', 'open', 'problem', 'here', 'the', 'gyroscopic', 'motion', 'of', 'current', 'and', 'fielddriven', 'magnetic', 'vortices', 'in', 'small', 'thinfilm', 'elements', 'is', '... | [-0.21329025832156456, 0.20574192990052112, -0.03502910427186032, 0.006390446503267645, -0.03714959132809972, -0.05941889029494379, 0.019705143751749813, 0.39532362357821577, -0.2774015320898142, -0.2899688712299563, 0.07109534529005286, -0.24399766665991657, -0.12609751188456145, 0.2397734130878911, 0.0222565471790297... |
710.0533 | Preliminary results on the homogenization of thin piezoelectric
perforated shells | We consider a composite piezoelectric material whose reference configuration
is a thin shell with fixed thickness. In this work, we give a new approach
based on the periodic unfolding method to justify the modelling of a thin
piezoelectric perforated shells and we establish the limit constitutive law by
letting the s... | math.NA math.AP | we consider a composite piezoelectric material whose reference configuration is a thin shell with fixed thickness in this work we give a new approach based on the periodic unfolding method to justify the modelling of a thin piezoelectric perforated shells and we establish the limit constitutive law by letting the size ... | [['we', 'consider', 'a', 'composite', 'piezoelectric', 'material', 'whose', 'reference', 'configuration', 'is', 'a', 'thin', 'shell', 'with', 'fixed', 'thickness', 'in', 'this', 'work', 'we', 'give', 'a', 'new', 'approach', 'based', 'on', 'the', 'periodic', 'unfolding', 'method', 'to', 'justify', 'the', 'modelling', 'o... | [-0.10632504867510749, 0.0673678619908048, -0.09579819953673846, -0.014053515321877482, -0.11627187340689654, -0.12267616761291956, 0.04521973341757843, 0.3647646322943173, -0.2788701869257085, -0.25551958943342234, 0.07948334126086155, -0.2550374703247829, -0.12419504204208588, 0.15804683489350047, -0.0668114253059755... |
710.0534 | On the chemical freeze-out criteria in a hot and dense fireball | Intensive investigations of freeze-out criteria in a hot and dense fireball
provide important information regarding particle emission from the fireball. A
systematic comparison of these proposals is presented here in the framework of
a thermodynamically consistent excluded volume model which has been found to
describ... | hep-ph | intensive investigations of freezeout criteria in a hot and dense fireball provide important information regarding particle emission from the fireball a systematic comparison of these proposals is presented here in the framework of a thermodynamically consistent excluded volume model which has been found to describe th... | [['intensive', 'investigations', 'of', 'freezeout', 'criteria', 'in', 'a', 'hot', 'and', 'dense', 'fireball', 'provide', 'important', 'information', 'regarding', 'particle', 'emission', 'from', 'the', 'fireball', 'a', 'systematic', 'comparison', 'of', 'these', 'proposals', 'is', 'presented', 'here', 'in', 'the', 'frame... | [-0.05958979080311732, 0.16982144837562052, -0.11599991967119856, 0.08613935245533952, 0.008883742813426286, -0.0996078238557117, 0.07191280285958104, 0.36434734044258765, -0.18809340711094324, -0.30974459512053065, 0.060485427746177683, -0.2995212492508901, -0.013578453184457717, 0.17566055762931376, -0.00354136139699... |
710.0535 | Antiferromagnetic order driven by the molecular orbital order of
C$_{60}$ in $\alpha'$--tetra--$kis$--(dimethylamino)--ethylene--C$_{60}$ | We have studied the ground state of a fullerene--based magnet, the
$\alpha'$--phase tetra--$kis$--(dimethylamino)--ethylene--C$_{60}$
($\alpha'$--TDAE--C$_{60}$), by electron spin resonance (ESR) and magnetic
torque measurements. Below T$_N=7$ K, non--paramagnetic field dependent
resonances with a finite excitation g... | cond-mat.mtrl-sci cond-mat.str-el | we have studied the ground state of a fullerenebased magnet the alphaphase tetrakisdimethylaminoethylenec_60 alphatdaec_60 by electron spin resonance esr and magnetic torque measurements below t_n7 k nonparamagnetic field dependent resonances with a finite excitation gap 17 ghz are observed along the aaxis strong enhan... | [['we', 'have', 'studied', 'the', 'ground', 'state', 'of', 'a', 'fullerenebased', 'magnet', 'the', 'alphaphase', 'tetrakisdimethylaminoethylenec_60', 'alphatdaec_60', 'by', 'electron', 'spin', 'resonance', 'esr', 'and', 'magnetic', 'torque', 'measurements', 'below', 't_n7', 'k', 'nonparamagnetic', 'field', 'dependent',... | [-0.1928582706194768, 0.25779275953331693, -0.009732370295363372, -0.006560769780409202, -0.06479277015953767, -0.10226716373314257, 0.04843108241492119, 0.41335652492268654, -0.24155396470021395, -0.3142588179573783, 0.019606344856046995, -0.32529252703439016, -0.05173621295577251, 0.14405819388167534, 0.0956064552053... |
710.0536 | Chiral Limit and Light Quark Masses in 2+1 Flavor Domain Wall QCD | We present results for meson masses and decay constants measured on 24^3x64
lattices using the domain wall fermion formulation with an extension of the
fifth dimension of L_s=16 for N_f=2+1 dynamical quark flavors. The lightest
dynamical meson mass in our set-up is around 331 MeV, while partially quenched
mesons reac... | hep-lat | we present results for meson masses and decay constants measured on 243x64 lattices using the domain wall fermion formulation with an extension of the fifth dimension of l_s16 for n_f21 dynamical quark flavors the lightest dynamical meson mass in our setup is around 331 mev while partially quenched mesons reach masses ... | [['we', 'present', 'results', 'for', 'meson', 'masses', 'and', 'decay', 'constants', 'measured', 'on', '243x64', 'lattices', 'using', 'the', 'domain', 'wall', 'fermion', 'formulation', 'with', 'an', 'extension', 'of', 'the', 'fifth', 'dimension', 'of', 'l_s16', 'for', 'n_f21', 'dynamical', 'quark', 'flavors', 'the', 'l... | [-0.03345965455704625, 0.28395130470543983, -0.0790858701423175, 0.12165159037829364, -0.05048049321993713, -0.10101207016218129, 0.11730464274633973, 0.35671620749348804, -0.1516006724315061, -0.25809705898543633, 0.05093380862735617, -0.3105824594318435, 0.010966966343719674, 0.13744805398586113, 0.049754518305248435... |
710.0537 | Dispersion Law of the Form $\epsilon(p)=\hbar^2p^2/2m +\widetilde
V(p)-\widetilde V(0)$ for Elementary Excitations of Nonideal Fermi Gas in the
Pair Interaction Approximation $(i\leftrightarrow j)$, $V(|x_i-x_j|)$ | We give a derivation of the dispersion law $\epsilon(p)=\hbar^2p^2/2m
+\widetilde V(p)-\widetilde V(0)$, where $\widetilde V(p)$ is the Fourier
transform of the pair interaction potential $V(r)$. (The interaction between
particles $x_i$ and $x_j$ is $V(|x_i-x_j|)$.)
| math-ph math.MP | we give a derivation of the dispersion law epsilonphbar2p22m widetilde vpwidetilde v0 where widetilde vp is the fourier transform of the pair interaction potential vr the interaction between particles x_i and x_j is vx_ix_j | [['we', 'give', 'a', 'derivation', 'of', 'the', 'dispersion', 'law', 'epsilonphbar2p22m', 'widetilde', 'vpwidetilde', 'v0', 'where', 'widetilde', 'vp', 'is', 'the', 'fourier', 'transform', 'of', 'the', 'pair', 'interaction', 'potential', 'vr', 'the', 'interaction', 'between', 'particles', 'x_i', 'and', 'x_j', 'is', 'vx... | [-0.21735296701832163, 0.12957904989560765, -0.1443855496303689, 0.008505269982701829, -0.07758865644404243, -0.19723415974107, -0.0037741294739046887, 0.35124179279251444, -0.32796448670447836, -0.18322329739889792, -0.045084406426476854, -0.34438852196739567, -0.09212804008876124, 0.07466558729028029, 0.0335421900174... |
710.0538 | Gap theory of rectification in ballistic three-terminal conductors | We introduce a model for rectification in three-terminal ballistic
conductors, where the central connecting node is modeled as a chaotic cavity.
For bias voltages comparable to the Fermi energy, a strong nonlinearity is
created by the opening of a gap in the transport window. Both noninteracting
cavity electrons at a... | cond-mat.mes-hall | we introduce a model for rectification in threeterminal ballistic conductors where the central connecting node is modeled as a chaotic cavity for bias voltages comparable to the fermi energy a strong nonlinearity is created by the opening of a gap in the transport window both noninteracting cavity electrons at arbitrar... | [['we', 'introduce', 'a', 'model', 'for', 'rectification', 'in', 'threeterminal', 'ballistic', 'conductors', 'where', 'the', 'central', 'connecting', 'node', 'is', 'modeled', 'as', 'a', 'chaotic', 'cavity', 'for', 'bias', 'voltages', 'comparable', 'to', 'the', 'fermi', 'energy', 'a', 'strong', 'nonlinearity', 'is', 'cr... | [-0.15796441682191056, 0.1355070103688349, -0.03709990598938682, 0.06150865121956237, -0.006819899800713315, -0.19189270978059733, 0.03468653382063194, 0.3881332011554729, -0.27753269597958546, -0.30727656860130304, 0.02784516166623992, -0.3078635947807043, -0.10995968603035153, 0.2489633140450513, -0.01122475058990389... |
710.0539 | A Novel Solution to the ATT48 Benchmark Problem | A solution to the benchmark ATT48 Traveling Salesman Problem (from the
TSPLIB95 library) results from isolating the set of vertices into ten
open-ended zones with nine lengthwise boundaries. In each zone, a
minimum-length Hamiltonian Path (HP) is found for each combination of boundary
vertices, leading to an approxim... | cs.DS cs.CC | a solution to the benchmark att48 traveling salesman problem from the tsplib95 library results from isolating the set of vertices into ten openended zones with nine lengthwise boundaries in each zone a minimumlength hamiltonian path hp is found for each combination of boundary vertices leading to an approximation for t... | [['a', 'solution', 'to', 'the', 'benchmark', 'att48', 'traveling', 'salesman', 'problem', 'from', 'the', 'tsplib95', 'library', 'results', 'from', 'isolating', 'the', 'set', 'of', 'vertices', 'into', 'ten', 'openended', 'zones', 'with', 'nine', 'lengthwise', 'boundaries', 'in', 'each', 'zone', 'a', 'minimumlength', 'ha... | [-0.1311550721029849, 0.10687721494331, -0.046954093790171965, 0.017371155984552675, -0.10365306956840581, -0.1521127230536781, 0.11089990137537059, 0.3403547323161834, -0.264733125269413, -0.3388006687948578, 0.080106993738905, -0.30988074062686216, -0.10875352736758559, 0.16652524326192705, -0.007638832818912832, 0.0... |
710.054 | A disc in the heart of the Ant nebula | We present the discovery of a silicate disc at the centre of the planetary
nebula Mz3 (the Ant). The nebula was observed with MIDI on the Very Large
Telescope Interferometer (VLTI). The visibilities obtained at different
orientations clearly indicate the presence of a dusty, nearly edge-on disc in
the heart of the ne... | astro-ph | we present the discovery of a silicate disc at the centre of the planetary nebula mz3 the ant the nebula was observed with midi on the very large telescope interferometer vlti the visibilities obtained at different orientations clearly indicate the presence of a dusty nearly edgeon disc in the heart of the nebula an am... | [['we', 'present', 'the', 'discovery', 'of', 'a', 'silicate', 'disc', 'at', 'the', 'centre', 'of', 'the', 'planetary', 'nebula', 'mz3', 'the', 'ant', 'the', 'nebula', 'was', 'observed', 'with', 'midi', 'on', 'the', 'very', 'large', 'telescope', 'interferometer', 'vlti', 'the', 'visibilities', 'obtained', 'at', 'differe... | [-0.08658215012613006, 0.046047854036442, -0.08922205248170278, 0.04048136814010583, -0.060138870403170584, -0.06449263666502454, -0.04166375128763982, 0.44008268449794163, -0.21496833152857356, -0.3391208215193315, 0.046070445716296406, -0.23007436006922613, -0.06030072985555638, 0.18585018941243603, -0.03807999555190... |
710.0541 | Chiral Analysis of the Generalized Form Factors of the Nucleon | We apply the methods of Chiral Perturbation Theory to the analysis of the
first moments of the Generalized Parton Distributions in a Nucleon, usually
known as generalized form factors. These quantities are currently also under
investigation in Lattice QCD analyses of baryon structure, providing simulation
results at ... | hep-lat hep-ph nucl-th | we apply the methods of chiral perturbation theory to the analysis of the first moments of the generalized parton distributions in a nucleon usually known as generalized form factors these quantities are currently also under investigation in lattice qcd analyses of baryon structure providing simulation results at large... | [['we', 'apply', 'the', 'methods', 'of', 'chiral', 'perturbation', 'theory', 'to', 'the', 'analysis', 'of', 'the', 'first', 'moments', 'of', 'the', 'generalized', 'parton', 'distributions', 'in', 'a', 'nucleon', 'usually', 'known', 'as', 'generalized', 'form', 'factors', 'these', 'quantities', 'are', 'currently', 'also... | [-0.0608726478843842, 0.15303410488326533, -0.11658513004619146, 0.12197384559137582, -0.06293073800538167, -0.016327939747015432, 0.05942958213316061, 0.34126212634146214, -0.19787298599067998, -0.26249554230305716, 0.052151241650184, -0.2937628483197012, -0.0882710987768535, 0.128399510367387, 0.054008584510737735, 0... |
710.0542 | Nuclear skin emergence in Skyrme deformed Hartree-Fock calculations | A study of the charge and matter densities and the corresponding rms radii
for even-even isotopes of Ni, Kr, and Sn has been performed in the framework of
deformed self-consistent mean field Skyrme HF+BCS method. The resulting charge
radii and neutron skin thicknesses of these nuclei are compared with available
exper... | nucl-th | a study of the charge and matter densities and the corresponding rms radii for eveneven isotopes of ni kr and sn has been performed in the framework of deformed selfconsistent mean field skyrme hfbcs method the resulting charge radii and neutron skin thicknesses of these nuclei are compared with available experimental ... | [['a', 'study', 'of', 'the', 'charge', 'and', 'matter', 'densities', 'and', 'the', 'corresponding', 'rms', 'radii', 'for', 'eveneven', 'isotopes', 'of', 'ni', 'kr', 'and', 'sn', 'has', 'been', 'performed', 'in', 'the', 'framework', 'of', 'deformed', 'selfconsistent', 'mean', 'field', 'skyrme', 'hfbcs', 'method', 'the',... | [-0.009368459869199628, 0.1600886881196169, -0.07621583997217171, 0.11690423818121218, 0.02451952326526286, -0.05763384620678619, -0.006464518367962427, 0.36591974620809076, -0.16371243016622147, -0.3207276700291501, -0.008035986457301789, -0.34981687237829473, -5.174898190282974e-05, 0.16270156954454273, 0.01002343877... |
710.0543 | Bounds on the Light Quark Masses: the scalar channel revisited | We evaluate lower bounds on the sum of the up and down quark masses. The
bounds follow from the constraints provided by the dispersion relation obeyed
by the two--point function of the scalar current density when combined with
properties of the scalar spectral function at long--distances and perturbative
QCD at short... | hep-ph | we evaluate lower bounds on the sum of the up and down quark masses the bounds follow from the constraints provided by the dispersion relation obeyed by the twopoint function of the scalar current density when combined with properties of the scalar spectral function at longdistances and perturbative qcd at shortdistanc... | [['we', 'evaluate', 'lower', 'bounds', 'on', 'the', 'sum', 'of', 'the', 'up', 'and', 'down', 'quark', 'masses', 'the', 'bounds', 'follow', 'from', 'the', 'constraints', 'provided', 'by', 'the', 'dispersion', 'relation', 'obeyed', 'by', 'the', 'twopoint', 'function', 'of', 'the', 'scalar', 'current', 'density', 'when', ... | [-0.037229804016117536, 0.15003889936155507, -0.10749457235048925, 0.07721821081691554, -0.048759588439549716, -0.041809707866715534, 0.10624034638915743, 0.30326874059225833, -0.165353256583746, -0.32309973016381266, 0.06192477657958599, -0.31869341957249814, -0.05060350088668721, 0.20263556949794292, 0.07584432384797... |
710.0544 | Scalar-tensor analysis of an exponential Lagrangian for the
Gravitational Field | Within the scheme of modified gravity, an exponential Lagrangian density will
be considered, and the corresponding scalar-tensor description will be
addressed for both positive and negative values of the cosmological constant.
For negative values of the cosmological term, the potential of the scalar field
exhibits a ... | gr-qc | within the scheme of modified gravity an exponential lagrangian density will be considered and the corresponding scalartensor description will be addressed for both positive and negative values of the cosmological constant for negative values of the cosmological term the potential of the scalar field exhibits a minimum... | [['within', 'the', 'scheme', 'of', 'modified', 'gravity', 'an', 'exponential', 'lagrangian', 'density', 'will', 'be', 'considered', 'and', 'the', 'corresponding', 'scalartensor', 'description', 'will', 'be', 'addressed', 'for', 'both', 'positive', 'and', 'negative', 'values', 'of', 'the', 'cosmological', 'constant', 'f... | [-0.16174925147875477, 0.13768482006208385, -0.08894781642871451, 0.08020543185785524, -0.06241807496216871, -0.16169954081232757, -0.0360304563716332, 0.28721620398747333, -0.22389882116286614, -0.2606842134968002, 0.06148298777493912, -0.23189579558544862, -0.10335072893093326, 0.1752909180680429, -0.0090469338167927... |
710.0545 | Synchrotron emission from secondary leptons in microquasar jets | We present a model to estimate the synchrotron radio emission generated in
microquasar (MQ) jets due to secondary pairs created via decay of charged pions
produced in proton-proton collisions between stellar wind ions and jet
relativistic protons. Signatures of electrons/positrons are obtained from
consistent particl... | astro-ph | we present a model to estimate the synchrotron radio emission generated in microquasar mq jets due to secondary pairs created via decay of charged pions produced in protonproton collisions between stellar wind ions and jet relativistic protons signatures of electronspositrons are obtained from consistent particle energ... | [['we', 'present', 'a', 'model', 'to', 'estimate', 'the', 'synchrotron', 'radio', 'emission', 'generated', 'in', 'microquasar', 'mq', 'jets', 'due', 'to', 'secondary', 'pairs', 'created', 'via', 'decay', 'of', 'charged', 'pions', 'produced', 'in', 'protonproton', 'collisions', 'between', 'stellar', 'wind', 'ions', 'and... | [-0.031268061807195685, 0.2062172268078112, -0.06875766315991341, 0.21142541789044061, -0.07426245916620687, -0.0902242447482422, -0.011472955665367685, 0.43579932612677413, -0.24681200847650567, -0.32473904427917494, -0.018420685078264356, -0.2806202736453887, 0.0458504138950957, 0.1975630029654977, 0.0429866336229624... |
710.0546 | Surface Flows From Magnetograms | Estimates of velocities from time series of photospheric and/or chromospheric
vector magnetograms can be used to determine fluxes of magnetic energy (the
Poynting flux) and helicity across the magnetogram layer, and to provide
time-dependent boundary conditions for data-driven simulations of the solar
atmosphere abov... | astro-ph | estimates of velocities from time series of photospheric andor chromospheric vector magnetograms can be used to determine fluxes of magnetic energy the poynting flux and helicity across the magnetogram layer and to provide timedependent boundary conditions for datadriven simulations of the solar atmosphere above this l... | [['estimates', 'of', 'velocities', 'from', 'time', 'series', 'of', 'photospheric', 'andor', 'chromospheric', 'vector', 'magnetograms', 'can', 'be', 'used', 'to', 'determine', 'fluxes', 'of', 'magnetic', 'energy', 'the', 'poynting', 'flux', 'and', 'helicity', 'across', 'the', 'magnetogram', 'layer', 'and', 'to', 'provid... | [-0.11572802396695511, 0.14745865212183618, -0.05022325997244771, 0.05810531442307077, -0.140675994887838, -0.08980233244055623, -0.032612932776690376, 0.42458141196660604, -0.28730942083833116, -0.31263518383734334, 0.09425444936552695, -0.22870123810586734, -0.06705559413995052, 0.22151634004016166, -0.04455906456878... |
710.0547 | Anatomy of a Young Massive Star Cluster: NGC 1569-B | We present new H-band echelle spectra, obtained with the NIRSPEC spectrograph
at Keck II, for the massive star cluster "B" in the nearby dwarf irregular
galaxy NGC 1569. From spectral synthesis and equivalent width measurements we
obtain abundances and abundance patterns. We derive an Fe abundance of
[Fe/H]=-0.63+/-0... | astro-ph | we present new hband echelle spectra obtained with the nirspec spectrograph at keck ii for the massive star cluster b in the nearby dwarf irregular galaxy ngc 1569 from spectral synthesis and equivalent width measurements we obtain abundances and abundance patterns we derive an fe abundance of feh063008 a supersolar al... | [['we', 'present', 'new', 'hband', 'echelle', 'spectra', 'obtained', 'with', 'the', 'nirspec', 'spectrograph', 'at', 'keck', 'ii', 'for', 'the', 'massive', 'star', 'cluster', 'b', 'in', 'the', 'nearby', 'dwarf', 'irregular', 'galaxy', 'ngc', '1569', 'from', 'spectral', 'synthesis', 'and', 'equivalent', 'width', 'measur... | [-0.006173388549884339, 0.09489009284235911, -0.11309615376817643, 0.07621207209370771, -0.09552052633676555, -0.07217439148884236, 0.07223836434613837, 0.47609624924657284, -0.11231085131818917, -0.39830420834401653, 0.013968181917558378, -0.27788774247785086, 0.005947208865526606, 0.19156935522390042, -0.090199681247... |
710.0548 | Analyticity constraints on the strangeness changing vector current and
applications to $\tau\to K\pi \nu_\tau$, $\tau\to K\pi\pi \nu_\tau$ | We discuss matrix elements of the strangeness changing vector current using
their relation, due to analyticity, with $\pi K$ scattering in the $P$-wave. We
take into account experimental phase-shift measurements in the elastic channel
as well as results, obtained by the LASS collaboration, on the details of
inelastic... | hep-ph | we discuss matrix elements of the strangeness changing vector current using their relation due to analyticity with pi k scattering in the pwave we take into account experimental phaseshift measurements in the elastic channel as well as results obtained by the lass collaboration on the details of inelastic scattering wh... | [['we', 'discuss', 'matrix', 'elements', 'of', 'the', 'strangeness', 'changing', 'vector', 'current', 'using', 'their', 'relation', 'due', 'to', 'analyticity', 'with', 'pi', 'k', 'scattering', 'in', 'the', 'pwave', 'we', 'take', 'into', 'account', 'experimental', 'phaseshift', 'measurements', 'in', 'the', 'elastic', 'c... | [-0.10915373996771777, 0.23138477420036355, -0.07840831956276909, 0.07929864535347009, -0.06022396435141245, -0.12942971518555751, 0.0883446218063816, 0.3232905712360755, -0.26076501754359305, -0.20300585074095517, 0.031791900254738256, -0.34746934552915776, -0.0609290620081254, 0.1003725459982251, 0.08498942083082138,... |
710.0549 | Coulomb gauge Green functions and Gribov copies in SU(2) lattice gauge
theory | We reconsider the lattice measurement of Green functions in Coulomb gauge,
both in 2+1 and 3+1 dimensions, using an improved gauge fixing scheme. The
influence of Gribov copies is examined and we find clear indications that Green
functions are more strongly affected than previously assumed, in particular for
low mome... | hep-lat | we reconsider the lattice measurement of green functions in coulomb gauge both in 21 and 31 dimensions using an improved gauge fixing scheme the influence of gribov copies is examined and we find clear indications that green functions are more strongly affected than previously assumed in particular for low momenta qual... | [['we', 'reconsider', 'the', 'lattice', 'measurement', 'of', 'green', 'functions', 'in', 'coulomb', 'gauge', 'both', 'in', '21', 'and', '31', 'dimensions', 'using', 'an', 'improved', 'gauge', 'fixing', 'scheme', 'the', 'influence', 'of', 'gribov', 'copies', 'is', 'examined', 'and', 'we', 'find', 'clear', 'indications',... | [-0.09913654112176079, 0.14057953350867677, -0.09495408080545241, 0.09035349426878805, -0.0075000537039739065, -0.10517013310522273, 0.03830046876185182, 0.4388051812901445, -0.09162389216025063, -0.2745117817910901, 0.03549896566487471, -0.2707667528935101, -0.17253208916256393, 0.16562179954506565, -0.024186439704203... |
710.055 | Community Detection in Complex Networks by Dynamical Simplex Evolution | We benchmark the dynamical simplex evolution (DSE) method with several of the
currently available algorithms to detect communities in complex networks by
comparing the fraction of correctly identified nodes for different levels of
``fuzziness'' of random networks composed of well defined communities. The
potential be... | cond-mat.dis-nn cs.NI physics.soc-ph | we benchmark the dynamical simplex evolution dse method with several of the currently available algorithms to detect communities in complex networks by comparing the fraction of correctly identified nodes for different levels of fuzziness of random networks composed of well defined communities the potential benefits of... | [['we', 'benchmark', 'the', 'dynamical', 'simplex', 'evolution', 'dse', 'method', 'with', 'several', 'of', 'the', 'currently', 'available', 'algorithms', 'to', 'detect', 'communities', 'in', 'complex', 'networks', 'by', 'comparing', 'the', 'fraction', 'of', 'correctly', 'identified', 'nodes', 'for', 'different', 'level... | [-0.12073217862052843, 0.045699524061785915, -0.02564656702501668, 0.09174088473921105, -0.03228426405812724, -0.11116603002597389, 0.032059157752605566, 0.3930338739843692, -0.2824610098565029, -0.34559586025395633, 0.07049472602005354, -0.2683933283344416, -0.2167550186484547, 0.1534649652065867, -0.01141942237203909... |
710.0551 | 2+1 flavor QCD with the fixed point action in the $\epsilon$-regime | We generated configurations with the approximate fixed-point Dirac operator
$D_\mathrm{FP}$ on a $12^4$ lattice with $a \approx 0.13 $fm where the scale
was set by $r_0$. The distributions of the low lying eigenvalues in different
topological sectors were compared with those of the Random Matrix Theory which
leads to... | hep-lat | we generated configurations with the approximate fixedpoint dirac operator d_mathrmfp on a 124 lattice with a approx 013 fm where the scale was set by r_0 the distributions of the low lying eigenvalues in different topological sectors were compared with those of the random matrix theory which leads to a prediction of t... | [['we', 'generated', 'configurations', 'with', 'the', 'approximate', 'fixedpoint', 'dirac', 'operator', 'd_mathrmfp', 'on', 'a', '124', 'lattice', 'with', 'a', 'approx', '013', 'fm', 'where', 'the', 'scale', 'was', 'set', 'by', 'r_0', 'the', 'distributions', 'of', 'the', 'low', 'lying', 'eigenvalues', 'in', 'different'... | [-0.1254231145657185, 0.23009402768824389, -0.06624799996131549, 0.013239604834881093, -0.0031302528999124966, -0.10686877704035767, 0.06795885112067615, 0.33131440332228385, -0.19948358807919753, -0.30114649610887106, 0.09509105594716621, -0.3550609989712636, -0.08311704804913865, 0.09782942910506218, 0.01402378832507... |
710.0552 | High loop renormalization constants by NSPT: a status report | We present an update on Numerical Stochastic Perturbation Theory projects for
Lattice QCD, which are by now run on apeNEXT. As a first issue, we discuss a
strategy to tackle finite size effects which can be quite sizeable in the
computation of logarithmically divergent renormalization constants. Our first
high loop d... | hep-lat | we present an update on numerical stochastic perturbation theory projects for lattice qcd which are by now run on apenext as a first issue we discuss a strategy to tackle finite size effects which can be quite sizeable in the computation of logarithmically divergent renormalization constants our first high loop determi... | [['we', 'present', 'an', 'update', 'on', 'numerical', 'stochastic', 'perturbation', 'theory', 'projects', 'for', 'lattice', 'qcd', 'which', 'are', 'by', 'now', 'run', 'on', 'apenext', 'as', 'a', 'first', 'issue', 'we', 'discuss', 'a', 'strategy', 'to', 'tackle', 'finite', 'size', 'effects', 'which', 'can', 'be', 'quite... | [-0.10770591875044269, 0.20044905446789443, -0.12082460405593172, 0.08169012086064611, -0.08842238083028992, -0.11883464092594566, 0.08831077521777511, 0.38524260353399903, -0.18838907957066736, -0.26757261707596686, 0.09396841152100335, -0.2466293224223596, -0.09702847643886585, 0.12424808844038959, -0.027263146855685... |
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