id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
710.2953 | A Quantum Singlet Pump | We provide provide a detailed study of biasless coherent transport of singlet
electron pairs in one-dimensional (1D) channels induced by electron-electron
interactions that are time-varying in certain spatially localized regions of
the channel. When the time variation is cyclic, the mechanism is analogous to
the adia... | cond-mat.mes-hall | we provide provide a detailed study of biasless coherent transport of singlet electron pairs in onedimensional 1d channels induced by electronelectron interactions that are timevarying in certain spatially localized regions of the channel when the time variation is cyclic the mechanism is analogous to the adiabatic qua... | [['we', 'provide', 'provide', 'a', 'detailed', 'study', 'of', 'biasless', 'coherent', 'transport', 'of', 'singlet', 'electron', 'pairs', 'in', 'onedimensional', '1d', 'channels', 'induced', 'by', 'electronelectron', 'interactions', 'that', 'are', 'timevarying', 'in', 'certain', 'spatially', 'localized', 'regions', 'of'... | [-0.14209318775215699, 0.1826499089253119, -0.04189539996977877, 0.05494513288916399, -0.01235155593923421, -0.15021498034041667, 0.016615477827144787, 0.39247973617531506, -0.2572538633659646, -0.24635938800843982, 0.041808590236434934, -0.25095684887549163, -0.13646038905169597, 0.20688427539083504, 0.019457959250419... |
710.2954 | Low-Ionization Emission Regions in Quasars: Gas Properties Probed with
Broad O I and Ca II Lines | We have compiled the emission-line fluxes of O I 8446, O I 11287, and the
near-IR Ca II triplet (8579) observed in 11 quasars. These lines are considered
to emerge from the same gas as do the Fe II lines in the low-ionized portion of
the broad emission line region (BELR). The compiled quasars are distributed
over wid... | astro-ph | we have compiled the emissionline fluxes of o i 8446 o i 11287 and the nearir ca ii triplet 8579 observed in 11 quasars these lines are considered to emerge from the same gas as do the fe ii lines in the lowionized portion of the broad emission line region belr the compiled quasars are distributed over wide ranges of r... | [['we', 'have', 'compiled', 'the', 'emissionline', 'fluxes', 'of', 'o', 'i', '8446', 'o', 'i', '11287', 'and', 'the', 'nearir', 'ca', 'ii', 'triplet', '8579', 'observed', 'in', '11', 'quasars', 'these', 'lines', 'are', 'considered', 'to', 'emerge', 'from', 'the', 'same', 'gas', 'as', 'do', 'the', 'fe', 'ii', 'lines', '... | [-0.03490087013074117, 0.08082196305531397, 0.02093931871422683, 0.08350015188761972, -0.0209918348946303, -0.11779176969685068, 0.04709003188759198, 0.4744104749552207, -0.1511304846216035, -0.3162720965592598, 0.02404172476144595, -0.3066175659205328, 0.037986030406500504, 0.16043839997064424, 9.074925890217855e-05, ... |
710.2955 | A 610-MHz Galactic Plane Pulsar Search with the Giant Meterwave Radio
Telescope | We report on the discovery of three new pulsars in the first blind survey of
the north Galactic plane (45 < l < 135 ; |b| < 1) with the Giant Meterwave
Radio telescope (GMRT) at an intermediate frequency of 610 MHz. The timing
parameters, obtained in follow up observations with the Lovell Telescope at
Jodrell Bank Ob... | astro-ph | we report on the discovery of three new pulsars in the first blind survey of the north galactic plane 45 l 135 b 1 with the giant meterwave radio telescope gmrt at an intermediate frequency of 610 mhz the timing parameters obtained in follow up observations with the lovell telescope at jodrell bank observatory and the ... | [['we', 'report', 'on', 'the', 'discovery', 'of', 'three', 'new', 'pulsars', 'in', 'the', 'first', 'blind', 'survey', 'of', 'the', 'north', 'galactic', 'plane', '45', 'l', '135', 'b', '1', 'with', 'the', 'giant', 'meterwave', 'radio', 'telescope', 'gmrt', 'at', 'an', 'intermediate', 'frequency', 'of', '610', 'mhz', 'th... | [-0.1672332974434909, 0.11120409827301539, -0.012403390547892048, -0.003564289092259892, -0.17894468099762828, -0.07546477193423247, 0.10287178803424714, 0.42638089634099247, -0.11544013678459293, -0.37943798171009047, 0.16829125051607646, -0.3062741347288681, -0.0876345057040453, 0.2721339917477315, 0.0909844722314658... |
710.2956 | Near Extremal Black Hole Entropy as Entanglement Entropy via AdS2/CFT1 | We point out that the entropy of (near) extremal black holes can be
interpreted as the entanglement entropy of dual conformal quantum mechanics via
AdS2/CFT1. As an explicit example, we study near extremal BTZ black holes and
derive this claim from AdS3/CFT2. We also analytically compute the entanglement
entropy in t... | hep-th gr-qc | we point out that the entropy of near extremal black holes can be interpreted as the entanglement entropy of dual conformal quantum mechanics via ads2cft1 as an explicit example we study near extremal btz black holes and derive this claim from ads3cft2 we also analytically compute the entanglement entropy in the two di... | [['we', 'point', 'out', 'that', 'the', 'entropy', 'of', 'near', 'extremal', 'black', 'holes', 'can', 'be', 'interpreted', 'as', 'the', 'entanglement', 'entropy', 'of', 'dual', 'conformal', 'quantum', 'mechanics', 'via', 'ads2cft1', 'as', 'an', 'explicit', 'example', 'we', 'study', 'near', 'extremal', 'btz', 'black', 'h... | [-0.10654924487040102, 0.15613944125556833, -0.11879183531094056, 0.14776709396775894, 0.002854284697345325, -0.17376730580824418, 0.058413180376781705, 0.26331441407091916, -0.19208217289165727, -0.212031707935199, 0.08675454791691564, -0.3643977212512374, -0.12977289654068894, 0.17076932229255173, -0.0714072235297043... |
710.2957 | Status reports from the GRACE Group | We discuss a new approach for the numerical evaluation of loop integrals. The
fully numerical calculations of an infrared one-loop vertex and a box diagram
are demonstrated. To perform these calculations, we apply an extrapolation
method based on the $\epsilon$-algorithm. In our approach, the super high
precision con... | hep-ph | we discuss a new approach for the numerical evaluation of loop integrals the fully numerical calculations of an infrared oneloop vertex and a box diagram are demonstrated to perform these calculations we apply an extrapolation method based on the epsilonalgorithm in our approach the super high precision control in the ... | [['we', 'discuss', 'a', 'new', 'approach', 'for', 'the', 'numerical', 'evaluation', 'of', 'loop', 'integrals', 'the', 'fully', 'numerical', 'calculations', 'of', 'an', 'infrared', 'oneloop', 'vertex', 'and', 'a', 'box', 'diagram', 'are', 'demonstrated', 'to', 'perform', 'these', 'calculations', 'we', 'apply', 'an', 'ex... | [-0.08273581343970887, 0.009016113423133167, -0.1278177660775103, 0.07357803629615586, -0.05210577153077681, -0.09548912890740249, 0.06443744117062386, 0.4078343520323708, -0.21287349024659966, -0.26772402804217316, 0.11686690564567147, -0.27418326781679914, -0.16408313014735915, 0.22586732852425784, -0.030267284915157... |
710.2958 | Centre Vortices in SU(3) | We investigate the effectiveness of using smearing as a means to generate a
preconditioning transformation for gauge fields prior to fixing to Maximal
Centre Gauge. This still leaves the gauge-fixed field in the original gauge
orbit. As expected, we find that this preconditioning leads to higher maxima of
the gauge-f... | hep-lat | we investigate the effectiveness of using smearing as a means to generate a preconditioning transformation for gauge fields prior to fixing to maximal centre gauge this still leaves the gaugefixed field in the original gauge orbit as expected we find that this preconditioning leads to higher maxima of the gaugefixing c... | [['we', 'investigate', 'the', 'effectiveness', 'of', 'using', 'smearing', 'as', 'a', 'means', 'to', 'generate', 'a', 'preconditioning', 'transformation', 'for', 'gauge', 'fields', 'prior', 'to', 'fixing', 'to', 'maximal', 'centre', 'gauge', 'this', 'still', 'leaves', 'the', 'gaugefixed', 'field', 'in', 'the', 'original... | [-0.09209113851454848, 0.15419287982483193, -0.0975353048571875, 0.08791814060262453, -0.0644667819790427, -0.09838821213529206, 0.06823847991697606, 0.3625998364511839, -0.23325854211988062, -0.3516746550587188, 0.09617218653402608, -0.22227927944478915, -0.13084488948711107, 0.15587666897660063, -0.07902390533846985,... |
710.2959 | Galois Group of Elliptic Curves and Flavor Symmetry | Putting emphasis on the relation between rational conformal field theory
(RCFT) and algebraic number theory, we consider a brane configuration in which
the D-brane intersection is an elliptic curve corresponding to RCFT. A new
approach to the generation structure of fermions is proposed in which the
flavor symmetry i... | hep-th hep-ph | putting emphasis on the relation between rational conformal field theory rcft and algebraic number theory we consider a brane configuration in which the dbrane intersection is an elliptic curve corresponding to rcft a new approach to the generation structure of fermions is proposed in which the flavor symmetry includin... | [['putting', 'emphasis', 'on', 'the', 'relation', 'between', 'rational', 'conformal', 'field', 'theory', 'rcft', 'and', 'algebraic', 'number', 'theory', 'we', 'consider', 'a', 'brane', 'configuration', 'in', 'which', 'the', 'dbrane', 'intersection', 'is', 'an', 'elliptic', 'curve', 'corresponding', 'to', 'rcft', 'a', '... | [-0.20964017728277082, 0.1098745225381208, -0.12496030934354556, 0.08562340039393998, -0.12356600188026537, -0.13821434439991467, -0.022390165499213514, 0.31335676800725715, -0.27296616544897134, -0.2736179576729358, 0.07931238698594305, -0.24995465581417062, -0.1230913331336134, 0.20439247680561884, -0.086301369609178... |
710.296 | Systematic study of high-$p_T$ hadron and photon production with the
PHENIX experiment | The suppression of hadrons with large transverse momentum ($p_{\rm T}$) in
central Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 200 GeV compared to a binary
scaled p+p reference is one of the major discoveries at RHIC. To understand the
nature of this suppression PHENIX has performed detailed studies of the energy
and s... | nucl-ex | the suppression of hadrons with large transverse momentum p_rm t in central auau collisions at sqrts_rm nn 200 gev compared to a binary scaled pp reference is one of the major discoveries at rhic to understand the nature of this suppression phenix has performed detailed studies of the energy and systemsize dependence o... | [['the', 'suppression', 'of', 'hadrons', 'with', 'large', 'transverse', 'momentum', 'p_rm', 't', 'in', 'central', 'auau', 'collisions', 'at', 'sqrts_rm', 'nn', '200', 'gev', 'compared', 'to', 'a', 'binary', 'scaled', 'pp', 'reference', 'is', 'one', 'of', 'the', 'major', 'discoveries', 'at', 'rhic', 'to', 'understand', ... | [-0.09855119416397776, 0.2452560323417162, -0.16148627932247428, 0.10366956103070575, 0.011009938552805031, -0.10984499339469289, -0.047774672917026376, 0.34114909961016293, -0.22189530283070474, -0.32849421498600306, -0.05758824340824948, -0.40413347056547877, 0.14559107274444683, 0.18907041589637066, 0.06912724112866... |
710.2961 | Maximal regularity and Hardy spaces | In this work, we consider the Cauchy problem for $u' - Au = f$ with $A$ the
Laplacian operator on some Riemannian manifolds or a sublapacian on some Lie
groups or some second order elliptic operators on a domain. We show the
boundedness of the operator of maximal regularity $f\mapsto Au$ and its adjoint
on appropriat... | math.CA math.AP math.FA | in this work we consider the cauchy problem for u au f with a the laplacian operator on some riemannian manifolds or a sublapacian on some lie groups or some second order elliptic operators on a domain we show the boundedness of the operator of maximal regularity fmapsto au and its adjoint on appropriate hardy spaces w... | [['in', 'this', 'work', 'we', 'consider', 'the', 'cauchy', 'problem', 'for', 'u', 'au', 'f', 'with', 'a', 'the', 'laplacian', 'operator', 'on', 'some', 'riemannian', 'manifolds', 'or', 'a', 'sublapacian', 'on', 'some', 'lie', 'groups', 'or', 'some', 'second', 'order', 'elliptic', 'operators', 'on', 'a', 'domain', 'we',... | [-0.13854598022284514, 0.03719223271926037, -0.03981273323527457, 0.12910084818190906, -0.10076841532919602, -0.08355210723217439, -0.004478038081692325, 0.35461169613502275, -0.31721074096743523, -0.17303734334591017, 0.20363968085888542, -0.3063654870162775, -0.12367510488889191, 0.16994829648921703, -0.1176566546667... |
710.2962 | Doping-dependence of nodal quasiparticle properties in high-$T_{\rm c}$
cuprates studied by laser-excited angle-resolved photoemission spectroscopy | We investigate the doping dependent low energy, low temperature ($T$ = 5 K)
properties of nodal quasiparticles in the d-wave superconductor
Bi$_{2.1}$Sr$_{1.9}$CaCu$_2$O$_{8+\delta}$ (Bi2212). By utilizing ultrahigh
resolution laser-excited angle-resolved photoemission spectroscopy, we obtain
precise band dispersions... | cond-mat.supr-con | we investigate the doping dependent low energy low temperature t 5 k properties of nodal quasiparticles in the dwave superconductor bi_21sr_19cacu_2o_8delta bi2212 by utilizing ultrahigh resolution laserexcited angleresolved photoemission spectroscopy we obtain precise band dispersions near e_f mean free paths and scat... | [['we', 'investigate', 'the', 'doping', 'dependent', 'low', 'energy', 'low', 'temperature', 't', '5', 'k', 'properties', 'of', 'nodal', 'quasiparticles', 'in', 'the', 'dwave', 'superconductor', 'bi_21sr_19cacu_2o_8delta', 'bi2212', 'by', 'utilizing', 'ultrahigh', 'resolution', 'laserexcited', 'angleresolved', 'photoemi... | [-0.18274234358549996, 0.26350283402628694, -0.03656452314677734, 0.07084742757665902, -0.014378086565954596, -0.181674396497894, 0.18425129865836196, 0.41847626847888053, -0.23133181460874797, -0.31019852370681134, -0.09453624351822748, -0.420713737990488, 0.01426173314381735, 0.1700828658845354, 0.055678632679471686,... |
710.2963 | Cinderella - Comparison of INDEpendent RELative Least-squares Amplitudes | The identification of increasingly smaller signal from objects observed with
a non-perfect instrument in a noisy environment poses a challenge for a
statistically clean data analysis. We want to compute the probability of
frequencies determined in various data sets to be related or not, which cannot
be answered with ... | astro-ph stat.ME | the identification of increasingly smaller signal from objects observed with a nonperfect instrument in a noisy environment poses a challenge for a statistically clean data analysis we want to compute the probability of frequencies determined in various data sets to be related or not which cannot be answered with a sim... | [['the', 'identification', 'of', 'increasingly', 'smaller', 'signal', 'from', 'objects', 'observed', 'with', 'a', 'nonperfect', 'instrument', 'in', 'a', 'noisy', 'environment', 'poses', 'a', 'challenge', 'for', 'a', 'statistically', 'clean', 'data', 'analysis', 'we', 'want', 'to', 'compute', 'the', 'probability', 'of',... | [-0.07707858307615177, 0.07284915394986015, -0.10856818407244812, 0.10479210738258464, -0.05336431613735234, -0.11854336151824982, 0.07190333235044047, 0.40786475990546134, -0.2318990439128935, -0.3242939688974399, 0.1059376222286973, -0.28498827399071713, -0.08292201373842545, 0.2347297435741039, -0.06888359293842575,... |
710.2964 | Prime and zero distributions for meromorphic Euler products | The aim of the present paper is to study the relations between the prime
distribution and the zero distribution for generalized zeta functions which are
expressed by Euler products and is analytically continued as meromorphic
functions of finite order. In this paper, we give an inequality between the
order of the zet... | math.NT | the aim of the present paper is to study the relations between the prime distribution and the zero distribution for generalized zeta functions which are expressed by euler products and is analytically continued as meromorphic functions of finite order in this paper we give an inequality between the order of the zeta fu... | [['the', 'aim', 'of', 'the', 'present', 'paper', 'is', 'to', 'study', 'the', 'relations', 'between', 'the', 'prime', 'distribution', 'and', 'the', 'zero', 'distribution', 'for', 'generalized', 'zeta', 'functions', 'which', 'are', 'expressed', 'by', 'euler', 'products', 'and', 'is', 'analytically', 'continued', 'as', 'm... | [-0.1876492969302544, 0.05877891308892998, -0.14783816298108493, 0.10626584692656604, -0.03666631707838222, -0.022337233056939805, -0.004880651845527229, 0.2749181998573911, -0.3095247682406386, -0.2616469127668151, 0.07304982657877923, -0.2643979442142534, -0.16998579489317403, 0.1730631611991062, -0.00381201739186671... |
710.2965 | Running alpha(s) from Landau-gauge gluon and ghost correlations | We estimate the running coupling constant of the strong interactions within
the nonperturbative framework of lattice QCD in Landau gauge. Our calculation
is based on the ghost-gluon vertex which in the particular case of Landau gauge
allows for a definition of alpha(s) in a MOM scheme solely in terms of the
gluon and... | hep-lat | we estimate the running coupling constant of the strong interactions within the nonperturbative framework of lattice qcd in landau gauge our calculation is based on the ghostgluon vertex which in the particular case of landau gauge allows for a definition of alphas in a mom scheme solely in terms of the gluon and ghost... | [['we', 'estimate', 'the', 'running', 'coupling', 'constant', 'of', 'the', 'strong', 'interactions', 'within', 'the', 'nonperturbative', 'framework', 'of', 'lattice', 'qcd', 'in', 'landau', 'gauge', 'our', 'calculation', 'is', 'based', 'on', 'the', 'ghostgluon', 'vertex', 'which', 'in', 'the', 'particular', 'case', 'of... | [-0.13674755497797303, 0.17104719120575346, -0.10638960678375976, 0.0557262525999, -0.06875207918147518, -0.04649796513904345, 0.0912608737763885, 0.3504212978359771, -0.14871984249465678, -0.2345648770769165, 0.032395532450396315, -0.23288346186925318, -0.15059947349491518, 0.10701203938216379, 0.039566460183553705, 0... |
710.2966 | Search for W' bosons decaying to an electron and a neutrino with the D0
detector | This Letter describes the search for a new heavy charged gauge boson W'
decaying into an electron and a neutrino. The data were collected with the D0
detector at the Fermilab Tevatron proton-antiproton Collider at a
center-of-mass energy of 1.96 TeV, and correspond to an integrated luminosity
of about 1 inverse femto... | hep-ex | this letter describes the search for a new heavy charged gauge boson w decaying into an electron and a neutrino the data were collected with the d0 detector at the fermilab tevatron protonantiproton collider at a centerofmass energy of 196 tev and correspond to an integrated luminosity of about 1 inverse femtobarn lack... | [['this', 'letter', 'describes', 'the', 'search', 'for', 'a', 'new', 'heavy', 'charged', 'gauge', 'boson', 'w', 'decaying', 'into', 'an', 'electron', 'and', 'a', 'neutrino', 'the', 'data', 'were', 'collected', 'with', 'the', 'd0', 'detector', 'at', 'the', 'fermilab', 'tevatron', 'protonantiproton', 'collider', 'at', 'a... | [-0.043315231553216496, 0.21749197887857008, -0.02120869010520567, 0.11325556656811386, -0.05010698946924614, -0.13086532379799923, 0.07547963575260448, 0.31706857769417446, -0.16349456445667393, -0.36670563629429254, 0.01622471221864024, -0.4032150615572131, 0.13895766020453135, 0.19770440160729258, 0.0717599006727271... |
710.2967 | Theory of pairing symmetry inside the Abrikosov vortex core | We show that the Cooper pair wave function at the center of an Abrikosov
vortex with vorticity m has different parity with respect to frequency from
that in the bulk if m is an odd number and has the same parity if m is an even
number. As a result, in a conventional vortex with m=1, the local density of
states at the... | cond-mat.supr-con | we show that the cooper pair wave function at the center of an abrikosov vortex with vorticity m has different parity with respect to frequency from that in the bulk if m is an odd number and has the same parity if m is an even number as a result in a conventional vortex with m1 the local density of states at the fermi... | [['we', 'show', 'that', 'the', 'cooper', 'pair', 'wave', 'function', 'at', 'the', 'center', 'of', 'an', 'abrikosov', 'vortex', 'with', 'vorticity', 'm', 'has', 'different', 'parity', 'with', 'respect', 'to', 'frequency', 'from', 'that', 'in', 'the', 'bulk', 'if', 'm', 'is', 'an', 'odd', 'number', 'and', 'has', 'the', '... | [-0.21976320142106665, 0.19434943429606852, -0.09719578695974203, 0.017891004649041, -0.03680351660186325, -0.13195993672675824, 0.050297282415852754, 0.331169886832496, -0.23045780608851102, -0.2957004951044006, -0.013886974983027465, -0.3176371115009471, -0.05633717770588093, 0.14150497020642844, 0.012866203953582112... |
710.2968 | Gravitino Dark Matter with Weak-Scale Right-Handed Sneutrino | We consider cosmological implications of supersymmetric models with
right-handed (s)neutrinos where the neutrino masses are purely Dirac-type. We
pay particular attention to the case where gravitino is the lightest
superparticle while one of the right-handed sneutrinos is next-to-the-lightest
superparticle. We study ... | hep-ph | we consider cosmological implications of supersymmetric models with righthanded sneutrinos where the neutrino masses are purely diractype we pay particular attention to the case where gravitino is the lightest superparticle while one of the righthanded sneutrinos is nexttothelightest superparticle we study constraints ... | [['we', 'consider', 'cosmological', 'implications', 'of', 'supersymmetric', 'models', 'with', 'righthanded', 'sneutrinos', 'where', 'the', 'neutrino', 'masses', 'are', 'purely', 'diractype', 'we', 'pay', 'particular', 'attention', 'to', 'the', 'case', 'where', 'gravitino', 'is', 'the', 'lightest', 'superparticle', 'whi... | [-0.09582230140479793, 0.25130139833596427, -0.027017862185736936, 0.2031139264416889, -0.1439256235067032, -0.16295676996346267, -0.00933422905030306, 0.29948137994171575, -0.22230408558275846, -0.33759912775944817, 0.10894939205835912, -0.26135838555946816, 0.0010141789319768415, 0.15176259093110211, -0.0030866254005... |
710.2969 | On sensitivity calculations for neutrino oscillation experiments | Calculations of sensitivities of future experiments are a necessary
ingredient in experimental high energy physics. Especially in the context of
measurements of the neutrino oscillation parameters extensive studies are
performed to arrive at the optimal configuration. In this note we clarify the
definition of sensiti... | hep-ph | calculations of sensitivities of future experiments are a necessary ingredient in experimental high energy physics especially in the context of measurements of the neutrino oscillation parameters extensive studies are performed to arrive at the optimal configuration in this note we clarify the definition of sensitivity... | [['calculations', 'of', 'sensitivities', 'of', 'future', 'experiments', 'are', 'a', 'necessary', 'ingredient', 'in', 'experimental', 'high', 'energy', 'physics', 'especially', 'in', 'the', 'context', 'of', 'measurements', 'of', 'the', 'neutrino', 'oscillation', 'parameters', 'extensive', 'studies', 'are', 'performed', ... | [-0.09313417103193286, 0.08012987340076103, -0.0758459140236179, 0.10950217712670565, -0.034475049296290514, -0.05039171196209888, 0.068152138704641, 0.36403014527426825, -0.2110540413414128, -0.34365807025072476, 0.11099217663415605, -0.2773969177984529, -0.12131087161186668, 0.23176361113114075, -0.014079385457767381... |
710.297 | A generic attack to ciphers | In this paper, we present a generic attack for ciphers, which is in essence a
collision attack on the secret keys of ciphers .
| cs.CR | in this paper we present a generic attack for ciphers which is in essence a collision attack on the secret keys of ciphers | [['in', 'this', 'paper', 'we', 'present', 'a', 'generic', 'attack', 'for', 'ciphers', 'which', 'is', 'in', 'essence', 'a', 'collision', 'attack', 'on', 'the', 'secret', 'keys', 'of', 'ciphers']] | [-0.27815454275063844, -0.028909064059996086, -0.12051717200033042, 0.06311992604447447, 0.014893462395538454, -0.2590643842502133, 0.06973387178985159, 0.27260861080139875, -0.24649591517189276, -0.18436258512994516, 0.16881687438074985, -0.265323202247205, -0.1932019733864328, 0.1782899954882653, -0.2093208746417709,... |
710.2971 | Analysis of $K^+ \to e^+ \nu_{e}\gamma$ in light-front quark model and
chiral perturbation theory of order $p^6$ | Within the frameworks of the light-front quark model (LFQM) and chiral
perturbation theory (ChPT) of $O(p^6)$, we reevaluate the form factors of the
$K^+ \to \gamma$ transition. We use these form factors to study the decay of
$K^+ \to e^+ \nu_{e}\gamma$, which is dominated by the structure dependent
contribution. We ... | hep-ph hep-ex | within the frameworks of the lightfront quark model lfqm and chiral perturbation theory chpt of op6 we reevaluate the form factors of the k to gamma transition we use these form factors to study the decay of k to e nu_egamma which is dominated by the structure dependent contribution we show the differential decay branc... | [['within', 'the', 'frameworks', 'of', 'the', 'lightfront', 'quark', 'model', 'lfqm', 'and', 'chiral', 'perturbation', 'theory', 'chpt', 'of', 'op6', 'we', 'reevaluate', 'the', 'form', 'factors', 'of', 'the', 'k', 'to', 'gamma', 'transition', 'we', 'use', 'these', 'form', 'factors', 'to', 'study', 'the', 'decay', 'of',... | [-0.10150759371306496, 0.19851781015705244, -0.07321025795177914, 0.0702081863363184, -0.024194056826392904, -0.05898998314380431, 0.11450082336243493, 0.3234188371481231, -0.20361447252798826, -0.27998439072129816, -0.02693641951415115, -0.332258523755277, -0.04190248597520762, 0.09098705280876647, 0.09062476583998293... |
710.2972 | Z Pole Observables in the MSSM | We present the currently most accurate prediction of Z pole observables such
as sin^2 theta_eff, Gamma_Z, R_b, R_l, and sigma^0_had in the Minimal
Supersymmetric Standard Model (MSSM). We take into account the complete
one-loop results including the full complex phase dependence, all available
MSSM two-loop correctio... | hep-ph | we present the currently most accurate prediction of z pole observables such as sin2 theta_eff gamma_z r_b r_l and sigma0_had in the minimal supersymmetric standard model mssm we take into account the complete oneloop results including the full complex phase dependence all available mssm twoloop corrections as well as ... | [['we', 'present', 'the', 'currently', 'most', 'accurate', 'prediction', 'of', 'z', 'pole', 'observables', 'such', 'as', 'sin2', 'theta_eff', 'gamma_z', 'r_b', 'r_l', 'and', 'sigma0_had', 'in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'we', 'take', 'into', 'account', 'the', 'complete', 'oneloop'... | [-0.08029300208683267, 0.1771858093642081, -0.017808516929631656, 0.19122201784612666, -0.07127283224624327, -0.12234817459036341, 0.04810904863530375, 0.2991381262633667, -0.14928826527532443, -0.25756547337567265, 0.04540646026725881, -0.3089163454697524, -0.04648415907506591, 0.1695493734706278, 0.047594555004528076... |
710.2973 | Local Convexity Properties of Quasihyperbolic Balls in Punctured Space | This paper deals with local convexity properties of the quasihyperbolic
metric in the punctured space. We consider convexity and starlikeness of
quasihyperbolic balls.
| math.MG | this paper deals with local convexity properties of the quasihyperbolic metric in the punctured space we consider convexity and starlikeness of quasihyperbolic balls | [['this', 'paper', 'deals', 'with', 'local', 'convexity', 'properties', 'of', 'the', 'quasihyperbolic', 'metric', 'in', 'the', 'punctured', 'space', 'we', 'consider', 'convexity', 'and', 'starlikeness', 'of', 'quasihyperbolic', 'balls']] | [-0.23196735872846583, -0.014546044342948691, -0.05543086912644946, 0.11073091741064159, -0.10934433494896992, -0.03724554027228252, -0.02108517588298444, 0.37923209369182587, -0.34020707027419755, -0.14508729650760474, 0.13635519203102298, -0.34690610185751447, -0.13677945020406143, 0.07052958108808684, -0.30238461121... |
710.2974 | Separable p-harmonic functions in a cone and related quasilinear
equations on manifolds | In considering a class of quasilinear elliptic equations on a Riemannian
manifold with nonnegative Ricci curvature, we give a new proof of Tolksdorf's
result on the construction of separable $p$-harmonic functions in a cone.
| math.AP | in considering a class of quasilinear elliptic equations on a riemannian manifold with nonnegative ricci curvature we give a new proof of tolksdorfs result on the construction of separable pharmonic functions in a cone | [['in', 'considering', 'a', 'class', 'of', 'quasilinear', 'elliptic', 'equations', 'on', 'a', 'riemannian', 'manifold', 'with', 'nonnegative', 'ricci', 'curvature', 'we', 'give', 'a', 'new', 'proof', 'of', 'tolksdorfs', 'result', 'on', 'the', 'construction', 'of', 'separable', 'pharmonic', 'functions', 'in', 'a', 'cone... | [-0.20585886422883382, 0.02572697437735218, -0.13986323220711766, 0.05308930640757987, -0.15439709106629546, -0.17308284381799627, -0.09669927298796899, 0.2911690828023535, -0.2717586997331995, -0.1806973757391626, 0.10768268169891654, -0.28247199732471595, -0.14911161893696495, 0.2212640157279869, -0.12614620584204342... |
710.2975 | Study of Stability of a Charged Topological Soliton in the System of Two
Interacting Scalar Fields | An analytical-numerical analysis of the singular self-adjoint spectral
problem for a system of three linear ordinary second-order differential
equations defined on the entire real exis is presented. This problem comes to
existence in the nonlinear field theory. The dependence of the differential
equations on the spec... | hep-th math-ph math.MP | an analyticalnumerical analysis of the singular selfadjoint spectral problem for a system of three linear ordinary secondorder differential equations defined on the entire real exis is presented this problem comes to existence in the nonlinear field theory the dependence of the differential equations on the spectral pa... | [['an', 'analyticalnumerical', 'analysis', 'of', 'the', 'singular', 'selfadjoint', 'spectral', 'problem', 'for', 'a', 'system', 'of', 'three', 'linear', 'ordinary', 'secondorder', 'differential', 'equations', 'defined', 'on', 'the', 'entire', 'real', 'exis', 'is', 'presented', 'this', 'problem', 'comes', 'to', 'existen... | [-0.17823454647025624, 0.0022820510974790004, -0.08623255151906051, 0.046621671264542135, -0.13061527365685574, -0.1044174388683002, -0.09606578769203875, 0.24145229559923923, -0.32753421851832953, -0.2213486637587526, 0.11299466084372918, -0.3175934818573296, -0.1899320026859641, 0.20563905825838447, -0.03523457974993... |
710.2976 | A note on the Hamiltonian formalism for higher-derivative theories | An alternative version of Hamiltonian formalism for higher-derivative
theories is presented. It is related to the standard Ostrogradski approach by a
canonical transformation. The advantage of the approach presented is that the
Lagrangian is nonsingular and the Legendre transformation is performed in a
straightforwar... | hep-th | an alternative version of hamiltonian formalism for higherderivative theories is presented it is related to the standard ostrogradski approach by a canonical transformation the advantage of the approach presented is that the lagrangian is nonsingular and the legendre transformation is performed in a straightforward way | [['an', 'alternative', 'version', 'of', 'hamiltonian', 'formalism', 'for', 'higherderivative', 'theories', 'is', 'presented', 'it', 'is', 'related', 'to', 'the', 'standard', 'ostrogradski', 'approach', 'by', 'a', 'canonical', 'transformation', 'the', 'advantage', 'of', 'the', 'approach', 'presented', 'is', 'that', 'the... | [-0.11554291396298343, 0.05901908310835198, -0.1838631123718288, 0.08789215485513624, -0.11749183473487695, -0.12635048509885868, -0.06510436145795716, 0.3161010804275672, -0.2493318441013495, -0.2380944713536236, 0.03152766276099202, -0.23345922815303008, -0.23594199766715368, 0.1794242756234275, -0.07498754465745555,... |
710.2977 | An explicit formula for the Skorokhod map on $[0,a]$ | The Skorokhod map is a convenient tool for constructing solutions to
stochastic differential equations with reflecting boundary conditions. In this
work, an explicit formula for the Skorokhod map $\Gamma_{0,a}$ on $[0,a]$ for
any $a>0$ is derived. Specifically, it is shown that on the space
$\mathcal{D}[0,\infty)$ of... | math.PR | the skorokhod map is a convenient tool for constructing solutions to stochastic differential equations with reflecting boundary conditions in this work an explicit formula for the skorokhod map gamma_0a on 0a for any a0 is derived specifically it is shown that on the space mathcald0infty of rightcontinuous functions wi... | [['the', 'skorokhod', 'map', 'is', 'a', 'convenient', 'tool', 'for', 'constructing', 'solutions', 'to', 'stochastic', 'differential', 'equations', 'with', 'reflecting', 'boundary', 'conditions', 'in', 'this', 'work', 'an', 'explicit', 'formula', 'for', 'the', 'skorokhod', 'map', 'gamma_0a', 'on', '0a', 'for', 'any', 'a... | [-0.08477274857543628, 0.06329302800535087, -0.05222472331815344, 0.06453720370773226, -0.0803322218495476, -0.12603170520571225, -0.014433695102000937, 0.3862825965618386, -0.26803017297540516, -0.18868040257023977, 0.14354780076537282, -0.2725463512189248, -0.13267688375404652, 0.2505518833284869, -0.0819275574758648... |
710.2978 | Consistency conditions in the chiral ring of super Yang-Mills theories | Starting from the generalized Konishi anomaly equations at the
non-perturbative level, we demonstrate that the algebraic consistency of the
quantum chiral ring of the N=1 super Yang-Mills theory with gauge group U(N),
one adjoint chiral superfield X and N_f<=2N flavours of quarks implies that the
periods of the merom... | hep-th | starting from the generalized konishi anomaly equations at the nonperturbative level we demonstrate that the algebraic consistency of the quantum chiral ring of the n1 super yangmills theory with gauge group un one adjoint chiral superfield x and n_f2n flavours of quarks implies that the periods of the meromorphic onef... | [['starting', 'from', 'the', 'generalized', 'konishi', 'anomaly', 'equations', 'at', 'the', 'nonperturbative', 'level', 'we', 'demonstrate', 'that', 'the', 'algebraic', 'consistency', 'of', 'the', 'quantum', 'chiral', 'ring', 'of', 'the', 'n1', 'super', 'yangmills', 'theory', 'with', 'gauge', 'group', 'un', 'one', 'adj... | [-0.19133188796815337, 0.2154741333029473, -0.12341168490130473, 0.07731582362987294, -0.06709242346168486, -0.12942421057659978, -0.027552382382036177, 0.268330872663748, -0.21843164100206083, -0.21289117336417213, 0.05386724192937164, -0.26044540791010207, -0.1798175459333993, 0.08850640394561685, -0.0424605975522822... |
710.2979 | Search for the decays $J/\psi\to\gamma \rho \phi$ and $J/\psi\to\gamma
\rho \omega$ | Using 58 million $J/\psi$ events collected with the Beijing Spectrometer
(BESII) at the Beijing Electron-Positron Collider, the decays $J/\psi\to
\gamma\phi\rho$ and $J/\psi\to \gamma\omega\rho$ are searched for, and upper
limits on their branching fractions are reported at the 90% C. L. No clear
structures are obser... | hep-ex | using 58 million jpsi events collected with the beijing spectrometer besii at the beijing electronpositron collider the decays jpsito gammaphirho and jpsito gammaomegarho are searched for and upper limits on their branching fractions are reported at the 90 c l no clear structures are observed in the gamma rho gamma phi... | [['using', '58', 'million', 'jpsi', 'events', 'collected', 'with', 'the', 'beijing', 'spectrometer', 'besii', 'at', 'the', 'beijing', 'electronpositron', 'collider', 'the', 'decays', 'jpsito', 'gammaphirho', 'and', 'jpsito', 'gammaomegarho', 'are', 'searched', 'for', 'and', 'upper', 'limits', 'on', 'their', 'branching'... | [-0.13391010944615117, 0.2586440303495952, -0.09183956310818238, 0.12305139623848456, -0.028296706745667116, -0.12875523237245423, 0.10329035393660888, 0.34752673194078465, -0.13873710468968575, -0.26869763817105974, -0.0471187074701967, -0.47021110377141406, 0.12773893659801355, 0.22119843439930784, 0.1648691078847540... |
710.298 | A generalization of Snoek's law to ferromagnetic films and composites | The present paper establishes characteristics of the relative magnetic
permeability spectrum $\mu$(f) of magnetic materials at microwave frequencies.
The integral of the imaginary part of $\mu$(f) multiplied with the frequency f
gives remarkable properties. A generalisation of Snoek's law consists in this
quantity be... | physics.optics | the present paper establishes characteristics of the relative magnetic permeability spectrum muf of magnetic materials at microwave frequencies the integral of the imaginary part of muf multiplied with the frequency f gives remarkable properties a generalisation of snoeks law consists in this quantity being bounded by ... | [['the', 'present', 'paper', 'establishes', 'characteristics', 'of', 'the', 'relative', 'magnetic', 'permeability', 'spectrum', 'muf', 'of', 'magnetic', 'materials', 'at', 'microwave', 'frequencies', 'the', 'integral', 'of', 'the', 'imaginary', 'part', 'of', 'muf', 'multiplied', 'with', 'the', 'frequency', 'f', 'gives'... | [-0.1445021542908294, 0.12508627758342236, -0.039440175616124895, -0.003445589542197286, -0.08545893406372809, -0.09615776645318594, 0.020025411292569475, 0.4001114617749558, -0.23225499542215416, -0.3001519897080759, 0.08234110674145344, -0.2945528020726569, -0.137593818449994, 0.2739340482804725, -0.0007869276838998,... |
710.2981 | Relativistic electrodynamics as an extrapolation of relativistic
kinematics | After having identified all the possible relationships between the electric
field and the magnetic field in a given inertial reference frame we derive the
transformation equations for the components of these fields. Special relativity
is involved via the addition law of parallel speeds or via the Lorentz
transformati... | physics.gen-ph | after having identified all the possible relationships between the electric field and the magnetic field in a given inertial reference frame we derive the transformation equations for the components of these fields special relativity is involved via the addition law of parallel speeds or via the lorentz transformations... | [['after', 'having', 'identified', 'all', 'the', 'possible', 'relationships', 'between', 'the', 'electric', 'field', 'and', 'the', 'magnetic', 'field', 'in', 'a', 'given', 'inertial', 'reference', 'frame', 'we', 'derive', 'the', 'transformation', 'equations', 'for', 'the', 'components', 'of', 'these', 'fields', 'specia... | [-0.17373863037953036, 0.1429776338305562, -0.06695917772037532, 0.04410079576352492, -0.07780659091262583, -0.09016282022732527, 0.010236869328358073, 0.3235817574747303, -0.2822412170130423, -0.315030057062494, 0.049594080359229145, -0.23319494888988979, -0.12707633389645515, 0.19704502473208815, 0.000448648015314594... |
710.2982 | MSSM precision physics at the Z resonance | LEP and SLC provide accurate data on the process (e^+e^- -> f bar f) at the Z
resonance. The GigaZ option at a future linear e^+e^- collider (ILC) will
further improve these measurements. As a consequence, theory predictions with
sufficiently smaller errors are necessary in order to fully exploit the
experimental acc... | hep-ph | lep and slc provide accurate data on the process ee f bar f at the z resonance the gigaz option at a future linear ee collider ilc will further improve these measurements as a consequence theory predictions with sufficiently smaller errors are necessary in order to fully exploit the experimental accuracies and to deriv... | [['lep', 'and', 'slc', 'provide', 'accurate', 'data', 'on', 'the', 'process', 'ee', 'f', 'bar', 'f', 'at', 'the', 'z', 'resonance', 'the', 'gigaz', 'option', 'at', 'a', 'future', 'linear', 'ee', 'collider', 'ilc', 'will', 'further', 'improve', 'these', 'measurements', 'as', 'a', 'consequence', 'theory', 'predictions', ... | [-0.04529764754697681, 0.12296863823076305, -0.030880430114010107, 0.1674906188000339, -0.09650754851653524, -0.16128322170723391, 0.03629156386874535, 0.3020110742431944, -0.2124486956451817, -0.2887838235894299, 0.09121821048952963, -0.3314354977125059, -0.04551524221492202, 0.21444749463471058, 0.06545031315687558, ... |
710.2983 | Experimental Test of Momentum Cooling Model Predictions at COSY and
Conclusions for WASA and HESR | The High-Energy Storage Ring (HESR) of the future International Facility for
Antiproton and Ion Research (FAIR) at GSI in Darmstadt is planned as an
anti-proton cooler ring in the momentum range from 1.5 to 15 GeV/c. An
important and challenging feature of the new facility is the combination of
highly dense phase spa... | nucl-ex | the highenergy storage ring hesr of the future international facility for antiproton and ion research fair at gsi in darmstadt is planned as an antiproton cooler ring in the momentum range from 15 to 15 gevc an important and challenging feature of the new facility is the combination of highly dense phase space cooled b... | [['the', 'highenergy', 'storage', 'ring', 'hesr', 'of', 'the', 'future', 'international', 'facility', 'for', 'antiproton', 'and', 'ion', 'research', 'fair', 'at', 'gsi', 'in', 'darmstadt', 'is', 'planned', 'as', 'an', 'antiproton', 'cooler', 'ring', 'in', 'the', 'momentum', 'range', 'from', '15', 'to', '15', 'gevc', 'a... | [-0.059256440674452564, 0.14077068873829657, -0.10444506816726563, 0.025062325145599657, -0.05109184553910946, -0.14529303879766114, 0.024791928470648567, 0.4150763412006199, -0.22015441150629314, -0.31254692248807386, 0.04402884140305607, -0.3074778241972471, 0.06115589404221752, 0.24759587866157806, 0.041325230087185... |
710.2984 | Polarizational stopping power of heavy-ion diclusters in two-dimensional
electron liquids | The in-plane polarizational stopping power of heavy-ion diclusters in a
two-dimensional strongly coupled electron liquid is studied. Analytical
expressions for the stopping power of both fast and slow projectiles are
derived. To go beyond the random-phase approximation we make use of the inverse
dielectric function o... | cond-mat.str-el | the inplane polarizational stopping power of heavyion diclusters in a twodimensional strongly coupled electron liquid is studied analytical expressions for the stopping power of both fast and slow projectiles are derived to go beyond the randomphase approximation we make use of the inverse dielectric function obtained ... | [['the', 'inplane', 'polarizational', 'stopping', 'power', 'of', 'heavyion', 'diclusters', 'in', 'a', 'twodimensional', 'strongly', 'coupled', 'electron', 'liquid', 'is', 'studied', 'analytical', 'expressions', 'for', 'the', 'stopping', 'power', 'of', 'both', 'fast', 'and', 'slow', 'projectiles', 'are', 'derived', 'to'... | [-0.08868323172509918, 0.1137173696042737, -0.07884964332333766, 0.08458402154246869, -0.023719624034129083, -0.1316747332457453, 0.02161777679430088, 0.37371529209485743, -0.24290689415647648, -0.23887810931773856, 0.022463315193817834, -0.29979134362656623, -0.09464391091023572, 0.212631625297945, 0.07265668872423703... |
710.2985 | LSND versus MiniBooNE: Sterile neutrinos with energy dependent masses
and mixing? | Standard active--sterile neutrino oscillations do not provide a satisfactory
description of the LSND evidence for neutrino oscillations together with the
constraints from MiniBooNE and other null-result short-baseline oscillation
experiments. However, if the mass or the mixing of the sterile neutrino depends
in an ex... | hep-ph | standard activesterile neutrino oscillations do not provide a satisfactory description of the lsnd evidence for neutrino oscillations together with the constraints from miniboone and other nullresult shortbaseline oscillation experiments however if the mass or the mixing of the sterile neutrino depends in an exotic way... | [['standard', 'activesterile', 'neutrino', 'oscillations', 'do', 'not', 'provide', 'a', 'satisfactory', 'description', 'of', 'the', 'lsnd', 'evidence', 'for', 'neutrino', 'oscillations', 'together', 'with', 'the', 'constraints', 'from', 'miniboone', 'and', 'other', 'nullresult', 'shortbaseline', 'oscillation', 'experim... | [-0.07096672689061094, 0.26593746998070183, 0.00218480620039812, 0.18100963842928633, -0.06919830517218115, -0.1479756876075369, 0.0700851489561579, 0.27290666397562285, -0.21100770676853936, -0.36688600986192177, 0.04628075714861444, -0.3486634368039914, 0.008956493177630056, 0.22304913806590246, 0.04292519042724805, ... |
710.2986 | Dissipationless Disk Accretion | We consider disk accretion resulting purely from the loss of angular momentum
due to the outflow of plasma from a magnetized disk. In this limiting case, the
dissipation due to the viscosity and finite electrical conductivity of the
plasma can be neglected. We have obtained self-consistent, self-similar
solutions for... | astro-ph | we consider disk accretion resulting purely from the loss of angular momentum due to the outflow of plasma from a magnetized disk in this limiting case the dissipation due to the viscosity and finite electrical conductivity of the plasma can be neglected we have obtained selfconsistent selfsimilar solutions for dissipa... | [['we', 'consider', 'disk', 'accretion', 'resulting', 'purely', 'from', 'the', 'loss', 'of', 'angular', 'momentum', 'due', 'to', 'the', 'outflow', 'of', 'plasma', 'from', 'a', 'magnetized', 'disk', 'in', 'this', 'limiting', 'case', 'the', 'dissipation', 'due', 'to', 'the', 'viscosity', 'and', 'finite', 'electrical', 'c... | [-0.10271869220550318, 0.14885269127492057, -0.05559341851499324, 0.07043161677460089, -0.08356647186079308, -0.012992105894035808, -0.027199439292369215, 0.3777957164045227, -0.24343852492931642, -0.31656032283545327, 0.06276640739739187, -0.2540963791114719, 0.03479821461032292, 0.2267403456406962, -0.048561657570596... |
710.2987 | An unconditionnally stable pressure correction scheme for compressible
barotropic Navier-Stokes equations | We present in this paper a pressure correction scheme for barotropic
compressible Navier-Stokes equations, which enjoys an unconditional stability
property, in the sense that the energy and maximum-principle-based a priori
estimates of the continuous problem also hold for the discrete solution. The
stability proof is... | math.NA | we present in this paper a pressure correction scheme for barotropic compressible navierstokes equations which enjoys an unconditional stability property in the sense that the energy and maximumprinciplebased a priori estimates of the continuous problem also hold for the discrete solution the stability proof is based o... | [['we', 'present', 'in', 'this', 'paper', 'a', 'pressure', 'correction', 'scheme', 'for', 'barotropic', 'compressible', 'navierstokes', 'equations', 'which', 'enjoys', 'an', 'unconditional', 'stability', 'property', 'in', 'the', 'sense', 'that', 'the', 'energy', 'and', 'maximumprinciplebased', 'a', 'priori', 'estimates... | [-0.10751116849824793, 0.061665750787816484, -0.1201358633075183, 0.03745341621554242, -0.07374358585697006, -0.10395074551729681, 0.03425811800920124, 0.32731960435117874, -0.2792556016914338, -0.2519004429475619, 0.1450404249248909, -0.2385409756765499, -0.08945510940751634, 0.18135819223325153, -0.07922429141386614,... |
710.2988 | Using Description Logics for Recognising Textual Entailment | The aim of this paper is to show how we can handle the Recognising Textual
Entailment (RTE) task by using Description Logics (DLs). To do this, we propose
a representation of natural language semantics in DLs inspired by existing
representations in first-order logic. But our most significant contribution is
the defin... | cs.CL | the aim of this paper is to show how we can handle the recognising textual entailment rte task by using description logics dls to do this we propose a representation of natural language semantics in dls inspired by existing representations in firstorder logic but our most significant contribution is the definition of t... | [['the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'show', 'how', 'we', 'can', 'handle', 'the', 'recognising', 'textual', 'entailment', 'rte', 'task', 'by', 'using', 'description', 'logics', 'dls', 'to', 'do', 'this', 'we', 'propose', 'a', 'representation', 'of', 'natural', 'language', 'semantics', 'in', 'dls', 'inspir... | [-0.043626532846035945, -0.007255115006388962, -0.08841274858222924, 0.10536401237671573, -0.20641380845420604, -0.11491009519448962, 0.04317798083681829, 0.4197782725635646, -0.3228290799036757, -0.3427575209542461, 0.018831021945410663, -0.26323553288112517, -0.17664127580929492, 0.15805509787869465, -0.1810315962057... |
710.2989 | CO, HI, recent Spitzer SAGE results in the Large Magellanic Cloud | Formation of GMCs is one of the most crucial issues in galaxy evolution. I
will compare CO and HI in the LMC in 3 dimensional space for the first time
aiming at revealing the physical connection between GMCs and associated HI gas
at a ~40 pc scale. The present major findings are 1) [total CO intensity]
[total HI inte... | astro-ph | formation of gmcs is one of the most crucial issues in galaxy evolution i will compare co and hi in the lmc in 3 dimensional space for the first time aiming at revealing the physical connection between gmcs and associated hi gas at a 40 pc scale the present major findings are 1 total co intensity total hi intensity08 f... | [['formation', 'of', 'gmcs', 'is', 'one', 'of', 'the', 'most', 'crucial', 'issues', 'in', 'galaxy', 'evolution', 'i', 'will', 'compare', 'co', 'and', 'hi', 'in', 'the', 'lmc', 'in', '3', 'dimensional', 'space', 'for', 'the', 'first', 'time', 'aiming', 'at', 'revealing', 'the', 'physical', 'connection', 'between', 'gmcs... | [-0.10742241504442424, 0.09561224196352495, 0.0027660241625695066, 0.08960067005616358, 0.0030805918211040417, 0.005233283991702209, 0.011603565800026798, 0.4169560568907475, -0.17901959083685728, -0.3217244311120392, 0.053522161891191335, -0.25274016152420814, -0.06698547252107503, 0.1438640374103407, 0.03144942040839... |
710.299 | Invariant variational principle for Hamiltonian mechanics | It is shown that the action for Hamiltonian equations of motion can be
brought into invariant symplectic form. In other words, it can be formulated
directly in terms of the symplectic structure $\omega$ without any need to
choose some 1-form $\gamma$, such that $\omega= d \gamma$, which is not unique
and does not eve... | math-ph math.DS math.MP | it is shown that the action for hamiltonian equations of motion can be brought into invariant symplectic form in other words it can be formulated directly in terms of the symplectic structure omega without any need to choose some 1form gamma such that omega d gamma which is not unique and does not even generally exist ... | [['it', 'is', 'shown', 'that', 'the', 'action', 'for', 'hamiltonian', 'equations', 'of', 'motion', 'can', 'be', 'brought', 'into', 'invariant', 'symplectic', 'form', 'in', 'other', 'words', 'it', 'can', 'be', 'formulated', 'directly', 'in', 'terms', 'of', 'the', 'symplectic', 'structure', 'omega', 'without', 'any', 'ne... | [-0.15234988271064745, 0.14946521455422043, -0.13287140351409713, 0.06316028849299377, -0.1694187297175328, -0.17789340608287602, -0.026088195852935314, 0.3727915738010779, -0.3376409144761662, -0.2557576443922395, 0.06596544903489605, -0.22220028097120423, -0.18015729719772935, 0.17007875304067663, -0.0900395062208796... |
710.2991 | Moment Methods for Exotic Volatility Derivatives | The latest generation of volatility derivatives goes beyond variance and
volatility swaps and probes our ability to price realized variance and sojourn
times along bridges for the underlying stock price process. In this paper, we
give an operator algebraic treatment of this problem based on Dyson expansions
and momen... | q-fin.ST math.GN math.PR | the latest generation of volatility derivatives goes beyond variance and volatility swaps and probes our ability to price realized variance and sojourn times along bridges for the underlying stock price process in this paper we give an operator algebraic treatment of this problem based on dyson expansions and moment me... | [['the', 'latest', 'generation', 'of', 'volatility', 'derivatives', 'goes', 'beyond', 'variance', 'and', 'volatility', 'swaps', 'and', 'probes', 'our', 'ability', 'to', 'price', 'realized', 'variance', 'and', 'sojourn', 'times', 'along', 'bridges', 'for', 'the', 'underlying', 'stock', 'price', 'process', 'in', 'this', ... | [-0.06472059180183957, 0.08019917287805987, -0.07442726862306397, 0.18790875502046825, -0.10647805125659539, -0.13552563213549243, 0.08186067465430824, 0.42789965003935826, -0.28253640099299243, -0.23078666749643162, 0.1624347461119113, -0.27894554734424065, -0.10947906996362791, 0.19451138620691685, -0.113672701833416... |
710.2992 | Urban traffic from the perspective of dual graph | In this paper, urban traffic is modeled using dual graph representation of
urban transportation network where roads are mapped to nodes and intersections
are mapped to links. The proposed model considers both the navigation of
vehicles on the network and the motion of vehicles along roads. The road's
capacity and the... | physics.soc-ph physics.data-an | in this paper urban traffic is modeled using dual graph representation of urban transportation network where roads are mapped to nodes and intersections are mapped to links the proposed model considers both the navigation of vehicles on the network and the motion of vehicles along roads the roads capacity and the vehic... | [['in', 'this', 'paper', 'urban', 'traffic', 'is', 'modeled', 'using', 'dual', 'graph', 'representation', 'of', 'urban', 'transportation', 'network', 'where', 'roads', 'are', 'mapped', 'to', 'nodes', 'and', 'intersections', 'are', 'mapped', 'to', 'links', 'the', 'proposed', 'model', 'considers', 'both', 'the', 'navigat... | [-0.193847693971575, 0.09475737757547277, -0.04222476217145068, 0.028560907356160018, -0.04006061020130613, -0.12553911248286223, 0.08215533442702948, 0.36414704882065113, -0.2538509077336318, -0.29252902221673266, 0.11122364162744408, -0.29401243724539106, -0.19091131904860958, 0.18156205154483704, -0.1647166966075270... |
710.2993 | Inflation-Produced Magnetic Fields in Nonlinear Electrodynamics | We study the generation of primeval magnetic fields during inflation era in
nonlinear theories of electrodynamics. Although the intensity of the produced
fields strongly depends on characteristics of inflation and on the form of
electromagnetic Lagrangian, our results do not exclude the possibility that
these fields ... | astro-ph | we study the generation of primeval magnetic fields during inflation era in nonlinear theories of electrodynamics although the intensity of the produced fields strongly depends on characteristics of inflation and on the form of electromagnetic lagrangian our results do not exclude the possibility that these fields coul... | [['we', 'study', 'the', 'generation', 'of', 'primeval', 'magnetic', 'fields', 'during', 'inflation', 'era', 'in', 'nonlinear', 'theories', 'of', 'electrodynamics', 'although', 'the', 'intensity', 'of', 'the', 'produced', 'fields', 'strongly', 'depends', 'on', 'characteristics', 'of', 'inflation', 'and', 'on', 'the', 'f... | [-0.1759076257236302, 0.23361519324593247, -0.08103394594043493, 0.08703794422093779, -0.11573200810700655, -0.04529083198867738, -0.06086582563817501, 0.33835385132581, -0.18597477521747352, -0.3177683836966753, 0.07614207315957174, -0.20493627548217774, -0.15839651064015925, 0.26390926162013784, 0.0197410930134356, -... |
710.2994 | Toroidal automorphic forms for some function fields | Zagier introduced toroidal automorphic forms to study the zeros of zeta
functions: an automorphic form on GL_2 is toroidal if all its right translates
integrate to zero over all nonsplit tori in GL_2, and an Eisenstein series is
toroidal if its weight is a zero of the zeta function of the corresponding
field. We comp... | math.NT math.AG | zagier introduced toroidal automorphic forms to study the zeros of zeta functions an automorphic form on gl_2 is toroidal if all its right translates integrate to zero over all nonsplit tori in gl_2 and an eisenstein series is toroidal if its weight is a zero of the zeta function of the corresponding field we compute t... | [['zagier', 'introduced', 'toroidal', 'automorphic', 'forms', 'to', 'study', 'the', 'zeros', 'of', 'zeta', 'functions', 'an', 'automorphic', 'form', 'on', 'gl_2', 'is', 'toroidal', 'if', 'all', 'its', 'right', 'translates', 'integrate', 'to', 'zero', 'over', 'all', 'nonsplit', 'tori', 'in', 'gl_2', 'and', 'an', 'eisens... | [-0.24755565723865677, 0.07207845570880027, -0.1387718233596021, 0.07791970926977762, -0.11794378223974224, -0.06709444007639764, -0.02985843557249242, 0.28074277201752873, -0.29742094325841567, -0.20373705607932915, 0.08292272735340094, -0.24859099722373376, -0.1575885120920256, 0.2676131371686389, -0.0378193623693916... |
710.2995 | On the growth rate of minor-closed classes of graphs | A minor-closed class of graphs is a set of labelled graphs which is closed
under isomorphism and under taking minors. For a minor-closed class $C$, we let
$c_n$ be the number of graphs in $C$ which have $n$ vertices. A recent result
of Norine et al. shows that for all minor-closed class $C$, there is a constant
$r$ s... | math.CO | a minorclosed class of graphs is a set of labelled graphs which is closed under isomorphism and under taking minors for a minorclosed class c we let c_n be the number of graphs in c which have n vertices a recent result of norine et al shows that for all minorclosed class c there is a constant r such that c_n rn n our ... | [['a', 'minorclosed', 'class', 'of', 'graphs', 'is', 'a', 'set', 'of', 'labelled', 'graphs', 'which', 'is', 'closed', 'under', 'isomorphism', 'and', 'under', 'taking', 'minors', 'for', 'a', 'minorclosed', 'class', 'c', 'we', 'let', 'c_n', 'be', 'the', 'number', 'of', 'graphs', 'in', 'c', 'which', 'have', 'n', 'vertices... | [-0.20161755237495527, 0.15600914249565298, 0.037817352082735546, -0.05537344882516967, -0.043474383317516185, -0.21170820187641462, 0.00913808219290028, 0.349654711545251, -0.25379336381835554, -0.29959315282758325, 0.07376700933067089, -0.29893429127211374, -0.11695114415488206, 0.19365920830508307, -0.07086648340433... |
710.2996 | Collective and static properties of model two-component plasmas | Classical MD data on the charge-charge dynamic structure factor of
two-component plasmas (TCP) modeled in Phys. Rev. A 23, 2041 (1981) are
analyzed using the sum rules and other exact relations. The convergent power
moments of the imaginary part of the model system dielectric function are
expressed in terms of its pa... | physics.plasm-ph | classical md data on the chargecharge dynamic structure factor of twocomponent plasmas tcp modeled in phys rev a 23 2041 1981 are analyzed using the sum rules and other exact relations the convergent power moments of the imaginary part of the model system dielectric function are expressed in terms of its partial static... | [['classical', 'md', 'data', 'on', 'the', 'chargecharge', 'dynamic', 'structure', 'factor', 'of', 'twocomponent', 'plasmas', 'tcp', 'modeled', 'in', 'phys', 'rev', 'a', '23', '2041', '1981', 'are', 'analyzed', 'using', 'the', 'sum', 'rules', 'and', 'other', 'exact', 'relations', 'the', 'convergent', 'power', 'moments',... | [-0.1242836787814981, 0.08000235232636975, -0.05763013853193742, 0.06230002995941724, -0.01302473625601751, -0.10697935166736615, 0.05244332114470408, 0.3572804359960017, -0.2504183029121687, -0.29141488709037416, 0.05151675262885842, -0.30276326831141165, -0.12811879449572158, 0.18406558832844142, 0.043792946813106214... |
710.2997 | The effect of clouds in a galactic wind on the evolution of gas-rich
dwarf galaxies | (Abridged)
We study the effects of interstellar clouds on the dynamical and chemical
evolution of gas-rich dwarf galaxies. In particular, we focus on two model
galaxies similar to IZw18 and NGC1569 in comparison to models in which a smooth
initial distribution of gas is assumed. We use a 2-D hydrodynamical code
cou... | astro-ph | abridged we study the effects of interstellar clouds on the dynamical and chemical evolution of gasrich dwarf galaxies in particular we focus on two model galaxies similar to izw18 and ngc1569 in comparison to models in which a smooth initial distribution of gas is assumed we use a 2d hydrodynamical code coupled with a... | [['abridged', 'we', 'study', 'the', 'effects', 'of', 'interstellar', 'clouds', 'on', 'the', 'dynamical', 'and', 'chemical', 'evolution', 'of', 'gasrich', 'dwarf', 'galaxies', 'in', 'particular', 'we', 'focus', 'on', 'two', 'model', 'galaxies', 'similar', 'to', 'izw18', 'and', 'ngc1569', 'in', 'comparison', 'to', 'model... | [-0.0537633920020337, 0.1558549723331915, -0.04963303726044152, 0.08506505306113622, -0.04227772412695369, -0.05944118530576323, 0.06704961385487153, 0.4067009049783445, -0.2139526560421149, -0.3562123815773718, 0.048680067658266525, -0.2904588830135901, -0.0028805983177843993, 0.15515948420363848, -0.00510186865981036... |
710.2998 | Weak convergence of measure-valued processes and $r$-point functions | We prove a sufficient set of conditions for a sequence of finite measures on
the space of cadlag measure-valued paths to converge to the canonical measure
of super-Brownian motion in the sense of convergence of finite-dimensional
distributions. The conditions are convergence of the Fourier transform of the
$r$-point ... | math.PR | we prove a sufficient set of conditions for a sequence of finite measures on the space of cadlag measurevalued paths to converge to the canonical measure of superbrownian motion in the sense of convergence of finitedimensional distributions the conditions are convergence of the fourier transform of the rpoint functions... | [['we', 'prove', 'a', 'sufficient', 'set', 'of', 'conditions', 'for', 'a', 'sequence', 'of', 'finite', 'measures', 'on', 'the', 'space', 'of', 'cadlag', 'measurevalued', 'paths', 'to', 'converge', 'to', 'the', 'canonical', 'measure', 'of', 'superbrownian', 'motion', 'in', 'the', 'sense', 'of', 'convergence', 'of', 'fin... | [-0.10912129326283725, 0.12453638877098759, -0.11917703284675049, 0.09117910754682979, -0.005365084181539715, -0.08566512157623139, 0.06397657453004892, 0.37737179663446213, -0.28227970983005235, -0.19639840240900716, 0.12607959299736346, -0.2487321817005674, -0.11022168985930168, 0.18745334620277088, -0.07471719971961... |
710.2999 | Nonadiabatic corrections to the wave function and energy | Nonadiabatic corrections in molecules composed of a few atoms are considered.
It is demonstrated that a systematic perturbative expansion around the
adiabatic solution is possible, with the expansion parameter being the
electron-nucleus mass ratio to the power 3/4. Closed form formulae for the
leading corrections to ... | physics.chem-ph physics.gen-ph | nonadiabatic corrections in molecules composed of a few atoms are considered it is demonstrated that a systematic perturbative expansion around the adiabatic solution is possible with the expansion parameter being the electronnucleus mass ratio to the power 34 closed form formulae for the leading corrections to the wav... | [['nonadiabatic', 'corrections', 'in', 'molecules', 'composed', 'of', 'a', 'few', 'atoms', 'are', 'considered', 'it', 'is', 'demonstrated', 'that', 'a', 'systematic', 'perturbative', 'expansion', 'around', 'the', 'adiabatic', 'solution', 'is', 'possible', 'with', 'the', 'expansion', 'parameter', 'being', 'the', 'electr... | [-0.11701814101087217, 0.10726219820515456, -0.03221980142935189, 0.05933671942479985, 0.020717029911033885, -0.085764240497512, 0.05508537995677019, 0.36264970735406754, -0.1930218368730287, -0.28813311275209963, 0.03883289819770521, -0.3086467300608908, -0.03779425847430512, 0.20492277327761746, 0.06842479519738057, ... |
710.3 | Spacetime Dependent Lagrangians and Electrogravity Duality | We apply the spacetime dependent lagrangian formalism [1] to the action in
general relativity. We obtain a Barriola-Vilenkin type monopole solution by
exploiting theelectrogravity duality of the vacuum Einstein equations and using
a modified definition of empty space. An {\it upper bound} is obtained on the
monopole ... | gr-qc astro-ph hep-th | we apply the spacetime dependent lagrangian formalism 1 to the action in general relativity we obtain a barriolavilenkin type monopole solution by exploiting theelectrogravity duality of the vacuum einstein equations and using a modified definition of empty space an it upper bound is obtained on the monopole mass tt m ... | [['we', 'apply', 'the', 'spacetime', 'dependent', 'lagrangian', 'formalism', '1', 'to', 'the', 'action', 'in', 'general', 'relativity', 'we', 'obtain', 'a', 'barriolavilenkin', 'type', 'monopole', 'solution', 'by', 'exploiting', 'theelectrogravity', 'duality', 'of', 'the', 'vacuum', 'einstein', 'equations', 'and', 'usi... | [-0.16354820483497212, 0.12038679565490124, -0.0943352331207799, 0.1526591393198552, -0.1145569954666176, -0.15870180014254792, -0.006843577471694776, 0.24524043381347188, -0.16683499994022505, -0.29316106593635466, 0.04985957077671108, -0.2594767617061734, -0.1291602717180337, 0.09647704249447478, -0.01820325473589556... |
710.3001 | Greedy and quasi-greedy expansions in non-integer bases | We generalize several theorems of R\'enyi, Parry, Dar\'oczy and K\'atai by
characterizing the greedy and quasi-greedy expansions in non-integer bases.
| math.NT math.GM | we generalize several theorems of renyi parry daroczy and katai by characterizing the greedy and quasigreedy expansions in noninteger bases | [['we', 'generalize', 'several', 'theorems', 'of', 'renyi', 'parry', 'daroczy', 'and', 'katai', 'by', 'characterizing', 'the', 'greedy', 'and', 'quasigreedy', 'expansions', 'in', 'noninteger', 'bases']] | [-0.14012623137157215, 0.16400783817822995, -0.10015484068150583, 0.16180332593227686, -0.025695794261991978, -0.11862459269009139, 0.12057460959706652, 0.27139070277151306, -0.23332229295843526, -0.14680511161292853, 0.10688826882304918, -0.32792666319169494, -0.18789358731163175, 0.19848628891141792, -0.1403480594683... |
710.3002 | Rigorous derivation of the hydrodynamical equations for rotating
superfluids | Using a modified WKB approach, we present a rigorous semi-classical analysis
for solutions of nonlinear Schroedinger equations with rotational forcing. This
yields a rigorous justification for the hydrodynamical system of rotating
superfluids. In particular it is shown that global-in-time semi-classical
convergence h... | math.AP math-ph math.MP | using a modified wkb approach we present a rigorous semiclassical analysis for solutions of nonlinear schroedinger equations with rotational forcing this yields a rigorous justification for the hydrodynamical system of rotating superfluids in particular it is shown that globalintime semiclassical convergence holds when... | [['using', 'a', 'modified', 'wkb', 'approach', 'we', 'present', 'a', 'rigorous', 'semiclassical', 'analysis', 'for', 'solutions', 'of', 'nonlinear', 'schroedinger', 'equations', 'with', 'rotational', 'forcing', 'this', 'yields', 'a', 'rigorous', 'justification', 'for', 'the', 'hydrodynamical', 'system', 'of', 'rotating... | [-0.17188875667858294, 0.021050336613104893, -0.1700107135165196, 0.10954478769563139, -0.06851877888234761, -0.1377487371245829, -0.02349970627647753, 0.27157833685095495, -0.18099765995374092, -0.1736764957698492, 0.04748329865352179, -0.2594718015537812, -0.13745327049221556, 0.21018368931343923, -0.0387845818383189... |
710.3003 | A polynomial oracle-time algorithm for convex integer minimization | In this paper we consider the solution of certain convex integer minimization
problems via greedy augmentation procedures. We show that a greedy augmentation
procedure that employs only directions from certain Graver bases needs only
polynomially many augmentation steps to solve the given problem. We extend
these res... | math.OC math.CO | in this paper we consider the solution of certain convex integer minimization problems via greedy augmentation procedures we show that a greedy augmentation procedure that employs only directions from certain graver bases needs only polynomially many augmentation steps to solve the given problem we extend these results... | [['in', 'this', 'paper', 'we', 'consider', 'the', 'solution', 'of', 'certain', 'convex', 'integer', 'minimization', 'problems', 'via', 'greedy', 'augmentation', 'procedures', 'we', 'show', 'that', 'a', 'greedy', 'augmentation', 'procedure', 'that', 'employs', 'only', 'directions', 'from', 'certain', 'graver', 'bases', ... | [-0.11558506607917356, -0.012448677833387514, -0.0545853207140793, 0.07386105612098573, -0.1612511206717219, -0.22999344541357808, 0.060816972431680764, 0.4187367629305816, -0.4348696162119324, -0.23781621871792055, 0.16565811332677388, -0.23492218190689146, -0.25526694527878946, 0.17744890060045837, -0.142535598290348... |
710.3004 | Inverse sequences, rooted trees and their end spaces | In this paper we prove that if we consider the standard real metric on
simplicial rooted trees then the category Tower-Set of inverse sequences can be
described by means of the bounded coarse geometry of the naturally associated
trees. Using this we give a geometrical characterization of Mittag-Leffler
property in in... | math.GT | in this paper we prove that if we consider the standard real metric on simplicial rooted trees then the category towerset of inverse sequences can be described by means of the bounded coarse geometry of the naturally associated trees using this we give a geometrical characterization of mittagleffler property in inverse... | [['in', 'this', 'paper', 'we', 'prove', 'that', 'if', 'we', 'consider', 'the', 'standard', 'real', 'metric', 'on', 'simplicial', 'rooted', 'trees', 'then', 'the', 'category', 'towerset', 'of', 'inverse', 'sequences', 'can', 'be', 'described', 'by', 'means', 'of', 'the', 'bounded', 'coarse', 'geometry', 'of', 'the', 'na... | [-0.09018393271470175, 0.10791296148400238, -0.07448373342606615, 0.13310123030641216, -0.11423322890805913, -0.054746788738176545, 0.018548507535671617, 0.3968535460893342, -0.3891568559994723, -0.1966580419028376, 0.1236741423750534, -0.2301186553222385, -0.20997541603146794, 0.1674095328421669, -0.18909244648517765,... |
710.3005 | X-ray Irradiation-induced Carrier Doping Effects in Organic Dimer-Mott
Insulators | We report X-ray irradiation-induced carrier doping effects on the electrical
conductivity in the organic dimer-Mott insulators $\kappa$-(ET)$_{2}$$X$ with
$X =$ Cu[N(CN)$_{2}$]Cl and Cu$_{2}$(CN)$_{3}$. For
$\kappa$-(ET)$_{2}$Cu[N(CN)$_{2}$]Cl, we have observed a large decrease of the
resistivity by 40 % with the irr... | cond-mat.str-el cond-mat.supr-con | we report xray irradiationinduced carrier doping effects on the electrical conductivity in the organic dimermott insulators kappaet_2x with x cuncn_2cl and cu_2cn_3 for kappaet_2cuncn_2cl we have observed a large decrease of the resistivity by 40 with the irradiation at 300 k and the metallike temperature dependence do... | [['we', 'report', 'xray', 'irradiationinduced', 'carrier', 'doping', 'effects', 'on', 'the', 'electrical', 'conductivity', 'in', 'the', 'organic', 'dimermott', 'insulators', 'kappaet_2x', 'with', 'x', 'cuncn_2cl', 'and', 'cu_2cn_3', 'for', 'kappaet_2cuncn_2cl', 'we', 'have', 'observed', 'a', 'large', 'decrease', 'of', ... | [-0.13219045222531137, 0.23287313064387025, 0.017521454411190608, 0.021378868595198837, 0.04567128588001482, -0.13708643019226444, 0.17408109483103332, 0.3908928939422896, -0.24655373853652976, -0.33366741450113613, -0.004071512214871947, -0.397565386886167, -0.06442512113730921, 0.1119267704279357, 0.03038602869762757... |
710.3006 | Nonlinear Phenomena in Canonical Stochastic Quantization | Stochastic quantization provides a connection between quantum field theory
and statistical mechanics, with applications especially in gauge field
theories. Euclidean quantum field theory is viewed as the equilibrium limit of
a statistical system coupled to a thermal reservoir. Nonlinear phenomena in
stochastic quanti... | hep-th | stochastic quantization provides a connection between quantum field theory and statistical mechanics with applications especially in gauge field theories euclidean quantum field theory is viewed as the equilibrium limit of a statistical system coupled to a thermal reservoir nonlinear phenomena in stochastic quantizatio... | [['stochastic', 'quantization', 'provides', 'a', 'connection', 'between', 'quantum', 'field', 'theory', 'and', 'statistical', 'mechanics', 'with', 'applications', 'especially', 'in', 'gauge', 'field', 'theories', 'euclidean', 'quantum', 'field', 'theory', 'is', 'viewed', 'as', 'the', 'equilibrium', 'limit', 'of', 'a', ... | [-0.13755852294226106, 0.16510866422837492, -0.12087137307971715, 0.09158919451396147, -0.0683098920298597, -0.18092320463978329, -0.008009769018882743, 0.3009636951323885, -0.3265790673904121, -0.2511146470080488, 0.03147561433545958, -0.22375687720397344, -0.2443133821281103, 0.16245179604738952, -0.08840449842839287... |
710.3007 | Three-dimensional transformation for point rotation coordinate frames | We consider the transformation for the point rotation frames with the angle,
spatial coordinate along the axis of rotation and time as variables. The
problem arises when light, propagating through 3-fold electrooptical crystal,
is modulated by the circularly polarized electromagnetic wave traveling along
the optical ... | physics.optics physics.gen-ph | we consider the transformation for the point rotation frames with the angle spatial coordinate along the axis of rotation and time as variables the problem arises when light propagating through 3fold electrooptical crystal is modulated by the circularly polarized electromagnetic wave traveling along the optical axis of... | [['we', 'consider', 'the', 'transformation', 'for', 'the', 'point', 'rotation', 'frames', 'with', 'the', 'angle', 'spatial', 'coordinate', 'along', 'the', 'axis', 'of', 'rotation', 'and', 'time', 'as', 'variables', 'the', 'problem', 'arises', 'when', 'light', 'propagating', 'through', '3fold', 'electrooptical', 'crysta... | [-0.20855263822810038, 0.1830595055598359, -0.05923949335211594, -0.01622396829464522, -0.10808880040585472, -0.08246343916184024, 0.02325150527452168, 0.4569293351419139, -0.3232997551544063, -0.2337758624640277, 0.09247024971154404, -0.23219440941159664, -0.13388987011766354, 0.19579166659203015, 0.003739691188297512... |
710.3008 | Compactified Picard stacks over $\bar{\mathcal M}_g$ | We study algebraic (Artin) stacks over $\bar{\mathcal M}_g$ giving a
functorial way of compactifying the relative degree $d$ Picard variety for
families of stable curves. We also describe for every $d$ the locus of genus
$g$ stable curves over which we get Deligne-Mumford stacks strongly
representable over $\bar{\mat... | math.AG | we study algebraic artin stacks over barmathcal m_g giving a functorial way of compactifying the relative degree d picard variety for families of stable curves we also describe for every d the locus of genus g stable curves over which we get delignemumford stacks strongly representable over barmathcal m_g | [['we', 'study', 'algebraic', 'artin', 'stacks', 'over', 'barmathcal', 'm_g', 'giving', 'a', 'functorial', 'way', 'of', 'compactifying', 'the', 'relative', 'degree', 'd', 'picard', 'variety', 'for', 'families', 'of', 'stable', 'curves', 'we', 'also', 'describe', 'for', 'every', 'd', 'the', 'locus', 'of', 'genus', 'g', ... | [-0.25905797678064935, 0.05429020989686251, -0.19319598591525336, 0.07445419817326629, -0.05422550310589829, -0.17090525847802662, 0.024950179898617218, 0.37460157294206475, -0.36945196590861495, -0.1948214915333962, 0.005766031893008217, -0.16872229329690488, -0.09265586421159762, 0.31137669215701064, -0.2253207555610... |
710.3009 | Microscopic entropy of the charged BTZ black hole | The charged BTZ black hole is characterized by a power-law curvature
singularity generated by the electric charge of the hole. The curvature
singularity produces ln r terms in the asymptotic expansion of the
gravitational field and divergent contributions to the boundary terms. We show
that these boundary deformation... | hep-th gr-qc | the charged btz black hole is characterized by a powerlaw curvature singularity generated by the electric charge of the hole the curvature singularity produces ln r terms in the asymptotic expansion of the gravitational field and divergent contributions to the boundary terms we show that these boundary deformations can... | [['the', 'charged', 'btz', 'black', 'hole', 'is', 'characterized', 'by', 'a', 'powerlaw', 'curvature', 'singularity', 'generated', 'by', 'the', 'electric', 'charge', 'of', 'the', 'hole', 'the', 'curvature', 'singularity', 'produces', 'ln', 'r', 'terms', 'in', 'the', 'asymptotic', 'expansion', 'of', 'the', 'gravitationa... | [-0.14556975280071877, 0.1598410776017871, -0.0941615975497998, 0.08649809815733181, -0.026566076812572604, -0.14305267508625408, -0.020491131424340746, 0.26426394628866234, -0.1914096830210598, -0.2378329428403761, 0.04703982404068603, -0.33278179021614024, -0.1051274285933306, 0.14814505906587885, -0.0735372587850736... |
710.301 | It's a wonderful tail: the mass loss history of Mira | Recent observations of the Mira AB binary system have revealed a surrounding
arc-like structure and a stream of material stretching 2 degrees away in
opposition to the arc. The alignment of the proper motion vector and the
arc-like structure shows the structures to be a bow shock and accompanying
tail. We have succes... | astro-ph | recent observations of the mira ab binary system have revealed a surrounding arclike structure and a stream of material stretching 2 degrees away in opposition to the arc the alignment of the proper motion vector and the arclike structure shows the structures to be a bow shock and accompanying tail we have successfully... | [['recent', 'observations', 'of', 'the', 'mira', 'ab', 'binary', 'system', 'have', 'revealed', 'a', 'surrounding', 'arclike', 'structure', 'and', 'a', 'stream', 'of', 'material', 'stretching', '2', 'degrees', 'away', 'in', 'opposition', 'to', 'the', 'arc', 'the', 'alignment', 'of', 'the', 'proper', 'motion', 'vector', ... | [-0.1021671161834652, 0.11407615350416074, -0.15079137448293084, 0.05430397483138129, -0.11388202477246523, -0.0434187739323347, 0.026957532841539105, 0.4457034536422445, -0.2868929534431141, -0.3013528685539197, 0.09165121777078662, -0.2679623775787126, -0.08966048409183247, 0.1302571466112008, -0.042795976825679344, ... |
710.3011 | Antiferromagnetic fluctuations and the Fulde-Ferrell-Larkin-Ovchinnikov
state in CeCoIn5 | The heavy-fermion superconductor CeCoIn5 is the first material, where
different experimental probes show strong evidence pointing to the realization
of the Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) state. The inhomogeneous
superconducting FFLO state with a periodically modulated order parameter was
predicted to appear ... | cond-mat.str-el cond-mat.supr-con | the heavyfermion superconductor cecoin5 is the first material where different experimental probes show strong evidence pointing to the realization of the fuldeferrelllarkinovchinnikov fflo state the inhomogeneous superconducting fflo state with a periodically modulated order parameter was predicted to appear in paulili... | [['the', 'heavyfermion', 'superconductor', 'cecoin5', 'is', 'the', 'first', 'material', 'where', 'different', 'experimental', 'probes', 'show', 'strong', 'evidence', 'pointing', 'to', 'the', 'realization', 'of', 'the', 'fuldeferrelllarkinovchinnikov', 'fflo', 'state', 'the', 'inhomogeneous', 'superconducting', 'fflo', ... | [-0.23216050230314375, 0.27826933673123355, -0.0608727186525168, 0.03695346712355514, -0.0613561777803176, -0.19189385307556647, 0.12043025357158879, 0.33103328760011824, -0.25853692696810787, -0.24693898216809157, 0.024762567146318398, -0.3241350534432507, -0.04363860050972261, 0.17285954954205443, 0.08207830422037801... |
710.3012 | Asymptotic Stability for a Class of Metriplectic Systems | Using the framework of metriplectic systems on $\R^n$ we will describe a
constructive geometric method to add a dissipation term to a Hamilton-Poisson
system such that any solution starting in a neighborhood of a nonlinear stable
equilibrium converges towards a certain invariant set. The dissipation term
depends only... | math-ph math.MP math.SG | using the framework of metriplectic systems on rn we will describe a constructive geometric method to add a dissipation term to a hamiltonpoisson system such that any solution starting in a neighborhood of a nonlinear stable equilibrium converges towards a certain invariant set the dissipation term depends only on the ... | [['using', 'the', 'framework', 'of', 'metriplectic', 'systems', 'on', 'rn', 'we', 'will', 'describe', 'a', 'constructive', 'geometric', 'method', 'to', 'add', 'a', 'dissipation', 'term', 'to', 'a', 'hamiltonpoisson', 'system', 'such', 'that', 'any', 'solution', 'starting', 'in', 'a', 'neighborhood', 'of', 'a', 'nonline... | [-0.20350413105916232, 0.05027356545906514, -0.14668281329795718, 0.06535298758535646, -0.0673856316799564, -0.12076974216116858, 0.04632386237582458, 0.2700565044901201, -0.30235108813004835, -0.20524265148144746, 0.07740909856303395, -0.279369296106909, -0.1921848748211882, 0.19300041381003602, -0.06128233533870896, ... |
710.3013 | Spectra of phase point operators in odd prime dimensions and the
extended Clifford group | We analyse the role of the Extended Clifford group in classifying the spectra
of phase point operators within the framework laid out by Gibbons et al for
setting up Wigner distributions on discrete phase spaces based on finite
fields. To do so we regard the set of all the discrete phase spaces as a
symplectic vector ... | quant-ph | we analyse the role of the extended clifford group in classifying the spectra of phase point operators within the framework laid out by gibbons et al for setting up wigner distributions on discrete phase spaces based on finite fields to do so we regard the set of all the discrete phase spaces as a symplectic vector spa... | [['we', 'analyse', 'the', 'role', 'of', 'the', 'extended', 'clifford', 'group', 'in', 'classifying', 'the', 'spectra', 'of', 'phase', 'point', 'operators', 'within', 'the', 'framework', 'laid', 'out', 'by', 'gibbons', 'et', 'al', 'for', 'setting', 'up', 'wigner', 'distributions', 'on', 'discrete', 'phase', 'spaces', 'b... | [-0.10694068362808799, 0.13523614368312162, -0.08862030057057943, 0.0651525571967845, -0.07155220326808065, -0.030315455393738127, 0.0786356670345014, 0.3650309887574348, -0.24225938385224913, -0.24954789432964913, 0.08804845475521551, -0.23227216171942752, -0.12051287548591012, 0.20335011664069935, -0.0810533083930662... |
710.3014 | Higgs-Boson Benchmarks in Agreement with CDM, EWPO and BPO | We explore `benchmark planes' in the Minimal Supersymmetric Standard Model
(MSSM) that are in agreement with the measured cold dark matter (CDM) density,
electroweak precision observables (EWPO) and B physics observables (BPO). The
M_A-tan_beta planes are specified assuming that gaugino masses m_{1/2}, soft
trilinear... | hep-ph | we explore benchmark planes in the minimal supersymmetric standard model mssm that are in agreement with the measured cold dark matter cdm density electroweak precision observables ewpo and b physics observables bpo the m_atan_beta planes are specified assuming that gaugino masses m_12 soft trilinear supersymmetrybreak... | [['we', 'explore', 'benchmark', 'planes', 'in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'that', 'are', 'in', 'agreement', 'with', 'the', 'measured', 'cold', 'dark', 'matter', 'cdm', 'density', 'electroweak', 'precision', 'observables', 'ewpo', 'and', 'b', 'physics', 'observables', 'bpo', 'the',... | [-0.1064542014750519, 0.29054364633674806, -0.0034311388793227438, 0.22117389207398827, -0.0909240118453054, -0.22088977363943071, -0.021379702693813448, 0.35202457672394405, -0.19521310580075607, -0.32316591537424494, 0.02343692822934507, -0.28856410312844993, 0.03892626159998414, 0.15812046576936084, 0.05215020705357... |
710.3015 | Optical phase diagram of perovskite-type colossal magnetoresistance
manganites with near-half doping | We present a systematic optical study for a bandwidth-controlled series of
nearly half doped colossal magnetoresistive manganites
RE$_{0.55}$AE$_{0.45}$MnO$_3$ (RE and AE being rare earth and alkaline earth
ions, respectively) under the presence of quenched disorder over a broad
temperature region $T=10-800$ K. The g... | cond-mat.str-el | we present a systematic optical study for a bandwidthcontrolled series of nearly half doped colossal magnetoresistive manganites re_055ae_045mno_3 re and ae being rare earth and alkaline earth ions respectively under the presence of quenched disorder over a broad temperature region t10800 k the ground state of the comp... | [['we', 'present', 'a', 'systematic', 'optical', 'study', 'for', 'a', 'bandwidthcontrolled', 'series', 'of', 'nearly', 'half', 'doped', 'colossal', 'magnetoresistive', 'manganites', 're_055ae_045mno_3', 're', 'and', 'ae', 'being', 'rare', 'earth', 'and', 'alkaline', 'earth', 'ions', 'respectively', 'under', 'the', 'pre... | [-0.1887150728912532, 0.2565676270631161, -0.009159103594940016, 0.03255994025339704, 0.008562164193344355, -0.13044579515128202, 0.11611595966211818, 0.37098049362769947, -0.2547390457563419, -0.2588441070511867, 0.030237721817958925, -0.3643035889023317, -0.056333697816128576, 0.11395299280686129, 0.05944837462958567... |
710.3016 | Associated Higgs Production in CP-violating supersymmetry: probing the
`open hole' at the Large Hadron Collider | A benchmark CP-violating supersymmetric scenario (known in the literature as
`CPX-scenario') is studied in the context of the Large Hadron Collider (LHC).
It is shown that the LHC, with low to moderate accumulated luminosity, will be
able to probe the existing `hole' in the $m_{h_1}$-$\tan\beta$ plane, which
cannot b... | hep-ph | a benchmark cpviolating supersymmetric scenario known in the literature as cpxscenario is studied in the context of the large hadron collider lhc it is shown that the lhc with low to moderate accumulated luminosity will be able to probe the existing hole in the m_h_1tanbeta plane which cannot be ruled out by the large ... | [['a', 'benchmark', 'cpviolating', 'supersymmetric', 'scenario', 'known', 'in', 'the', 'literature', 'as', 'cpxscenario', 'is', 'studied', 'in', 'the', 'context', 'of', 'the', 'large', 'hadron', 'collider', 'lhc', 'it', 'is', 'shown', 'that', 'the', 'lhc', 'with', 'low', 'to', 'moderate', 'accumulated', 'luminosity', '... | [-0.05423496459042568, 0.2252752648136758, -0.0702743384359114, 0.16423168912350516, -0.07888637349188943, -0.19508336574573992, 0.003612688426441009, 0.32198814097621026, -0.21522967571631893, -0.3088000338490403, 0.061159229697446006, -0.3203422911636053, 0.031529946124540006, 0.1889084096946711, 0.03246640295661781,... |
710.3017 | Stringy Model of Cosmological Dark Energy | A string field theory(SFT) nonlocal model of the cosmological dark energy
providing w<-1 is briefly surveyed. We summarize recent developments and open
problems, as well as point out some theoretical issues related with others
applications of the SFT nonlocal models in cosmology, in particular, in
inflation and cosmo... | hep-th | a string field theorysft nonlocal model of the cosmological dark energy providing w1 is briefly surveyed we summarize recent developments and open problems as well as point out some theoretical issues related with others applications of the sft nonlocal models in cosmology in particular in inflation and cosmological si... | [['a', 'string', 'field', 'theorysft', 'nonlocal', 'model', 'of', 'the', 'cosmological', 'dark', 'energy', 'providing', 'w1', 'is', 'briefly', 'surveyed', 'we', 'summarize', 'recent', 'developments', 'and', 'open', 'problems', 'as', 'well', 'as', 'point', 'out', 'some', 'theoretical', 'issues', 'related', 'with', 'othe... | [-0.11473834411784385, 0.06887869170168415, -0.07954063533300844, 0.15557156907986305, -0.11987789941485971, -0.17966462073187964, -0.037971530691720545, 0.32181310102654, -0.2558205918758176, -0.29158366836297017, 0.1514097280766388, -0.28609423828311265, -0.13087923236889765, 0.19775549123975603, -0.07140337029704824... |
710.3018 | On the Nature of Dark Matter and Dark Energy | It is shown that some problems connected with dark matter and dark energy can
be solved in the framework of the byuon theory
| physics.gen-ph | it is shown that some problems connected with dark matter and dark energy can be solved in the framework of the byuon theory | [['it', 'is', 'shown', 'that', 'some', 'problems', 'connected', 'with', 'dark', 'matter', 'and', 'dark', 'energy', 'can', 'be', 'solved', 'in', 'the', 'framework', 'of', 'the', 'byuon', 'theory']] | [-0.10229351749876514, 0.14680810966952282, -0.1937814727213911, 0.1487410998405804, -0.07602269994094968, -0.15071746732362293, -0.11136513379592956, 0.34698462596332486, -0.3203462375835939, -0.40953305329788814, 0.06626459238098258, -0.22569349966943264, -0.13535624742507935, 0.20766244540837678, -0.0107638567516749... |
710.3019 | New class of self-similar solutions for vacuum plasma expansion
admitting mono-energetic ion spectra | We report a new class of self-similar solutions for plasma expanding into
vacuum that allows for quasi-monoenergetic ion spectra. A simple analytical
model takes into account externally controlled time-dependent temperature of
the hot electrons. When the laser temporal profile is tailored properly, the
quasi-neutral ... | physics.plasm-ph physics.acc-ph | we report a new class of selfsimilar solutions for plasma expanding into vacuum that allows for quasimonoenergetic ion spectra a simple analytical model takes into account externally controlled timedependent temperature of the hot electrons when the laser temporal profile is tailored properly the quasineutral selfsimil... | [['we', 'report', 'a', 'new', 'class', 'of', 'selfsimilar', 'solutions', 'for', 'plasma', 'expanding', 'into', 'vacuum', 'that', 'allows', 'for', 'quasimonoenergetic', 'ion', 'spectra', 'a', 'simple', 'analytical', 'model', 'takes', 'into', 'account', 'externally', 'controlled', 'timedependent', 'temperature', 'of', 't... | [-0.08279412566978288, 0.2124765795199078, -0.11171510886449955, 0.03701219405415223, 0.012304606901383713, -0.16477600560082417, 0.010133981042982717, 0.4315718721402319, -0.2195361887545962, -0.2538472525971501, -0.014898248801105901, -0.23508104862182672, 0.0359402106486653, 0.23803240116440544, 0.04010720771100176,... |
710.302 | Minimal flavour violations and tree level FCNC | Consequences of a specific class of two Higgs doublet models in which the
Higgs induced tree level flavour changing neutral currents (FCNC) display
minimal flavour violation (MFV) are considered. These FCNC are fixed in terms
of the CKM matrix elements and the down quark masses. The minimal model in this
category wit... | hep-ph | consequences of a specific class of two higgs doublet models in which the higgs induced tree level flavour changing neutral currents fcnc display minimal flavour violation mfv are considered these fcnc are fixed in terms of the ckm matrix elements and the down quark masses the minimal model in this category with only t... | [['consequences', 'of', 'a', 'specific', 'class', 'of', 'two', 'higgs', 'doublet', 'models', 'in', 'which', 'the', 'higgs', 'induced', 'tree', 'level', 'flavour', 'changing', 'neutral', 'currents', 'fcnc', 'display', 'minimal', 'flavour', 'violation', 'mfv', 'are', 'considered', 'these', 'fcnc', 'are', 'fixed', 'in', '... | [-0.13609752966646826, 0.2981954245547694, 0.021117985528963868, 0.12644033420139983, -0.07745726392178806, -0.20815330966105383, 0.1180439607424271, 0.2898592241358773, -0.23756833259368024, -0.258209139479184, 0.022656798159318065, -0.30139859193705665, -0.045045954365250704, 0.0792363271034593, 0.03764974423964265, ... |
710.3021 | Ghetto of Venice: Access to the Target Node and the Random Target Access
Time | Random walks defined on undirected graphs assign the absolute scores to all
nodes based on the quality of path they provide for random walkers. In city
space syntax, the notion of segregation acquires a statistical interpretation
with respect to random walks. We analyze the spatial network of Venetian canals
and dete... | physics.soc-ph physics.data-an | random walks defined on undirected graphs assign the absolute scores to all nodes based on the quality of path they provide for random walkers in city space syntax the notion of segregation acquires a statistical interpretation with respect to random walks we analyze the spatial network of venetian canals and detect it... | [['random', 'walks', 'defined', 'on', 'undirected', 'graphs', 'assign', 'the', 'absolute', 'scores', 'to', 'all', 'nodes', 'based', 'on', 'the', 'quality', 'of', 'path', 'they', 'provide', 'for', 'random', 'walkers', 'in', 'city', 'space', 'syntax', 'the', 'notion', 'of', 'segregation', 'acquires', 'a', 'statistical', ... | [-0.11803451844775048, 0.1391821854437391, -0.08380134589970112, 0.04052576678805053, -0.09093110652104246, -0.13803529450105448, 0.07151656920993418, 0.45657814909337147, -0.2514847824014864, -0.28998736218482285, 0.06914234073712688, -0.28563284152892954, -0.13948776867508775, 0.08907296023134029, -0.1103617126037451... |
710.3022 | Electroweak Precision Physics from Low to High Energies | Electroweak precision observables (EWPO) can give valuable information about
the last unknown paramter of the Standard Model (SM), the Higgs-boson mass
M_H^SM. EWPO can also restrict the parameter space of new physics models (NPM)
such as the Minimal Supersymmetric Standard Model (MSSM). We review the
respective cons... | hep-ph | electroweak precision observables ewpo can give valuable information about the last unknown paramter of the standard model sm the higgsboson mass m_hsm ewpo can also restrict the parameter space of new physics models npm such as the minimal supersymmetric standard model mssm we review the respective constraints from th... | [['electroweak', 'precision', 'observables', 'ewpo', 'can', 'give', 'valuable', 'information', 'about', 'the', 'last', 'unknown', 'paramter', 'of', 'the', 'standard', 'model', 'sm', 'the', 'higgsboson', 'mass', 'm_hsm', 'ewpo', 'can', 'also', 'restrict', 'the', 'parameter', 'space', 'of', 'new', 'physics', 'models', 'n... | [-0.06340397524049962, 0.2715469440796746, 0.002079286331416301, 0.22132530977690312, -0.13476577007545615, -0.16964824667270734, 0.04572916549536013, 0.283403066582187, -0.23045596306405539, -0.35117990275809785, 0.049693743836679405, -0.23677336406138427, 0.050350470004937135, 0.16047307524285367, 0.0383578789143665,... |
710.3023 | Large Eddy Simulation of Solar Photosphere Convection with Realistic
Physics | Three-dimensional large eddy simulations of solar surface convection using
realistic model physics are conducted. The thermal structure of convective
motions into the upper radiative layers of the photosphere, the range of
convection cell sizes, and the penetration depths of convection are
investigated. A portion of ... | astro-ph | threedimensional large eddy simulations of solar surface convection using realistic model physics are conducted the thermal structure of convective motions into the upper radiative layers of the photosphere the range of convection cell sizes and the penetration depths of convection are investigated a portion of the sol... | [['threedimensional', 'large', 'eddy', 'simulations', 'of', 'solar', 'surface', 'convection', 'using', 'realistic', 'model', 'physics', 'are', 'conducted', 'the', 'thermal', 'structure', 'of', 'convective', 'motions', 'into', 'the', 'upper', 'radiative', 'layers', 'of', 'the', 'photosphere', 'the', 'range', 'of', 'conv... | [-0.11834206493666112, 0.18503703560364776, -0.009668022030875703, 0.0370991734049867, -0.03554213982033359, -0.05940484779092383, 0.042080248448219004, 0.32719310933966084, -0.2701585495181508, -0.38695134819316873, 0.1063089247715349, -0.2553794572740204, -0.005048058974414559, 0.2030854391014351, 0.01058008695415242... |
710.3024 | Apparition de structures tourbillonnaires de type G\"ortler dans une
cavit\'e parall\'el\'epip\'edique ouverte de forme variable | The interaction between a laminar boundary layer and an open cavity is
investigated experimentally for Reynolds numbers between 860 and 32300. Flow
visualizations are carried out for different observation directions in order to
understand the spatial development of dynamical structures. The study is
conducted by chan... | physics.class-ph | the interaction between a laminar boundary layer and an open cavity is investigated experimentally for reynolds numbers between 860 and 32300 flow visualizations are carried out for different observation directions in order to understand the spatial development of dynamical structures the study is conducted by changing... | [['the', 'interaction', 'between', 'a', 'laminar', 'boundary', 'layer', 'and', 'an', 'open', 'cavity', 'is', 'investigated', 'experimentally', 'for', 'reynolds', 'numbers', 'between', '860', 'and', '32300', 'flow', 'visualizations', 'are', 'carried', 'out', 'for', 'different', 'observation', 'directions', 'in', 'order'... | [-0.2054419852466437, 0.19418238909833904, -0.07072021705997095, 0.024932460749129717, -0.055301841479121594, -0.08115354350465759, -0.022507922191850906, 0.3978791164490599, -0.3079469119149603, -0.28078192087674614, 0.1253114274576339, -0.24453112359665202, -0.1186330974624868, 0.2088485679082703, 0.01342428450292924... |
710.3025 | Formation of collective spins in frustrated clusters | Using magnetization, specific heat and neutron scattering measurements, as
well as exact calculations on realistic models, the magnetic properties of the
\lacuvo compound are characterized on a wide temperature range. At high
temperature, this oxide is well described by strongly correlated atomic $S$=1/2
spins while ... | cond-mat.str-el | using magnetization specific heat and neutron scattering measurements as well as exact calculations on realistic models the magnetic properties of the lacuvo compound are characterized on a wide temperature range at high temperature this oxide is well described by strongly correlated atomic s12 spins while decreasing t... | [['using', 'magnetization', 'specific', 'heat', 'and', 'neutron', 'scattering', 'measurements', 'as', 'well', 'as', 'exact', 'calculations', 'on', 'realistic', 'models', 'the', 'magnetic', 'properties', 'of', 'the', 'lacuvo', 'compound', 'are', 'characterized', 'on', 'a', 'wide', 'temperature', 'range', 'at', 'high', '... | [-0.1537231541278356, 0.27168196555662977, 0.042930216473983006, 0.03558922321640916, -0.030986008739614105, -0.17680794077905568, 0.04060550909390316, 0.40626060431624983, -0.2840684930932649, -0.30650083331311956, 0.05576121124458757, -0.35727067774240956, -0.02297549076041484, 0.17847926937913067, 0.1150169230581439... |
710.3026 | Pion-nucleon P_33 and P_11 scatterings in the Lippmann-Schwinger
approach | We study the pion-nucleon P_33 and P_11 scattering, where the Delta and the
Roper resonances are seen, respectively. We use the Lippmann-Schwinger equation
extended to couple to a one-body state, and investigate nature of these
resonances by taking and omitting a one-baryon state into account. We see
validity and puz... | nucl-th | we study the pionnucleon p_33 and p_11 scattering where the delta and the roper resonances are seen respectively we use the lippmannschwinger equation extended to couple to a onebody state and investigate nature of these resonances by taking and omitting a onebaryon state into account we see validity and puzzle of the ... | [['we', 'study', 'the', 'pionnucleon', 'p_33', 'and', 'p_11', 'scattering', 'where', 'the', 'delta', 'and', 'the', 'roper', 'resonances', 'are', 'seen', 'respectively', 'we', 'use', 'the', 'lippmannschwinger', 'equation', 'extended', 'to', 'couple', 'to', 'a', 'onebody', 'state', 'and', 'investigate', 'nature', 'of', '... | [-0.09311110748421925, 0.13599071906355675, -0.08362849813420326, 0.14076986047439277, -0.06799728980695363, -0.09836878658097703, 0.07087470743863378, 0.2988457327737706, -0.1959432695293799, -0.2618084404457477, 0.0017612514420761727, -0.3358009520743508, -0.09143160536768846, 0.0652365417299734, 0.09683759225299582,... |
710.3027 | Classical Capacities of Averaged and Compound Quantum Channels | We determine the capacity of compound classical-quantum channels. As a
consequence we obtain the capacity formula for the averaged classical-quantum
channels. The capacity result for compound channels demonstrates, as in the
classical setting, the existence of reliable universal classical-quantum codes
in scenarios w... | quant-ph cs.IT math-ph math.IT math.MP | we determine the capacity of compound classicalquantum channels as a consequence we obtain the capacity formula for the averaged classicalquantum channels the capacity result for compound channels demonstrates as in the classical setting the existence of reliable universal classicalquantum codes in scenarios where the ... | [['we', 'determine', 'the', 'capacity', 'of', 'compound', 'classicalquantum', 'channels', 'as', 'a', 'consequence', 'we', 'obtain', 'the', 'capacity', 'formula', 'for', 'the', 'averaged', 'classicalquantum', 'channels', 'the', 'capacity', 'result', 'for', 'compound', 'channels', 'demonstrates', 'as', 'in', 'the', 'clas... | [-0.16306968602121516, 0.045599407982081175, -0.11679416889404898, 0.08601706797227023, -0.016442555673820997, -0.2243979922696067, 0.18293383902549665, 0.27822778215731986, -0.2947340342466549, -0.20942150094416193, 0.07699003052942816, -0.20959223966334536, -0.13158607988377974, 0.256832453812803, -0.0903884279792026... |
710.3028 | Approximation of definable sets by compact families, and upper bounds on
homotopy and homology | We prove new upper bounds on homotopy and homology groups of o-minimal sets
in terms of their approximations by compact o-minimal sets. In particular, we
improve the known upper bounds on Betti numbers of semialgebraic sets defined
by quantifier-free formulae, and obtain for the first time a singly exponential
bound ... | math.AG math.LO | we prove new upper bounds on homotopy and homology groups of ominimal sets in terms of their approximations by compact ominimal sets in particular we improve the known upper bounds on betti numbers of semialgebraic sets defined by quantifierfree formulae and obtain for the first time a singly exponential bound on betti... | [['we', 'prove', 'new', 'upper', 'bounds', 'on', 'homotopy', 'and', 'homology', 'groups', 'of', 'ominimal', 'sets', 'in', 'terms', 'of', 'their', 'approximations', 'by', 'compact', 'ominimal', 'sets', 'in', 'particular', 'we', 'improve', 'the', 'known', 'upper', 'bounds', 'on', 'betti', 'numbers', 'of', 'semialgebraic'... | [-0.20415688688600703, 0.095625692898076, -0.038570051189578534, 0.1875121535267681, -0.05083469178394547, -0.04291380867860945, 0.1400764092270817, 0.2442920161078551, -0.25401387363672256, -0.2951605677870767, 0.12154947184275702, -0.21215389549200023, -0.08847986520101715, 0.308341028967074, -0.12742626711925759, 0.... |
710.3029 | Glassiness in Simple Liquids | In previous work the parameter of glassiness was introduced to distinguish
between a liquid and a glass, using a formal analogy with the quantum Bose
system. The glassiness is defined in such a way that it is unity in a frozen
system and less than one in a liquid. In the present letter we revise first the
results obt... | cond-mat.stat-mech | in previous work the parameter of glassiness was introduced to distinguish between a liquid and a glass using a formal analogy with the quantum bose system the glassiness is defined in such a way that it is unity in a frozen system and less than one in a liquid in the present letter we revise first the results obtained... | [['in', 'previous', 'work', 'the', 'parameter', 'of', 'glassiness', 'was', 'introduced', 'to', 'distinguish', 'between', 'a', 'liquid', 'and', 'a', 'glass', 'using', 'a', 'formal', 'analogy', 'with', 'the', 'quantum', 'bose', 'system', 'the', 'glassiness', 'is', 'defined', 'in', 'such', 'a', 'way', 'that', 'it', 'is', ... | [-0.11014815873932093, 0.14729696636519898, -0.1331832270068979, 0.049452245122261554, -0.0037977130290258814, -0.11297785865004968, 0.0638763834161822, 0.3265934057050833, -0.2400803359147782, -0.2769567767692799, 0.09547255224660384, -0.28776766844438734, -0.17029610115827787, 0.13419960995842875, -0.0113209539731205... |
710.303 | A transient low-frequency QPO from the black hole binary GRS 1915+105 | We present the results of the timing analysis of five Rossi X-ray Timing
Explorer observations of the Black Hole Candidate GRS 1915+105 between 1996
September and 1997 December. The aim was to investigate the possible presence
of a type-B quasi-periodic oscillation (QPO). Since in other systems this QPO
is found to a... | astro-ph | we present the results of the timing analysis of five rossi xray timing explorer observations of the black hole candidate grs 1915105 between 1996 september and 1997 december the aim was to investigate the possible presence of a typeb quasiperiodic oscillation qpo since in other systems this qpo is found to appear duri... | [['we', 'present', 'the', 'results', 'of', 'the', 'timing', 'analysis', 'of', 'five', 'rossi', 'xray', 'timing', 'explorer', 'observations', 'of', 'the', 'black', 'hole', 'candidate', 'grs', '1915105', 'between', '1996', 'september', 'and', '1997', 'december', 'the', 'aim', 'was', 'to', 'investigate', 'the', 'possible'... | [-0.16791420824010855, 0.1097630831762217, -0.046850972293759695, 0.1363840773170523, -0.10352455691900105, -0.12355133104865672, 0.0632184474292444, 0.40754910294199365, -0.18455085134191904, -0.3283607517136261, 0.1381548481840582, -0.30735718992364125, -0.07847941895015538, 0.21290129862027243, -0.04838506394880824,... |
710.3031 | On a rigidity condition for Berwald Spaces | We show that which that for a Berwald structure, any Riemannian structure
that is preserved by the Berwald connection leaves the indicatrix invariant
under horizontal parallel transport. We also obtain the converse result: if
$({\bf M},F)$ is a Finsler structure such that there exists a Riemannian
structure that leav... | math.DG | we show that which that for a berwald structure any riemannian structure that is preserved by the berwald connection leaves the indicatrix invariant under horizontal parallel transport we also obtain the converse result if bf mf is a finsler structure such that there exists a riemannian structure that leaves invariant ... | [['we', 'show', 'that', 'which', 'that', 'for', 'a', 'berwald', 'structure', 'any', 'riemannian', 'structure', 'that', 'is', 'preserved', 'by', 'the', 'berwald', 'connection', 'leaves', 'the', 'indicatrix', 'invariant', 'under', 'horizontal', 'parallel', 'transport', 'we', 'also', 'obtain', 'the', 'converse', 'result',... | [-0.21133191757100192, 0.10096735500525315, -0.1224894835368583, 0.11919446071781414, -0.15438024487934615, -0.17787604135902305, -0.04403537799310135, 0.4227357294802603, -0.31963742628301445, -0.1918180901459173, 0.09397672817209049, -0.1703934886345738, -0.2603672820609063, 0.12790778053581323, -0.09102848441291013,... |
710.3032 | Hypergraph regularity and the multidimensional Szemer\'edi theorem | We prove analogues for hypergraphs of Szemer\'edi's regularity lemma and the
associated counting lemma for graphs. As an application, we give the first
combinatorial proof of the multidimensional Szemer\'edi theorem of Furstenberg
and Katznelson, and the first proof that provides an explicit bound. Similar
results wi... | math.CO | we prove analogues for hypergraphs of szemeredis regularity lemma and the associated counting lemma for graphs as an application we give the first combinatorial proof of the multidimensional szemeredi theorem of furstenberg and katznelson and the first proof that provides an explicit bound similar results with the same... | [['we', 'prove', 'analogues', 'for', 'hypergraphs', 'of', 'szemeredis', 'regularity', 'lemma', 'and', 'the', 'associated', 'counting', 'lemma', 'for', 'graphs', 'as', 'an', 'application', 'we', 'give', 'the', 'first', 'combinatorial', 'proof', 'of', 'the', 'multidimensional', 'szemeredi', 'theorem', 'of', 'furstenberg'... | [-0.08865282648850738, 0.014744930991891109, -0.17681650244394095, 0.13035685701643007, -0.08701900133204063, -0.12628793896381127, 0.06292532217073238, 0.24839577684968206, -0.26090417521358544, -0.31113821043932843, 0.15066413754218463, -0.25082157309151304, -0.13148169391551764, 0.2463930854731697, -0.20221963677934... |
710.3033 | Photoproduction of $\omega$ and $\omega$ in the Nuclear Medium | We reanalyze data from ELSA on $\omega$ production in nuclei, from where
claims of a large shift of the mass were made earlier, which are tied to a
certain election of the background in nuclei, very different in shape to the
one on the proton. The reanalysis shows that the data demand a very large width
of the $\omeg... | nucl-th | we reanalyze data from elsa on omega production in nuclei from where claims of a large shift of the mass were made earlier which are tied to a certain election of the background in nuclei very different in shape to the one on the proton the reanalysis shows that the data demand a very large width of the omega in the me... | [['we', 'reanalyze', 'data', 'from', 'elsa', 'on', 'omega', 'production', 'in', 'nuclei', 'from', 'where', 'claims', 'of', 'a', 'large', 'shift', 'of', 'the', 'mass', 'were', 'made', 'earlier', 'which', 'are', 'tied', 'to', 'a', 'certain', 'election', 'of', 'the', 'background', 'in', 'nuclei', 'very', 'different', 'in'... | [-0.09906803017275896, 0.14530042890184278, -0.11449860238752191, 0.0714533340659355, -0.04452097167935998, -0.09445605527776788, 0.06268523512376885, 0.3673669343826755, -0.22153278827767245, -0.3102946615459135, 0.07010265073001434, -0.30766823007131383, -0.033943741301062126, 0.18462298033155827, -0.0128251429500320... |
710.3034 | Effect of electron-electron interaction on the Fermi surface topology of
doped graphene | The electron-electron interactions effects on the shape of the Fermi surface
of doped graphene are investigated. The actual discrete nature of the lattice
is fully taken into account. A $\pi$-band tight-binding model, with
nearest-neighbor hopping integrals, is considered. We calculate the self-energy
corrections at ... | cond-mat.str-el cond-mat.mes-hall | the electronelectron interactions effects on the shape of the fermi surface of doped graphene are investigated the actual discrete nature of the lattice is fully taken into account a piband tightbinding model with nearestneighbor hopping integrals is considered we calculate the selfenergy corrections at zero temperatur... | [['the', 'electronelectron', 'interactions', 'effects', 'on', 'the', 'shape', 'of', 'the', 'fermi', 'surface', 'of', 'doped', 'graphene', 'are', 'investigated', 'the', 'actual', 'discrete', 'nature', 'of', 'the', 'lattice', 'is', 'fully', 'taken', 'into', 'account', 'a', 'piband', 'tightbinding', 'model', 'with', 'near... | [-0.17238599614990233, 0.17654231404968068, -0.06256916869608932, 0.12676868333782076, -0.057581021147574074, -0.13775535894607285, 0.025723804174757572, 0.39399585588546715, -0.267749588829424, -0.2680783128629612, -0.03925076492987903, -0.3747598758478344, -0.10887230898921205, 0.13706903169405507, 0.0581991531746049... |
710.3035 | NNLO Virtual corrections to W+ W- production at the LHC | We report on a recent calculation of the two-loop virtual QCD corrections to
the W boson pair production in the quark-anti-quark-annihilation channel in the
limit where all kinematical invariants are large compared to the mass of the W
boson. Our result is exact up to terms suppressed by powers of the W boson
mass. T... | hep-ph | we report on a recent calculation of the twoloop virtual qcd corrections to the w boson pair production in the quarkantiquarkannihilation channel in the limit where all kinematical invariants are large compared to the mass of the w boson our result is exact up to terms suppressed by powers of the w boson mass the infra... | [['we', 'report', 'on', 'a', 'recent', 'calculation', 'of', 'the', 'twoloop', 'virtual', 'qcd', 'corrections', 'to', 'the', 'w', 'boson', 'pair', 'production', 'in', 'the', 'quarkantiquarkannihilation', 'channel', 'in', 'the', 'limit', 'where', 'all', 'kinematical', 'invariants', 'are', 'large', 'compared', 'to', 'the'... | [-0.1306718555558473, 0.17557837419832747, -0.06152984254372617, 0.10093104945806165, -0.027620764371628564, -0.05609823708112041, 0.06937493187685807, 0.3084465159475803, -0.17610828448086976, -0.24858898852020503, 0.008141276310198009, -0.3055156475305557, -0.03094296375910441, 0.16810505244570473, 0.0389441766217351... |
710.3036 | On cardinality constrained cycle and path polytopes | Given a directed graph D = (N, A) and a sequence of positive integers 1 <=
c_1 < c_2 < ... < c_m <= |N|, we consider those path and cycle polytopes that
are defined as the convex hulls of simple paths and cycles of D of cardinality
c_p for some p, respectively. We present integer characterizations of these
polytopes ... | math.CO math.OC | given a directed graph d n a and a sequence of positive integers 1 c_1 c_2 c_m n we consider those path and cycle polytopes that are defined as the convex hulls of simple paths and cycles of d of cardinality c_p for some p respectively we present integer characterizations of these polytopes by facet defining linear ine... | [['given', 'a', 'directed', 'graph', 'd', 'n', 'a', 'and', 'a', 'sequence', 'of', 'positive', 'integers', '1', 'c_1', 'c_2', 'c_m', 'n', 'we', 'consider', 'those', 'path', 'and', 'cycle', 'polytopes', 'that', 'are', 'defined', 'as', 'the', 'convex', 'hulls', 'of', 'simple', 'paths', 'and', 'cycles', 'of', 'd', 'of', 'c... | [-0.2050364053130827, 0.16666620726781814, -0.02166705714030699, 0.05907752209089019, -0.06237527835606174, -0.20781491273082792, 0.07602361312707548, 0.3744036275131459, -0.3653918842700395, -0.25946832561272787, 0.1108543720964173, -0.30006109433756634, -0.15403395442884754, 0.18009741396526807, -0.09496594681986607,... |
710.3037 | The Stellar Population of the Chamaeleon I Star-Forming Region | I present a new census of the stellar population in the Chamaeleon I
star-forming region. Using optical and near-IR photometry and followup
spectroscopy, I have discovered 50 new members of Chamaeleon I, expanding the
census of known members to 226 objects. Fourteen of these new members have
spectral types later than... | astro-ph | i present a new census of the stellar population in the chamaeleon i starforming region using optical and nearir photometry and followup spectroscopy i have discovered 50 new members of chamaeleon i expanding the census of known members to 226 objects fourteen of these new members have spectral types later than m6 whic... | [['i', 'present', 'a', 'new', 'census', 'of', 'the', 'stellar', 'population', 'in', 'the', 'chamaeleon', 'i', 'starforming', 'region', 'using', 'optical', 'and', 'nearir', 'photometry', 'and', 'followup', 'spectroscopy', 'i', 'have', 'discovered', '50', 'new', 'members', 'of', 'chamaeleon', 'i', 'expanding', 'the', 'ce... | [-0.03237906973057638, 0.1241070219484066, -0.0781736937800837, 0.09753862457418076, -0.08177743939519581, -0.071902997981, 0.1144821457774703, 0.4008931564380493, -0.1322841585424902, -0.3747472425610146, 0.0563142304192761, -0.28879224060036507, 0.00902310832203236, 0.1589356877676868, -0.06627311257460429, -0.077888... |
710.3038 | Finite ma Errors of the Overlap Fermion | In this talk, we shall assess the finite ma errors from the overlap fermion.
We shall present results on the speed of light from the dispersion relation and
hyperfine splitting between the vector and pseudoscalar mesons as a function to
ma to reveal the m\Lambda_{QCD}a^2 and m^2a^2 errors. We conclude from this
study... | hep-lat | in this talk we shall assess the finite ma errors from the overlap fermion we shall present results on the speed of light from the dispersion relation and hyperfine splitting between the vector and pseudoscalar mesons as a function to ma to reveal the mlambda_qcda2 and m2a2 errors we conclude from this study that one s... | [['in', 'this', 'talk', 'we', 'shall', 'assess', 'the', 'finite', 'ma', 'errors', 'from', 'the', 'overlap', 'fermion', 'we', 'shall', 'present', 'results', 'on', 'the', 'speed', 'of', 'light', 'from', 'the', 'dispersion', 'relation', 'and', 'hyperfine', 'splitting', 'between', 'the', 'vector', 'and', 'pseudoscalar', 'm... | [-0.07759648564541222, 0.17301348723642723, -0.04804908399666218, 0.09528831805188306, -0.06591716009241186, -0.07399651772146554, 0.1494796861202064, 0.3861831854048528, -0.2330953229745654, -0.3343005083305271, 0.0593893546028994, -0.2757710320384879, -0.06018995843202758, 0.1592787227127701, -0.056082625530268014, -... |
710.3039 | The Speed of Light and the Hubble Parameter: The Mass-Boom Effect | We prove here that Newtons universal gravitation and momentum conservation
laws together reproduce Weinbergs relation. It is shown that the Hubble
parameter H must be built in this relation, or equivalently the age of the
Universe t. Using a wave-to-particle interaction technique we then prove that
the speed of light... | physics.gen-ph | we prove here that newtons universal gravitation and momentum conservation laws together reproduce weinbergs relation it is shown that the hubble parameter h must be built in this relation or equivalently the age of the universe t using a wavetoparticle interaction technique we then prove that the speed of light c decr... | [['we', 'prove', 'here', 'that', 'newtons', 'universal', 'gravitation', 'and', 'momentum', 'conservation', 'laws', 'together', 'reproduce', 'weinbergs', 'relation', 'it', 'is', 'shown', 'that', 'the', 'hubble', 'parameter', 'h', 'must', 'be', 'built', 'in', 'this', 'relation', 'or', 'equivalently', 'the', 'age', 'of', ... | [-0.12421229945756683, 0.1816969734106577, -0.10672203785327307, 0.05296111118748484, -0.08886847051873104, -0.11417742959151807, 0.03370963590182114, 0.31958065658960894, -0.24611157119499158, -0.3283324370960761, 0.061495203508029776, -0.24052140382181028, -0.03643532353055358, 0.17599848626750278, -0.018905690848716... |
710.304 | Relating on-shell and off-shell formalism in perturbative quantum field
theory | In the on-shell formalism (mostly used in perturbative quantum field theory)
the entries of the time ordered product T are on-shell fields (i.e. the basic
fields satisfy the free field equations). With that, (multi)linearity of T is
incompatible with the Action Ward identity. This can be circumvented by using
the off... | hep-th | in the onshell formalism mostly used in perturbative quantum field theory the entries of the time ordered product t are onshell fields ie the basic fields satisfy the free field equations with that multilinearity of t is incompatible with the action ward identity this can be circumvented by using the offshell formalism... | [['in', 'the', 'onshell', 'formalism', 'mostly', 'used', 'in', 'perturbative', 'quantum', 'field', 'theory', 'the', 'entries', 'of', 'the', 'time', 'ordered', 'product', 't', 'are', 'onshell', 'fields', 'ie', 'the', 'basic', 'fields', 'satisfy', 'the', 'free', 'field', 'equations', 'with', 'that', 'multilinearity', 'of... | [-0.13478211518836392, 0.1979482357079784, -0.08187694870708447, 0.08771977085639171, -0.06437874174531118, -0.12894059801600924, -0.005038061513419763, 0.3326533410419412, -0.21412203534740676, -0.2594460270107806, 0.05505889742896531, -0.24031960538138641, -0.1658374253758641, 0.1257039155291558, -0.02986230351407790... |
710.3041 | Effect of Rotation on the Stability of a Stalled Cylindrical Shock and
its Consequences for Core-Collapse Supernovae | A perturbative analysis is used to investigate the effect of rotation on the
instability of a steady accretion shock (SASI) in a simple toy-model, in view
of better understanding supernova explosions in which the collapsing core
contains angular momentum. A cylindrical geometry is chosen for the sake of
simplicity. E... | astro-ph | a perturbative analysis is used to investigate the effect of rotation on the instability of a steady accretion shock sasi in a simple toymodel in view of better understanding supernova explosions in which the collapsing core contains angular momentum a cylindrical geometry is chosen for the sake of simplicity even when... | [['a', 'perturbative', 'analysis', 'is', 'used', 'to', 'investigate', 'the', 'effect', 'of', 'rotation', 'on', 'the', 'instability', 'of', 'a', 'steady', 'accretion', 'shock', 'sasi', 'in', 'a', 'simple', 'toymodel', 'in', 'view', 'of', 'better', 'understanding', 'supernova', 'explosions', 'in', 'which', 'the', 'collap... | [-0.18213177586420431, 0.1596453352457112, -0.07410236330264632, 0.07607363901656716, -0.1050869806702914, -0.06958512214849852, -0.003558751097841173, 0.325465095159989, -0.2167352825489302, -0.25087966702628034, 0.09017752880864471, -0.22609901158608683, -0.06102858573206145, 0.22786349832166394, -0.00925583849534976... |
710.3042 | Large-Angular-Scale Clustering as a Clue to the Source of UHECRs | We show that future Ultra-High Energy Cosmic Ray samples should be able to
distinguish whether the sources of UHECRs are hosted by galaxy clusters or
ordinary galaxies, or whether the sources are uncorrelated with the large-scale
structure of the universe. Moreover, this is true independently of arrival
direction unc... | astro-ph | we show that future ultrahigh energy cosmic ray samples should be able to distinguish whether the sources of uhecrs are hosted by galaxy clusters or ordinary galaxies or whether the sources are uncorrelated with the largescale structure of the universe moreover this is true independently of arrival direction uncertaint... | [['we', 'show', 'that', 'future', 'ultrahigh', 'energy', 'cosmic', 'ray', 'samples', 'should', 'be', 'able', 'to', 'distinguish', 'whether', 'the', 'sources', 'of', 'uhecrs', 'are', 'hosted', 'by', 'galaxy', 'clusters', 'or', 'ordinary', 'galaxies', 'or', 'whether', 'the', 'sources', 'are', 'uncorrelated', 'with', 'the... | [-0.08673950621111241, 0.1749710204991667, -0.05101256396058792, 0.16577328394729798, -0.12883812273988346, -0.049599272528818496, -0.010870944194418067, 0.4308679933116461, -0.22096100742540634, -0.3908849825820653, 0.040247619884515494, -0.31162424240392284, -0.038470880242433246, 0.21904456410508524, 0.0058226641170... |
710.3043 | Quantum central limit theorem for continuous-time quantum walks on odd
graphs in quantum probability theory | The method of the quantum probability theory only requires simple structural
data of graph and allows us to avoid a heavy combinational argument often
necessary to obtain full description of spectrum of the adjacency matrix. In
the present paper, by using the idea of calculation of the probability
amplitudes for cont... | quant-ph | the method of the quantum probability theory only requires simple structural data of graph and allows us to avoid a heavy combinational argument often necessary to obtain full description of spectrum of the adjacency matrix in the present paper by using the idea of calculation of the probability amplitudes for continuo... | [['the', 'method', 'of', 'the', 'quantum', 'probability', 'theory', 'only', 'requires', 'simple', 'structural', 'data', 'of', 'graph', 'and', 'allows', 'us', 'to', 'avoid', 'a', 'heavy', 'combinational', 'argument', 'often', 'necessary', 'to', 'obtain', 'full', 'description', 'of', 'spectrum', 'of', 'the', 'adjacency',... | [-0.09898129857004914, 0.1223120200128792, -0.1091643141021263, 0.08241577948481865, -0.03166753364956542, -0.13982601040872197, 0.11730059170106757, 0.32240333341776506, -0.22522909552088544, -0.27062540073968366, 0.049557451672265176, -0.22551856537318424, -0.18088049063943837, 0.16360237694358173, -0.090769784658994... |
710.3044 | A Short Proof of the VPN Tree Routing Conjecture on Ring Networks | The VPN Tree Routing Conjecture states that there always exists an optimal
solution to the symmetric Virtual Private Network Design (sVPND) problem where
the paths between all terminals form a tree. Only recently, Hurkens, Keijsper,
and Stougie gave a proof of this conjecture for the special case of ring
networks. Th... | math.CO math.OC | the vpn tree routing conjecture states that there always exists an optimal solution to the symmetric virtual private network design svpnd problem where the paths between all terminals form a tree only recently hurkens keijsper and stougie gave a proof of this conjecture for the special case of ring networks their proof... | [['the', 'vpn', 'tree', 'routing', 'conjecture', 'states', 'that', 'there', 'always', 'exists', 'an', 'optimal', 'solution', 'to', 'the', 'symmetric', 'virtual', 'private', 'network', 'design', 'svpnd', 'problem', 'where', 'the', 'paths', 'between', 'all', 'terminals', 'form', 'a', 'tree', 'only', 'recently', 'hurkens'... | [-0.21314417094032725, 0.05855156609465231, -0.10616912553086877, 0.08679761633950124, -0.10941418469124271, -0.23751345223686454, 0.10242325681737503, 0.32576588014869584, -0.2629401807916229, -0.24198939600635483, 0.08865435010343588, -0.2093840305612463, -0.18084016552134213, 0.18704616124539272, -0.0840924788094328... |
710.3045 | Fano resonance in a two-level quantum dot side-coupled to leads | We theoretically study Fano resonance in a two-level quantum dot side-coupled
to two leads, which are connected by a direct channel. The resonance lineshape
is found to be deformed, from the conventional Fano form, by interlevel Coulomb
interaction and interlevel interference. We derive the connection between the
lin... | cond-mat.mes-hall cond-mat.str-el | we theoretically study fano resonance in a twolevel quantum dot sidecoupled to two leads which are connected by a direct channel the resonance lineshape is found to be deformed from the conventional fano form by interlevel coulomb interaction and interlevel interference we derive the connection between the lineshape de... | [['we', 'theoretically', 'study', 'fano', 'resonance', 'in', 'a', 'twolevel', 'quantum', 'dot', 'sidecoupled', 'to', 'two', 'leads', 'which', 'are', 'connected', 'by', 'a', 'direct', 'channel', 'the', 'resonance', 'lineshape', 'is', 'found', 'to', 'be', 'deformed', 'from', 'the', 'conventional', 'fano', 'form', 'by', '... | [-0.19060179700387553, 0.12371179369455647, -0.06238762277089769, 0.0797650655648405, -0.03895642986476776, -0.2031706788665837, 0.05411568673610288, 0.38411938221681685, -0.2583946022842567, -0.2576103345130659, -0.03052144793244744, -0.2823426772152916, -0.19795990999167165, 0.17075026580797775, 0.019309596646399724,... |
710.3046 | Topological Analysis of Foams and tetrahedral structures | In this paper we characterize foams and tetrahedral structures in a unified
way, by a simplified representation of both that conserves the system topology.
The paper presents a workflow for an automated characterization of the topology
of the void space, using a partition of the void space into polyhedral cells
conne... | cond-mat.mtrl-sci | in this paper we characterize foams and tetrahedral structures in a unified way by a simplified representation of both that conserves the system topology the paper presents a workflow for an automated characterization of the topology of the void space using a partition of the void space into polyhedral cells connected ... | [['in', 'this', 'paper', 'we', 'characterize', 'foams', 'and', 'tetrahedral', 'structures', 'in', 'a', 'unified', 'way', 'by', 'a', 'simplified', 'representation', 'of', 'both', 'that', 'conserves', 'the', 'system', 'topology', 'the', 'paper', 'presents', 'a', 'workflow', 'for', 'an', 'automated', 'characterization', '... | [-0.1114178716026722, 0.13263536319325483, -0.1251292671621876, 0.04837375811296218, -0.04199359244964224, -0.05952851697208082, 0.03986289071047956, 0.33492819967610327, -0.2400264209990905, -0.2752429482507262, 0.02550923929951015, -0.21873590257018805, -0.19175816757327063, 0.15605065186428738, -0.09936814653152164,... |
710.3047 | Quantum stability of self-organized atomic insulator-like states in
optical resonators | We investigate a paradigm example of cavity quantum electrodynamics with many
body systems: an ultracold atomic gas inside a pumped optical resonator. In
particular, we study the stability of atomic insulator-like states, confined by
the mechanical potential emerging from the cavity field spatial mode structure.
As i... | cond-mat.other quant-ph | we investigate a paradigm example of cavity quantum electrodynamics with many body systems an ultracold atomic gas inside a pumped optical resonator in particular we study the stability of atomic insulatorlike states confined by the mechanical potential emerging from the cavity field spatial mode structure as in open s... | [['we', 'investigate', 'a', 'paradigm', 'example', 'of', 'cavity', 'quantum', 'electrodynamics', 'with', 'many', 'body', 'systems', 'an', 'ultracold', 'atomic', 'gas', 'inside', 'a', 'pumped', 'optical', 'resonator', 'in', 'particular', 'we', 'study', 'the', 'stability', 'of', 'atomic', 'insulatorlike', 'states', 'conf... | [-0.16910241049776278, 0.21867877706788447, -0.04583418738432936, 0.01098080771854383, 0.03252523210005764, -0.1620004253898146, 0.05832308775427032, 0.3530834677711695, -0.25733764844952456, -0.2546867026794183, 0.03290863474462582, -0.27471100397797044, -0.10965643686985102, 0.15509080909829162, 0.031916393909479576,... |
710.3048 | Theoretical progress on cusp effect and Kl4 decays | The cusp effect in K \to 3\pi and data on K_e4 decays allow one to extract
experimental information on the elastic \pi\pi scattering amplitude near
threshold, and to confront the outcome of the analyses with predictions made in
the framework of QCD. In my talk I pointed out that these predictions concern
an isospin s... | hep-ph | the cusp effect in k to 3pi and data on k_e4 decays allow one to extract experimental information on the elastic pipi scattering amplitude near threshold and to confront the outcome of the analyses with predictions made in the framework of qcd in my talk i pointed out that these predictions concern an isospin symmetric... | [['the', 'cusp', 'effect', 'in', 'k', 'to', '3pi', 'and', 'data', 'on', 'k_e4', 'decays', 'allow', 'one', 'to', 'extract', 'experimental', 'information', 'on', 'the', 'elastic', 'pipi', 'scattering', 'amplitude', 'near', 'threshold', 'and', 'to', 'confront', 'the', 'outcome', 'of', 'the', 'analyses', 'with', 'predictio... | [-0.08809468941133772, 0.17897244756563482, -0.1115214951604611, 0.11429743718110479, -0.0639407527349839, -0.12548292567324196, 0.07840231720852112, 0.3402204541111919, -0.20112966844887548, -0.24483613316221414, 0.041367281024577096, -0.37135382499419956, -0.07192253246525857, 0.14019200734391407, 0.07888095711383063... |
710.3049 | Group Analysis of Variable Coefficient Diffusion-Convection Equations.
II. Contractions and Exact Solutions | This is the second part of the series of papers on symmetry properties of a
class of variable coefficient (1+1)-dimensional nonlinear diffusion-convection
equations of general form $f(x)u_t=(g(x)A(u)u_x)_x+h(x)B(u)u_x$. At first, we
review the results of Part 1 of the series on equivalence transformations and
group c... | math-ph math.MP | this is the second part of the series of papers on symmetry properties of a class of variable coefficient 11dimensional nonlinear diffusionconvection equations of general form fxu_tgxauu_x_xhxbuu_x at first we review the results of part 1 of the series on equivalence transformations and group classification of the clas... | [['this', 'is', 'the', 'second', 'part', 'of', 'the', 'series', 'of', 'papers', 'on', 'symmetry', 'properties', 'of', 'a', 'class', 'of', 'variable', 'coefficient', '11dimensional', 'nonlinear', 'diffusionconvection', 'equations', 'of', 'general', 'form', 'fxu_tgxauu_x_xhxbuu_x', 'at', 'first', 'we', 'review', 'the', '... | [-0.1569598385684744, 0.04819926114901642, -0.035063784324598536, 0.016721065175995507, -0.10389919308255668, -0.085045313100434, -0.015927160933993205, 0.2756832254114906, -0.27314231856553645, -0.2539751630000494, 0.13521287892858877, -0.28280236556462046, -0.15933417223945812, 0.20913408597310384, -0.035353291845294... |
710.305 | Theoretical progress on pi pi scattering lengths and phases | pi pi scattering at low energy is sensitive to the structure of the QCD
vacuum. I review the calculations of the pi pi scattering lengths and phases,
and group them in three cathegories: 1. those based on very general theoretical
constraints (like dispersion relations and crossing symmetry) and
phenomenology, 2. thos... | hep-ph hep-lat | pi pi scattering at low energy is sensitive to the structure of the qcd vacuum i review the calculations of the pi pi scattering lengths and phases and group them in three cathegories 1 those based on very general theoretical constraints like dispersion relations and crossing symmetry and phenomenology 2 those which in... | [['pi', 'pi', 'scattering', 'at', 'low', 'energy', 'is', 'sensitive', 'to', 'the', 'structure', 'of', 'the', 'qcd', 'vacuum', 'i', 'review', 'the', 'calculations', 'of', 'the', 'pi', 'pi', 'scattering', 'lengths', 'and', 'phases', 'and', 'group', 'them', 'in', 'three', 'cathegories', '1', 'those', 'based', 'on', 'very'... | [-0.10402107418579336, 0.18279941800041216, -0.10307510107718777, 0.05393399326430431, -0.08455202518962324, -0.0879380409559696, 0.058597940137831143, 0.38341054429143373, -0.2302839777404719, -0.2803140232007545, 0.0738168155663822, -0.3258768011825067, -0.1031295919772422, 0.136634340180121, 0.07042233251256518, 0.0... |
710.3051 | Pair correlations in sandpile model: a check of logarithmic conformal
field theory | We compute the correlations of two height variables in the two-dimensional
Abelian sandpile model. We extend the known result for two minimal heights to
the case when one of the heights is bigger than one. We find that the most
dominant correlation log r/r^4 exactly fits the prediction obtained within the
logarithmic... | cond-mat.stat-mech hep-th math-ph math.MP | we compute the correlations of two height variables in the twodimensional abelian sandpile model we extend the known result for two minimal heights to the case when one of the heights is bigger than one we find that the most dominant correlation log rr4 exactly fits the prediction obtained within the logarithmic confor... | [['we', 'compute', 'the', 'correlations', 'of', 'two', 'height', 'variables', 'in', 'the', 'twodimensional', 'abelian', 'sandpile', 'model', 'we', 'extend', 'the', 'known', 'result', 'for', 'two', 'minimal', 'heights', 'to', 'the', 'case', 'when', 'one', 'of', 'the', 'heights', 'is', 'bigger', 'than', 'one', 'we', 'fin... | [-0.09376352525281685, 0.10946233073870341, -0.0479976600251609, 0.173865746467426, 0.005323961860051862, -0.1530960743246531, -0.018451716817152273, 0.3224586834527414, -0.25655054471119204, -0.2706328229116345, 0.046734184259009826, -0.3050708878371451, -0.12844760526247598, 0.21693343458335018, 0.019413743560478366,... |
710.3052 | ALICE potential for heavy-flavour physics | The Large Hadron Collider (LHC), where lead nuclei will collide at the
unprecedented c.m.s. energy of 5.5 TeV per nucleon-nucleon pair, will offer new
and unique opportunities for the study of the properties of strongly
interacting matter at high energy density over extended volumes. We will
briefly explain why heavy... | nucl-ex | the large hadron collider lhc where lead nuclei will collide at the unprecedented cms energy of 55 tev per nucleonnucleon pair will offer new and unique opportunities for the study of the properties of strongly interacting matter at high energy density over extended volumes we will briefly explain why heavyflavour part... | [['the', 'large', 'hadron', 'collider', 'lhc', 'where', 'lead', 'nuclei', 'will', 'collide', 'at', 'the', 'unprecedented', 'cms', 'energy', 'of', '55', 'tev', 'per', 'nucleonnucleon', 'pair', 'will', 'offer', 'new', 'and', 'unique', 'opportunities', 'for', 'the', 'study', 'of', 'the', 'properties', 'of', 'strongly', 'i... | [-0.05592963392720432, 0.25061726993000183, -0.14233543076930014, 0.15622815913426363, -0.047803657075918805, -0.14468956376878997, -0.038664945835449, 0.3605355847173849, -0.24385673819562872, -0.3264090682984003, 0.03141521622121611, -0.3667813265645826, 0.0004429771703340717, 0.1940064098232904, 0.03683188811221437,... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.