id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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707.403 | Killing spinors on supersymmetric P-branes | A class of p-brane solutions for supersymmetric gravity theories with
negative cosmological constant are proposed and analyzed. The solutions are
purely bosonic and contain a worldsheet and a transverse section. The
classification relays on the number of intrinsic Killing spinors on the
worldsheet and the transverse ... | hep-th | a class of pbrane solutions for supersymmetric gravity theories with negative cosmological constant are proposed and analyzed the solutions are purely bosonic and contain a worldsheet and a transverse section the classification relays on the number of intrinsic killing spinors on the worldsheet and the transverse secti... | [['a', 'class', 'of', 'pbrane', 'solutions', 'for', 'supersymmetric', 'gravity', 'theories', 'with', 'negative', 'cosmological', 'constant', 'are', 'proposed', 'and', 'analyzed', 'the', 'solutions', 'are', 'purely', 'bosonic', 'and', 'contain', 'a', 'worldsheet', 'and', 'a', 'transverse', 'section', 'the', 'classificat... | [-0.19472849985859433, 0.11340067413498144, -0.023250183014229674, 0.0920707891011977, -0.11131821768205674, -0.17824388677101644, -0.06367429093931054, 0.3168020628270556, -0.11018245501565885, -0.23866805800648985, 0.09364355125294647, -0.32732085725597915, -0.11323070733762178, 0.1566736898461326, -0.009321128659438... |
707.4031 | Spin-triplet pairing instability of the spinon Fermi surface in a U(1)
spin liquid | Recent experiments on the organic compound \kappa-(ET)_2Cu_2(CN)_3 have
provided a promising example of a two dimensional spin liquid state. This phase
is described by a two-dimensional spinon Fermi sea coupled to a U(1) gauge
field. We study Kohn-Luttinger-like pairing instabilities of the spinon Fermi
surface due t... | cond-mat.str-el cond-mat.supr-con | recent experiments on the organic compound kappaet_2cu_2cn_3 have provided a promising example of a two dimensional spin liquid state this phase is described by a twodimensional spinon fermi sea coupled to a u1 gauge field we study kohnluttingerlike pairing instabilities of the spinon fermi surface due to singular inte... | [['recent', 'experiments', 'on', 'the', 'organic', 'compound', 'kappaet_2cu_2cn_3', 'have', 'provided', 'a', 'promising', 'example', 'of', 'a', 'two', 'dimensional', 'spin', 'liquid', 'state', 'this', 'phase', 'is', 'described', 'by', 'a', 'twodimensional', 'spinon', 'fermi', 'sea', 'coupled', 'to', 'a', 'u1', 'gauge',... | [-0.24491126530954396, 0.26664301195620177, -0.05693536003887215, 0.10333753406217404, -0.032274754820665455, -0.17718625904115684, 0.050643229322946244, 0.3469179073376033, -0.2009482041877859, -0.19431877122149352, 0.038285709114621994, -0.3064152828061624, -0.18673653910210466, 0.17772786675349755, 0.038380345603560... |
707.4032 | One-way Hash Function Based on Neural Network | A hash function is constructed based on a three-layer neural network. The
three neuron-layers are used to realize data confusion, diffusion and
compression respectively, and the multi-block hash mode is presented to support
the plaintext with variable length. Theoretical analysis and experimental
results show that th... | cs.CR cs.NE | a hash function is constructed based on a threelayer neural network the three neuronlayers are used to realize data confusion diffusion and compression respectively and the multiblock hash mode is presented to support the plaintext with variable length theoretical analysis and experimental results show that this hash f... | [['a', 'hash', 'function', 'is', 'constructed', 'based', 'on', 'a', 'threelayer', 'neural', 'network', 'the', 'three', 'neuronlayers', 'are', 'used', 'to', 'realize', 'data', 'confusion', 'diffusion', 'and', 'compression', 'respectively', 'and', 'the', 'multiblock', 'hash', 'mode', 'is', 'presented', 'to', 'support', '... | [-0.14913564854198033, 0.019322084319881267, -0.09461959579752552, 0.0726135719050136, -0.09324066791062553, -0.2683936793460614, 0.0781152479402307, 0.4394804916758504, -0.3004478111035294, -0.2609992012588514, 0.13336222485716764, -0.2732638924072186, -0.178757922594539, 0.21332952733565536, -0.08811085967140066, 0.1... |
707.4033 | Some gradient estimates for a diffusion equation on Riemannian manifolds | In this note we present some gradient estimates for the diffusion equation
$\partial_t u=\Delta u-\nabla \phi \cdot \nabla u $ on Riemannian manifolds,
where $\phi $ is a C^2 function, which generalize estimates of R. Hamilton's
and Qi S. Zhang's on the heat equation.
| math.DG | in this note we present some gradient estimates for the diffusion equation partial_t udelta unabla phi cdot nabla u on riemannian manifolds where phi is a c2 function which generalize estimates of r hamiltons and qi s zhangs on the heat equation | [['in', 'this', 'note', 'we', 'present', 'some', 'gradient', 'estimates', 'for', 'the', 'diffusion', 'equation', 'partial_t', 'udelta', 'unabla', 'phi', 'cdot', 'nabla', 'u', 'on', 'riemannian', 'manifolds', 'where', 'phi', 'is', 'a', 'c2', 'function', 'which', 'generalize', 'estimates', 'of', 'r', 'hamiltons', 'and', ... | [-0.19824783890951603, 0.021445799330692916, -0.03171367592932213, 0.007741517936145621, -0.1349300816544287, -0.21547779439771103, -0.08024155116263068, 0.27129016621481805, -0.3325468084020984, -0.1800940495782665, 0.07967419846681878, -0.4110703293256284, -0.11089751142121497, 0.1674743096477219, -0.1077121306609894... |
707.4034 | Multiplicative Order of Gauss Periods | We obtain a lower bound on the multiplicative order of Gauss periods which
generate normal bases over finite fields. This bound improves the previous
bound of J. von zur Gathen and I. E. Shparlinski.
| math.NT | we obtain a lower bound on the multiplicative order of gauss periods which generate normal bases over finite fields this bound improves the previous bound of j von zur gathen and i e shparlinski | [['we', 'obtain', 'a', 'lower', 'bound', 'on', 'the', 'multiplicative', 'order', 'of', 'gauss', 'periods', 'which', 'generate', 'normal', 'bases', 'over', 'finite', 'fields', 'this', 'bound', 'improves', 'the', 'previous', 'bound', 'of', 'j', 'von', 'zur', 'gathen', 'and', 'i', 'e', 'shparlinski']] | [-0.16366333843154066, 0.167146030566929, -0.10153556330239072, 0.012044864525224137, -0.07232521312749561, -0.12980078762013683, 0.12488809594994082, 0.21964782731169286, -0.19380722983795054, -0.2966185047784272, 0.02490338364013416, -0.26284732894632995, -0.08528665253235136, 0.25298609757138524, -0.1201879885869429... |
707.4035 | Submillimeter Array Observation of the Proto-Planetary Nebula CRL 618 in
the CO J=6-5 Line | We report on the results of a Submillimeter Array interferometric observation
of the proto-planetary nebula CRL 618 in the 12CO J=6-5 line. With the new
capability of SMA enabling us to use two receivers at a time, we also observed
simultaneously in the 12CO J=2-1 and 13CO J=2-1 lines. The 12CO J=6-5 and 13CO
J=2-1 l... | astro-ph | we report on the results of a submillimeter array interferometric observation of the protoplanetary nebula crl 618 in the 12co j65 line with the new capability of sma enabling us to use two receivers at a time we also observed simultaneously in the 12co j21 and 13co j21 lines the 12co j65 and 13co j21 lines were first ... | [['we', 'report', 'on', 'the', 'results', 'of', 'a', 'submillimeter', 'array', 'interferometric', 'observation', 'of', 'the', 'protoplanetary', 'nebula', 'crl', '618', 'in', 'the', '12co', 'j65', 'line', 'with', 'the', 'new', 'capability', 'of', 'sma', 'enabling', 'us', 'to', 'use', 'two', 'receivers', 'at', 'a', 'time... | [-0.08914705589551276, 0.03804963609442261, 0.04112034119560103, -0.032616293866398374, -0.05147572612708774, -0.09599487339674032, 0.022562019450112884, 0.5125463230562914, -0.1540211234081151, -0.2800935839114738, 0.09567671246755538, -0.2107638823306601, -0.00016126215338633566, 0.10453499851374443, 0.04399548842227... |
707.4036 | Disrupting Terrorist Networks, a dynamic fitness landscape approach | Over a period of approximately five years, Pankaj Ghemawat of Harvard
Business School and Daniel Levinthal of the Wharton School have been working on
a detailed simulation (producing approximately a million fitness landscape
graphs) in order to determine optimal patterns of decision-making for
corporations. In 2006, ... | nlin.AO | over a period of approximately five years pankaj ghemawat of harvard business school and daniel levinthal of the wharton school have been working on a detailed simulation producing approximately a million fitness landscape graphs in order to determine optimal patterns of decisionmaking for corporations in 2006 we adapt... | [['over', 'a', 'period', 'of', 'approximately', 'five', 'years', 'pankaj', 'ghemawat', 'of', 'harvard', 'business', 'school', 'and', 'daniel', 'levinthal', 'of', 'the', 'wharton', 'school', 'have', 'been', 'working', 'on', 'a', 'detailed', 'simulation', 'producing', 'approximately', 'a', 'million', 'fitness', 'landscap... | [-0.08982562742970565, 0.1035449548483178, -0.08879291074556397, 0.07953798563755468, -0.12599195897972315, -0.13801435199355586, 0.1199525263495088, 0.3936052042967523, -0.22748157941155958, -0.35179113979736837, 0.1366423550237382, -0.2877770170687005, -0.1656217377512346, 0.1681174332002206, -0.11797666782732637, -0... |
707.4037 | Feynman Diagrams and Differential Equations | We review in a pedagogical way the method of differential equations for the
evaluation of D-dimensionally regulated Feynman integrals. After dealing with
the general features of the technique, we discuss its application in the
context of one- and two-loop corrections to the photon propagator in QED, by
computing the ... | hep-ph | we review in a pedagogical way the method of differential equations for the evaluation of ddimensionally regulated feynman integrals after dealing with the general features of the technique we discuss its application in the context of one and twoloop corrections to the photon propagator in qed by computing the vacuum p... | [['we', 'review', 'in', 'a', 'pedagogical', 'way', 'the', 'method', 'of', 'differential', 'equations', 'for', 'the', 'evaluation', 'of', 'ddimensionally', 'regulated', 'feynman', 'integrals', 'after', 'dealing', 'with', 'the', 'general', 'features', 'of', 'the', 'technique', 'we', 'discuss', 'its', 'application', 'in',... | [-0.16671817733706057, 0.07254800115908056, -0.0764008192263805, 0.10395019779210551, -0.06884022440818514, -0.09726965665131022, -0.010432657520205044, 0.30696045175979014, -0.2104326602635219, -0.26324031068412423, 0.08123717785776152, -0.32379428783366293, -0.18063036430823176, 0.21392150704030014, -0.01515518482815... |
707.4038 | Dynamic modeling of competing technology designs, pricing and consumer
dynamics | The modeling of technology succession and new technology adoption includes a
wide array of techniques from complexity theory. In our previous work, we
applied the results of the Windrum-Birchenhall model to technology policy and
technology development strategies. However, as we began to explore the
Windrum-Birchenhal... | nlin.AO | the modeling of technology succession and new technology adoption includes a wide array of techniques from complexity theory in our previous work we applied the results of the windrumbirchenhall model to technology policy and technology development strategies however as we began to explore the windrumbirchenhall simula... | [['the', 'modeling', 'of', 'technology', 'succession', 'and', 'new', 'technology', 'adoption', 'includes', 'a', 'wide', 'array', 'of', 'techniques', 'from', 'complexity', 'theory', 'in', 'our', 'previous', 'work', 'we', 'applied', 'the', 'results', 'of', 'the', 'windrumbirchenhall', 'model', 'to', 'technology', 'policy... | [-0.06293462620681671, 0.058423715555796125, -0.08593642318117448, 0.03645271558570294, -0.08892857979555599, -0.11066679182447127, 0.06615190942710662, 0.36463507400734013, -0.24367033666167714, -0.3607901732215933, 0.10688069549515142, -0.24602132824203762, -0.20413469823008618, 0.23505074264229747, -0.09865384206145... |
707.4039 | Closed conformal Killing-Yano tensor and geodesic integrability | Assuming the existence of a single rank-2 closed conformal Killing-Yano
tensor with a certain symmetry we show that there exist mutually commuting
rank-2 Killing tensors and Killing vectors. We also discuss the condition of
separation of variables for the geodesic Hamilton-Jacobi equations.
| hep-th gr-qc | assuming the existence of a single rank2 closed conformal killingyano tensor with a certain symmetry we show that there exist mutually commuting rank2 killing tensors and killing vectors we also discuss the condition of separation of variables for the geodesic hamiltonjacobi equations | [['assuming', 'the', 'existence', 'of', 'a', 'single', 'rank2', 'closed', 'conformal', 'killingyano', 'tensor', 'with', 'a', 'certain', 'symmetry', 'we', 'show', 'that', 'there', 'exist', 'mutually', 'commuting', 'rank2', 'killing', 'tensors', 'and', 'killing', 'vectors', 'we', 'also', 'discuss', 'the', 'condition', 'o... | [-0.30231580324470997, 0.17908630674217074, -0.018626451802750427, 0.0031234532805337082, -0.1510496759742853, -0.16864585185872524, -0.09892993675367463, 0.31414465859000174, -0.25870328469734105, -0.1315445201027961, 0.08212930832052648, -0.2802885913822268, -0.19862492044367605, 0.036244898746233614, 0.0072521148692... |
707.404 | Leakage-induced decoherence during single electron spin manipulation in
a double quantum dot | Coherent single electron spin oscillation in a double quantum dot system
driven by a magnetic electron spin resonance field is studied theoretically
using a Bloch-type rate equation approach. The oscillation frequency and
relaxation time obtained using typical model parameters are consistent with
experiment findings.... | cond-mat.mes-hall quant-ph | coherent single electron spin oscillation in a double quantum dot system driven by a magnetic electron spin resonance field is studied theoretically using a blochtype rate equation approach the oscillation frequency and relaxation time obtained using typical model parameters are consistent with experiment findings the ... | [['coherent', 'single', 'electron', 'spin', 'oscillation', 'in', 'a', 'double', 'quantum', 'dot', 'system', 'driven', 'by', 'a', 'magnetic', 'electron', 'spin', 'resonance', 'field', 'is', 'studied', 'theoretically', 'using', 'a', 'blochtype', 'rate', 'equation', 'approach', 'the', 'oscillation', 'frequency', 'and', 'r... | [-0.17659143971072302, 0.24379626801900384, -0.05690117471644448, 0.08681393360667344, -0.010065063254700767, -0.1822668479807261, 0.049124307449286184, 0.3710823698279758, -0.29256215668800806, -0.2760351409100824, 0.02823142165499222, -0.2512758443442484, -0.07151144806606075, 0.2583366686762828, 0.04867227144228915,... |
707.4041 | Persistent Current in Two Coupled Rings | We report the solution of the persistent current in two coupled rings in the
presence of external magnetic fluxes. We showed that the magnetic fluxes modify
the global phase of the electronic wave function for multiple connected
geometry formed by the coupled rings. We obtained an exact solution for the
persistent cu... | cond-mat.mtrl-sci | we report the solution of the persistent current in two coupled rings in the presence of external magnetic fluxes we showed that the magnetic fluxes modify the global phase of the electronic wave function for multiple connected geometry formed by the coupled rings we obtained an exact solution for the persistent curren... | [['we', 'report', 'the', 'solution', 'of', 'the', 'persistent', 'current', 'in', 'two', 'coupled', 'rings', 'in', 'the', 'presence', 'of', 'external', 'magnetic', 'fluxes', 'we', 'showed', 'that', 'the', 'magnetic', 'fluxes', 'modify', 'the', 'global', 'phase', 'of', 'the', 'electronic', 'wave', 'function', 'for', 'mul... | [-0.21870413978331696, 0.07707977432675472, 0.011771483251076435, 0.002777706640206765, 0.0118712365940631, -0.10123919349198586, -0.005807846589840809, 0.3506180400498838, -0.21433196984509997, -0.292231078929851, 0.04546455731049667, -0.27065817276277, -0.1492839349938609, 0.17754668347258992, -0.025678074674976764, ... |
707.4042 | The passage time distribution for a birth-and-death chain: Strong
stationary duality gives a first stochastic proof | A well-known theorem usually attributed to Keilson states that, for an
irreducible continuous-time birth-and-death chain on the nonnegative integers
and any d, the passage time from state 0 to state d is distributed as a sum of
d independent exponential random variables. Until now, no probabilistic proof
of the theor... | math.PR | a wellknown theorem usually attributed to keilson states that for an irreducible continuoustime birthanddeath chain on the nonnegative integers and any d the passage time from state 0 to state d is distributed as a sum of d independent exponential random variables until now no probabilistic proof of the theorem has bee... | [['a', 'wellknown', 'theorem', 'usually', 'attributed', 'to', 'keilson', 'states', 'that', 'for', 'an', 'irreducible', 'continuoustime', 'birthanddeath', 'chain', 'on', 'the', 'nonnegative', 'integers', 'and', 'any', 'd', 'the', 'passage', 'time', 'from', 'state', '0', 'to', 'state', 'd', 'is', 'distributed', 'as', 'a'... | [-0.13665314602576906, 0.14785535877163056, -0.12001691558398306, 0.05253076126445237, -0.05537999553628088, -0.16108487643789324, 0.0803552666956204, 0.3244677339730385, -0.319981886803483, -0.220534024321075, 0.12237582376248957, -0.23278501734048837, -0.11794699778602946, 0.16200187324901066, -0.06544222415735325, 0... |
707.4043 | Created-by-current states in long Josephson junctions | Critical curves "critical current - external magnetic field" of long
Josephson junctions with inhomogeneity and variable width are studied. We
demonstrate the existence of the regions of magnetic field where some fluxon
states are stable only, if the external current through the junction is
different from zero. Posit... | cond-mat.supr-con cond-mat.mtrl-sci | critical curves critical current external magnetic field of long josephson junctions with inhomogeneity and variable width are studied we demonstrate the existence of the regions of magnetic field where some fluxon states are stable only if the external current through the junction is different from zero position and s... | [['critical', 'curves', 'critical', 'current', 'external', 'magnetic', 'field', 'of', 'long', 'josephson', 'junctions', 'with', 'inhomogeneity', 'and', 'variable', 'width', 'are', 'studied', 'we', 'demonstrate', 'the', 'existence', 'of', 'the', 'regions', 'of', 'magnetic', 'field', 'where', 'some', 'fluxon', 'states', ... | [-0.2618503377312498, 0.1826778177891604, -0.0029127998277544975, 0.005144092488229613, -0.040434831545942206, -0.12897847658446568, 0.03423538319766521, 0.36974796894937756, -0.26240205208940265, -0.27763057982718403, 0.037905278244182807, -0.27012041641229934, -0.06437859028916468, 0.18689992460422217, 0.020839739815... |
707.4044 | Four- and Five-Body Scattering Calculations | We study the five-quark system $uudd{\bar s}$ in the standard
non-relativistic quark model by solving the scattering problem. Using the
Gaussian Expansion Method (GEM), we perform the almost precise multi-quark
calculations by treating a very large five-body modelspace including the NK
scattering channel explicitly. ... | hep-ph | we study the fivequark system uuddbar s in the standard nonrelativistic quark model by solving the scattering problem using the gaussian expansion method gem we perform the almost precise multiquark calculations by treating a very large fivebody modelspace including the nk scattering channel explicitly although a lot o... | [['we', 'study', 'the', 'fivequark', 'system', 'uuddbar', 's', 'in', 'the', 'standard', 'nonrelativistic', 'quark', 'model', 'by', 'solving', 'the', 'scattering', 'problem', 'using', 'the', 'gaussian', 'expansion', 'method', 'gem', 'we', 'perform', 'the', 'almost', 'precise', 'multiquark', 'calculations', 'by', 'treati... | [-0.10753485267408765, 0.18973525802676494, -0.05590199033658092, 0.09582871238593585, 0.024394928420392367, -0.1297825204530874, 0.04778470228282878, 0.3491224685755487, -0.18672477793163406, -0.2681348584019221, -0.006963970196039344, -0.3107556218138108, -0.005868994779526614, 0.10745833131054847, 0.1009944048629572... |
707.4045 | Tubular Neighborhoods of Nodal Sets and Diophantine Approximation | We give upper and lower bounds on the volume of a tubular neighborhood of the
nodal set of an eigenfunction of the Laplacian on a real analytic closed
Riemannian manifold M. As an application we consider the question of
approximating points on M by nodal sets, and explore analogy with approximation
by rational number... | math.SP math.DG | we give upper and lower bounds on the volume of a tubular neighborhood of the nodal set of an eigenfunction of the laplacian on a real analytic closed riemannian manifold m as an application we consider the question of approximating points on m by nodal sets and explore analogy with approximation by rational numbers | [['we', 'give', 'upper', 'and', 'lower', 'bounds', 'on', 'the', 'volume', 'of', 'a', 'tubular', 'neighborhood', 'of', 'the', 'nodal', 'set', 'of', 'an', 'eigenfunction', 'of', 'the', 'laplacian', 'on', 'a', 'real', 'analytic', 'closed', 'riemannian', 'manifold', 'm', 'as', 'an', 'application', 'we', 'consider', 'the', ... | [-0.2117028772417042, 0.03965094373874039, -0.021981685310257255, 0.0804514779743773, -0.07362484035116655, -0.05714110359204588, 0.12547401649256548, 0.2848341615085869, -0.21324573457241058, -0.2901224913851668, 0.11627705685828847, -0.31114065471208757, -0.15371240205476405, 0.2369771689452507, -0.07530246969070975,... |
707.4046 | Clifford's theorem for coherent systems | Final version to appear in Archiv der Mathematik.
| math.AG | final version to appear in archiv der mathematik | [['final', 'version', 'to', 'appear', 'in', 'archiv', 'der', 'mathematik']] | [-0.08902360196225345, 0.019959306810051203, -0.13364478922449052, 0.061997453682124615, 0.027479460346512496, -0.17133128247223794, -0.04674345982493833, 0.17210850911214948, -0.13880314864218235, -0.3052022964693606, -0.06040488365397323, -0.3310390617698431, -0.14203363191336393, 0.19298049388453364, -0.228926629759... |
707.4047 | A construction of noncontractible simply connected cell-like two
dimensional Peano continua | Using the topologist sine curve we present a new functorial construction of
cone-like spaces, starting in the category of all path-connected topological
spaces with a base point and continuous maps, and ending in the subcategory of
all simply connected spaces. If one starts by a noncontractible n-dimensional
Peano co... | math.GT math.GN | using the topologist sine curve we present a new functorial construction of conelike spaces starting in the category of all pathconnected topological spaces with a base point and continuous maps and ending in the subcategory of all simply connected spaces if one starts by a noncontractible ndimensional peano continuum ... | [['using', 'the', 'topologist', 'sine', 'curve', 'we', 'present', 'a', 'new', 'functorial', 'construction', 'of', 'conelike', 'spaces', 'starting', 'in', 'the', 'category', 'of', 'all', 'pathconnected', 'topological', 'spaces', 'with', 'a', 'base', 'point', 'and', 'continuous', 'maps', 'and', 'ending', 'in', 'the', 'su... | [-0.15846944803280044, 0.14007172651910854, -0.09675185703729958, 0.07978540581915482, -0.09634842309686872, -0.19783428290077013, 0.0492934553084872, 0.3772041583318769, -0.29017154734443734, -0.10182942379909901, 0.12084660631529758, -0.2724607453486066, -0.1352024900721225, 0.1601125028754734, -0.1663034210027552, -... |
707.4048 | Theory for Magnetic Anisotropy of Field-Induced Insulator-to-Metal
Transition in Cubic Kondo Insulator YbB_{12} | Magnetization and energy gap of Kondo insulator YbB_{12} are calculated
theoretically based on the previously proposed tight-binding model composed of
Yb 5d$\epsilon$ and 4f $\Gamma_8$ orbitals. It is found that magnetization
curves are almost isotropic, naturally expected from the cubic symmetry, but
that the gap-cl... | cond-mat.str-el | magnetization and energy gap of kondo insulator ybb_12 are calculated theoretically based on the previously proposed tightbinding model composed of yb 5depsilon and 4f gamma_8 orbitals it is found that magnetization curves are almost isotropic naturally expected from the cubic symmetry but that the gapclosing field has... | [['magnetization', 'and', 'energy', 'gap', 'of', 'kondo', 'insulator', 'ybb_12', 'are', 'calculated', 'theoretically', 'based', 'on', 'the', 'previously', 'proposed', 'tightbinding', 'model', 'composed', 'of', 'yb', '5depsilon', 'and', '4f', 'gamma_8', 'orbitals', 'it', 'is', 'found', 'that', 'magnetization', 'curves',... | [-0.15554433654140787, 0.1602078403084306, -0.034613053562450355, 0.054633082492303135, -0.029956134682451594, -0.12413331218690515, 0.03770241558238446, 0.410699354715332, -0.22022057230210054, -0.32799107689306, -0.003089864436911297, -0.31977359783426623, -0.08148813958140526, 0.2069903117224844, 0.05828488285644589... |
707.4049 | A Dark Energy Model Characterized by the Age of the Universe | Quantum mechanics together with general relativity leads to the
K\'arolyh\'azy relation and a corresponding energy density of quantum
fluctuations of space-time. Based on the energy density we propose a dark
energy model, in which the age of the universe is introduced as the length
measure. This dark energy is cons... | hep-th astro-ph gr-qc hep-ph | quantum mechanics together with general relativity leads to the karolyhazy relation and a corresponding energy density of quantum fluctuations of spacetime based on the energy density we propose a dark energy model in which the age of the universe is introduced as the length measure this dark energy is consistent with ... | [['quantum', 'mechanics', 'together', 'with', 'general', 'relativity', 'leads', 'to', 'the', 'karolyhazy', 'relation', 'and', 'a', 'corresponding', 'energy', 'density', 'of', 'quantum', 'fluctuations', 'of', 'spacetime', 'based', 'on', 'the', 'energy', 'density', 'we', 'propose', 'a', 'dark', 'energy', 'model', 'in', '... | [-0.12143183907028288, 0.15436669340137346, -0.16612352455350837, 0.10475260962786186, -0.06380637392742626, -0.09648179435420648, -0.017578969209612945, 0.3011266560684557, -0.242938976327423, -0.3470137164528881, 0.027637320511920343, -0.26124843534281744, -0.023160406005834893, 0.13442483080975112, -0.00019068221860... |
707.405 | A universal property for the Jiang-Su algebra | We prove that the infinite tensor power of a unital separable C*-algebra
absorbs the Jiang-Su algebra Z tensorially if and only if it contains,
unitally, a subhomogeneous algebra without characters. This yields a succinct
universal property for Z in a category so large that there are no unital
separable C*-algebras w... | math.OA | we prove that the infinite tensor power of a unital separable calgebra absorbs the jiangsu algebra z tensorially if and only if it contains unitally a subhomogeneous algebra without characters this yields a succinct universal property for z in a category so large that there are no unital separable calgebras without cha... | [['we', 'prove', 'that', 'the', 'infinite', 'tensor', 'power', 'of', 'a', 'unital', 'separable', 'calgebra', 'absorbs', 'the', 'jiangsu', 'algebra', 'z', 'tensorially', 'if', 'and', 'only', 'if', 'it', 'contains', 'unitally', 'a', 'subhomogeneous', 'algebra', 'without', 'characters', 'this', 'yields', 'a', 'succinct', ... | [-0.11097658036316049, 0.16256728577472657, -0.06431214569766126, 0.03981337943983356, -0.13874490804393108, -0.19724089382413093, -0.017244635605659912, 0.41718275995242976, -0.3610310083989736, -0.08773709534549377, 0.13839132244892183, -0.2660441416656782, -0.08400198557696134, 0.2136775931236039, -0.161105276695387... |
707.4051 | Zero delay synchronization of chaos in coupled map lattices | We show that two coupled map lattices that are mutually coupled to one
another with a delay can display zero delay synchronization if they are driven
by a third coupled map lattice. We analytically estimate the parametric regimes
that lead to synchronization and show that the presence of mutual delays
enhances synchr... | nlin.CD nlin.AO | we show that two coupled map lattices that are mutually coupled to one another with a delay can display zero delay synchronization if they are driven by a third coupled map lattice we analytically estimate the parametric regimes that lead to synchronization and show that the presence of mutual delays enhances synchroni... | [['we', 'show', 'that', 'two', 'coupled', 'map', 'lattices', 'that', 'are', 'mutually', 'coupled', 'to', 'one', 'another', 'with', 'a', 'delay', 'can', 'display', 'zero', 'delay', 'synchronization', 'if', 'they', 'are', 'driven', 'by', 'a', 'third', 'coupled', 'map', 'lattice', 'we', 'analytically', 'estimate', 'the', ... | [-0.24293264116059585, 0.16825392542698656, -0.03917335530361497, 0.041822729796361945, -0.03440182810896132, -0.2280320465138339, 0.07795786554083588, 0.4106042085282774, -0.2931718935366686, -0.24532509507633835, 0.11913830015621799, -0.2727401147804122, -0.20383783949802753, 0.17708596077478345, -0.065689709347691, ... |
707.4052 | Interacting Agegraphic Dark Energy | A new dark energy model, named "agegraphic dark energy", has been proposed
recently, based on the so-called K\'{a}rolyh\'{a}zy uncertainty relation, which
arises from quantum mechanics together with general relativity. In this note,
we extend the original agegraphic dark energy model by including the
interaction betw... | hep-th astro-ph gr-qc hep-ph | a new dark energy model named agegraphic dark energy has been proposed recently based on the socalled karolyhazy uncertainty relation which arises from quantum mechanics together with general relativity in this note we extend the original agegraphic dark energy model by including the interaction between agegraphic dark... | [['a', 'new', 'dark', 'energy', 'model', 'named', 'agegraphic', 'dark', 'energy', 'has', 'been', 'proposed', 'recently', 'based', 'on', 'the', 'socalled', 'karolyhazy', 'uncertainty', 'relation', 'which', 'arises', 'from', 'quantum', 'mechanics', 'together', 'with', 'general', 'relativity', 'in', 'this', 'note', 'we', ... | [-0.10717153510726664, 0.15016423151625888, -0.24152683856917304, 0.23933753860562676, -0.14128465009043398, -0.211593260052209, -0.10852135492377388, 0.2697803267713069, -0.21832595674483024, -0.49814111943883094, -0.12989156478357947, -0.2825428154218294, -0.039734810322482626, 0.0832200470739854, 0.03718188706704456... |
707.4053 | Microlensing optical depth as a function of source apparent magnitude | Measurements of the microlensing optical depth, tau, towards the Galactic
bulge appear to depend on the method used to obtain them. Those values based on
the lensing of red clump giants (RCGs) appear to be significantly lower than
those based on the lensing of all stars along the line of sight. This
discrepancy is st... | astro-ph | measurements of the microlensing optical depth tau towards the galactic bulge appear to depend on the method used to obtain them those values based on the lensing of red clump giants rcgs appear to be significantly lower than those based on the lensing of all stars along the line of sight this discrepancy is still not ... | [['measurements', 'of', 'the', 'microlensing', 'optical', 'depth', 'tau', 'towards', 'the', 'galactic', 'bulge', 'appear', 'to', 'depend', 'on', 'the', 'method', 'used', 'to', 'obtain', 'them', 'those', 'values', 'based', 'on', 'the', 'lensing', 'of', 'red', 'clump', 'giants', 'rcgs', 'appear', 'to', 'be', 'significant... | [-0.0862087918185564, 0.12050384879762004, -0.08806782203271639, 0.10798912837527433, -0.09715777130385991, -0.08422527352434604, 0.08481112706886475, 0.3648339583040323, -0.22208141182362492, -0.36117363504545635, 0.08746089809736626, -0.290670592090938, -0.048428942024881065, 0.2557990345733002, -0.02082188801407113,... |
707.4054 | Deformations of Lie algebras of vector fields arising from families of
schemes | Fialowski and Schlichenmaier constructed examples of global deformations of
Lie algebras of vector fields from deforming the underlying variety. We
formulate their approach in a conceptual way. Namely, we construct a stack of
deformations and a morphism form the moduli stack of stable marked curves. The
morphism asso... | math.AG math-ph math.MP | fialowski and schlichenmaier constructed examples of global deformations of lie algebras of vector fields from deforming the underlying variety we formulate their approach in a conceptual way namely we construct a stack of deformations and a morphism form the moduli stack of stable marked curves the morphism associates... | [['fialowski', 'and', 'schlichenmaier', 'constructed', 'examples', 'of', 'global', 'deformations', 'of', 'lie', 'algebras', 'of', 'vector', 'fields', 'from', 'deforming', 'the', 'underlying', 'variety', 'we', 'formulate', 'their', 'approach', 'in', 'a', 'conceptual', 'way', 'namely', 'we', 'construct', 'a', 'stack', 'o... | [-0.2050416220859107, 0.052818839510695804, -0.10844665316657888, 0.036175302473000354, -0.09601888271152145, -0.10234446506429877, 0.014198638564751793, 0.3782213444304135, -0.3960046361924873, -0.21711838868343167, 0.06924288752876843, -0.2262673835787508, -0.1918580131398307, 0.20731708716808095, -0.1391885802460213... |
707.4055 | Photo-induced precession of magnetization in ferromagnetic (Ga,Mn)As | Precession of magnetization induced by pulsed optical excitation is observed
in a ferromagnetic semiconductor (Ga,Mn)As by time-resolved magneto-optical
measurements. It appears as complicated oscillations of polarization plane of
linearly-polarized probe pulses, but is reproduced by gyromagnetic theory
incorporating... | cond-mat.mtrl-sci | precession of magnetization induced by pulsed optical excitation is observed in a ferromagnetic semiconductor gamnas by timeresolved magnetooptical measurements it appears as complicated oscillations of polarization plane of linearlypolarized probe pulses but is reproduced by gyromagnetic theory incorporating an impuls... | [['precession', 'of', 'magnetization', 'induced', 'by', 'pulsed', 'optical', 'excitation', 'is', 'observed', 'in', 'a', 'ferromagnetic', 'semiconductor', 'gamnas', 'by', 'timeresolved', 'magnetooptical', 'measurements', 'it', 'appears', 'as', 'complicated', 'oscillations', 'of', 'polarization', 'plane', 'of', 'linearly... | [-0.13929309005034157, 0.2610399014698487, -0.048428579696337695, 0.050202455783437475, -0.050647377752466125, -0.08870520304772071, 0.023503583679848818, 0.43651517580728977, -0.2822664583101869, -0.3435438220971264, -0.03863764067064039, -0.2532789714983664, -0.06254648249596358, 0.2597138792858459, 0.027694971702294... |
707.4056 | Inclusive Charm Production in Upsilon(nS) Decay | Based on the NRQCD factorization formalism, we calculate the inclusive charm
production rate in Upsilon(nS) decay at leading order in the strong coupling
constant alpha_s and the relative velocity v of the b quark in the quarkonium
rest frame. The branching fractions for Upsilon(nS) to charm for n=1, 2, and 3
are all... | hep-ph | based on the nrqcd factorization formalism we calculate the inclusive charm production rate in upsilonns decay at leading order in the strong coupling constant alpha_s and the relative velocity v of the b quark in the quarkonium rest frame the branching fractions for upsilonns to charm for n1 2 and 3 are all around 79 ... | [['based', 'on', 'the', 'nrqcd', 'factorization', 'formalism', 'we', 'calculate', 'the', 'inclusive', 'charm', 'production', 'rate', 'in', 'upsilonns', 'decay', 'at', 'leading', 'order', 'in', 'the', 'strong', 'coupling', 'constant', 'alpha_s', 'and', 'the', 'relative', 'velocity', 'v', 'of', 'the', 'b', 'quark', 'in',... | [-0.03103317369721819, 0.31274017991584746, -0.12280534466201992, 0.14569040687232235, -0.03144139893417961, -0.07531151870200627, 0.061629672787222624, 0.3113252219207975, -0.182721631649508, -0.16328000096972425, -0.12760654361417711, -0.40486444346877465, 0.14958800465345037, 0.07897885877444127, 0.12790746926763202... |
707.4057 | Inclusive Jet Production in DIS at High Q^2 and Extraction of the Strong
Coupling | Inclusive jet production is studied in neutral current deep-inelastic
positron-proton scattering at large four momentum transfer squared Q^2>150
GeV^2 with the H1 detector at HERA. The measurements are found to be well
described by calculations at next-to-leading order in perturbative QCD.
The running of the strong... | hep-ex | inclusive jet production is studied in neutral current deepinelastic positronproton scattering at large four momentum transfer squared q2150 gev2 with the h1 detector at hera the measurements are found to be well described by calculations at nexttoleading order in perturbative qcd the running of the strong coupling is ... | [['inclusive', 'jet', 'production', 'is', 'studied', 'in', 'neutral', 'current', 'deepinelastic', 'positronproton', 'scattering', 'at', 'large', 'four', 'momentum', 'transfer', 'squared', 'q2150', 'gev2', 'with', 'the', 'h1', 'detector', 'at', 'hera', 'the', 'measurements', 'are', 'found', 'to', 'be', 'well', 'describe... | [-0.08317982890346849, 0.19962042385542936, -0.04161820187318054, 0.09785514348398217, 0.015938526307317343, -0.05631220089906657, -0.07360652129758488, 0.3755385912277482, -0.18029811810702084, -0.28162463872947474, 0.00219261932017451, -0.39864715642549775, 0.10132722522724759, 0.1328720150007443, 0.16123220817270603... |
707.4058 | Low energy effects of neutrino masses | While all models of Majorana neutrino masses lead to the same dimension five
effective operator, which does not conserve lepton number, the dimension six
operators induced at low energies conserve lepton number and differ depending
on the high energy model of new physics. We derive the low-energy dimension six
operat... | hep-ph | while all models of majorana neutrino masses lead to the same dimension five effective operator which does not conserve lepton number the dimension six operators induced at low energies conserve lepton number and differ depending on the high energy model of new physics we derive the lowenergy dimension six operators wh... | [['while', 'all', 'models', 'of', 'majorana', 'neutrino', 'masses', 'lead', 'to', 'the', 'same', 'dimension', 'five', 'effective', 'operator', 'which', 'does', 'not', 'conserve', 'lepton', 'number', 'the', 'dimension', 'six', 'operators', 'induced', 'at', 'low', 'energies', 'conserve', 'lepton', 'number', 'and', 'diffe... | [-0.1097121077708583, 0.2638931431021568, -0.0014721266198771219, 0.1369107152460843, -0.07506426390267062, -0.19285677488008185, 0.012823012217293915, 0.28132893213117166, -0.23775786439663604, -0.31382232814934763, 0.06507556260801217, -0.3060577521827204, -0.047274174903526055, 0.1605647570017646, 0.0534145924467461... |
707.4059 | Summary of H1 Results on the Strong Coupling from Inclusive and Final
States | Several determinations of the strong coupling from the H1 Collaboration are
reviewed.
| hep-ex | several determinations of the strong coupling from the h1 collaboration are reviewed | [['several', 'determinations', 'of', 'the', 'strong', 'coupling', 'from', 'the', 'h1', 'collaboration', 'are', 'reviewed']] | [-0.17550666288783154, 0.1846836827074488, 0.012350821169093251, 0.09476926107890904, -0.030152034635345142, -0.031351433135569096, -0.0426976860811313, 0.3657774192591508, -0.1968939770013094, -0.3292480440189441, 0.1187954768538475, -0.42107149834434193, 0.021688092810412247, 0.22600860831638178, 0.16706366080325097,... |
707.406 | Detection of warm molecular hydrogen in the circumstellar disk around
the Herbig Ae star HD97048 | We present high resolution spectroscopic mid-infrared observations of the
circumstellar disk around the Herbig Ae star HD97048 with the VLT Imager and
Spectrometer for the mid-InfraRed (VISIR). We detect the S(1) pure rotational
line of molecular hydrogen (H2) at 17.035 microns arising from the disk around
the star. ... | astro-ph | we present high resolution spectroscopic midinfrared observations of the circumstellar disk around the herbig ae star hd97048 with the vlt imager and spectrometer for the midinfrared visir we detect the s1 pure rotational line of molecular hydrogen h2 at 17035 microns arising from the disk around the star this detectio... | [['we', 'present', 'high', 'resolution', 'spectroscopic', 'midinfrared', 'observations', 'of', 'the', 'circumstellar', 'disk', 'around', 'the', 'herbig', 'ae', 'star', 'hd97048', 'with', 'the', 'vlt', 'imager', 'and', 'spectrometer', 'for', 'the', 'midinfrared', 'visir', 'we', 'detect', 'the', 's1', 'pure', 'rotational... | [-0.04147610612218434, 0.10848008904727685, -0.028739410192160125, 0.06506283951788237, -0.04135822481200231, -0.05838225975070568, 0.028897638563562693, 0.41924027562934973, -0.18371667990119322, -0.35865241065400943, 0.09014690668079671, -0.2706143745888003, 0.0200252174010594, 0.13532793127446704, -0.021126874718407... |
707.4061 | Generation of mesoscopic superpositions of a binary Bose-Einstein
condensate in a slightly asymmetric double well | A previous publication [Europhysics Letters 78, 10009 (2007)] suggested to
coherently generate mesoscopic superpositions of a two-component Bose-Einstein
condensate in a double well under perfectly symmetric conditions. However,
already tiny asymmetries can destroy the entanglement properties of the ground
state. Nev... | cond-mat.other | a previous publication europhysics letters 78 10009 2007 suggested to coherently generate mesoscopic superpositions of a twocomponent boseeinstein condensate in a double well under perfectly symmetric conditions however already tiny asymmetries can destroy the entanglement properties of the ground state nevertheless ev... | [['a', 'previous', 'publication', 'europhysics', 'letters', '78', '10009', '2007', 'suggested', 'to', 'coherently', 'generate', 'mesoscopic', 'superpositions', 'of', 'a', 'twocomponent', 'boseeinstein', 'condensate', 'in', 'a', 'double', 'well', 'under', 'perfectly', 'symmetric', 'conditions', 'however', 'already', 'ti... | [-0.1570141341567419, 0.2384901641074706, -0.09996506992589545, 0.1049796433524332, -0.006632891423241408, -0.1601203911403125, 0.01826714482848291, 0.33914385949847875, -0.19015539589303512, -0.2816284925987323, 0.009024485917675688, -0.22981787597139677, -0.08135973075749697, 0.18236218861097264, -0.04344898193246788... |
707.4062 | Quantum suppression of chaotic tunneling | The interplay between chaotic tunneling and dynamical localization in mixed
phase space is investigated. Semiclassical analysis using complex classical
orbits reveals that tunneling through torus regions and transport in chaotic
regions are not independent processes, rather they are strongly correlated and
described ... | nlin.CD quant-ph | the interplay between chaotic tunneling and dynamical localization in mixed phase space is investigated semiclassical analysis using complex classical orbits reveals that tunneling through torus regions and transport in chaotic regions are not independent processes rather they are strongly correlated and described by c... | [['the', 'interplay', 'between', 'chaotic', 'tunneling', 'and', 'dynamical', 'localization', 'in', 'mixed', 'phase', 'space', 'is', 'investigated', 'semiclassical', 'analysis', 'using', 'complex', 'classical', 'orbits', 'reveals', 'that', 'tunneling', 'through', 'torus', 'regions', 'and', 'transport', 'in', 'chaotic', ... | [-0.21020296641985292, 0.23130388126115908, -0.11684104071041061, 0.1311862139581618, 0.010804837807716633, -0.14863158344682728, 0.03249163640959358, 0.31865199645769526, -0.288231811507351, -0.23668772367421875, 0.05354712300918023, -0.26900116746335034, -0.24204877532214264, 0.22378098710694097, -0.04114234451712532... |
707.4063 | On classical and pseudobulges: The nature of bulges of early-type
spirals | Historically, galactic bulges are thought to be elliptical galaxy-like
objects sitting in the middle of a generally larger disk. There are, however,
more and more claims that some bulges are much more similar to disks. John
Kormendy has named these bulges pseudo-bulges. In this paper I discuss some
recent integral fi... | astro-ph | historically galactic bulges are thought to be elliptical galaxylike objects sitting in the middle of a generally larger disk there are however more and more claims that some bulges are much more similar to disks john kormendy has named these bulges pseudobulges in this paper i discuss some recent integral field spectr... | [['historically', 'galactic', 'bulges', 'are', 'thought', 'to', 'be', 'elliptical', 'galaxylike', 'objects', 'sitting', 'in', 'the', 'middle', 'of', 'a', 'generally', 'larger', 'disk', 'there', 'are', 'however', 'more', 'and', 'more', 'claims', 'that', 'some', 'bulges', 'are', 'much', 'more', 'similar', 'to', 'disks', ... | [-0.06964193507349895, 0.07222498335565129, -0.11837310976504038, 0.16256137473198276, -0.14560239689065688, -0.054854324040934446, -0.025329206481789393, 0.442126554188629, -0.12687725309903422, -0.3346552449821805, 0.03369691138407992, -0.2834569121633346, -0.10195425916075086, 0.2314348580354514, -0.0775705675647865... |
707.4064 | Local Leaders in Random Networks | We consider local leaders in random uncorrelated networks, i.e. nodes whose
degree is higher or equal than the degree of all of their neighbors. An
analytical expression is found for the probability of a node of degree $k$ to
be a local leader. This quantity is shown to exhibit a transition from a
situation where hig... | physics.soc-ph | we consider local leaders in random uncorrelated networks ie nodes whose degree is higher or equal than the degree of all of their neighbors an analytical expression is found for the probability of a node of degree k to be a local leader this quantity is shown to exhibit a transition from a situation where high degree ... | [['we', 'consider', 'local', 'leaders', 'in', 'random', 'uncorrelated', 'networks', 'ie', 'nodes', 'whose', 'degree', 'is', 'higher', 'or', 'equal', 'than', 'the', 'degree', 'of', 'all', 'of', 'their', 'neighbors', 'an', 'analytical', 'expression', 'is', 'found', 'for', 'the', 'probability', 'of', 'a', 'node', 'of', 'd... | [-0.15706112379242163, 0.15848672224228721, -0.06798203380700822, 0.03336064530958538, -0.0310441254429558, -0.17426739781027814, 0.04067168658002629, 0.3605775284037615, -0.25054562019067816, -0.2850274724866419, 0.05345312218196341, -0.3208750909640609, -0.16630403086552784, 0.12342498590927183, -0.02708391747122126,... |
707.4065 | C IV absorption in damped and sub-damped Lyman-alpha systems:
correlations with metallicity and implications for galactic winds at z~2-3 | We present a study of C IV absorption in a sample of 63 damped Lyman-alpha
(DLA) systems and 11 sub-DLAs in the redshift range 1.75<z_abs<3.61, using a
dataset of high-resolution (6.6 km/s FWHM), high signal-to-noise VLT/UVES
spectra. Narrow and broad C IV absorption line components indicate the presence
of both warm... | astro-ph | we present a study of c iv absorption in a sample of 63 damped lymanalpha dla systems and 11 subdlas in the redshift range 175z_abs361 using a dataset of highresolution 66 kms fwhm high signaltonoise vltuves spectra narrow and broad c iv absorption line components indicate the presence of both warm photoionized and hot... | [['we', 'present', 'a', 'study', 'of', 'c', 'iv', 'absorption', 'in', 'a', 'sample', 'of', '63', 'damped', 'lymanalpha', 'dla', 'systems', 'and', '11', 'subdlas', 'in', 'the', 'redshift', 'range', '175z_abs361', 'using', 'a', 'dataset', 'of', 'highresolution', '66', 'kms', 'fwhm', 'high', 'signaltonoise', 'vltuves', 's... | [-0.07437540992043179, 0.10371583003256006, 0.05510530181022154, 0.05306367354462808, -0.01929123388048299, -0.1478696213611825, 0.0634768725585887, 0.4390258629765575, -0.16697699288125792, -0.3343607876293035, -0.009555686855391186, -0.33072594165965064, 0.03646751335329731, 0.15875399920004435, 0.034067240646359846,... |
707.4066 | Fulde-Ferrell-Larkin-Ovchinnikov states in one-dimensional
spin-polarized ultracold atomic Fermi gases | We present a systematic study of quantum phases in a one-dimensional
spin-polarized Fermi gas. Three comparative theoretical methods are used to
explore the phase diagram at zero temperature: the mean-field theory with
either an order parameter in a single-plane-wave form or a self-consistently
determined order param... | cond-mat.stat-mech cond-mat.str-el | we present a systematic study of quantum phases in a onedimensional spinpolarized fermi gas three comparative theoretical methods are used to explore the phase diagram at zero temperature the meanfield theory with either an order parameter in a singleplanewave form or a selfconsistently determined order parameter using... | [['we', 'present', 'a', 'systematic', 'study', 'of', 'quantum', 'phases', 'in', 'a', 'onedimensional', 'spinpolarized', 'fermi', 'gas', 'three', 'comparative', 'theoretical', 'methods', 'are', 'used', 'to', 'explore', 'the', 'phase', 'diagram', 'at', 'zero', 'temperature', 'the', 'meanfield', 'theory', 'with', 'either'... | [-0.1641398792809692, 0.1944400330462991, -0.11249466450230795, 0.058916127025787274, -0.008917997092274683, -0.10959048346904594, 0.0860078699964409, 0.3458222226306264, -0.2363892129445929, -0.24263663363129284, 0.05341384093746513, -0.27053931168380324, -0.10401361536360272, 0.1274064324402605, 0.04640443839681601, ... |
707.4067 | The Equation of State of Dense Matter : from Nuclear Collisions to
Neutron Stars | The Equation of State (EoS) of dense matter represents a central issue in the
study of compact astrophysical objects and heavy ion reactions at intermediate
and relativistic energies. We have derived a nuclear EoS with nucleons and
hyperons within the Brueckner-Hartree-Fock approach, and joined it with quark
matter E... | nucl-th astro-ph hep-ph | the equation of state eos of dense matter represents a central issue in the study of compact astrophysical objects and heavy ion reactions at intermediate and relativistic energies we have derived a nuclear eos with nucleons and hyperons within the bruecknerhartreefock approach and joined it with quark matter eos for t... | [['the', 'equation', 'of', 'state', 'eos', 'of', 'dense', 'matter', 'represents', 'a', 'central', 'issue', 'in', 'the', 'study', 'of', 'compact', 'astrophysical', 'objects', 'and', 'heavy', 'ion', 'reactions', 'at', 'intermediate', 'and', 'relativistic', 'energies', 'we', 'have', 'derived', 'a', 'nuclear', 'eos', 'with... | [-0.023291925481451606, 0.2356049665077417, -0.1357303774587948, 0.11811452643531892, -0.05745329444848553, -0.12339147982722218, 0.02257073669763351, 0.36458365450164787, -0.13519191814810727, -0.35692997300066054, 0.020594468921276362, -0.29244712279695606, 0.04908663038750766, 0.09848288509399733, 0.0667658320916989... |
707.4068 | Experimental macroscopic coherence by phase-covariant cloning of a
single photon | We investigate the multiphoton states generated by high-gain optical
parametric amplification of a single injected photon, polarization encoded as a
''qubit''. The experiment configuration exploits the optimal phase-covariant
cloning in the high gain regime. The interference fringe pattern showing the
non local trans... | quant-ph | we investigate the multiphoton states generated by highgain optical parametric amplification of a single injected photon polarization encoded as a qubit the experiment configuration exploits the optimal phasecovariant cloning in the high gain regime the interference fringe pattern showing the non local transfer of cohe... | [['we', 'investigate', 'the', 'multiphoton', 'states', 'generated', 'by', 'highgain', 'optical', 'parametric', 'amplification', 'of', 'a', 'single', 'injected', 'photon', 'polarization', 'encoded', 'as', 'a', 'qubit', 'the', 'experiment', 'configuration', 'exploits', 'the', 'optimal', 'phasecovariant', 'cloning', 'in',... | [-0.1541951902098718, 0.1732394853223681, -0.07828693957174127, 0.07369268451569767, -0.012099716694483275, -0.19980748006602442, 0.04229108404214907, 0.38829458082872853, -0.2800577307956977, -0.29690030421708014, 0.000613378856001021, -0.2636458069510475, -0.039801186263042534, 0.19610695724811736, 0.0124207245940460... |
707.4069 | Atomic cluster state build up with macroscopic heralding | We describe a measurement-based state preparation scheme for the efficient
build up of cluster states in atom-cavity systems. As in a recent proposal for
the generation of maximally entangled atom pairs [Metz et al., Phys. Rev. Lett.
97, 040503 (2006)], we use an electron shelving technique to avoid the
necessity for... | quant-ph | we describe a measurementbased state preparation scheme for the efficient build up of cluster states in atomcavity systems as in a recent proposal for the generation of maximally entangled atom pairs metz et al phys rev lett 97 040503 2006 we use an electron shelving technique to avoid the necessity for the detection o... | [['we', 'describe', 'a', 'measurementbased', 'state', 'preparation', 'scheme', 'for', 'the', 'efficient', 'build', 'up', 'of', 'cluster', 'states', 'in', 'atomcavity', 'systems', 'as', 'in', 'a', 'recent', 'proposal', 'for', 'the', 'generation', 'of', 'maximally', 'entangled', 'atom', 'pairs', 'metz', 'et', 'al', 'phys... | [-0.08764737494978665, 0.17000990381984593, -0.00480425835121423, -0.03972928357325145, 0.02931234399875393, -0.13065838043500358, 0.10361504636360526, 0.35957604653473635, -0.16442172956036907, -0.33847966545727104, -0.013740568359935423, -0.26712888456434786, -0.052779310892219655, 0.23979946370066804, -0.08739869560... |
707.407 | Gauged Discrete Symmetries and Proton Stability | We discuss the results of a search for anomaly free Abelian Z_N discrete
symmetries that lead to automatic R-parity conservation and prevents dangerous
higher-dimensional proton decay operators in simple extensions of the minimal
supersymmetric extension of the standard model (MSSM) based on the left-right
symmetric ... | hep-ph | we discuss the results of a search for anomaly free abelian z_n discrete symmetries that lead to automatic rparity conservation and prevents dangerous higherdimensional proton decay operators in simple extensions of the minimal supersymmetric extension of the standard model mssm based on the leftright symmetric group t... | [['we', 'discuss', 'the', 'results', 'of', 'a', 'search', 'for', 'anomaly', 'free', 'abelian', 'z_n', 'discrete', 'symmetries', 'that', 'lead', 'to', 'automatic', 'rparity', 'conservation', 'and', 'prevents', 'dangerous', 'higherdimensional', 'proton', 'decay', 'operators', 'in', 'simple', 'extensions', 'of', 'the', 'm... | [-0.11546936169193656, 0.192483964472023, -0.02732020184539222, 0.16731784473556807, -0.15055367374089637, -0.1752882521781002, 0.03703466267332117, 0.3182890625697944, -0.1920964404091458, -0.29254360741698276, 0.10879649227147228, -0.22444259322376228, -0.07536071817637147, 0.1027437351032288, -0.054044535153034125, ... |
707.4071 | Dynamic heterogeneities in attractive colloids | We study the formation of a colloidal gel by means of Molecular Dynamics
simulations of a model for colloidal suspensions. A slowing down with gel-like
features is observed at low temperatures and low volume fractions, due to the
formation of persistent structures. We show that at low volume fraction the
dynamic susc... | cond-mat.soft cond-mat.dis-nn | we study the formation of a colloidal gel by means of molecular dynamics simulations of a model for colloidal suspensions a slowing down with gellike features is observed at low temperatures and low volume fractions due to the formation of persistent structures we show that at low volume fraction the dynamic susceptibi... | [['we', 'study', 'the', 'formation', 'of', 'a', 'colloidal', 'gel', 'by', 'means', 'of', 'molecular', 'dynamics', 'simulations', 'of', 'a', 'model', 'for', 'colloidal', 'suspensions', 'a', 'slowing', 'down', 'with', 'gellike', 'features', 'is', 'observed', 'at', 'low', 'temperatures', 'and', 'low', 'volume', 'fractions... | [-0.15019770570570076, 0.23968094102987694, -0.07295750390495295, 0.00926052870573071, 0.02721739358916555, -0.06973653092737431, 0.09284598837080209, 0.3381319163610106, -0.270128540330283, -0.29772415680041453, 0.06228680388860242, -0.2743248974985403, -0.13147334047471698, 0.10885497410781682, 0.010486843680463726, ... |
707.4072 | Families of dendrograms | A conceptual framework for cluster analysis from the viewpoint of p-adic
geometry is introduced by describing the space of all dendrograms for n
datapoints and relating it to the moduli space of p-adic Riemannian spheres
with punctures using a method recently applied by Murtagh (2004b). This method
embeds a dendrogra... | stat.ML | a conceptual framework for cluster analysis from the viewpoint of padic geometry is introduced by describing the space of all dendrograms for n datapoints and relating it to the moduli space of padic riemannian spheres with punctures using a method recently applied by murtagh 2004b this method embeds a dendrogram as a ... | [['a', 'conceptual', 'framework', 'for', 'cluster', 'analysis', 'from', 'the', 'viewpoint', 'of', 'padic', 'geometry', 'is', 'introduced', 'by', 'describing', 'the', 'space', 'of', 'all', 'dendrograms', 'for', 'n', 'datapoints', 'and', 'relating', 'it', 'to', 'the', 'moduli', 'space', 'of', 'padic', 'riemannian', 'sphe... | [-0.08165075976541951, 0.09286858050116137, -0.13152197881273048, 0.09318823122770946, -0.09888197199952807, -0.06763871799350954, 0.06975624884887342, 0.28416487310702604, -0.2900570040093918, -0.326956615290221, 0.06517858252353857, -0.24742289208898358, -0.18130519315280824, 0.2075124106360782, -0.13958863357045487,... |
707.4073 | Constraints on extremal self-dual CFTs | We argue that the existence of a modular differential equation implies that a
certain vector vanishes in Zhu's C2 quotient space, and we check this assertion
in numerous examples. If this connection is true in general, it would imply
that the recently conjectured extremal self-dual conformal field theories at
c=24 k ... | hep-th | we argue that the existence of a modular differential equation implies that a certain vector vanishes in zhus c2 quotient space and we check this assertion in numerous examples if this connection is true in general it would imply that the recently conjectured extremal selfdual conformal field theories at c24 k cannot e... | [['we', 'argue', 'that', 'the', 'existence', 'of', 'a', 'modular', 'differential', 'equation', 'implies', 'that', 'a', 'certain', 'vector', 'vanishes', 'in', 'zhus', 'c2', 'quotient', 'space', 'and', 'we', 'check', 'this', 'assertion', 'in', 'numerous', 'examples', 'if', 'this', 'connection', 'is', 'true', 'in', 'gener... | [-0.22585759596212915, 0.12952633468401537, -0.08727279028512146, 0.12058132355665102, -0.11048381659610752, -0.18555039162502476, -0.02318074627730407, 0.3291055322216268, -0.23478488686184087, -0.23314961500204445, 0.0986327259462294, -0.24811673840801968, -0.22634007402679376, 0.16318164800146692, -0.084989603347422... |
707.4074 | Suzaku Spectroscopy of the Extended X-Ray Emission in M17 | We present the results of a Suzaku spectroscopic study of the soft extended
X-ray emission in the HII region M17. The spectrum of the extended emission was
obtained with a high signal-to-noise ratio in a spatially-resolved manner using
the X-ray Imaging Spectrometer (XIS). We established that the contamination by
unr... | astro-ph | we present the results of a suzaku spectroscopic study of the soft extended xray emission in the hii region m17 the spectrum of the extended emission was obtained with a high signaltonoise ratio in a spatiallyresolved manner using the xray imaging spectrometer xis we established that the contamination by unresolved poi... | [['we', 'present', 'the', 'results', 'of', 'a', 'suzaku', 'spectroscopic', 'study', 'of', 'the', 'soft', 'extended', 'xray', 'emission', 'in', 'the', 'hii', 'region', 'm17', 'the', 'spectrum', 'of', 'the', 'extended', 'emission', 'was', 'obtained', 'with', 'a', 'high', 'signaltonoise', 'ratio', 'in', 'a', 'spatiallyres... | [-0.0394651546444931, 0.11271541727422131, 0.0014962002286287748, 0.07775983817930669, -0.005315805677979436, -0.06699632387714605, 0.028038392874697164, 0.46829866937714626, -0.19196543843617245, -0.34542678700139123, 0.04810554102503325, -0.34255535083240296, 0.02532366181608953, 0.17814486202349053, 0.04004800172198... |
707.4075 | Statistical hadronization model predictions for charmed hadrons at LHC | We present predictions of the statistical hadronization model for charmed
hadrons production in Pb+Pb collisions at LHC.
| nucl-th | we present predictions of the statistical hadronization model for charmed hadrons production in pbpb collisions at lhc | [['we', 'present', 'predictions', 'of', 'the', 'statistical', 'hadronization', 'model', 'for', 'charmed', 'hadrons', 'production', 'in', 'pbpb', 'collisions', 'at', 'lhc']] | [0.06036375683513196, 0.3282268536551034, -0.2719452459748615, 0.25108233401004004, 0.07235610380987911, -0.12848243391250863, -0.12956039515762208, 0.29669442948173075, -0.1305135859943488, -0.17656135318033836, -0.21565833020106176, -0.4953014673117329, 0.2891549926305957, 0.022375851198483038, 0.16872907857246258, 0... |
707.4076 | Thermal model predictions of hadron ratios at LHC | We present predictions of the thermal model for hadron ratios in central
Pb+Pb collisions at LHC.
| nucl-th | we present predictions of the thermal model for hadron ratios in central pbpb collisions at lhc | [['we', 'present', 'predictions', 'of', 'the', 'thermal', 'model', 'for', 'hadron', 'ratios', 'in', 'central', 'pbpb', 'collisions', 'at', 'lhc']] | [-0.013428169972030446, 0.2224650772404857, -0.2074546739750076, 0.12304976442828774, 0.13792405754793435, -0.12681088759563863, -0.13404684835404623, 0.3305762013187632, -0.11971865361556411, -0.23591765633318573, -0.0795921491298941, -0.39953028387390077, 0.21264762736973353, 0.13303383903985377, 0.11485276895109564,... |
707.4077 | The Polarised Valence Quark Distribution from semi-inclusive DIS | The semi-inclusive difference asymmetry A^{h^{+}-h^{-}} for hadrons of
opposite charge has been measured by the COMPASS experiment at CERN. The data
were collected in the years 2002-2004 using a 160 GeV polarised muon beam
scattered off a large polarised ^6LiD target and cover the range 0.006 < x <
0.7 and 1 < Q^2 < ... | hep-ex | the semiinclusive difference asymmetry ahh for hadrons of opposite charge has been measured by the compass experiment at cern the data were collected in the years 20022004 using a 160 gev polarised muon beam scattered off a large polarised 6lid target and cover the range 0006 x 07 and 1 q2 100 gevc2 in leading order qc... | [['the', 'semiinclusive', 'difference', 'asymmetry', 'ahh', 'for', 'hadrons', 'of', 'opposite', 'charge', 'has', 'been', 'measured', 'by', 'the', 'compass', 'experiment', 'at', 'cern', 'the', 'data', 'were', 'collected', 'in', 'the', 'years', '20022004', 'using', 'a', '160', 'gev', 'polarised', 'muon', 'beam', 'scatter... | [-0.07769260083908054, 0.23795371335271565, -0.06049924961982036, 0.11368913489042332, 0.005854129192992946, -0.11740256388307801, 0.06918493887048757, 0.33365941529982535, -0.19716577762074844, -0.3066047088471272, -0.02964671231753853, -0.3908716133666157, 0.11660429710115226, 0.13623456933554137, 0.02909113657938328... |
707.4078 | KLOE extraction of $a_\mu^{\pi\pi}$ in the mass range [0.35,0.95] GeV^2 | The KLOE Experiment at the $\phi$ factory DA$\Phi$NE, has measured the cross
section $\sigma(e^+e^-\to\pi^+\pi^-\gamma)$ using two different selection
schemes: requiring the photon emission at small polar angle and detecting the
photon at large polar angle in the calorimeter. Using a theoretical radiator
function we ... | hep-ex | the kloe experiment at the phi factory daphine has measured the cross section sigmaeetopipigamma using two different selection schemes requiring the photon emission at small polar angle and detecting the photon at large polar angle in the calorimeter using a theoretical radiator function we extract the pion form factor... | [['the', 'kloe', 'experiment', 'at', 'the', 'phi', 'factory', 'daphine', 'has', 'measured', 'the', 'cross', 'section', 'sigmaeetopipigamma', 'using', 'two', 'different', 'selection', 'schemes', 'requiring', 'the', 'photon', 'emission', 'at', 'small', 'polar', 'angle', 'and', 'detecting', 'the', 'photon', 'at', 'large',... | [-0.07027897732629579, 0.12917065991604568, -0.09483901573285619, 0.03335622668345558, -0.04878783842271313, -0.09054406617391617, 0.05446119427970769, 0.3500818529939081, -0.2045190147684015, -0.35171817715138576, 0.013666240050100741, -0.37915964341385566, 0.03163746675535878, 0.20083593020334523, 0.06733807278896108... |
707.4079 | The dwarf low surface brightness population in different environments of
the Local Universe | The nature of the dwarf galaxy population as a function of location in the
cluster and within different environments is investigated. We have previously
described the results of a search for low surface brightness objects in data
drawn from an East-West strip of the Virgo cluster (Sabatini et al., 2003) and
have comp... | astro-ph | the nature of the dwarf galaxy population as a function of location in the cluster and within different environments is investigated we have previously described the results of a search for low surface brightness objects in data drawn from an eastwest strip of the virgo cluster sabatini et al 2003 and have compared thi... | [['the', 'nature', 'of', 'the', 'dwarf', 'galaxy', 'population', 'as', 'a', 'function', 'of', 'location', 'in', 'the', 'cluster', 'and', 'within', 'different', 'environments', 'is', 'investigated', 'we', 'have', 'previously', 'described', 'the', 'results', 'of', 'a', 'search', 'for', 'low', 'surface', 'brightness', 'ob... | [-0.06436645597980128, 0.04906812802347823, -0.09366235049704763, 0.054763525324576186, -0.07576004422058873, -0.00764328068736648, 0.05820361488981475, 0.4046993814311258, -0.16017654203171036, -0.3668321562255611, 0.07032004251517843, -0.2828010009304274, -0.04792733336871987, 0.21585974608138397, -0.0730170946525890... |
707.408 | QCD prerequisites for extra dimension searches | For the dilepton production at hadron collider in TeV scale gravity models,
inclusion of QCD corrections to NLO stabilises the cross section with respect
to scale variations. The K-factors for the various distributions for the ADD
and RS model at both LHC and Tevatron are presented.
| hep-ph | for the dilepton production at hadron collider in tev scale gravity models inclusion of qcd corrections to nlo stabilises the cross section with respect to scale variations the kfactors for the various distributions for the add and rs model at both lhc and tevatron are presented | [['for', 'the', 'dilepton', 'production', 'at', 'hadron', 'collider', 'in', 'tev', 'scale', 'gravity', 'models', 'inclusion', 'of', 'qcd', 'corrections', 'to', 'nlo', 'stabilises', 'the', 'cross', 'section', 'with', 'respect', 'to', 'scale', 'variations', 'the', 'kfactors', 'for', 'the', 'various', 'distributions', 'fo... | [-0.0023597075512794695, 0.18981719051447252, -0.11618173711568765, 0.19303607770606226, -0.006966224324929974, -0.13417955428240416, -0.09393136259978233, 0.3386879554828224, -0.20387116886432405, -0.28190317628120637, 0.006069228668069548, -0.39478417289564793, 0.13244382227244583, 0.14822598675812554, 0.108494624414... |
707.4081 | Geometrical derivation of the Boltzmann factor | We show that the Boltzmann factor has a geometrical origin. Its derivation
follows from the microcanonical picture. The Maxwell-Boltzmann distribution or
the wealth distribution in human society are some direct applications of this
new interpretation.
| nlin.CD cond-mat.stat-mech cs.MA physics.soc-ph | we show that the boltzmann factor has a geometrical origin its derivation follows from the microcanonical picture the maxwellboltzmann distribution or the wealth distribution in human society are some direct applications of this new interpretation | [['we', 'show', 'that', 'the', 'boltzmann', 'factor', 'has', 'a', 'geometrical', 'origin', 'its', 'derivation', 'follows', 'from', 'the', 'microcanonical', 'picture', 'the', 'maxwellboltzmann', 'distribution', 'or', 'the', 'wealth', 'distribution', 'in', 'human', 'society', 'are', 'some', 'direct', 'applications', 'of'... | [-0.07263117608215128, 0.0762375934049487, -0.22385596739394323, 0.09451574835859772, -0.11729364879429341, -0.07881072438987238, 0.032152215294939064, 0.3436230157635042, -0.3128257381363905, -0.2412284220967974, 0.002517804633160787, -0.2924903899431229, -0.150808176085619, 0.17092284695245324, -0.0697982105027352, 0... |
707.4082 | Dewetting of a solid monolayer | We report on the dewetting of a monolayer on a solid substrate, where mass
transport occurs via surface diffusion. For a wide range of parameters, a
labyrinthine pattern of bilayer islands is formed. An irreversible regime and a
thermodynamic regime are identified. In both regimes, the velocity of a
dewetting front, ... | cond-mat.soft cond-mat.stat-mech | we report on the dewetting of a monolayer on a solid substrate where mass transport occurs via surface diffusion for a wide range of parameters a labyrinthine pattern of bilayer islands is formed an irreversible regime and a thermodynamic regime are identified in both regimes the velocity of a dewetting front the wavel... | [['we', 'report', 'on', 'the', 'dewetting', 'of', 'a', 'monolayer', 'on', 'a', 'solid', 'substrate', 'where', 'mass', 'transport', 'occurs', 'via', 'surface', 'diffusion', 'for', 'a', 'wide', 'range', 'of', 'parameters', 'a', 'labyrinthine', 'pattern', 'of', 'bilayer', 'islands', 'is', 'formed', 'an', 'irreversible', '... | [-0.19709762054041896, 0.18424972124419833, -0.10346655865553124, -0.011411167253022906, 0.016656290787946563, -0.08788691758948924, 0.10970457066278691, 0.3449143649817541, -0.26026877101467943, -0.2574379950890253, 0.07645774098921396, -0.2438025378525771, -0.14594240737115516, 0.2303161758276495, 0.03043297833452622... |
707.4083 | Chain of Separable Binary Goppa Codes and their Minimal Distance | It is shown that subclasses of separable binary Goppa codes, $\Gamma(L,G)$ -
codes, with $L=\{\alpha \in GF(2^{2l}):G(\alpha)\neq 0 \}$ and special Goppa
polynomials G(x) can be presented as a chain of embedded codes. The true
minimal distance has been obtained for all codes of the chain.
| cs.IT math.IT | it is shown that subclasses of separable binary goppa codes gammalg codes with lalpha in gf22lgalphaneq 0 and special goppa polynomials gx can be presented as a chain of embedded codes the true minimal distance has been obtained for all codes of the chain | [['it', 'is', 'shown', 'that', 'subclasses', 'of', 'separable', 'binary', 'goppa', 'codes', 'gammalg', 'codes', 'with', 'lalpha', 'in', 'gf22lgalphaneq', '0', 'and', 'special', 'goppa', 'polynomials', 'gx', 'can', 'be', 'presented', 'as', 'a', 'chain', 'of', 'embedded', 'codes', 'the', 'true', 'minimal', 'distance', 'h... | [-0.192213232094045, 0.07048686844341102, -0.043046866942729266, 0.13203888020888416, 0.012780570901841634, -0.31843714224218966, -0.07720488172379278, 0.42128030732939287, -0.3424778932794219, -0.19132111301379545, 0.16503117990491556, -0.269507174563062, -0.09116930678664219, 0.26384385813781547, -0.08626426244154572... |
707.4084 | Local structure of directed networks | Previous work on undirected small-world networks established the paradigm
that locally structured networks tend to have high density of short loops. On
the other hand, many realistic networks are directed. Here we investigate the
local organization of directed networks and find, surprisingly, that real
networks often... | physics.soc-ph cond-mat.dis-nn | previous work on undirected smallworld networks established the paradigm that locally structured networks tend to have high density of short loops on the other hand many realistic networks are directed here we investigate the local organization of directed networks and find surprisingly that real networks often have ve... | [['previous', 'work', 'on', 'undirected', 'smallworld', 'networks', 'established', 'the', 'paradigm', 'that', 'locally', 'structured', 'networks', 'tend', 'to', 'have', 'high', 'density', 'of', 'short', 'loops', 'on', 'the', 'other', 'hand', 'many', 'realistic', 'networks', 'are', 'directed', 'here', 'we', 'investigate... | [-0.1495283788928013, 0.1219933342654258, -0.042357714188730584, 0.12040880211102574, -0.07388002115413142, -0.18507289042336988, 0.03882819540044495, 0.4891990664739, -0.22648480502412777, -0.2838411117175027, 0.11597647222832007, -0.2345382192010141, -0.25250267692203837, 0.1965139040156551, -0.0087187654470377, 0.03... |
707.4085 | 1-join composition for $\alpha$-critical graphs | Given two graphs G and H its 1-{\it join} is the graph obtained by taking the
disjoint union of G and H and adding all the edges between a nonempty subset of
vertices of G and a nonempty subset of vertices of H. In general, composition
operations of graphs has played a fundamental role in some structural results
of g... | math.CO | given two graphs g and h its 1it join is the graph obtained by taking the disjoint union of g and h and adding all the edges between a nonempty subset of vertices of g and a nonempty subset of vertices of h in general composition operations of graphs has played a fundamental role in some structural results of graph the... | [['given', 'two', 'graphs', 'g', 'and', 'h', 'its', '1it', 'join', 'is', 'the', 'graph', 'obtained', 'by', 'taking', 'the', 'disjoint', 'union', 'of', 'g', 'and', 'h', 'and', 'adding', 'all', 'the', 'edges', 'between', 'a', 'nonempty', 'subset', 'of', 'vertices', 'of', 'g', 'and', 'a', 'nonempty', 'subset', 'of', 'vert... | [-0.20152224805964114, 0.11145727601847179, -0.059742094234151895, 0.013472835801888345, -0.11020952872173904, -0.10945122976852364, 0.054344406421837764, 0.38757236285221786, -0.257230336273219, -0.3344570194479338, 0.08999405323668534, -0.2976949185804399, -0.1257577740879686, 0.1286310731888164, -0.09769269644477686... |
707.4086 | The electron electric dipole moment enhancement factors of Rubidium and
Caesium atoms | The enhancement factors of the electric dipole moment (EDM) of the ground
states of two paramagnetic atoms; rubidium (Rb) and caesium (Cs) which are
sensitive to the electron EDM are computed using the relativistic
coupled-cluster theory and our results are compared with the available
calculations and measurements. T... | physics.atom-ph | the enhancement factors of the electric dipole moment edm of the ground states of two paramagnetic atoms rubidium rb and caesium cs which are sensitive to the electron edm are computed using the relativistic coupledcluster theory and our results are compared with the available calculations and measurements the possibil... | [['the', 'enhancement', 'factors', 'of', 'the', 'electric', 'dipole', 'moment', 'edm', 'of', 'the', 'ground', 'states', 'of', 'two', 'paramagnetic', 'atoms', 'rubidium', 'rb', 'and', 'caesium', 'cs', 'which', 'are', 'sensitive', 'to', 'the', 'electron', 'edm', 'are', 'computed', 'using', 'the', 'relativistic', 'coupled... | [-0.04347398036868492, 0.18267663626639702, 0.013830968470715764, 0.01706200060538892, 0.06021117511441681, -0.08042099496433094, 0.08860696915019331, 0.35367641308859216, -0.1757101072901999, -0.30015131163952957, 0.009506533214294198, -0.36937277997607615, -0.019256618374319218, 0.19039728757647326, 0.088220479835603... |
707.4087 | Non-independent continuous time random walks | The usual development of the continuous time random walk (CTRW) assumes that
jumps and time intervals are a two-dimensional set of independent and
identically distributed random variables. In this paper we address the
theoretical setting of non-independent CTRW's where consecutive jumps and/or
time intervals are corr... | physics.data-an | the usual development of the continuous time random walk ctrw assumes that jumps and time intervals are a twodimensional set of independent and identically distributed random variables in this paper we address the theoretical setting of nonindependent ctrws where consecutive jumps andor time intervals are correlated an... | [['the', 'usual', 'development', 'of', 'the', 'continuous', 'time', 'random', 'walk', 'ctrw', 'assumes', 'that', 'jumps', 'and', 'time', 'intervals', 'are', 'a', 'twodimensional', 'set', 'of', 'independent', 'and', 'identically', 'distributed', 'random', 'variables', 'in', 'this', 'paper', 'we', 'address', 'the', 'theo... | [-0.12382097573434883, 0.1551939060982067, -0.07630451101188858, 0.10283175991273376, -0.04653387139593293, -0.16555723312587753, 0.05657812310823214, 0.41196539182517977, -0.28992735189259855, -0.2423592273750015, 0.12463250113147739, -0.2596640731270954, -0.16191646348693417, 0.16801274436114877, -0.0947383783740906,... |
707.4088 | An integrable discretization of the rational su(2) Gaudin model and
related systems | The first part of the present paper is devoted to a systematic construction
of continuous-time finite-dimensional integrable systems arising from the
rational su(2) Gaudin model through certain contraction procedures. In the
second part, we derive an explicit integrable Poisson map discretizing a
particular Hamiltoni... | nlin.SI math-ph math.MP | the first part of the present paper is devoted to a systematic construction of continuoustime finitedimensional integrable systems arising from the rational su2 gaudin model through certain contraction procedures in the second part we derive an explicit integrable poisson map discretizing a particular hamiltonian flow ... | [['the', 'first', 'part', 'of', 'the', 'present', 'paper', 'is', 'devoted', 'to', 'a', 'systematic', 'construction', 'of', 'continuoustime', 'finitedimensional', 'integrable', 'systems', 'arising', 'from', 'the', 'rational', 'su2', 'gaudin', 'model', 'through', 'certain', 'contraction', 'procedures', 'in', 'the', 'seco... | [-0.11383047462063464, 0.02597882211813231, -0.07484415603323362, 0.05001070689743485, -0.10760512515097051, -0.10866133092172645, -0.02630415211456853, 0.29487102386868885, -0.3359362316361905, -0.16333229101036448, 0.1406269276143379, -0.19756863005711017, -0.2120653015334864, 0.1749929432549539, -0.07852352637092809... |
707.4089 | Neutrino production states in oscillation phenomena - are they pure or
mixed? | General quantum mechanical states of neutrinos produced by mechanisms outside
the Standard Model are discussed. The neutrino state is described by the
Maki-Nakagawa-Sakata-Pontecorvo unitary mixing matrix only in the case of
relativistic neutrinos and Standard Model left-handed charge current
interaction. The problem... | hep-ph | general quantum mechanical states of neutrinos produced by mechanisms outside the standard model are discussed the neutrino state is described by the makinakagawasakatapontecorvo unitary mixing matrix only in the case of relativistic neutrinos and standard model lefthanded charge current interaction the problem of wign... | [['general', 'quantum', 'mechanical', 'states', 'of', 'neutrinos', 'produced', 'by', 'mechanisms', 'outside', 'the', 'standard', 'model', 'are', 'discussed', 'the', 'neutrino', 'state', 'is', 'described', 'by', 'the', 'makinakagawasakatapontecorvo', 'unitary', 'mixing', 'matrix', 'only', 'in', 'the', 'case', 'of', 'rel... | [-0.09695851790186549, 0.28942775538279897, 0.0036873844565456066, 0.11801373233264756, 0.011885045101821777, -0.12497365300854048, 0.012782202137722855, 0.3290433322035131, -0.27571173933822485, -0.2828592574179527, 0.027929645744595853, -0.2719574912584254, -0.048509165449511435, 0.14252075672016612, 0.05221985226630... |
707.409 | On some properties of $\sigma(N)$ | We show asymptotic upper and lower bounds for the greatest common divisor of
N and $\sigma(N)$. We also show that there are infinitely many integers N with
fairly large g.c.d. of N and $\sigma(N)$.
| math.NT | we show asymptotic upper and lower bounds for the greatest common divisor of n and sigman we also show that there are infinitely many integers n with fairly large gcd of n and sigman | [['we', 'show', 'asymptotic', 'upper', 'and', 'lower', 'bounds', 'for', 'the', 'greatest', 'common', 'divisor', 'of', 'n', 'and', 'sigman', 'we', 'also', 'show', 'that', 'there', 'are', 'infinitely', 'many', 'integers', 'n', 'with', 'fairly', 'large', 'gcd', 'of', 'n', 'and', 'sigman']] | [-0.24527711136376157, 0.16057733550448627, -0.06292879881392069, 0.10029671297353857, 0.026900515891611576, -0.2175262556411326, 0.03841922651318943, 0.3222154484349577, -0.21251071354045586, -0.28482170450939415, 0.05093571403995156, -0.34993306415922504, -0.19202074180494116, 0.2410975061083103, -0.00307425275883253... |
707.4091 | Kinetic Energy Density Study of Some Representative Semilocal Kinetic
Energy Functionals | There is a number of explicit kinetic energy density functionals for
non-interacting electron systems that are obtained in terms of the electron
density and its derivatives. These semilocal functionals have been widely used
in the literature. In this work we present a comparative study of the kinetic
energy density o... | cond-mat.other cond-mat.stat-mech | there is a number of explicit kinetic energy density functionals for noninteracting electron systems that are obtained in terms of the electron density and its derivatives these semilocal functionals have been widely used in the literature in this work we present a comparative study of the kinetic energy density of the... | [['there', 'is', 'a', 'number', 'of', 'explicit', 'kinetic', 'energy', 'density', 'functionals', 'for', 'noninteracting', 'electron', 'systems', 'that', 'are', 'obtained', 'in', 'terms', 'of', 'the', 'electron', 'density', 'and', 'its', 'derivatives', 'these', 'semilocal', 'functionals', 'have', 'been', 'widely', 'used... | [-0.10316133480291287, 0.07698792527037807, -0.09985669733166856, 0.1435477664164627, 0.023225643259533885, -0.017827084189301113, 0.021043088657872588, 0.3541339743356018, -0.2301159738487078, -0.3523457246508611, 0.021304737806887082, -0.30322909969380935, -0.07487782048005813, 0.14979833152787964, -0.004848311858950... |
707.4092 | Protection of entanglement from sudden death using continuous dynamical
decoupling | We show that continuous dynamical decoupling can protect a two-qubit
entangled state from sudden death at finite temperature due to uncorrelated
dephasing, bit flipping, and dissipation. We consider a situation where an
entangled state shared between two non-interacting qubits is initially prepared
and left evolve un... | quant-ph | we show that continuous dynamical decoupling can protect a twoqubit entangled state from sudden death at finite temperature due to uncorrelated dephasing bit flipping and dissipation we consider a situation where an entangled state shared between two noninteracting qubits is initially prepared and left evolve under the... | [['we', 'show', 'that', 'continuous', 'dynamical', 'decoupling', 'can', 'protect', 'a', 'twoqubit', 'entangled', 'state', 'from', 'sudden', 'death', 'at', 'finite', 'temperature', 'due', 'to', 'uncorrelated', 'dephasing', 'bit', 'flipping', 'and', 'dissipation', 'we', 'consider', 'a', 'situation', 'where', 'an', 'entan... | [-0.1938510307246882, 0.27315675298401465, -0.05167770786001609, 0.05789619833466419, 0.05776729280511022, -0.2471762321735052, 0.07202371368393971, 0.3346022508640805, -0.28979376050528516, -0.2365292359687639, 0.05020747047958875, -0.277258571284415, -0.029452866236313005, 0.13302497979086103, -0.04647834444146478, 0... |
707.4093 | Twisted mass lattice QCD | I review the theoretical foundations, properties as well as the simulation
results obtained so far of a variant of the Wilson lattice QCD formulation:
Wilson twisted mass lattice QCD. Emphasis is put on the discretization errors
and on the effects of these discretization errors on the phase structure for
Wilson-like ... | hep-lat | i review the theoretical foundations properties as well as the simulation results obtained so far of a variant of the wilson lattice qcd formulation wilson twisted mass lattice qcd emphasis is put on the discretization errors and on the effects of these discretization errors on the phase structure for wilsonlike fermio... | [['i', 'review', 'the', 'theoretical', 'foundations', 'properties', 'as', 'well', 'as', 'the', 'simulation', 'results', 'obtained', 'so', 'far', 'of', 'a', 'variant', 'of', 'the', 'wilson', 'lattice', 'qcd', 'formulation', 'wilson', 'twisted', 'mass', 'lattice', 'qcd', 'emphasis', 'is', 'put', 'on', 'the', 'discretizat... | [-0.09550224746162274, 0.22333706544532653, -0.08765913361784475, 0.1044203594848738, -0.07064933911336205, -0.07278355101617165, 0.11412349700680878, 0.391717642366168, -0.2140492802059435, -0.21918571228722492, 0.11455518300420638, -0.2926018057076866, -0.09936194811352944, 0.12080198309821896, -0.013131549329418376,... |
707.4094 | Bounds for the Superfluid Fraction from Exact Quantum Monte Carlo Local
Densities | For solid 4He and solid p-H2, using the flow-energy-minimizing one-body phase
function and exact T=0 K Monte Carlo calculations of the local density, we have
calculated the phase function, the velocity profile and upper bounds for the
superfluid fraction f_s. At the melting pressure for solid 4He we find that f_s
< 0... | cond-mat.other | for solid 4he and solid ph2 using the flowenergyminimizing onebody phase function and exact t0 k monte carlo calculations of the local density we have calculated the phase function the velocity profile and upper bounds for the superfluid fraction f_s at the melting pressure for solid 4he we find that f_s 020021 about t... | [['for', 'solid', '4he', 'and', 'solid', 'ph2', 'using', 'the', 'flowenergyminimizing', 'onebody', 'phase', 'function', 'and', 'exact', 't0', 'k', 'monte', 'carlo', 'calculations', 'of', 'the', 'local', 'density', 'we', 'have', 'calculated', 'the', 'phase', 'function', 'the', 'velocity', 'profile', 'and', 'upper', 'bou... | [-0.0850314316178103, 0.24059991327036792, -0.12841204427079195, 0.04333919189715137, 0.05704586365674105, -0.056994566001877606, 0.12594085819728207, 0.33017476761920583, -0.19780994386463943, -0.3046411185318397, 0.0497004241656719, -0.33088731015514994, -0.06722442040012942, 0.18393565182405938, 0.11267866543494165,... |
707.4095 | High-pressure study of X-ray diffuse scattering in ferroelectric
perovskites | We present a high-pressure x-ray diffuse scattering study of the ABO$_3$
ferroelectric perovskites BaTiO_3 and KNbO_3. The well-known diffuse lines are
observed in all the phases studied. In KNbO_3, we show that the lines are
present up to 21.8 GPa, with constant width and a slightly decreasing
intensity. At variance... | cond-mat.mtrl-sci | we present a highpressure xray diffuse scattering study of the abo_3 ferroelectric perovskites batio_3 and knbo_3 the wellknown diffuse lines are observed in all the phases studied in knbo_3 we show that the lines are present up to 218 gpa with constant width and a slightly decreasing intensity at variance the intensit... | [['we', 'present', 'a', 'highpressure', 'xray', 'diffuse', 'scattering', 'study', 'of', 'the', 'abo_3', 'ferroelectric', 'perovskites', 'batio_3', 'and', 'knbo_3', 'the', 'wellknown', 'diffuse', 'lines', 'are', 'observed', 'in', 'all', 'the', 'phases', 'studied', 'in', 'knbo_3', 'we', 'show', 'that', 'the', 'lines', 'a... | [-0.10955784688220296, 0.19199427256313295, 0.027595700640862777, -0.00302216450494351, -0.015075834617965807, -0.09923964544688746, 0.0915773387138053, 0.4800467183339899, -0.2587919645958533, -0.25408762881494823, 0.037336631781634703, -0.366818963644742, -0.09312888681572878, 0.1502061580954972, 0.044294675634542514... |
707.4096 | Concavity for nuclear binding energies, thermodynamical functions and
density functionals | Sequences of experimental ground-state energies for both odd and even $A$ are
mapped onto concave patterns cured from convexities due to pairing and/or shell
effects. The same patterns, completed by a list of excitation energies, give
numerical estimates of the grand potential $\Omega(\beta,\mu)$ for a mixture of
nuc... | nucl-th | sequences of experimental groundstate energies for both odd and even a are mapped onto concave patterns cured from convexities due to pairing andor shell effects the same patterns completed by a list of excitation energies give numerical estimates of the grand potential omegabetamu for a mixture of nuclei at low or mod... | [['sequences', 'of', 'experimental', 'groundstate', 'energies', 'for', 'both', 'odd', 'and', 'even', 'a', 'are', 'mapped', 'onto', 'concave', 'patterns', 'cured', 'from', 'convexities', 'due', 'to', 'pairing', 'andor', 'shell', 'effects', 'the', 'same', 'patterns', 'completed', 'by', 'a', 'list', 'of', 'excitation', 'e... | [-0.08301395461837083, 0.1678089200179301, -0.06938831360628368, 0.1506372856839997, 0.005687845287338635, -0.12174621873742177, 0.10482502163367714, 0.36830603709030485, -0.22502764563340646, -0.3199064340959821, 0.05664157408597178, -0.27924863524013843, -0.04235928517731803, 0.15839991994334363, 0.03444490957337374,... |
707.4097 | Gravitational moduli forces in small nuclei and analytical computation
of the Newton constant | The magnitude of gravity at subatomic distances was investigated in the
nuclear size range by examining the vibrational kinetic energy of baryons and
quarks, treated as waveparticles and strings, in the 4He and 2H nuclei. Due to
the relativistic increase in mass and concomitant wave particle confinement at
high vibra... | hep-ph | the magnitude of gravity at subatomic distances was investigated in the nuclear size range by examining the vibrational kinetic energy of baryons and quarks treated as waveparticles and strings in the 4he and 2h nuclei due to the relativistic increase in mass and concomitant wave particle confinement at high vibrationa... | [['the', 'magnitude', 'of', 'gravity', 'at', 'subatomic', 'distances', 'was', 'investigated', 'in', 'the', 'nuclear', 'size', 'range', 'by', 'examining', 'the', 'vibrational', 'kinetic', 'energy', 'of', 'baryons', 'and', 'quarks', 'treated', 'as', 'waveparticles', 'and', 'strings', 'in', 'the', '4he', 'and', '2h', 'nuc... | [-0.06618278837503538, 0.2719854285614085, -0.04870587824027717, 0.12516842070083642, 0.03974267414089331, -0.07479454053700277, 0.020627797851290975, 0.36092358568836885, -0.19551000593364545, -0.3452455012887457, -0.0756199125154904, -0.32455255316820036, 0.010211411987181715, 0.14010066951303407, 0.07551968919554937... |
707.4098 | Rank-based inference for bivariate extreme-value copulas | Consider a continuous random pair $(X,Y)$ whose dependence is characterized
by an extreme-value copula with Pickands dependence function $A$. When the
marginal distributions of $X$ and $Y$ are known, several consistent estimators
of $A$ are available. Most of them are variants of the estimators due to
Pickands [Bull.... | math.ST stat.TH | consider a continuous random pair xy whose dependence is characterized by an extremevalue copula with pickands dependence function a when the marginal distributions of x and y are known several consistent estimators of a are available most of them are variants of the estimators due to pickands bull inst internat statis... | [['consider', 'a', 'continuous', 'random', 'pair', 'xy', 'whose', 'dependence', 'is', 'characterized', 'by', 'an', 'extremevalue', 'copula', 'with', 'pickands', 'dependence', 'function', 'a', 'when', 'the', 'marginal', 'distributions', 'of', 'x', 'and', 'y', 'are', 'known', 'several', 'consistent', 'estimators', 'of', ... | [-0.03623888368113382, 0.04220416811388402, -0.08536940291690241, 0.12977102821875763, -0.03414171318540216, -0.13553859733843376, 0.06292290533560195, 0.4089849057474307, -0.19557937484517293, -0.2831373108484383, 0.14836037864692375, -0.29897808647448465, -0.1304159248646881, 0.21296788904416775, -0.13663218302068084... |
707.4099 | Microscopic studies of solid 4He with Path Integral Projector Monte
Carlo | We have investigated the ground state properties of solid $^4$He with the
Shadow Path Integral Ground State method. This exact T=0 K projector method
allows to describes quantum solids without introducing any a priori equilibrium
position. We have found that the efficiency in computing off-diagonal
properties in the ... | cond-mat.other | we have investigated the ground state properties of solid 4he with the shadow path integral ground state method this exact t0 k projector method allows to describes quantum solids without introducing any a priori equilibrium position we have found that the efficiency in computing offdiagonal properties in the solid pha... | [['we', 'have', 'investigated', 'the', 'ground', 'state', 'properties', 'of', 'solid', '4he', 'with', 'the', 'shadow', 'path', 'integral', 'ground', 'state', 'method', 'this', 'exact', 't0', 'k', 'projector', 'method', 'allows', 'to', 'describes', 'quantum', 'solids', 'without', 'introducing', 'any', 'a', 'priori', 'eq... | [-0.11500849939514396, 0.21610394259053226, -0.10268954179986421, 0.0014545300793579192, 0.005512158385250921, -0.09666134543550103, 0.08658207450826555, 0.38449453136684436, -0.21987627719098063, -0.2843013558703572, 0.039764348163260195, -0.2756510333063814, -0.08044061977277274, 0.1283974076565633, 0.019503578112752... |
707.41 | Collinear improvement of the BFKL kernel in the electroproduction of two
light vector mesons | The use of the BFKL kernel improved by the inclusion of subleading terms
generated by renormalization group (RG) analysis has been suggested to cure the
instabilities in the behavior of the BFKL Green's function in the
next-to-leading approximation (NLA). We test the performance of a RG-improved
kernel in the determi... | hep-ph | the use of the bfkl kernel improved by the inclusion of subleading terms generated by renormalization group rg analysis has been suggested to cure the instabilities in the behavior of the bfkl greens function in the nexttoleading approximation nla we test the performance of a rgimproved kernel in the determination of t... | [['the', 'use', 'of', 'the', 'bfkl', 'kernel', 'improved', 'by', 'the', 'inclusion', 'of', 'subleading', 'terms', 'generated', 'by', 'renormalization', 'group', 'rg', 'analysis', 'has', 'been', 'suggested', 'to', 'cure', 'the', 'instabilities', 'in', 'the', 'behavior', 'of', 'the', 'bfkl', 'greens', 'function', 'in', '... | [-0.10676853385974922, 0.07950934940175611, -0.18219950023280868, 0.09959071301732442, -0.044709260717539466, -0.026517146231480323, 0.012446707278348, 0.3319079191345027, -0.20322835652189233, -0.23331280279967745, 0.030998172713009545, -0.2952232711901099, -0.0840102625414887, 0.1563231532414586, 0.04199464385539799,... |
707.4101 | On the ternary Goldbach problem with primes in arithmetic progressions
of a common module | For A,epsilon>0 and any sufficiently large odd n we show that for almost all
k up to n^{1/5-epsilon} there exists a representation n=p1+p2+p3 with primes in
residue classes b1,b2,b3 mod k for almost all admissible triplets b1,b2,b3 of
reduced residues mod k.
| math.NT | for aepsilon0 and any sufficiently large odd n we show that for almost all k up to n15epsilon there exists a representation np1p2p3 with primes in residue classes b1b2b3 mod k for almost all admissible triplets b1b2b3 of reduced residues mod k | [['for', 'aepsilon0', 'and', 'any', 'sufficiently', 'large', 'odd', 'n', 'we', 'show', 'that', 'for', 'almost', 'all', 'k', 'up', 'to', 'n15epsilon', 'there', 'exists', 'a', 'representation', 'np1p2p3', 'with', 'primes', 'in', 'residue', 'classes', 'b1b2b3', 'mod', 'k', 'for', 'almost', 'all', 'admissible', 'triplets',... | [-0.27502505496345664, 0.19221152025400787, -0.047290723846369495, 0.012824852170573699, 0.06086946714266732, -0.20478351543833678, 0.05402736922523881, 0.34545736480504274, -0.27082193134402904, -0.2848142905513177, -0.049292224663863515, -0.3047511398389533, -0.10616816368230896, 0.1710742735178084, 0.035348283202462... |
707.4102 | A deterministic version of Pollard's p-1 algorithm | In this article we present applications of smooth numbers to the
unconditional derandomization of some well-known integer factoring algorithms.
We begin with Pollard's $p-1$ algorithm, which finds in random polynomial
time the prime divisors $p$ of an integer $n$ such that $p-1$ is smooth. We
show that these prime ... | math.NT | in this article we present applications of smooth numbers to the unconditional derandomization of some wellknown integer factoring algorithms we begin with pollards p1 algorithm which finds in random polynomial time the prime divisors p of an integer n such that p1 is smooth we show that these prime factors can be reco... | [['in', 'this', 'article', 'we', 'present', 'applications', 'of', 'smooth', 'numbers', 'to', 'the', 'unconditional', 'derandomization', 'of', 'some', 'wellknown', 'integer', 'factoring', 'algorithms', 'we', 'begin', 'with', 'pollards', 'p1', 'algorithm', 'which', 'finds', 'in', 'random', 'polynomial', 'time', 'the', 'p... | [-0.21855460811148297, 0.10060719599611061, -0.07921039859388383, 0.07191041590160611, -0.046452596891637755, -0.20440884765955697, 0.03164126514457166, 0.3300390119428735, -0.3209994865268615, -0.27078052581826517, 0.05740539715428983, -0.2477264104843005, -0.14809800070676818, 0.20795477877359791, -0.0819160989752174... |
707.4103 | EDGE: Explorer of Diffuse emission and Gamma-ray burst Explosions | How structures on various scales formed and evolved from the early Universe
up to present time is a fundamental question of astrophysical cosmology. EDGE
will trace the cosmic history of the baryons from the early generations of
massive star by Gamma-Ray Burst (GRB) explosions, through the period of cluster
formation... | astro-ph | how structures on various scales formed and evolved from the early universe up to present time is a fundamental question of astrophysical cosmology edge will trace the cosmic history of the baryons from the early generations of massive star by gammaray burst grb explosions through the period of cluster formation down t... | [['how', 'structures', 'on', 'various', 'scales', 'formed', 'and', 'evolved', 'from', 'the', 'early', 'universe', 'up', 'to', 'present', 'time', 'is', 'a', 'fundamental', 'question', 'of', 'astrophysical', 'cosmology', 'edge', 'will', 'trace', 'the', 'cosmic', 'history', 'of', 'the', 'baryons', 'from', 'the', 'early', ... | [-0.08446539344614128, 0.16449348021867788, -0.0812139343389491, 0.09627716698345136, -0.1217902714875762, -0.0629743017159835, 0.028334665934160126, 0.38765230176575255, -0.21158882471111914, -0.38359524564572955, 0.08487293601031368, -0.2758093301601934, -0.009482665885841906, 0.19521668760077746, 0.02745768830010836... |
707.4104 | Queues, stores, and tableaux | Consider the single server queue with an infinite buffer and a FIFO
discipline, either of type M/M/1 or Geom/Geom/1. Denote by A the arrival
process and by s the services. Assume the stability condition to be satisfied.
Denote by D the departure process in equilibrium and by r the time spent by the
customers at the v... | cs.DM math.CO | consider the single server queue with an infinite buffer and a fifo discipline either of type mm1 or geomgeom1 denote by a the arrival process and by s the services assume the stability condition to be satisfied denote by d the departure process in equilibrium and by r the time spent by the customers at the very back o... | [['consider', 'the', 'single', 'server', 'queue', 'with', 'an', 'infinite', 'buffer', 'and', 'a', 'fifo', 'discipline', 'either', 'of', 'type', 'mm1', 'or', 'geomgeom1', 'denote', 'by', 'a', 'the', 'arrival', 'process', 'and', 'by', 's', 'the', 'services', 'assume', 'the', 'stability', 'condition', 'to', 'be', 'satisfi... | [-0.13583225527034865, 0.12084668977687874, -0.11480690879297667, 0.021169268938131702, -0.013252979574789261, -0.1668626575056335, 0.11216831025506915, 0.30619346500727634, -0.3514631471596658, -0.289848696442064, 0.14002821738911986, -0.27300632846509587, -0.06185520982594583, 0.1325415616501765, -0.07520478661172092... |
707.4105 | Semiclassical theory of charged pion radiation by nucleons in a strong
homogeneous magnetic field | Charged pions produced in very high energy hadronic interactions might be the
dominant source of cosmic neutrinos in the GeV--TeV range. Spectral energy
power of \pi^+ radiation by high energy protons moving in strong magnetic
fields typical for magnetars is determined with a semiclassical treatment of
the effective ... | astro-ph | charged pions produced in very high energy hadronic interactions might be the dominant source of cosmic neutrinos in the gevtev range spectral energy power of pi radiation by high energy protons moving in strong magnetic fields typical for magnetars is determined with a semiclassical treatment of the effective pionnucl... | [['charged', 'pions', 'produced', 'in', 'very', 'high', 'energy', 'hadronic', 'interactions', 'might', 'be', 'the', 'dominant', 'source', 'of', 'cosmic', 'neutrinos', 'in', 'the', 'gevtev', 'range', 'spectral', 'energy', 'power', 'of', 'pi', 'radiation', 'by', 'high', 'energy', 'protons', 'moving', 'in', 'strong', 'mag... | [-0.11495358704699464, 0.23973188342486498, -0.06554605070594198, 0.1628049668337729, -0.023627659426100792, -0.07371831768422678, 0.03057120184718271, 0.3456046483229085, -0.2279663277910121, -0.3287177663096177, -0.08492841762090002, -0.3061433168108104, 0.05531870367466121, 0.18194525169899628, 0.04047189824882724, ... |
707.4106 | Parton Distributions: Progress and Challenges | We briefly discuss recent research on the spin-averaged parton densities of
the proton, focusing on some aspects relevant to hard processes at the LHC.
Specifically, after recalling the basic framework and the need for higher-order
calculations, we address the evolution equations governing the scale dependence
of the... | hep-ph | we briefly discuss recent research on the spinaveraged parton densities of the proton focusing on some aspects relevant to hard processes at the lhc specifically after recalling the basic framework and the need for higherorder calculations we address the evolution equations governing the scale dependence of the parton ... | [['we', 'briefly', 'discuss', 'recent', 'research', 'on', 'the', 'spinaveraged', 'parton', 'densities', 'of', 'the', 'proton', 'focusing', 'on', 'some', 'aspects', 'relevant', 'to', 'hard', 'processes', 'at', 'the', 'lhc', 'specifically', 'after', 'recalling', 'the', 'basic', 'framework', 'and', 'the', 'need', 'for', '... | [-0.035766648973027865, 0.17290092992285888, -0.12325879922757546, 0.13405813357482355, -0.07663594922361275, -0.06105603815910096, 0.012368217334151268, 0.3674179567893346, -0.23176404982805252, -0.2718407370708883, 0.10656640664984783, -0.32193659771233796, -0.03191480992982785, 0.17142846185403565, 0.049073002673685... |
707.4107 | Post Common Envelope Binaries from SDSS. I: 101 white dwarf main
sequence binaries with multiple SDSS spectroscopy | We present a detailed analysis of 101 white dwarf-main sequence binaries
(WDMS) from the Sloan Digital Sky Survey (SDSS) for which multiple SDSS spectra
are available. We detect significant radial velocity variations in 18 WDMS,
identifying them as post common envelope binaries (PCEBs) or strong PCEB
candidates. Stri... | astro-ph | we present a detailed analysis of 101 white dwarfmain sequence binaries wdms from the sloan digital sky survey sdss for which multiple sdss spectra are available we detect significant radial velocity variations in 18 wdms identifying them as post common envelope binaries pcebs or strong pceb candidates strict upper lim... | [['we', 'present', 'a', 'detailed', 'analysis', 'of', '101', 'white', 'dwarfmain', 'sequence', 'binaries', 'wdms', 'from', 'the', 'sloan', 'digital', 'sky', 'survey', 'sdss', 'for', 'which', 'multiple', 'sdss', 'spectra', 'are', 'available', 'we', 'detect', 'significant', 'radial', 'velocity', 'variations', 'in', '18',... | [-0.07991265505121556, 0.09665933459065855, -0.06248586171492934, 0.12494543655961753, -0.09148494188021869, -0.0663661426641047, 0.12523225335031749, 0.38557881373725833, -0.1771544552911073, -0.3806144372075796, 0.07926678181206807, -0.335382916238741, -0.04677205860288814, 0.23104369607660918, -0.08416129383910448, ... |
707.4108 | What hydrodynamical simulations tell us about the radial properties of
the stellar populations in Ellipticals | Elliptical galaxies probably host the most metal rich stellar populations in
the Universe. The processes leading to both the formation and the evolution of
such stars are discussed by means of a new gas dynamical model which implements
detailed chemical evolution prescriptions. Moreover, the radial variations in
the ... | astro-ph | elliptical galaxies probably host the most metal rich stellar populations in the universe the processes leading to both the formation and the evolution of such stars are discussed by means of a new gas dynamical model which implements detailed chemical evolution prescriptions moreover the radial variations in the metal... | [['elliptical', 'galaxies', 'probably', 'host', 'the', 'most', 'metal', 'rich', 'stellar', 'populations', 'in', 'the', 'universe', 'the', 'processes', 'leading', 'to', 'both', 'the', 'formation', 'and', 'the', 'evolution', 'of', 'such', 'stars', 'are', 'discussed', 'by', 'means', 'of', 'a', 'new', 'gas', 'dynamical', '... | [-0.0531949060913149, 0.12885646959556277, -0.09494206548989409, 0.1322706438065638, -0.06795229397366866, -0.02781448668029454, 0.02602745502618915, 0.4113734411970202, -0.17958991225324783, -0.3413379768825183, 0.04365659528411925, -0.24983899876222773, -0.0423117603141141, 0.16696196225850637, -0.008441792124892863,... |
707.4109 | Direct observation of mixing of spin-multiplets in an antiferromagnetic
molecular nanomagnet by electron paramagnetic resonance | High-frequency electron paramagnetic resonance (EPR) studies of the
antiferromagnetic Mn-$[3\times 3]$ molecular grid clearly reveal a breaking of
the $\Delta S = 0$ selection rule, providing direct evidence for the mixing of
spin wavefunctions ($S$-mixing) induced by the comparable exchange and
magneto-anisotropy en... | cond-mat.other | highfrequency electron paramagnetic resonance epr studies of the antiferromagnetic mn3times 3 molecular grid clearly reveal a breaking of the delta s 0 selection rule providing direct evidence for the mixing of spin wavefunctions smixing induced by the comparable exchange and magnetoanisotropy energy scales within the ... | [['highfrequency', 'electron', 'paramagnetic', 'resonance', 'epr', 'studies', 'of', 'the', 'antiferromagnetic', 'mn3times', '3', 'molecular', 'grid', 'clearly', 'reveal', 'a', 'breaking', 'of', 'the', 'delta', 's', '0', 'selection', 'rule', 'providing', 'direct', 'evidence', 'for', 'the', 'mixing', 'of', 'spin', 'wavef... | [-0.18266456405847117, 0.16343413048889488, -0.0171598063972898, 0.10151595949458006, -0.05117778016779667, -0.11601157570018983, 0.11245052235869643, 0.3672228031672346, -0.24124587500372377, -0.32267938752491504, 0.008104196664554855, -0.29026431788523227, -0.013330734146830555, 0.15115535068952551, 0.134508798527232... |
707.411 | Functional renormalization group in the broken symmetry phase: momentum
dependence and two-parameter scaling of the self-energy | We include spontaneous symmetry breaking into the functional renormalization
group (RG) equations for the irreducible vertices of Ginzburg-Landau theories
by augmenting these equations by a flow equation for the order parameter, which
is determined from the requirement that at each RG step the vertex with one
externa... | cond-mat.stat-mech hep-th | we include spontaneous symmetry breaking into the functional renormalization group rg equations for the irreducible vertices of ginzburglandau theories by augmenting these equations by a flow equation for the order parameter which is determined from the requirement that at each rg step the vertex with one external leg ... | [['we', 'include', 'spontaneous', 'symmetry', 'breaking', 'into', 'the', 'functional', 'renormalization', 'group', 'rg', 'equations', 'for', 'the', 'irreducible', 'vertices', 'of', 'ginzburglandau', 'theories', 'by', 'augmenting', 'these', 'equations', 'by', 'a', 'flow', 'equation', 'for', 'the', 'order', 'parameter', ... | [-0.2074298248487702, 0.19430406873358325, -0.09662184910363673, 0.01592002279565869, -0.06079930132753881, -0.15887072806418429, 0.06358577819940235, 0.2876750016418685, -0.2610297595993394, -0.2534564733061762, 0.01212212667520535, -0.31854660514398436, -0.09844782312644557, 0.07073317592342694, 0.07469801019206421, ... |
707.4111 | Dependence of spin dephasing on initial spin polarization in a
high-mobility two-dimensional electron system | We have studied the spin dynamics of a high-mobility two-dimensional electron
system in a GaAs/Al_{0.3}Ga_{0.7}As single quantum well by time-resolved
Faraday rotation and time-resolved Kerr rotation in dependence on the initial
degree of spin polarization, P, of the electrons. By increasing the initial
spin polariza... | cond-mat.mtrl-sci cond-mat.other | we have studied the spin dynamics of a highmobility twodimensional electron system in a gaasal_03ga_07as single quantum well by timeresolved faraday rotation and timeresolved kerr rotation in dependence on the initial degree of spin polarization p of the electrons by increasing the initial spin polarization from the lo... | [['we', 'have', 'studied', 'the', 'spin', 'dynamics', 'of', 'a', 'highmobility', 'twodimensional', 'electron', 'system', 'in', 'a', 'gaasal_03ga_07as', 'single', 'quantum', 'well', 'by', 'timeresolved', 'faraday', 'rotation', 'and', 'timeresolved', 'kerr', 'rotation', 'in', 'dependence', 'on', 'the', 'initial', 'degree... | [-0.12295914542704375, 0.2116368818223355, -0.01526770661028264, -0.004502195304983457, 0.005237101300103266, -0.1328613220349602, 0.03019545814237537, 0.368333445663903, -0.2426000620977467, -0.3270597213818489, 0.0014681483691041965, -0.32455478409183736, -0.06026559501732782, 0.21821137593613696, 0.06520738362640892... |
707.4112 | Modeling of Transitional Channel Flow Using Balanced Proper Orthogonal
Decomposition | We study reduced-order models of three-dimensional perturbations in
linearized channel flow using balanced proper orthogonal decomposition (BPOD).
The models are obtained from three-dimensional simulations in physical space as
opposed to the traditional single-wavenumber approach, and are therefore better
able to cap... | math.OC math.DS | we study reducedorder models of threedimensional perturbations in linearized channel flow using balanced proper orthogonal decomposition bpod the models are obtained from threedimensional simulations in physical space as opposed to the traditional singlewavenumber approach and are therefore better able to capture the e... | [['we', 'study', 'reducedorder', 'models', 'of', 'threedimensional', 'perturbations', 'in', 'linearized', 'channel', 'flow', 'using', 'balanced', 'proper', 'orthogonal', 'decomposition', 'bpod', 'the', 'models', 'are', 'obtained', 'from', 'threedimensional', 'simulations', 'in', 'physical', 'space', 'as', 'opposed', 't... | [-0.09031681906431914, 0.08090557186243434, -0.08922697660409742, 0.07810368512136241, -0.05641741506858832, -0.11818975022890502, -0.01706853546616104, 0.3596247629924781, -0.2494950685179275, -0.268696870046616, 0.120899726785202, -0.23695545439918836, -0.156108365525498, 0.20341733288226857, -0.05638476738499271, 0.... |
707.4113 | Mean-field description of ultracold Bosons on disordered two-dimensional
optical lattices | In the present paper we describe the properties induced by disorder on an
ultracold gas of Bosonic atoms loaded into a two-dimensional optical lattice
with global confinement ensured by a parabolic potential. Our analysis is
centered on the spatial distribution of the various phases, focusing
particularly on the supe... | cond-mat.dis-nn cond-mat.mes-hall | in the present paper we describe the properties induced by disorder on an ultracold gas of bosonic atoms loaded into a twodimensional optical lattice with global confinement ensured by a parabolic potential our analysis is centered on the spatial distribution of the various phases focusing particularly on the superflui... | [['in', 'the', 'present', 'paper', 'we', 'describe', 'the', 'properties', 'induced', 'by', 'disorder', 'on', 'an', 'ultracold', 'gas', 'of', 'bosonic', 'atoms', 'loaded', 'into', 'a', 'twodimensional', 'optical', 'lattice', 'with', 'global', 'confinement', 'ensured', 'by', 'a', 'parabolic', 'potential', 'our', 'analysi... | [-0.16316664975229053, 0.21167502813328518, -0.06522929352015638, 0.011883951475819906, 0.03325368581005396, -0.1217204896458544, 0.04610289732227102, 0.3823777858693248, -0.2531099913116449, -0.2192113313358277, 0.0850533312992551, -0.2807434971193568, -0.1429951285274747, 0.14052478874770877, 0.007422636430232952, 0.... |
707.4114 | Evidence for out-of-equilibrium crystal nucleation in suspensions of
oppositely charged colloids | We report a numerical study of the rate of crystal nucleation in a binary
suspension of oppositely charged colloids. Two different crystal structures
compete in the thermodynamic conditions under study. We find that the crystal
phase that nucleates is metastable and, more surprisingly, its nucleation free
energy barr... | cond-mat.soft cond-mat.mtrl-sci | we report a numerical study of the rate of crystal nucleation in a binary suspension of oppositely charged colloids two different crystal structures compete in the thermodynamic conditions under study we find that the crystal phase that nucleates is metastable and more surprisingly its nucleation free energy barrier is... | [['we', 'report', 'a', 'numerical', 'study', 'of', 'the', 'rate', 'of', 'crystal', 'nucleation', 'in', 'a', 'binary', 'suspension', 'of', 'oppositely', 'charged', 'colloids', 'two', 'different', 'crystal', 'structures', 'compete', 'in', 'the', 'thermodynamic', 'conditions', 'under', 'study', 'we', 'find', 'that', 'the'... | [-0.11736367758813752, 0.24115269617208815, -0.10189636989134895, 0.04334220446045857, -0.06264061686459713, -0.11885362762326668, 0.05837946741125923, 0.410557073964314, -0.2663220511181742, -0.23697412007850063, 0.05716908545414186, -0.2524854364412383, -0.13637154473161156, 0.15115292111704173, 0.02698864393736705, ... |
707.4115 | Dynamics of the attractive 1D Bose gas: analytical treatment from
integrability | The physics of the attractive one-dimensional Bose gas (Lieb-Liniger model)
is investigated with techniques based on the integrability of the system.
Combining a knowledge of particle quasi-momenta to exponential precision in the
system size with determinant representations of matrix elements of local
operators comin... | cond-mat.str-el cond-mat.stat-mech hep-th quant-ph | the physics of the attractive onedimensional bose gas liebliniger model is investigated with techniques based on the integrability of the system combining a knowledge of particle quasimomenta to exponential precision in the system size with determinant representations of matrix elements of local operators coming from t... | [['the', 'physics', 'of', 'the', 'attractive', 'onedimensional', 'bose', 'gas', 'liebliniger', 'model', 'is', 'investigated', 'with', 'techniques', 'based', 'on', 'the', 'integrability', 'of', 'the', 'system', 'combining', 'a', 'knowledge', 'of', 'particle', 'quasimomenta', 'to', 'exponential', 'precision', 'in', 'the'... | [-0.10767631196341175, 0.10130576288933496, -0.0942530295059803, 0.06880648003425449, -0.007872488579701587, -0.15148026553538055, 0.04203538997772049, 0.33225069212985325, -0.21988373928624821, -0.23063303507213673, 0.07342115780394749, -0.30368693296359967, -0.11289071642614183, 0.1954992460998628, 0.0806934167799281... |
707.4116 | Note on deconfinement temperature with chemical potential from AdS/CFT | In this note we study the first-order Hawking-Page phase transition of
R-charged black hole in truncated Anti-de Sitter space of various dimensions.
This corresponds to confinement/deconfinement phase transition in the dual
gauge field theory with fixed chemical potential. We demonstrate in general
this critical temp... | hep-th | in this note we study the firstorder hawkingpage phase transition of rcharged black hole in truncated antide sitter space of various dimensions this corresponds to confinementdeconfinement phase transition in the dual gauge field theory with fixed chemical potential we demonstrate in general this critical temperature d... | [['in', 'this', 'note', 'we', 'study', 'the', 'firstorder', 'hawkingpage', 'phase', 'transition', 'of', 'rcharged', 'black', 'hole', 'in', 'truncated', 'antide', 'sitter', 'space', 'of', 'various', 'dimensions', 'this', 'corresponds', 'to', 'confinementdeconfinement', 'phase', 'transition', 'in', 'the', 'dual', 'gauge'... | [-0.13464631304906852, 0.25435710877857426, -0.06540854276919907, 0.05335118415215137, -0.029562385282902556, -0.1266904155300422, 0.06768690002870492, 0.36689452095465225, -0.145701770670712, -0.25430281182581727, 0.04625670724463734, -0.31523296282711355, -0.16145765408873558, 0.013956743241711096, -0.056903118868781... |
707.4117 | Renormalization group approach to exact sampling | In this Letter, we use a general renormalization-group algorithm to implement
Propp and Wilson's "coupling from the past" approach to complex physical
systems. Our algorithm follows the evolution of the entire configuration space
under the Markov chain Monte Carlo dynamics from parts of the configurations
(patches) o... | cond-mat.stat-mech cond-mat.dis-nn | in this letter we use a general renormalizationgroup algorithm to implement propp and wilsons coupling from the past approach to complex physical systems our algorithm follows the evolution of the entire configuration space under the markov chain monte carlo dynamics from parts of the configurations patches on increasi... | [['in', 'this', 'letter', 'we', 'use', 'a', 'general', 'renormalizationgroup', 'algorithm', 'to', 'implement', 'propp', 'and', 'wilsons', 'coupling', 'from', 'the', 'past', 'approach', 'to', 'complex', 'physical', 'systems', 'our', 'algorithm', 'follows', 'the', 'evolution', 'of', 'the', 'entire', 'configuration', 'spa... | [-0.08286920678284433, 0.1282866433262825, -0.12203192884205943, 0.056282419560011475, -0.03477208024511735, -0.1124093735901018, 0.05496454470946143, 0.41682475643853345, -0.2656391353915549, -0.29481429470082127, 0.08620383084182524, -0.24677793525123787, -0.12848995350715187, 0.179100960224039, 0.030092049886782966,... |
707.4118 | The Hochschild cohomology of a Poincar\'e algebra | In this note, we define the notion of a cactus set, and show that its
geometric realization is naturally an algebra over Voronov's cactus operad,
which is equivalent to the framed 2-dimensional little disks operad
$\mathcal{D}_2$. Using this, we show that the Hochschild cohomology of a
Poincar\'e algebra A is an alge... | math.AT | in this note we define the notion of a cactus set and show that its geometric realization is naturally an algebra over voronovs cactus operad which is equivalent to the framed 2dimensional little disks operad mathcald_2 using this we show that the hochschild cohomology of a poincare algebra a is an algebra over the cha... | [['in', 'this', 'note', 'we', 'define', 'the', 'notion', 'of', 'a', 'cactus', 'set', 'and', 'show', 'that', 'its', 'geometric', 'realization', 'is', 'naturally', 'an', 'algebra', 'over', 'voronovs', 'cactus', 'operad', 'which', 'is', 'equivalent', 'to', 'the', 'framed', '2dimensional', 'little', 'disks', 'operad', 'mat... | [-0.19505193370699497, 0.03146525282575347, -0.10647856650456529, 0.07515157724867158, -0.12423926588661711, -0.03460487476068324, -0.09088008937522254, 0.3854762584749802, -0.438954911997606, -0.20127418446193995, 0.12778650923302912, -0.17123805179164328, -0.220025351142575, 0.15128244824129447, -0.23259390362313595,... |
707.4119 | Supersymmetry and Goldstino-like Mode in Bose-Fermi Mixtures | Supersymmetry is assumed to be a basic symmetry of the world in many high
energy theories, but none of the super partners of any known elementary
particle has been observed yet. We argue that supersymmetry can also be
realized and studied in ultracold atomic systems with a mixture of bosons and
fermions, with properl... | cond-mat.other cond-mat.str-el hep-th | supersymmetry is assumed to be a basic symmetry of the world in many high energy theories but none of the super partners of any known elementary particle has been observed yet we argue that supersymmetry can also be realized and studied in ultracold atomic systems with a mixture of bosons and fermions with properly tun... | [['supersymmetry', 'is', 'assumed', 'to', 'be', 'a', 'basic', 'symmetry', 'of', 'the', 'world', 'in', 'many', 'high', 'energy', 'theories', 'but', 'none', 'of', 'the', 'super', 'partners', 'of', 'any', 'known', 'elementary', 'particle', 'has', 'been', 'observed', 'yet', 'we', 'argue', 'that', 'supersymmetry', 'can', 'a... | [-0.1292397449420573, 0.2645117259306604, -0.06340270345517957, 0.12616847456522742, -0.054826823251093164, -0.20844460899631181, 0.03416701528170195, 0.3824673538145266, -0.2331475517916771, -0.29004482874287324, 0.07170741679963835, -0.250788711509749, -0.14337394522603095, 0.08664852575799287, -0.01444512604033215, ... |
707.412 | XMM-Newton temperature maps for five intermediate redshift clusters of
galaxies | We have analyzed XMM-Newton archive data for five clusters of galaxies
(redshifts 0.223 to 0.313) covering a wide range of dynamical states, from
relaxed objects to clusters undergoing several mergers. We present here
temperature maps of the X-ray gas together with a preliminary interpretation of
the formation histor... | astro-ph | we have analyzed xmmnewton archive data for five clusters of galaxies redshifts 0223 to 0313 covering a wide range of dynamical states from relaxed objects to clusters undergoing several mergers we present here temperature maps of the xray gas together with a preliminary interpretation of the formation history of these... | [['we', 'have', 'analyzed', 'xmmnewton', 'archive', 'data', 'for', 'five', 'clusters', 'of', 'galaxies', 'redshifts', '0223', 'to', '0313', 'covering', 'a', 'wide', 'range', 'of', 'dynamical', 'states', 'from', 'relaxed', 'objects', 'to', 'clusters', 'undergoing', 'several', 'mergers', 'we', 'present', 'here', 'tempera... | [-0.09853446009847354, 0.10546416946339841, -0.12882585982408593, 0.07899563595214311, -0.08398440907088418, 0.02459874287859409, 0.10365175354915361, 0.4554000330321929, -0.16727093181700683, -0.367018235372562, 0.08923681333259333, -0.31694471746610076, 0.007567466729704072, 0.23142892357838504, 0.023990452700458905,... |
707.4121 | Characterizations of probability distributions via bivariate regression
of record values | Bairamov et al. (Aust N Z J Stat 47:543-547, 2005) characterize the
exponential distribution in terms of the regression of a function of a record
value with its adjacent record values as covariates. We extend these results to
the case of non-adjacent covariates. We also consider a more general setting
involving monot... | math.PR | bairamov et al aust n z j stat 47543547 2005 characterize the exponential distribution in terms of the regression of a function of a record value with its adjacent record values as covariates we extend these results to the case of nonadjacent covariates we also consider a more general setting involving monotone transfo... | [['bairamov', 'et', 'al', 'aust', 'n', 'z', 'j', 'stat', '47543547', '2005', 'characterize', 'the', 'exponential', 'distribution', 'in', 'terms', 'of', 'the', 'regression', 'of', 'a', 'function', 'of', 'a', 'record', 'value', 'with', 'its', 'adjacent', 'record', 'values', 'as', 'covariates', 'we', 'extend', 'these', 'r... | [-0.08809479272576937, 0.08252329940296477, -0.018144684421713464, 0.06192276248475537, -0.06590070535094128, -0.1409354794304818, 0.08000172410902451, 0.35742987220874056, -0.23295433824387146, -0.2849000357964542, 0.07029127071837138, -0.28819843888413743, -0.1729630070658459, 0.17173999955412, -0.13358440015872475, ... |
707.4122 | The ATLAS Level-1 Trigger: Status of the System and First Results from
Cosmic-Ray Data | The ATLAS detector at CERN's Large Hadron Collider (LHC) will be exposed to
proton-proton collisions from beams crossing at 40 MHz. At the design
luminosity of 10^34 cm^-2 s^-1 there are on average 23 collisions per bunch
crossing. A three-level trigger system will select potentially interesting
events in order to re... | physics.ins-det | the atlas detector at cerns large hadron collider lhc will be exposed to protonproton collisions from beams crossing at 40 mhz at the design luminosity of 1034 cm2 s1 there are on average 23 collisions per bunch crossing a threelevel trigger system will select potentially interesting events in order to reduce the reado... | [['the', 'atlas', 'detector', 'at', 'cerns', 'large', 'hadron', 'collider', 'lhc', 'will', 'be', 'exposed', 'to', 'protonproton', 'collisions', 'from', 'beams', 'crossing', 'at', '40', 'mhz', 'at', 'the', 'design', 'luminosity', 'of', '1034', 'cm2', 's1', 'there', 'are', 'on', 'average', '23', 'collisions', 'per', 'bun... | [-0.10708448569264824, 0.16440882914789717, -0.0257998190832975, 0.046471694290593314, -0.010284352333170094, -0.1436929893081893, 0.009032935750900372, 0.3927653299274612, -0.18485060101614192, -0.40834889541801117, 0.10847884864699453, -0.3455305102070768, 0.06301443295853136, 0.23173318528139658, -0.0094149872263549... |
707.4123 | Systematic errors of bound-state parameters obtained with SVZ sum rules | We study systematic errors of the ground-state parameters obtained by
Shifman-Vainshtein-Zakharov (SVZ) sum rules, making use of the
harmonic-oscillator potential model as an example. In this case, one knows the
exact solution for the polarization operator, which allows one to obtain both
the OPE to any order and the... | hep-ph | we study systematic errors of the groundstate parameters obtained by shifmanvainshteinzakharov svz sum rules making use of the harmonicoscillator potential model as an example in this case one knows the exact solution for the polarization operator which allows one to obtain both the ope to any order and the parameters ... | [['we', 'study', 'systematic', 'errors', 'of', 'the', 'groundstate', 'parameters', 'obtained', 'by', 'shifmanvainshteinzakharov', 'svz', 'sum', 'rules', 'making', 'use', 'of', 'the', 'harmonicoscillator', 'potential', 'model', 'as', 'an', 'example', 'in', 'this', 'case', 'one', 'knows', 'the', 'exact', 'solution', 'for... | [-0.0734859924763441, 0.06690086672069111, -0.05598299995494577, 0.06991179482742714, -0.06262078726520905, -0.08437174534281859, 0.11372075545816468, 0.3592939953104808, -0.25695319972359215, -0.2825040329820835, 0.09879048397907844, -0.26346130864526807, -0.09200511482508424, 0.1709319968188468, 0.017480873012055573,... |
707.4124 | Services within a busy period of an M/M/1 queue and Dyck paths | We analyze the service times of customers in a stable M/M/1 queue in
equilibrium depending on their position in a busy period. We give the law of
the service of a customer at the beginning, at the end, or in the middle of the
busy period. It enables as a by-product to prove that the process of instants
of beginning o... | cs.DM | we analyze the service times of customers in a stable mm1 queue in equilibrium depending on their position in a busy period we give the law of the service of a customer at the beginning at the end or in the middle of the busy period it enables as a byproduct to prove that the process of instants of beginning of service... | [['we', 'analyze', 'the', 'service', 'times', 'of', 'customers', 'in', 'a', 'stable', 'mm1', 'queue', 'in', 'equilibrium', 'depending', 'on', 'their', 'position', 'in', 'a', 'busy', 'period', 'we', 'give', 'the', 'law', 'of', 'the', 'service', 'of', 'a', 'customer', 'at', 'the', 'beginning', 'at', 'the', 'end', 'or', '... | [-0.1966598466894572, 0.13009381042879628, -0.12921937940969924, 0.06975134362904066, -0.038209432942999735, -0.12744372319516348, 0.15633362045035162, 0.385565011072214, -0.2846131107588816, -0.25091700209735857, 0.11767824626143987, -0.26174184116017485, -0.10436064478967132, 0.15824734108065497, -0.09864160183955122... |
707.4125 | Nonrelativistic phase in gamma-ray burst afterglows | The discovery of multiband afterglows definitely shows that most $\gamma$-ray
bursts are of cosmological origin. $\gamma$-ray bursts are found to be one of
the most violent explosive phenomena in the Universe, in which astonishing
ultra-relativistic motions are involved. In this article, the multiband
observational c... | astro-ph | the discovery of multiband afterglows definitely shows that most gammaray bursts are of cosmological origin gammaray bursts are found to be one of the most violent explosive phenomena in the universe in which astonishing ultrarelativistic motions are involved in this article the multiband observational characteristics ... | [['the', 'discovery', 'of', 'multiband', 'afterglows', 'definitely', 'shows', 'that', 'most', 'gammaray', 'bursts', 'are', 'of', 'cosmological', 'origin', 'gammaray', 'bursts', 'are', 'found', 'to', 'be', 'one', 'of', 'the', 'most', 'violent', 'explosive', 'phenomena', 'in', 'the', 'universe', 'in', 'which', 'astonishi... | [-0.09098261373490095, 0.19884771604835988, -0.13231878654845058, 0.1851269494406879, -0.11557085473835468, -0.10985829527769238, -0.021557676997035743, 0.3976082418784499, -0.18811651794053613, -0.2597363739386201, 0.04994308703765273, -0.26882724292576315, -0.09270608723163605, 0.23919724761805264, -0.007906205146573... |
707.4126 | Cosmological WIMPs, Higgs Dark Matter and GLAST | Measurement of the extragalactic background (EGBR) of diffuse gamma-rays is
perhaps one of the most challenging tasks for future gamma-ray observatories,
such as GLAST. This is because any determination will depend on accurate
subtraction of the galactic diffuse and celestial foregrounds, as well as point
sources. Ho... | astro-ph hep-ph | measurement of the extragalactic background egbr of diffuse gammarays is perhaps one of the most challenging tasks for future gammaray observatories such as glast this is because any determination will depend on accurate subtraction of the galactic diffuse and celestial foregrounds as well as point sources however the ... | [['measurement', 'of', 'the', 'extragalactic', 'background', 'egbr', 'of', 'diffuse', 'gammarays', 'is', 'perhaps', 'one', 'of', 'the', 'most', 'challenging', 'tasks', 'for', 'future', 'gammaray', 'observatories', 'such', 'as', 'glast', 'this', 'is', 'because', 'any', 'determination', 'will', 'depend', 'on', 'accurate'... | [-0.0541350073809334, 0.13792080336475165, -0.07315121742029643, 0.19525670681052423, -0.1487565063068579, -0.09349232047539333, -0.02062284215674575, 0.3724650334245686, -0.21290773561400972, -0.3655114260566389, 0.067399130799358, -0.32977385837584733, -0.038978931873009125, 0.2343694675416718, -0.0007727075271822255... |
707.4127 | Star formation in isolated AMIGA galaxies: dynamical influence of bars | Star formation depends strongly both on the local environment of galaxies,
and on the internal dynamics of the interstellar medium. To disentangle the two
effects, we obtained, in the framework of the AMIGA project, Ha and Gunn r
photometric data for more than 200 spiral galaxies lying in very low-density
regions of ... | astro-ph | star formation depends strongly both on the local environment of galaxies and on the internal dynamics of the interstellar medium to disentangle the two effects we obtained in the framework of the amiga project ha and gunn r photometric data for more than 200 spiral galaxies lying in very lowdensity regions of the loca... | [['star', 'formation', 'depends', 'strongly', 'both', 'on', 'the', 'local', 'environment', 'of', 'galaxies', 'and', 'on', 'the', 'internal', 'dynamics', 'of', 'the', 'interstellar', 'medium', 'to', 'disentangle', 'the', 'two', 'effects', 'we', 'obtained', 'in', 'the', 'framework', 'of', 'the', 'amiga', 'project', 'ha',... | [-0.10717297994172743, 0.08857635412040867, -0.10169444448018278, 0.0878445425597337, -0.06213174210720216, -0.02023587369705748, 0.01240606306634039, 0.40000742906704545, -0.19652527196431588, -0.32277740440401953, 0.040335110056537705, -0.2603017271947906, -0.06636316976271867, 0.15672795764288766, 0.0112729116685152... |
707.4128 | Excitation of spin dynamics by spin-polarized current in vortex state
disks | A spin-polarized current with the polarization perpendicular to the plane of
a vortex-state disk results in renormalization of the effective damping for a
given magnetization mode, and the effective damping becomes zero if the current
exceeds a threshold value. The lowest threshold current corresponds to the
lowest f... | cond-mat.mtrl-sci | a spinpolarized current with the polarization perpendicular to the plane of a vortexstate disk results in renormalization of the effective damping for a given magnetization mode and the effective damping becomes zero if the current exceeds a threshold value the lowest threshold current corresponds to the lowest frequen... | [['a', 'spinpolarized', 'current', 'with', 'the', 'polarization', 'perpendicular', 'to', 'the', 'plane', 'of', 'a', 'vortexstate', 'disk', 'results', 'in', 'renormalization', 'of', 'the', 'effective', 'damping', 'for', 'a', 'given', 'magnetization', 'mode', 'and', 'the', 'effective', 'damping', 'becomes', 'zero', 'if',... | [-0.21888402581979066, 0.20733207421831024, 0.008217677259101318, 0.00012534580533750929, -0.08023022709844205, -0.09022911568769278, 0.08539184175419788, 0.30509983552381015, -0.24234864024970776, -0.24869669933254138, 0.07856416579288168, -0.23632250310709843, -0.025812458246946335, 0.23960694479636657, 0.05465879847... |
707.4129 | Vertex operator algebras associated to certain admissible modules for
affine Lie algebras of type A | Let $L(-{1/2}(l+1),0)$ be the simple vertex operator algebra associated to an
affine Lie algebra of type $A_{l}^{(1)}$ with the lowest admissible
half-integer level $-{1/2}(l+1)$, for even l. We study the category of weak
modules for that vertex operator algebra which are in category $\cal{O}$ as
modules for the asso... | math.QA math.RT | let l12l10 be the simple vertex operator algebra associated to an affine lie algebra of type a_l1 with the lowest admissible halfinteger level 12l1 for even l we study the category of weak modules for that vertex operator algebra which are in category calo as modules for the associated affine lie algebra we classify ir... | [['let', 'l12l10', 'be', 'the', 'simple', 'vertex', 'operator', 'algebra', 'associated', 'to', 'an', 'affine', 'lie', 'algebra', 'of', 'type', 'a_l1', 'with', 'the', 'lowest', 'admissible', 'halfinteger', 'level', '12l1', 'for', 'even', 'l', 'we', 'study', 'the', 'category', 'of', 'weak', 'modules', 'for', 'that', 'ver... | [-0.15836864343238255, 0.029209689571871422, 0.004379511736924686, 0.06063702207295194, -0.17891754860442782, -0.2010021915452348, -0.07946703716048173, 0.3775816737777657, -0.4173065254553443, -0.1520156841577282, 0.13850684951443876, -0.2020077896378343, -0.11655522859285748, 0.15429595941012458, -0.1742624808546333,... |
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