id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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709.1635 | Gaudin functions, and Euler-Poincar\'e characteristics | Given two positive integers n,r, we define the Gaudin function of level r to
be quotient of the numerator of the determinant det(1/ ((x_i-y_j)(x_i-ty_j) ...
(x_i-t^r y_j)), i,j=1..n, by the two Vandermonde in x and y. We show that it
can be characterized by specializing the x-variables into the y-variables,
multiplie... | math.CO | given two positive integers nr we define the gaudin function of level r to be quotient of the numerator of the determinant det1 x_iy_jx_ity_j x_itr y_j ij1n by the two vandermonde in x and y we show that it can be characterized by specializing the xvariables into the yvariables multiplied by powers of t this allows us ... | [['given', 'two', 'positive', 'integers', 'nr', 'we', 'define', 'the', 'gaudin', 'function', 'of', 'level', 'r', 'to', 'be', 'quotient', 'of', 'the', 'numerator', 'of', 'the', 'determinant', 'det1', 'x_iy_jx_ity_j', 'x_itr', 'y_j', 'ij1n', 'by', 'the', 'two', 'vandermonde', 'in', 'x', 'and', 'y', 'we', 'show', 'that', ... | [-0.14555816867887372, 0.05647111404687166, -0.06940518158741972, 0.045876667339759265, -0.04385930843500778, -0.12563203311421806, 0.013994853113392236, 0.2704853927716613, -0.3297383678757181, -0.24910085239080768, 0.07053796022147354, -0.24457838702632345, -0.17525012009410243, 0.17747526015216752, -0.07358076951156... |
709.1636 | Dark-Matter Content of Early-Type Galaxies with Planetary Nebulae | We examine the dark matter properties of nearby early-type galaxies using
planetary nebulae (PNe) as mass probes. We have designed a specialised
instrument, the Planetary Nebula Spectrograph (PN.S) operating at the William
Herschel telescope, with the purpose of measuring PN velocities with best
efficiency. The prima... | astro-ph | we examine the dark matter properties of nearby earlytype galaxies using planetary nebulae pne as mass probes we have designed a specialised instrument the planetary nebula spectrograph pns operating at the william herschel telescope with the purpose of measuring pn velocities with best efficiency the primary scientifi... | [['we', 'examine', 'the', 'dark', 'matter', 'properties', 'of', 'nearby', 'earlytype', 'galaxies', 'using', 'planetary', 'nebulae', 'pne', 'as', 'mass', 'probes', 'we', 'have', 'designed', 'a', 'specialised', 'instrument', 'the', 'planetary', 'nebula', 'spectrograph', 'pns', 'operating', 'at', 'the', 'william', 'hersch... | [-0.07382402039002045, 0.05472855627522222, -0.10790753420587862, 0.0915311618555279, -0.1411450579216762, -0.041019073491042946, -0.011391728316084482, 0.3825539832978393, -0.07668241691862931, -0.42042582150315866, 0.009982799623685423, -0.3051051446964266, -0.02100976710607938, 0.218375969081535, -0.0125897571851965... |
709.1637 | Photon propagator for axion electrodynamics | The axion modified electrodynamics is usually used as a model for description
of possible violation of Lorentz invariance in field theory. The low-energy
manifestation of Lorentz violation can hopefully be observed in experiments
with the electromagnetic waves. It justifies the importance of study how a
small axion a... | hep-th | the axion modified electrodynamics is usually used as a model for description of possible violation of lorentz invariance in field theory the lowenergy manifestation of lorentz violation can hopefully be observed in experiments with the electromagnetic waves it justifies the importance of study how a small axion additi... | [['the', 'axion', 'modified', 'electrodynamics', 'is', 'usually', 'used', 'as', 'a', 'model', 'for', 'description', 'of', 'possible', 'violation', 'of', 'lorentz', 'invariance', 'in', 'field', 'theory', 'the', 'lowenergy', 'manifestation', 'of', 'lorentz', 'violation', 'can', 'hopefully', 'be', 'observed', 'in', 'exper... | [-0.1575109608105938, 0.21385733869092177, -0.109451405645077, 0.13905999423933063, -0.154625675755942, -0.09541051291058995, 0.020142735875081978, 0.3100025534299733, -0.2495721331281776, -0.2992287720140966, 0.010622576400755515, -0.20932972654711332, -0.1748465424598065, 0.1602466427205319, -0.01391427513931088, 0.0... |
709.1638 | Cosmological implications of a supersymmetric extension of the
Brans-Dicke theory | In the Brans-Dicke theory the Planck mass is replaced by a dynamical scalar
field. We consider here the supersymmetric analogous of this mechanism
replacing in the supergravity Lagrangian the Planck mass with a chiral
superfield. This analysis is motivated by the research of possible connections
between supersymmetri... | hep-ph | in the bransdicke theory the planck mass is replaced by a dynamical scalar field we consider here the supersymmetric analogous of this mechanism replacing in the supergravity lagrangian the planck mass with a chiral superfield this analysis is motivated by the research of possible connections between supersymmetric dar... | [['in', 'the', 'bransdicke', 'theory', 'the', 'planck', 'mass', 'is', 'replaced', 'by', 'a', 'dynamical', 'scalar', 'field', 'we', 'consider', 'here', 'the', 'supersymmetric', 'analogous', 'of', 'this', 'mechanism', 'replacing', 'in', 'the', 'supergravity', 'lagrangian', 'the', 'planck', 'mass', 'with', 'a', 'chiral', ... | [-0.14708072188145974, 0.17847205624303908, -0.11055963887723491, 0.14598542707515696, -0.11449355073273182, -0.13383609778361907, -0.011732282292773472, 0.26289115882222996, -0.1885717184666325, -0.3128413736121729, 0.03339802328264341, -0.23914514777853207, -0.16897110924051673, 0.1226159740495039, -0.058399188496610... |
709.1639 | Lefschetz fibrations and symplectic homology | We show that for each k > 3 there are infinitely many finite type Stein
manifolds diffeomorphic to Euclidean space R^{2k} which are pairwise distinct
as symplectic manifolds.
| math.SG | we show that for each k 3 there are infinitely many finite type stein manifolds diffeomorphic to euclidean space r2k which are pairwise distinct as symplectic manifolds | [['we', 'show', 'that', 'for', 'each', 'k', '3', 'there', 'are', 'infinitely', 'many', 'finite', 'type', 'stein', 'manifolds', 'diffeomorphic', 'to', 'euclidean', 'space', 'r2k', 'which', 'are', 'pairwise', 'distinct', 'as', 'symplectic', 'manifolds']] | [-0.18317311084656804, 0.1293803213716105, -0.032048561644774896, 0.14312481383482614, -0.09241051999507127, -0.23822584582699668, -0.10713237855169508, 0.4526409397798556, -0.27308237745806024, -0.19820625817886106, 0.093769039803495, -0.3372820705106413, -0.18151802310927045, 0.19515836687275656, -0.15838939255034482... |
709.164 | Estimation of Missing Data Using Computational Intelligence and Decision
Trees | This paper introduces a novel paradigm to impute missing data that combines a
decision tree with an auto-associative neural network (AANN) based model and a
principal component analysis-neural network (PCA-NN) based model. For each
model, the decision tree is used to predict search bounds for a genetic
algorithm that... | stat.AP | this paper introduces a novel paradigm to impute missing data that combines a decision tree with an autoassociative neural network aann based model and a principal component analysisneural network pcann based model for each model the decision tree is used to predict search bounds for a genetic algorithm that minimize a... | [['this', 'paper', 'introduces', 'a', 'novel', 'paradigm', 'to', 'impute', 'missing', 'data', 'that', 'combines', 'a', 'decision', 'tree', 'with', 'an', 'autoassociative', 'neural', 'network', 'aann', 'based', 'model', 'and', 'a', 'principal', 'component', 'analysisneural', 'network', 'pcann', 'based', 'model', 'for', ... | [-0.01718318225888937, 0.004341294004452899, -0.08546069126083132, 0.06997159887310665, -0.08543546521561403, -0.18287135661561407, 0.1054181356870971, 0.3705705386020389, -0.2440745558260995, -0.3726407839715773, 0.09506471500179603, -0.29685981367148606, -0.16071317635257454, 0.16621760661056376, -0.08045300888810672... |
709.1641 | Geant4 applications in the heliospheric radiation environment | The high energy ionizing radiation environment in the solar system consists
of three main sources: the radiation belts, galactic cosmic rays and solar
energetic particles. Geant4 is a Monte Carlo radiation transport simulation
toolkit, with applications in areas as high energy physics, nuclear physics,
astrophysics o... | astro-ph | the high energy ionizing radiation environment in the solar system consists of three main sources the radiation belts galactic cosmic rays and solar energetic particles geant4 is a monte carlo radiation transport simulation toolkit with applications in areas as high energy physics nuclear physics astrophysics or medica... | [['the', 'high', 'energy', 'ionizing', 'radiation', 'environment', 'in', 'the', 'solar', 'system', 'consists', 'of', 'three', 'main', 'sources', 'the', 'radiation', 'belts', 'galactic', 'cosmic', 'rays', 'and', 'solar', 'energetic', 'particles', 'geant4', 'is', 'a', 'monte', 'carlo', 'radiation', 'transport', 'simulati... | [-0.041392536447928834, 0.18884049332490913, -0.031092873883542715, 0.13284332673946345, -0.06405804824788829, -0.02472374277390741, -0.07443628993162231, 0.36812840929036744, -0.21758953449609983, -0.42191893112770207, 0.04116660605503565, -0.34601782415028626, -0.05040054360765393, 0.25935129133925716, -0.04136493797... |
709.1642 | A devil's staircase from rotations and irrationality measures for
Liouville numbers | From Sturmian and Christoffel words we derive a strictly increasing function
$\Delta:[0,\infty)\to\mathbb{R}$. This function is continuous at every
irrational point, while at rational points, left-continuous but not
right-continuous. Moreover, it assumes algebraic integers at rationals, and
transcendental numbers at ... | math.NT math.CO math.DS | from sturmian and christoffel words we derive a strictly increasing function delta0inftytomathbbr this function is continuous at every irrational point while at rational points leftcontinuous but not rightcontinuous moreover it assumes algebraic integers at rationals and transcendental numbers at irrationals we also se... | [['from', 'sturmian', 'and', 'christoffel', 'words', 'we', 'derive', 'a', 'strictly', 'increasing', 'function', 'delta0inftytomathbbr', 'this', 'function', 'is', 'continuous', 'at', 'every', 'irrational', 'point', 'while', 'at', 'rational', 'points', 'leftcontinuous', 'but', 'not', 'rightcontinuous', 'moreover', 'it', ... | [-0.1916486995631001, 0.1432919159107971, -0.11910386324463482, 0.14567455804596344, -0.10483038785901887, -0.1952232991569434, 0.1436465370848223, 0.31664424875095765, -0.3765332153092863, -0.15266412146889638, 0.036387978966727304, -0.3750230685152389, -0.19466007769935662, 0.22449748789464744, -0.08642220478159962, ... |
709.1643 | Which mechanism underlies the water-like anomalies in core-softened
potentials? | Using molecular dynamics simulations we investigate the thermodynamic of
particles interacting with a continuous and a discrete versions of a
core-softened (CS) intermolecular potential composed by a repulsive shoulder.
Dynamic and structural properties are also analyzed by the simulations. We show
that in the contin... | cond-mat.stat-mech cond-mat.soft | using molecular dynamics simulations we investigate the thermodynamic of particles interacting with a continuous and a discrete versions of a coresoftened cs intermolecular potential composed by a repulsive shoulder dynamic and structural properties are also analyzed by the simulations we show that in the continuous ve... | [['using', 'molecular', 'dynamics', 'simulations', 'we', 'investigate', 'the', 'thermodynamic', 'of', 'particles', 'interacting', 'with', 'a', 'continuous', 'and', 'a', 'discrete', 'versions', 'of', 'a', 'coresoftened', 'cs', 'intermolecular', 'potential', 'composed', 'by', 'a', 'repulsive', 'shoulder', 'dynamic', 'and... | [-0.12884341787174344, 0.14685012803971767, -0.07233610023930669, 0.01652476111613214, 0.02821857790648937, -0.1010038291066885, 0.05262155672907829, 0.36313769028149545, -0.2624603491127491, -0.27082739882171153, 0.10757817604020238, -0.29603993938118217, -0.14845368049666285, 0.09922497992962599, 0.03680429564043879,... |
709.1644 | On the Area Functional of the Second Fundamental Form of Ovaloids | The expression for the variation of the area functional of the second
fundamental form of a hypersurface in a Euclidean space involves the so-called
"mean curvature of the second fundamental form". Several new characteristic
properties of (hyper)spheres, in which the mean curvature of the second
fundamental form occu... | math.DG | the expression for the variation of the area functional of the second fundamental form of a hypersurface in a euclidean space involves the socalled mean curvature of the second fundamental form several new characteristic properties of hyperspheres in which the mean curvature of the second fundamental form occurs are gi... | [['the', 'expression', 'for', 'the', 'variation', 'of', 'the', 'area', 'functional', 'of', 'the', 'second', 'fundamental', 'form', 'of', 'a', 'hypersurface', 'in', 'a', 'euclidean', 'space', 'involves', 'the', 'socalled', 'mean', 'curvature', 'of', 'the', 'second', 'fundamental', 'form', 'several', 'new', 'characterist... | [-0.18458314243368096, 0.08921857471607296, -0.08628753061653881, 0.0639467702639183, -0.044182893572540224, -0.052940035456956566, -0.005108106521818834, 0.27627892379613617, -0.28212910806878083, -0.25803641126125676, 0.11683731394248154, -0.2511199663122055, -0.21339576780984673, 0.2077387051916198, -0.0533148333949... |
709.1645 | On Zeta Functions and Families of Siegel Modular Forms | Let $p$ be a prime, and let $\Gamma=\Sp_g(\Z)$ be the Siegel modular group of
genus $g$. We study $p$-adic families of zeta functions and Siegel modular
forms. $L$-functions of Siegel modular forms are described in terms of motivic
$L$-functions attached to $\Sp_g$, and their analytic properties are given.
Critical v... | math.NT | let p be a prime and let gammasp_gz be the siegel modular group of genus g we study padic families of zeta functions and siegel modular forms lfunctions of siegel modular forms are described in terms of motivic lfunctions attached to sp_g and their analytic properties are given critical values for the spinor lfunctions... | [['let', 'p', 'be', 'a', 'prime', 'and', 'let', 'gammasp_gz', 'be', 'the', 'siegel', 'modular', 'group', 'of', 'genus', 'g', 'we', 'study', 'padic', 'families', 'of', 'zeta', 'functions', 'and', 'siegel', 'modular', 'forms', 'lfunctions', 'of', 'siegel', 'modular', 'forms', 'are', 'described', 'in', 'terms', 'of', 'mot... | [-0.29274862408219426, 0.05203288978127909, -0.21186310337500625, 0.08647271610137201, -0.10861337061427283, -0.1437352813121057, -0.04514477714592737, 0.2232759880801935, -0.27236126873935207, -0.2444306319537625, 0.054153421191299816, -0.21909682404019692, -0.155366704663199, 0.32927859919878205, -0.15115954033151435... |
709.1646 | Energy, Rapidity and Transverse Momentum Dependence of Multiplicity
Fluctuations in Heavy Ion Collisions at CERN SPS | Multiplicity fluctuations in the forward hemisphere were studied for
positively, negatively and all charged hadrons produced in central Pb+Pb
collisions at 20A, 30A, 40A, 80A and 158A GeV. The multiplicity distributions
and their scaled variances are presented as a function of collision energy,
rapidity and transvers... | nucl-ex | multiplicity fluctuations in the forward hemisphere were studied for positively negatively and all charged hadrons produced in central pbpb collisions at 20a 30a 40a 80a and 158a gev the multiplicity distributions and their scaled variances are presented as a function of collision energy rapidity and transverse momentu... | [['multiplicity', 'fluctuations', 'in', 'the', 'forward', 'hemisphere', 'were', 'studied', 'for', 'positively', 'negatively', 'and', 'all', 'charged', 'hadrons', 'produced', 'in', 'central', 'pbpb', 'collisions', 'at', '20a', '30a', '40a', '80a', 'and', '158a', 'gev', 'the', 'multiplicity', 'distributions', 'and', 'the... | [-0.05139607027511509, 0.21366666453562816, -0.1384189037942431, 0.1890436384311653, 0.11151536207008003, -0.09594521531404031, -0.04917498269760809, 0.3749366733762953, -0.1650761048162908, -0.3323819009863116, -0.050603499121886365, -0.3943927575558148, 0.1154724172083661, 0.15179086422668425, 0.015573082411989432, 0... |
709.1647 | Unfolding Restricted Convex Caps | This paper details an algorithm for unfolding a class of convex polyhedra,
where each polyhedron in the class consists of a convex cap over a rectangular
base, with several restrictions: the cap's faces are quadrilaterals, with
vertices over an underlying integer lattice, and such that the cap convexity is
``radially... | cs.CG | this paper details an algorithm for unfolding a class of convex polyhedra where each polyhedron in the class consists of a convex cap over a rectangular base with several restrictions the caps faces are quadrilaterals with vertices over an underlying integer lattice and such that the cap convexity is radially monotone ... | [['this', 'paper', 'details', 'an', 'algorithm', 'for', 'unfolding', 'a', 'class', 'of', 'convex', 'polyhedra', 'where', 'each', 'polyhedron', 'in', 'the', 'class', 'consists', 'of', 'a', 'convex', 'cap', 'over', 'a', 'rectangular', 'base', 'with', 'several', 'restrictions', 'the', 'caps', 'faces', 'are', 'quadrilatera... | [-0.13265360220034114, 0.014671886165588684, -0.051231341888470686, -0.003591022440506255, -0.1356818202252993, -0.11627095644892987, 0.006518404935965972, 0.36158256388871984, -0.3453453001874389, -0.1935030898586025, 0.1548830991001416, -0.2784426202552448, -0.13825360285666058, 0.16746460147859418, -0.15897643154569... |
709.1648 | Asymptotics: Particles, Processes and Inverse Problems. Festschrift for
Piet Groeneboom | In September 2006, Piet Groeneboom officially retired as professor of
statistics at Delft University of Technology and the Vrije Universiteit in
Amsterdam. He did so by delivering his farewell lecture `Summa Cogitatio' ([42]
in Piet's publication list) in the Aula of the university in Delft. To
celebrate Piet's impre... | math.ST stat.TH | in september 2006 piet groeneboom officially retired as professor of statistics at delft university of technology and the vrije universiteit in amsterdam he did so by delivering his farewell lecture summa cogitatio 42 in piets publication list in the aula of the university in delft to celebrate piets impressive contrib... | [['in', 'september', '2006', 'piet', 'groeneboom', 'officially', 'retired', 'as', 'professor', 'of', 'statistics', 'at', 'delft', 'university', 'of', 'technology', 'and', 'the', 'vrije', 'universiteit', 'in', 'amsterdam', 'he', 'did', 'so', 'by', 'delivering', 'his', 'farewell', 'lecture', 'summa', 'cogitatio', '42', '... | [-0.012228923102416698, 0.1066363488398132, -0.1015155778191651, 0.048039082793236175, -0.07223186910241133, -0.13196042324748955, 0.06091166451612177, 0.2777450373867482, -0.13707983268666016, -0.40597136674027534, 0.14002061478857372, -0.3732853598083325, -0.10514827367816386, 0.1909465033206202, -0.14341223308639156... |
709.1649 | The Vertical Structure of Planet-induced Gaps in Proto-Planetary Discs | Giant planets embedded in circumstellar discs are expected to open gaps in
these discs. We examine the vertical structure of the gap edges. We find that
the planet excites spiral arms with significant (Mach number of a half)
vertical motion of the gas, and discuss the implications of these motions. In
particular, the... | astro-ph | giant planets embedded in circumstellar discs are expected to open gaps in these discs we examine the vertical structure of the gap edges we find that the planet excites spiral arms with significant mach number of a half vertical motion of the gas and discuss the implications of these motions in particular the spiral a... | [['giant', 'planets', 'embedded', 'in', 'circumstellar', 'discs', 'are', 'expected', 'to', 'open', 'gaps', 'in', 'these', 'discs', 'we', 'examine', 'the', 'vertical', 'structure', 'of', 'the', 'gap', 'edges', 'we', 'find', 'that', 'the', 'planet', 'excites', 'spiral', 'arms', 'with', 'significant', 'mach', 'number', 'o... | [-0.15203953919546673, 0.15884514502827607, -0.08021159699279154, 0.059224777207676826, -0.11157341461285208, 0.005156622654659317, -0.005065200840459859, 0.42162425596768976, -0.27349309884143846, -0.31508388554558475, 0.06491117715977582, -0.23045515331129232, -0.05263357309142379, 0.12574899438083342, -0.04945256464... |
709.165 | Gapless superconductivity and the Fermi arc in the cuprates | We argue that the Fermi arc observed in angle resolved photoemission
measurements in underdoped cuprates can be understood as a consequence of
inelastic scattering in a d-wave superconductor. We analyze this phenomenon in
the context of strong coupling Eliashberg theory, deriving a `single lifetime'
model for describ... | cond-mat.str-el cond-mat.supr-con | we argue that the fermi arc observed in angle resolved photoemission measurements in underdoped cuprates can be understood as a consequence of inelastic scattering in a dwave superconductor we analyze this phenomenon in the context of strong coupling eliashberg theory deriving a single lifetime model for describing the... | [['we', 'argue', 'that', 'the', 'fermi', 'arc', 'observed', 'in', 'angle', 'resolved', 'photoemission', 'measurements', 'in', 'underdoped', 'cuprates', 'can', 'be', 'understood', 'as', 'a', 'consequence', 'of', 'inelastic', 'scattering', 'in', 'a', 'dwave', 'superconductor', 'we', 'analyze', 'this', 'phenomenon', 'in',... | [-0.1622317972019888, 0.18892706453692742, -0.0988341279184589, 0.13283685814553442, -0.02211681009771732, -0.15408369097142266, 0.10334161480423062, 0.37144469539993086, -0.3061815179597873, -0.3222090391298899, -0.04209757873501915, -0.3228930363861414, -0.10209523490988291, 0.16703979833087382, 0.03407041862463722, ... |
709.1651 | Local distinguishability of orthogonal 2\otimes3 pure states | We present a complete characterization for the local distinguishability of
orthogonal $2\otimes 3$ pure states except for some special cases of three
states. Interestingly, we find there is a large class of four or three states
that are indistinguishable by local projective measurements and classical
communication (L... | quant-ph | we present a complete characterization for the local distinguishability of orthogonal 2otimes 3 pure states except for some special cases of three states interestingly we find there is a large class of four or three states that are indistinguishable by local projective measurements and classical communication lpcc can ... | [['we', 'present', 'a', 'complete', 'characterization', 'for', 'the', 'local', 'distinguishability', 'of', 'orthogonal', '2otimes', '3', 'pure', 'states', 'except', 'for', 'some', 'special', 'cases', 'of', 'three', 'states', 'interestingly', 'we', 'find', 'there', 'is', 'a', 'large', 'class', 'of', 'four', 'or', 'three... | [-0.15747518905051083, 0.18258873051611565, -0.06032582494516332, 0.052608231145168556, 0.04048684669048095, -0.2509867959154942, 0.03530463611339258, 0.31810288528810027, -0.21644941104200333, -0.2960004560774615, 0.07026024119920653, -0.2566242819796747, -0.13463514773840352, 0.20634290359781257, -0.04121341397437979... |
709.1652 | Top Quarks, Axigluons and Charge Asymmetries at Hadron Colliders | Axigluons are colored heavy neutral gauge boson that couple to quarks through
an axial vector current and the same strong coupling as gluons. The most
important model-independent manifestation of axigluons is the generation of a
forward--backward asymmetry in top-antitop quark production at $p\bar{p}$
collisions whic... | hep-ph hep-ex | axigluons are colored heavy neutral gauge boson that couple to quarks through an axial vector current and the same strong coupling as gluons the most important modelindependent manifestation of axigluons is the generation of a forwardbackward asymmetry in topantitop quark production at pbarp collisions which originates... | [['axigluons', 'are', 'colored', 'heavy', 'neutral', 'gauge', 'boson', 'that', 'couple', 'to', 'quarks', 'through', 'an', 'axial', 'vector', 'current', 'and', 'the', 'same', 'strong', 'coupling', 'as', 'gluons', 'the', 'most', 'important', 'modelindependent', 'manifestation', 'of', 'axigluons', 'is', 'the', 'generation... | [-0.07464280931949238, 0.24689610299075768, -0.07947334969051283, 0.1603489306745925, -0.06065776150019185, -0.11196065744120828, 0.04124167119624798, 0.3113466360279032, -0.2003983184294083, -0.2921566599256334, -0.04244700621269215, -0.3448198494325216, 0.06324721356174229, 0.11798153048053987, 0.07675335749592853, 0... |
709.1653 | Counterexamples to continuity of optimal transportation on positively
curved Riemannian manifolds | Counterexamples to continuity of optimal transportation on Riemannian
manifolds with everywhere positive sectional curvature are provided. These
examples show that the condition A3w of Ma, Trudinger, & Wang is not guaranteed
by positivity of sectional curvature.
| math.DG math.AP | counterexamples to continuity of optimal transportation on riemannian manifolds with everywhere positive sectional curvature are provided these examples show that the condition a3w of ma trudinger wang is not guaranteed by positivity of sectional curvature | [['counterexamples', 'to', 'continuity', 'of', 'optimal', 'transportation', 'on', 'riemannian', 'manifolds', 'with', 'everywhere', 'positive', 'sectional', 'curvature', 'are', 'provided', 'these', 'examples', 'show', 'that', 'the', 'condition', 'a3w', 'of', 'ma', 'trudinger', 'wang', 'is', 'not', 'guaranteed', 'by', 'p... | [-0.20998165107199124, 0.06196792796254158, -0.027395715404834067, 0.11958418628533504, -0.14454835333994456, -0.2267685422141637, -0.05922480087195124, 0.3864563125584807, -0.216684760555758, -0.23625139242836407, 0.1935514172273023, -0.3030235373548099, -0.14606049824506045, 0.16101472254044244, -0.22574850198413646,... |
709.1654 | Localizing the Elliott Conjecture at Strongly Self-absorbing C*-algebras
--An Appendix | This note provides some technical support to the proof of a result of W.
Winter which shows that two unital separable simple amenable ${\cal
Z}$-absorbing C*-algebras with locally finite decomposition property satisfying
the UCT whose projections separate the traces are isomorphic if their
$K$-theory is finitely gene... | math.OA | this note provides some technical support to the proof of a result of w winter which shows that two unital separable simple amenable cal zabsorbing calgebras with locally finite decomposition property satisfying the uct whose projections separate the traces are isomorphic if their ktheory is finitely generated and thei... | [['this', 'note', 'provides', 'some', 'technical', 'support', 'to', 'the', 'proof', 'of', 'a', 'result', 'of', 'w', 'winter', 'which', 'shows', 'that', 'two', 'unital', 'separable', 'simple', 'amenable', 'cal', 'zabsorbing', 'calgebras', 'with', 'locally', 'finite', 'decomposition', 'property', 'satisfying', 'the', 'uc... | [-0.14326255300289226, 0.17707485719411462, -0.13495497833247538, 0.042223356178039, -0.10149326666443678, -0.17561767404657547, -0.061098559274493404, 0.39504470989211565, -0.3713138476704006, -0.13385305276002596, 0.14506549371785862, -0.25399351579512264, -0.0913860881873579, 0.20121027996625612, -0.1616688948297114... |
709.1655 | Network structure and dynamics of hydrogenated amorphous silicon | In this paper we discuss the application of current it ab initio computer
simulation techniques to hydrogenated amorphous silicon (a-Si:H). We begin by
discussing thermal fluctuation in the number of coordination defects in the
material, and its temperature dependence. We connect this to the ``fluctuating
bond center... | cond-mat.mtrl-sci | in this paper we discuss the application of current it ab initio computer simulation techniques to hydrogenated amorphous silicon asih we begin by discussing thermal fluctuation in the number of coordination defects in the material and its temperature dependence we connect this to the fluctuating bond center detachment... | [['in', 'this', 'paper', 'we', 'discuss', 'the', 'application', 'of', 'current', 'it', 'ab', 'initio', 'computer', 'simulation', 'techniques', 'to', 'hydrogenated', 'amorphous', 'silicon', 'asih', 'we', 'begin', 'by', 'discussing', 'thermal', 'fluctuation', 'in', 'the', 'number', 'of', 'coordination', 'defects', 'in', ... | [-0.10215871373580548, 0.15594558751878426, -0.04982761344811144, 0.049084688641749766, -0.004021725654111881, -0.1004165233186397, 0.07062368644600563, 0.41430822409395324, -0.3152931891967647, -0.2811744339016609, 0.03463566663834315, -0.3088344272569214, -0.1667021464672871, 0.1313920887845789, 0.013771816329129874,... |
709.1656 | Detection of a Third Planet in the HD 74156 System Using the
Hobby-Eberly Telescope | We report the discovery of a third planetary mass companion to the G0 star HD
74156. High precision radial velocity measurements made with the Hobby-Eberly
Telescope aided the detection of this object. The best fit triple Keplerian
model to all the available velocity data yields an orbital period of 347 days
and mini... | astro-ph | we report the discovery of a third planetary mass companion to the g0 star hd 74156 high precision radial velocity measurements made with the hobbyeberly telescope aided the detection of this object the best fit triple keplerian model to all the available velocity data yields an orbital period of 347 days and minimum m... | [['we', 'report', 'the', 'discovery', 'of', 'a', 'third', 'planetary', 'mass', 'companion', 'to', 'the', 'g0', 'star', 'hd', '74156', 'high', 'precision', 'radial', 'velocity', 'measurements', 'made', 'with', 'the', 'hobbyeberly', 'telescope', 'aided', 'the', 'detection', 'of', 'this', 'object', 'the', 'best', 'fit', '... | [-0.17217243651934885, 0.11912310736109978, -0.06161001970676679, 0.03461612260516759, -0.12186306031194555, -0.11273966503450909, 0.09955730860639678, 0.32903573011100606, -0.13269292514994216, -0.40275813090864204, 0.09037893038393903, -0.27569290463879054, -0.05689094891332247, 0.21019955881392505, -0.08462957546613... |
709.1657 | Time-evolution of ionization and heating around first stars and
miniquasars | A one dimensional radiative transfer code is developed to track the
ionization and heating pattern around the first miniquasars and Population III
stars. The code follows the evolution of the ionization of the species of
hydrogen and helium and the intergalactic medium temperature profiles as a
function of redshift. ... | astro-ph | a one dimensional radiative transfer code is developed to track the ionization and heating pattern around the first miniquasars and population iii stars the code follows the evolution of the ionization of the species of hydrogen and helium and the intergalactic medium temperature profiles as a function of redshift the ... | [['a', 'one', 'dimensional', 'radiative', 'transfer', 'code', 'is', 'developed', 'to', 'track', 'the', 'ionization', 'and', 'heating', 'pattern', 'around', 'the', 'first', 'miniquasars', 'and', 'population', 'iii', 'stars', 'the', 'code', 'follows', 'the', 'evolution', 'of', 'the', 'ionization', 'of', 'the', 'species',... | [-0.0423365262341422, 0.17381623233630067, -0.037405966009663526, 0.10321904001757502, -0.036543001621118135, -0.0786067635365674, 0.04621830035115258, 0.4016617381523521, -0.1974753237839015, -0.363591199282135, 0.06917784590546464, -0.2922501128553501, -0.01591108475882068, 0.19374997942611785, 0.029193378375175428, ... |
709.1658 | New path description for the M(k+1,2k+3) models and the dual Z_k graded
parafermions | We present a new path description for the states of the non-unitary
M(k+1,2k+3) models. This description differs from the one induced by the
Forrester-Baxter solution, in terms of configuration sums, of their
restricted-solid-on-solid model. The proposed path representation is actually
very similar to the one underly... | hep-th cond-mat.stat-mech math-ph math.CO math.MP | we present a new path description for the states of the nonunitary mk12k3 models this description differs from the one induced by the forresterbaxter solution in terms of configuration sums of their restrictedsolidonsolid model the proposed path representation is actually very similar to the one underlying the unitary ... | [['we', 'present', 'a', 'new', 'path', 'description', 'for', 'the', 'states', 'of', 'the', 'nonunitary', 'mk12k3', 'models', 'this', 'description', 'differs', 'from', 'the', 'one', 'induced', 'by', 'the', 'forresterbaxter', 'solution', 'in', 'terms', 'of', 'configuration', 'sums', 'of', 'their', 'restrictedsolidonsolid... | [-0.11773242526146761, 0.13718449565416763, -0.09937535556835225, 0.0703011744907314, -0.06407792072253998, -0.14821459210919913, 0.00553015821538113, 0.3000051053570151, -0.28837242925238576, -0.22274328901601786, 0.03810376688165383, -0.2513053554552372, -0.17084783287436672, 0.16245488500495375, -0.07392137824567128... |
709.1659 | On the localized phase of a copolymer in an emulsion: supercritical
percolation regime | In this paper we study a two-dimensional directed self-avoiding walk model of
a random copolymer in a random emulsion. The copolymer is a random
concatenation of monomers of two types, $A$ and $B$, each occurring with
density 1/2. The emulsion is a random mixture of liquids of two types, $A$ and
$B$, organised in lar... | math.PR | in this paper we study a twodimensional directed selfavoiding walk model of a random copolymer in a random emulsion the copolymer is a random concatenation of monomers of two types a and b each occurring with density 12 the emulsion is a random mixture of liquids of two types a and b organised in large square blocks oc... | [['in', 'this', 'paper', 'we', 'study', 'a', 'twodimensional', 'directed', 'selfavoiding', 'walk', 'model', 'of', 'a', 'random', 'copolymer', 'in', 'a', 'random', 'emulsion', 'the', 'copolymer', 'is', 'a', 'random', 'concatenation', 'of', 'monomers', 'of', 'two', 'types', 'a', 'and', 'b', 'each', 'occurring', 'with', '... | [-0.15455286616990604, 0.24620160384410592, -0.07467858494263158, -0.005595333941082609, 0.02682070907515784, -0.16380581710988798, 0.061242224609322216, 0.36978826637054424, -0.2656442309546483, -0.21601575985176855, 0.09399470957472965, -0.31246867433356784, -0.13026343869890675, 0.07930506606133707, 0.01105611135408... |
709.166 | Partial Gr\"obner bases for multiobjective integer linear optimization | In this paper we present a new methodology for solving multiobjective integer
linear programs using tools from algebraic geometry. We introduce the concept
of partial Gr\"obner basis for a family of multiobjective programs where the
right-hand side varies. This new structure extends the notion of Gr\"obner
basis for ... | math.OC math.AG | in this paper we present a new methodology for solving multiobjective integer linear programs using tools from algebraic geometry we introduce the concept of partial grobner basis for a family of multiobjective programs where the righthand side varies this new structure extends the notion of grobner basis for the singl... | [['in', 'this', 'paper', 'we', 'present', 'a', 'new', 'methodology', 'for', 'solving', 'multiobjective', 'integer', 'linear', 'programs', 'using', 'tools', 'from', 'algebraic', 'geometry', 'we', 'introduce', 'the', 'concept', 'of', 'partial', 'grobner', 'basis', 'for', 'a', 'family', 'of', 'multiobjective', 'programs',... | [-0.14461680494206047, 0.007206420168690731, -0.0740222481183772, 0.0530297543636748, -0.12423386474289856, -0.10660727984230463, 0.0379264971392561, 0.3134675414044538, -0.35321352187672567, -0.2722545010733536, 0.1261297283632595, -0.24317783907454946, -0.1761714518605464, 0.2090913939184937, -0.045084814144293085, 0... |
709.1661 | Bulk dominated fermion emission on a Schwarzschild background | Using the WKBJ approximation, and the Unruh method, we obtain semi-analytic
expressions for the absorption probability (in all energy regimes) for Dirac
fermions on a higher dimensional Schwarzschild background. We present an
analytic expression relating the absorption probability to the absorption
cross-section, and... | hep-th | using the wkbj approximation and the unruh method we obtain semianalytic expressions for the absorption probability in all energy regimes for dirac fermions on a higher dimensional schwarzschild background we present an analytic expression relating the absorption probability to the absorption crosssection and then use ... | [['using', 'the', 'wkbj', 'approximation', 'and', 'the', 'unruh', 'method', 'we', 'obtain', 'semianalytic', 'expressions', 'for', 'the', 'absorption', 'probability', 'in', 'all', 'energy', 'regimes', 'for', 'dirac', 'fermions', 'on', 'a', 'higher', 'dimensional', 'schwarzschild', 'background', 'we', 'present', 'an', 'a... | [-0.061038785885198434, 0.0784359432804386, -0.0848253813588567, 0.13431035309086406, -0.08112653517450222, -0.13126155453439997, 0.014129676947496799, 0.37421174406221036, -0.14887601115920565, -0.23755583228347332, 0.05140374362235889, -0.3005124356969374, -0.11992054735514614, 0.19841903341901407, -0.020165231021676... |
709.1662 | Teleportation of qubit states through dissipative channels: Conditions
for surpassing the no-cloning limit | We investigate quantum teleportation through dissipative channels and
calculate teleportation fidelity as a function of damping rates. It is found
that the average fidelity of teleportation and the range of states to be
teleported depend on the type and rate of the damping in the channel. Using the
fully entangled fr... | quant-ph | we investigate quantum teleportation through dissipative channels and calculate teleportation fidelity as a function of damping rates it is found that the average fidelity of teleportation and the range of states to be teleported depend on the type and rate of the damping in the channel using the fully entangled fracti... | [['we', 'investigate', 'quantum', 'teleportation', 'through', 'dissipative', 'channels', 'and', 'calculate', 'teleportation', 'fidelity', 'as', 'a', 'function', 'of', 'damping', 'rates', 'it', 'is', 'found', 'that', 'the', 'average', 'fidelity', 'of', 'teleportation', 'and', 'the', 'range', 'of', 'states', 'to', 'be', ... | [-0.15073408011459943, 0.17095718956693556, -0.04630518769422038, 0.028239169943018085, 0.03455331990156661, -0.17966732935076862, 0.0982629112490086, 0.35658079814165833, -0.25136446663686496, -0.2762619709596038, 0.11151970880578808, -0.2514496826086984, -0.05095195195665865, 0.23150535536450192, -0.05791293888381033... |
709.1663 | Uniform Bahadur Representation for Local Polynomial Estimates of
M-Regression and Its Application to The Additive Model | We use local polynomial fitting to estimate the nonparametric M-regression
function for strongly mixing stationary processes
$\{(Y_{i},\underline{X}_{i})\}$. We establish a strong uniform consistency rate
for the Bahadur representation of estimators of the regression function and its
derivatives. These results are fu... | math.ST stat.ME stat.TH | we use local polynomial fitting to estimate the nonparametric mregression function for strongly mixing stationary processes y_iunderlinex_i we establish a strong uniform consistency rate for the bahadur representation of estimators of the regression function and its derivatives these results are fundamental for statist... | [['we', 'use', 'local', 'polynomial', 'fitting', 'to', 'estimate', 'the', 'nonparametric', 'mregression', 'function', 'for', 'strongly', 'mixing', 'stationary', 'processes', 'y_iunderlinex_i', 'we', 'establish', 'a', 'strong', 'uniform', 'consistency', 'rate', 'for', 'the', 'bahadur', 'representation', 'of', 'estimator... | [-0.03107814506725653, 0.010372929295140478, -0.087662427894477, 0.11702938169994588, -0.06952499802297864, -0.10458386399611634, 0.03809062243243189, 0.39315984545177535, -0.28712846640203343, -0.26723786449905385, 0.13687835252954086, -0.23987770628943844, -0.147202585355875, 0.23317032136746044, -0.07767498516784001... |
709.1664 | Multiplicity Studies and Effective Energy in ALICE at the LHC | In this work we explore the possibility to perform ``effective energy''
studies in very high energy collisions at the CERN Large Hadron Collider (LHC).
In particular, we focus on the possibility to measure in $pp$ collisions the
average charged multiplicity as a function of the effective energy with the
ALICE experim... | hep-ph | in this work we explore the possibility to perform effective energy studies in very high energy collisions at the cern large hadron collider lhc in particular we focus on the possibility to measure in pp collisions the average charged multiplicity as a function of the effective energy with the alice experiment using it... | [['in', 'this', 'work', 'we', 'explore', 'the', 'possibility', 'to', 'perform', 'effective', 'energy', 'studies', 'in', 'very', 'high', 'energy', 'collisions', 'at', 'the', 'cern', 'large', 'hadron', 'collider', 'lhc', 'in', 'particular', 'we', 'focus', 'on', 'the', 'possibility', 'to', 'measure', 'in', 'pp', 'collisio... | [-0.05969635340547786, 0.18434999749715034, -0.1603874764402406, 0.1272807352898785, 0.02007712804351412, -0.11783754102368817, -0.040372249633006965, 0.3293918280062404, -0.19403416942805052, -0.3429555000256052, -0.01540560050116647, -0.33749127985116395, 0.040699394434271605, 0.14415025849142624, 0.04170021429239064... |
709.1665 | On some new congruences for binomial coefficients | In this paper we establish some new congruences involving central binomial
coefficients as well as Catalan numbers. Let $p$ be a prime and let $a$ be any
positive integer. We determine $\sum_{k=0}^{p^a-1}\binom{2k}{k+d}$ mod $p^2$
for $d=0,...,p^a$ and $\sum_{k=0}^{p^a-1}\binom{2k}{k+\delta}$ mod $p^3$ for
$\delta=0,... | math.NT math.CO | in this paper we establish some new congruences involving central binomial coefficients as well as catalan numbers let p be a prime and let a be any positive integer we determine sum_k0pa1binom2kkd mod p2 for d0pa and sum_k0pa1binom2kkdelta mod p3 for delta01 we also show that c_n1sum_k0pa1c_pank13n1pa13 mod p2 for eve... | [['in', 'this', 'paper', 'we', 'establish', 'some', 'new', 'congruences', 'involving', 'central', 'binomial', 'coefficients', 'as', 'well', 'as', 'catalan', 'numbers', 'let', 'p', 'be', 'a', 'prime', 'and', 'let', 'a', 'be', 'any', 'positive', 'integer', 'we', 'determine', 'sum_k0pa1binom2kkd', 'mod', 'p2', 'for', 'd0p... | [-0.25388479349598037, 0.12827542301077963, -0.06764161179505163, 0.05661973053534215, -0.09257784333490467, -0.23181648760189508, -0.0142034775107878, 0.2602944352853475, -0.3274762497867568, -0.2343345694875313, 0.04897462840042061, -0.3061429904931683, -0.19328765302770218, 0.2123998836061712, -0.12177920262566057, ... |
709.1666 | Inductive acceleration of UHECRs in sheared relativistic jets | Relativistic outflows carrying large scale magnetic fields have large
inductive potential and may accelerate protons to ultra high energies. We
discuss a novel scheme of Ultra-High Energy Cosmic Ray (UHECR) acceleration due
to drifts in magnetized, cylindrically collimated, sheared jets of powerful
active galaxies (w... | astro-ph | relativistic outflows carrying large scale magnetic fields have large inductive potential and may accelerate protons to ultra high energies we discuss a novel scheme of ultrahigh energy cosmic ray uhecr acceleration due to drifts in magnetized cylindrically collimated sheared jets of powerful active galaxies with jet l... | [['relativistic', 'outflows', 'carrying', 'large', 'scale', 'magnetic', 'fields', 'have', 'large', 'inductive', 'potential', 'and', 'may', 'accelerate', 'protons', 'to', 'ultra', 'high', 'energies', 'we', 'discuss', 'a', 'novel', 'scheme', 'of', 'ultrahigh', 'energy', 'cosmic', 'ray', 'uhecr', 'acceleration', 'due', 't... | [-0.12104860816048238, 0.29788498822189446, -0.021089892035100873, 0.11627843817714309, -0.0633297236782946, -0.13118382689440403, -0.03735254087859369, 0.4344284666159491, -0.24276643580350085, -0.31113864138253094, -0.04617002429202287, -0.26745776926702636, 0.07984594937677927, 0.16724696839741598, 0.031711062779430... |
709.1667 | Solving Constraint Satisfaction Problems through Belief
Propagation-guided decimation | Message passing algorithms have proved surprisingly successful in solving
hard constraint satisfaction problems on sparse random graphs. In such
applications, variables are fixed sequentially to satisfy the constraints.
Message passing is run after each step. Its outcome provides an heuristic to
make choices at next ... | cs.AI cond-mat.dis-nn cond-mat.stat-mech cs.CC | message passing algorithms have proved surprisingly successful in solving hard constraint satisfaction problems on sparse random graphs in such applications variables are fixed sequentially to satisfy the constraints message passing is run after each step its outcome provides an heuristic to make choices at next step t... | [['message', 'passing', 'algorithms', 'have', 'proved', 'surprisingly', 'successful', 'in', 'solving', 'hard', 'constraint', 'satisfaction', 'problems', 'on', 'sparse', 'random', 'graphs', 'in', 'such', 'applications', 'variables', 'are', 'fixed', 'sequentially', 'to', 'satisfy', 'the', 'constraints', 'message', 'passi... | [-0.11806823824327893, 0.05341935498261118, -0.13736105823843944, 0.0863458988970388, -0.10326720524495997, -0.20893711797756756, 0.09985969989462112, 0.44427276450413755, -0.27235395002474144, -0.2868230186570322, 0.12423033217759424, -0.22892360630013595, -0.18452204257340693, 0.15743210561321747, -0.0697384236827189... |
709.1668 | Anomalies in gauge theory and gerbes over quotient stacks | We give a new interpretation of the Faddeev-Mickelsson anomaly in certain
Yang-Mills theories in terms of S^1-central extensions of Lie groupoids.
| math.DG math-ph math.MP | we give a new interpretation of the faddeevmickelsson anomaly in certain yangmills theories in terms of s1central extensions of lie groupoids | [['we', 'give', 'a', 'new', 'interpretation', 'of', 'the', 'faddeevmickelsson', 'anomaly', 'in', 'certain', 'yangmills', 'theories', 'in', 'terms', 'of', 's1central', 'extensions', 'of', 'lie', 'groupoids']] | [-0.22576894210651516, 0.08504683426581323, -0.08660703506029677, 0.12249037809669971, -0.1482530971057713, -0.07628639617469161, -0.0027178328484296797, 0.29561173021793363, -0.21099370382726193, -0.2653271327726543, 0.09678423494333402, -0.19083973560482265, -0.2301111147738993, 0.1535904470831156, -0.181030046055093... |
709.1669 | Mott transition of fermionic atoms in a three-dimensional optical trap | We study theoretically the Mott metal-insulator transition for a system of
fermionic atoms confined in a three-dimensional optical lattice and a harmonic
trap. We describe an inhomogeneous system of several thousand sites using an
adaptation of dynamical mean field theory solved efficiently with the numerical
renorma... | cond-mat.str-el cond-mat.other | we study theoretically the mott metalinsulator transition for a system of fermionic atoms confined in a threedimensional optical lattice and a harmonic trap we describe an inhomogeneous system of several thousand sites using an adaptation of dynamical mean field theory solved efficiently with the numerical renormalizat... | [['we', 'study', 'theoretically', 'the', 'mott', 'metalinsulator', 'transition', 'for', 'a', 'system', 'of', 'fermionic', 'atoms', 'confined', 'in', 'a', 'threedimensional', 'optical', 'lattice', 'and', 'a', 'harmonic', 'trap', 'we', 'describe', 'an', 'inhomogeneous', 'system', 'of', 'several', 'thousand', 'sites', 'us... | [-0.1836140208865683, 0.19535494292825042, -0.07408318190405574, 0.03244680993688794, 0.0504799349567829, -0.1372410788287361, 0.08453423578071241, 0.40577816019933194, -0.2556428979747953, -0.2412774450599383, 0.05985345616220282, -0.29759313833589357, -0.15122330823960978, 0.13256894725446516, 0.061892034247135505, 0... |
709.167 | On approximate solutions of semilinear evolution equations II.
Generalizations, and applications to Navier-Stokes equations | In our previous paper [12] (Rev. Math. Phys. 16, 383-420 (2004)), a general
framework was outlined to treat the approximate solutions of semilinear
evolution equations; more precisely, a scheme was presented to infer from an
approximate solution the existence (local or global in time) of an exact
solution, and to est... | math.AP math-ph math.MP | in our previous paper 12 rev math phys 16 383420 2004 a general framework was outlined to treat the approximate solutions of semilinear evolution equations more precisely a scheme was presented to infer from an approximate solution the existence local or global in time of an exact solution and to estimate their distanc... | [['in', 'our', 'previous', 'paper', '12', 'rev', 'math', 'phys', '16', '383420', '2004', 'a', 'general', 'framework', 'was', 'outlined', 'to', 'treat', 'the', 'approximate', 'solutions', 'of', 'semilinear', 'evolution', 'equations', 'more', 'precisely', 'a', 'scheme', 'was', 'presented', 'to', 'infer', 'from', 'an', 'a... | [-0.11092053543103833, 0.0542310806589854, -0.08724323393601169, 0.07862745579071603, -0.06338709317818544, -0.0954383895195161, 0.03512700589437207, 0.31270622597824965, -0.2624101374917859, -0.31748516443413455, 0.14284510041955026, -0.2628405242588475, -0.08813020714963266, 0.19066578625470165, -0.018809066424341676... |
709.1671 | Gribov copies and confinement | We analyse the role of the Gribov ambiguity in the construction of physical
charges in gauge theories. It is shown explicitly how the Gribov copies prevent
the construction of physical coloured charges beyond perturbation theory. We
also present a new and manifestly non-perturbative class of Coulomb gauge
Gribov copi... | hep-th | we analyse the role of the gribov ambiguity in the construction of physical charges in gauge theories it is shown explicitly how the gribov copies prevent the construction of physical coloured charges beyond perturbation theory we also present a new and manifestly nonperturbative class of coulomb gauge gribov copies | [['we', 'analyse', 'the', 'role', 'of', 'the', 'gribov', 'ambiguity', 'in', 'the', 'construction', 'of', 'physical', 'charges', 'in', 'gauge', 'theories', 'it', 'is', 'shown', 'explicitly', 'how', 'the', 'gribov', 'copies', 'prevent', 'the', 'construction', 'of', 'physical', 'coloured', 'charges', 'beyond', 'perturbati... | [-0.15506868067016938, 0.22066624078671543, -0.1343240112788519, 0.10502748842569715, -0.08754519380781116, -0.0680054217263372, 0.036311096324091206, 0.3069444805079577, -0.1705689147418859, -0.2780301172514351, 0.007322773669979402, -0.2273344284265625, -0.19061901838499673, -0.0162376874715698, -0.13904768017557811,... |
709.1672 | Explore Physics Beyond the Standard Model with GLAST | We give an overview of the possibility of GLAST to explore theories beyond
the Standard Model of particle physics. Among the wide taxonomy we will focus
in particular on low scale supersymmetry and theories with extra space-time
dimensions. These theories give a suitable dark matter candidate whose
interactions and c... | astro-ph hep-ph | we give an overview of the possibility of glast to explore theories beyond the standard model of particle physics among the wide taxonomy we will focus in particular on low scale supersymmetry and theories with extra spacetime dimensions these theories give a suitable dark matter candidate whose interactions and compos... | [['we', 'give', 'an', 'overview', 'of', 'the', 'possibility', 'of', 'glast', 'to', 'explore', 'theories', 'beyond', 'the', 'standard', 'model', 'of', 'particle', 'physics', 'among', 'the', 'wide', 'taxonomy', 'we', 'will', 'focus', 'in', 'particular', 'on', 'low', 'scale', 'supersymmetry', 'and', 'theories', 'with', 'e... | [-0.09533451328595244, 0.19668892895149198, -0.09666235391066309, 0.16628458513878286, -0.11029174269768535, -0.15340434127751537, -0.011392205033287708, 0.3183560150398596, -0.25121051434276476, -0.37601578888810566, 0.037352132540183595, -0.2626686815952731, -0.1000874722754029, 0.19448474720844092, -0.00432021029897... |
709.1673 | Gravitational Higgs Mechanism and Massive Gravity | In arXiv:hep-th/0011245, in the context of domain wall backgrounds, it was
shown that spontaneous breaking of diffeomorphism invariance results in
gravitational Higgs mechanism. Recently in arXiv:0708.3184 't Hooft discussed
gravitational Higgs mechanism in the context of obtaining massive gravity
directly in four di... | hep-th gr-qc | in arxivhepth0011245 in the context of domain wall backgrounds it was shown that spontaneous breaking of diffeomorphism invariance results in gravitational higgs mechanism recently in arxiv07083184 t hooft discussed gravitational higgs mechanism in the context of obtaining massive gravity directly in four dimensions an... | [['in', 'arxivhepth0011245', 'in', 'the', 'context', 'of', 'domain', 'wall', 'backgrounds', 'it', 'was', 'shown', 'that', 'spontaneous', 'breaking', 'of', 'diffeomorphism', 'invariance', 'results', 'in', 'gravitational', 'higgs', 'mechanism', 'recently', 'in', 'arxiv07083184', 't', 'hooft', 'discussed', 'gravitational'... | [-0.20089019678804712, 0.24782893397024877, -0.04524082516408747, 0.11537713909846, -0.09425378749368801, -0.1822725600102872, -0.019886450496241673, 0.3049158085736313, -0.180626921413932, -0.24012511859057536, 0.07816633097605691, -0.2638388472135245, -0.12570577563851007, 0.10105046900987093, -0.02237467945087701, 0... |
709.1674 | Matrix-Lifting Semi-Definite Programming for Decoding in Multiple
Antenna Systems | This paper presents a computationally efficient decoder for multiple antenna
systems. The proposed algorithm can be used for any constellation (QAM or PSK)
and any labeling method. The decoder is based on matrix-lifting Semi-Definite
Programming (SDP). The strength of the proposed method lies in a new relaxation
algo... | cs.IT math.IT | this paper presents a computationally efficient decoder for multiple antenna systems the proposed algorithm can be used for any constellation qam or psk and any labeling method the decoder is based on matrixlifting semidefinite programming sdp the strength of the proposed method lies in a new relaxation algorithm appli... | [['this', 'paper', 'presents', 'a', 'computationally', 'efficient', 'decoder', 'for', 'multiple', 'antenna', 'systems', 'the', 'proposed', 'algorithm', 'can', 'be', 'used', 'for', 'any', 'constellation', 'qam', 'or', 'psk', 'and', 'any', 'labeling', 'method', 'the', 'decoder', 'is', 'based', 'on', 'matrixlifting', 'sem... | [-0.1513923132636895, -0.031113490254166678, -0.09181758837605064, 0.018955951863476497, -0.08475848252772156, -0.16481500011727665, 0.0965395288931728, 0.3480787695822955, -0.24391863272864034, -0.3394795940292886, 0.08178319001683232, -0.22640666738152504, -0.21249981269339155, 0.2257488441043251, -0.1099452539770440... |
709.1675 | Indirect control of the asymptotic states of a quantum dynamical
semigroup | In the dynamics of open quantum systems, the interaction with the external
environment usually leads to a contraction of the set of reachable states for
the system as time increases, eventually shrinking to a single stationary
point. In this contribution we describe to what extent it is possible to modify
this asympt... | quant-ph | in the dynamics of open quantum systems the interaction with the external environment usually leads to a contraction of the set of reachable states for the system as time increases eventually shrinking to a single stationary point in this contribution we describe to what extent it is possible to modify this asymptotic ... | [['in', 'the', 'dynamics', 'of', 'open', 'quantum', 'systems', 'the', 'interaction', 'with', 'the', 'external', 'environment', 'usually', 'leads', 'to', 'a', 'contraction', 'of', 'the', 'set', 'of', 'reachable', 'states', 'for', 'the', 'system', 'as', 'time', 'increases', 'eventually', 'shrinking', 'to', 'a', 'single',... | [-0.13862495258945273, 0.11585974956737168, -0.10478804376278375, 0.05902685535634314, -0.05451184047253903, -0.13513338876057518, 0.07459470651795257, 0.35544013861894, -0.29533138649689183, -0.28299958009124937, 0.12001894764850747, -0.23899850209960966, -0.1440634765391666, 0.2029891241329244, -0.0402196459031689, 0... |
709.1676 | What is a metric space? | The question in the title is discussed briefly, with emphasis on a few basic
examples and their properties.
| math.MG | the question in the title is discussed briefly with emphasis on a few basic examples and their properties | [['the', 'question', 'in', 'the', 'title', 'is', 'discussed', 'briefly', 'with', 'emphasis', 'on', 'a', 'few', 'basic', 'examples', 'and', 'their', 'properties']] | [-0.09521752637293604, 0.09977903760348757, 0.053325491233004466, 0.15275396642714945, -0.09165920969098806, -0.09806417547062868, 0.027324038816408977, 0.42366767343547607, -0.263085529829065, -0.27044113125238156, 0.22857732110423967, -0.3056031266330845, -0.1975731949528886, 0.27360976034671897, -0.09478607116681007... |
709.1677 | A remark on Frobenius descent for vector bundles | We give a class of examples of vector bundles on a relative smooth projective
curve over Spec Z such that for infinitely many prime reductions the bundle has
a Frobenius descent, but the restriction to the generic fiber in characteristic
zero is not semistable. In the third section of the paper we prove for a large
c... | math.AG math.AC | we give a class of examples of vector bundles on a relative smooth projective curve over spec z such that for infinitely many prime reductions the bundle has a frobenius descent but the restriction to the generic fiber in characteristic zero is not semistable in the third section of the paper we prove for a large class... | [['we', 'give', 'a', 'class', 'of', 'examples', 'of', 'vector', 'bundles', 'on', 'a', 'relative', 'smooth', 'projective', 'curve', 'over', 'spec', 'z', 'such', 'that', 'for', 'infinitely', 'many', 'prime', 'reductions', 'the', 'bundle', 'has', 'a', 'frobenius', 'descent', 'but', 'the', 'restriction', 'to', 'the', 'gene... | [-0.22250078751617489, 0.03534943421254866, -0.10801490371090335, 0.04605709058641632, -0.11287647737441836, -0.1871844260651316, -0.05435689489476735, 0.35650996308824096, -0.346574123420224, -0.13940311255990653, 0.09023936067997301, -0.19952169474768075, -0.1398737988862637, 0.2531844560006583, -0.18440201875401308,... |
709.1678 | Asymptotic integration and dispersion for hyperbolic equations | The aim of this paper is to establish time decay properties and dispersive
estimates for strictly hyperbolic equations with homogeneous symbols and with
time-dependent coefficients whose derivatives are integrable. For this purpose,
the method of asymptotic integration is developed for such equations and
representati... | math.AP math.FA | the aim of this paper is to establish time decay properties and dispersive estimates for strictly hyperbolic equations with homogeneous symbols and with timedependent coefficients whose derivatives are integrable for this purpose the method of asymptotic integration is developed for such equations and representation fo... | [['the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'establish', 'time', 'decay', 'properties', 'and', 'dispersive', 'estimates', 'for', 'strictly', 'hyperbolic', 'equations', 'with', 'homogeneous', 'symbols', 'and', 'with', 'timedependent', 'coefficients', 'whose', 'derivatives', 'are', 'integrable', 'for', 'this', 'pu... | [-0.11479565039252405, 0.07144467229848891, -0.10658124160169569, 0.08662424612148906, -0.07736849248261246, -0.09650708391756707, -0.0009207005307251057, 0.3123276574623506, -0.2753011020800925, -0.24439084367049452, 0.1642101044166796, -0.2828026565827972, -0.11721424208892299, 0.2302044364650709, -0.0064373911336829... |
709.1679 | The extremal values of the Wiener index of a tree with given degree
sequence | The Wiener index of a graph is the sum of the distances between all pairs of
vertices, it has been one of the main descriptors that correlate achemical
compound's molecular graph with experimentally gathered data regarding the
compound's characteristics. The tree that minimizes the Wiener index among
trees of given m... | math.CO | the wiener index of a graph is the sum of the distances between all pairs of vertices it has been one of the main descriptors that correlate achemical compounds molecular graph with experimentally gathered data regarding the compounds characteristics the tree that minimizes the wiener index among trees of given maximal... | [['the', 'wiener', 'index', 'of', 'a', 'graph', 'is', 'the', 'sum', 'of', 'the', 'distances', 'between', 'all', 'pairs', 'of', 'vertices', 'it', 'has', 'been', 'one', 'of', 'the', 'main', 'descriptors', 'that', 'correlate', 'achemical', 'compounds', 'molecular', 'graph', 'with', 'experimentally', 'gathered', 'data', 'r... | [-0.1477680938216309, 0.1397603751759823, -0.06837127055360438, 0.042436290393608994, -0.07588266208129998, -0.07439915030199575, 0.0797406949680171, 0.3938747662381103, -0.2892241197804066, -0.31825138026312605, 0.04986883981523346, -0.3585972336618459, -0.18696339550900132, 0.12169586937262179, -0.07473476273199059, ... |
709.168 | Towards new background independent representations for Loop Quantum
Gravity | Recently, uniqueness theorems were constructed for the representation used in
Loop Quantum Gravity. We explore the existence of alternate representations by
weakening the assumptions of the so called LOST uniqueness theorem. The
weakened assumptions seem physically reasonable and retain the key requirement
of explici... | gr-qc | recently uniqueness theorems were constructed for the representation used in loop quantum gravity we explore the existence of alternate representations by weakening the assumptions of the so called lost uniqueness theorem the weakened assumptions seem physically reasonable and retain the key requirement of explicit bac... | [['recently', 'uniqueness', 'theorems', 'were', 'constructed', 'for', 'the', 'representation', 'used', 'in', 'loop', 'quantum', 'gravity', 'we', 'explore', 'the', 'existence', 'of', 'alternate', 'representations', 'by', 'weakening', 'the', 'assumptions', 'of', 'the', 'so', 'called', 'lost', 'uniqueness', 'theorem', 'th... | [-0.1267830497135633, 0.09752308700137355, -0.10664381978005685, 0.15491235484208526, -0.14653706425351315, -0.15593703165008077, 0.05148372800061319, 0.3257904801967329, -0.22372915931367154, -0.2732157299038151, 0.10522780903607029, -0.17131240049714286, -0.10084932366514514, 0.1166772481921161, -0.11474812743735724,... |
709.1681 | Fractional dynamical systems and applications in mechanics and economics | Using the fractional integration and differentiation on R we build the
fractional jet fibre bundle on a differentiable manifold and we emphasize some
important geometrical objects. Euler-Lagrange fractional equations are
described. Some significant examples from mechanics and economics are
presented.
| math.DS math.DG | using the fractional integration and differentiation on r we build the fractional jet fibre bundle on a differentiable manifold and we emphasize some important geometrical objects eulerlagrange fractional equations are described some significant examples from mechanics and economics are presented | [['using', 'the', 'fractional', 'integration', 'and', 'differentiation', 'on', 'r', 'we', 'build', 'the', 'fractional', 'jet', 'fibre', 'bundle', 'on', 'a', 'differentiable', 'manifold', 'and', 'we', 'emphasize', 'some', 'important', 'geometrical', 'objects', 'eulerlagrange', 'fractional', 'equations', 'are', 'describe... | [-0.1313202324556187, 0.004845837666653097, -0.060610773239750414, 0.12554587854538113, -0.1679100416833535, -0.1395031624357216, -0.061774570366833356, 0.40321921748109163, -0.2769358734134585, -0.2672248930670321, 0.17202126083429903, -0.2655876215576427, -0.21163988253101707, 0.21808297075331212, -0.1740582252619788... |
709.1682 | Quantum risk-sensitive estimation and robustness | This paper studies a quantum risk-sensitive estimation problem and
investigates robustness properties of the filter. This is a direct extension to
the quantum case of analogous classical results. All investigations are based
on a discrete approximation model of the quantum system under consideration.
This allows us t... | quant-ph | this paper studies a quantum risksensitive estimation problem and investigates robustness properties of the filter this is a direct extension to the quantum case of analogous classical results all investigations are based on a discrete approximation model of the quantum system under consideration this allows us to stud... | [['this', 'paper', 'studies', 'a', 'quantum', 'risksensitive', 'estimation', 'problem', 'and', 'investigates', 'robustness', 'properties', 'of', 'the', 'filter', 'this', 'is', 'a', 'direct', 'extension', 'to', 'the', 'quantum', 'case', 'of', 'analogous', 'classical', 'results', 'all', 'investigations', 'are', 'based', ... | [-0.10096823514572212, -0.005324495404160448, -0.11196470305855785, 0.05935311574389094, -0.07803097330699009, -0.11388153715192208, 0.0668709528565939, 0.34289781069383024, -0.2621235514325755, -0.2540722382121852, 0.12403020014587257, -0.2460474335519913, -0.25242900767230564, 0.22596437963324467, -0.1409697753743135... |
709.1683 | Failure of the displaced-squeezed state for spin-boson models in the
thermodynamic limit | We present an analysis of a variational coherent-squeezed state that has been
discussed in the literature as a potential ground state for the spin-boson
model. We show that when the system-size scaling of the spin-bath coupling is
included properly, all squeezing effects and non-universal physics vanish in
the thermo... | cond-mat.mes-hall | we present an analysis of a variational coherentsqueezed state that has been discussed in the literature as a potential ground state for the spinboson model we show that when the systemsize scaling of the spinbath coupling is included properly all squeezing effects and nonuniversal physics vanish in the thermodynamic l... | [['we', 'present', 'an', 'analysis', 'of', 'a', 'variational', 'coherentsqueezed', 'state', 'that', 'has', 'been', 'discussed', 'in', 'the', 'literature', 'as', 'a', 'potential', 'ground', 'state', 'for', 'the', 'spinboson', 'model', 'we', 'show', 'that', 'when', 'the', 'systemsize', 'scaling', 'of', 'the', 'spinbath',... | [-0.11928440568347771, 0.18798296197802605, -0.10077972937064866, 0.10926384903024883, 0.0007775324645141761, -0.10295952362318833, 0.034389073047786954, 0.35372830179830395, -0.2301197801157832, -0.22507871783648928, 0.07773693156273415, -0.3077123753602306, -0.12180260744566719, 0.16642715949875614, 0.018701592056701... |
709.1684 | Thermal Charm Production in Quark-Gluon Plasma at LHC | Charm production from the quark-gluon plasma created in the midrapidity of
central heavy ion collisions at the Large Hadron Collider (LHC) is studied in
the next-to-leading order in QCD. Using a schematic longitudinally
boost-invariant and transversally expanding fire-cylinder model, we find that
charm production cou... | nucl-th hep-ph | charm production from the quarkgluon plasma created in the midrapidity of central heavy ion collisions at the large hadron collider lhc is studied in the nexttoleading order in qcd using a schematic longitudinally boostinvariant and transversally expanding firecylinder model we find that charm production could be appre... | [['charm', 'production', 'from', 'the', 'quarkgluon', 'plasma', 'created', 'in', 'the', 'midrapidity', 'of', 'central', 'heavy', 'ion', 'collisions', 'at', 'the', 'large', 'hadron', 'collider', 'lhc', 'is', 'studied', 'in', 'the', 'nexttoleading', 'order', 'in', 'qcd', 'using', 'a', 'schematic', 'longitudinally', 'boos... | [-0.01788485801944712, 0.35300697898492217, -0.16958355216659826, 0.10729469266019319, 0.032686173233507886, -0.07738088429121688, -0.03582527321569695, 0.330666597840367, -0.19889224123320368, -0.2049574425978826, -0.0258859077210326, -0.33305372066316336, 0.15681600069055462, 0.12940133233683757, 0.10042439403916055,... |
709.1685 | Entropies for complex systems: generalized-generalized entropies | Many complex systems are characterized by non-Boltzmann distribution
functions of their statistical variables. If one wants to -- justified or not
-- hold on to the maximum entropy principle for complex statistical systems
(non-Boltzmann) we demonstrate how the corresponding entropy has to look like,
given the form o... | cond-mat.stat-mech | many complex systems are characterized by nonboltzmann distribution functions of their statistical variables if one wants to justified or not hold on to the maximum entropy principle for complex statistical systems nonboltzmann we demonstrate how the corresponding entropy has to look like given the form of the correspo... | [['many', 'complex', 'systems', 'are', 'characterized', 'by', 'nonboltzmann', 'distribution', 'functions', 'of', 'their', 'statistical', 'variables', 'if', 'one', 'wants', 'to', 'justified', 'or', 'not', 'hold', 'on', 'to', 'the', 'maximum', 'entropy', 'principle', 'for', 'complex', 'statistical', 'systems', 'nonboltzm... | [-0.0814739168257169, 0.1302338327706346, -0.1488294461256136, 0.1630149889109737, -0.032875233759050784, -0.1840618734490936, 0.01831270819529891, 0.2946465407862611, -0.270602134971515, -0.24575374101734032, 0.08582689627579859, -0.3032851761328461, -0.07519939737191991, 0.2005080640396994, -0.08541520669570436, 0.09... |
709.1686 | Colliding Stellar Wind Models with Nonequilibrium Ionization: X-rays
from WR 147 | The effects of nonequilibrium ionization are explicitly taken into account in
a numerical model which describes colliding stellar winds (CSW) in massive
binary sytems. This new model is used to analyze the most recent X-ray spectra
of the WR+OB binary system WR 147. The basic result is that it can adequately
reproduc... | astro-ph | the effects of nonequilibrium ionization are explicitly taken into account in a numerical model which describes colliding stellar winds csw in massive binary sytems this new model is used to analyze the most recent xray spectra of the wrob binary system wr 147 the basic result is that it can adequately reproduce the ob... | [['the', 'effects', 'of', 'nonequilibrium', 'ionization', 'are', 'explicitly', 'taken', 'into', 'account', 'in', 'a', 'numerical', 'model', 'which', 'describes', 'colliding', 'stellar', 'winds', 'csw', 'in', 'massive', 'binary', 'sytems', 'this', 'new', 'model', 'is', 'used', 'to', 'analyze', 'the', 'most', 'recent', '... | [-0.0749830351966257, 0.17139306772387009, -0.052475262236957615, 0.1252826733709741, -0.05893856393727096, -0.11651364325268848, 0.027173087114115823, 0.3838525860192808, -0.19381621080589154, -0.37104128258856567, 0.06046615407449772, -0.25260206141282576, -0.0299062608828142, 0.1965476355100101, -0.05081868198247173... |
709.1687 | Co/Nb/Co low field superconducting spin switch | We report experiments on a superconducting spin switch based on
technologically relevant materials as elemental ferromagnetic Co and elemental
superconducting Nb. The Co/Nb/Co structure exhibits inverse spin switch effect,
can be operated at liquid helium temperature and can switch from
superconductive to normal stat... | cond-mat.supr-con | we report experiments on a superconducting spin switch based on technologically relevant materials as elemental ferromagnetic co and elemental superconducting nb the conbco structure exhibits inverse spin switch effect can be operated at liquid helium temperature and can switch from superconductive to normal state in r... | [['we', 'report', 'experiments', 'on', 'a', 'superconducting', 'spin', 'switch', 'based', 'on', 'technologically', 'relevant', 'materials', 'as', 'elemental', 'ferromagnetic', 'co', 'and', 'elemental', 'superconducting', 'nb', 'the', 'conbco', 'structure', 'exhibits', 'inverse', 'spin', 'switch', 'effect', 'can', 'be',... | [-0.1392814165867296, 0.2849196672258485, 0.005788009180428667, 0.013147129754846295, -0.06439472592642738, -0.19344305782578886, 0.10866160454396676, 0.4156155415500204, -0.2388961016614404, -0.3076984270850921, 0.052886312683565646, -0.26961167125652236, -0.05785589333067441, 0.2546114816375646, 0.09711429179878905, ... |
709.1688 | The Generalized Burnside Theorem | All groups have 2 generators. For every prime power q, the Generalized
Burnside Theorem (Theorem GB) produces an infinite number of solvable groups,
Some, such as groups of a prime power exponent, have only elements of finite
order and are therefore finite groups. Others have elements of infinite order
and are thus i... | math.GR | all groups have 2 generators for every prime power q the generalized burnside theorem theorem gb produces an infinite number of solvable groups some such as groups of a prime power exponent have only elements of finite order and are therefore finite groups others have elements of infinite order and are thus infinite gr... | [['all', 'groups', 'have', '2', 'generators', 'for', 'every', 'prime', 'power', 'q', 'the', 'generalized', 'burnside', 'theorem', 'theorem', 'gb', 'produces', 'an', 'infinite', 'number', 'of', 'solvable', 'groups', 'some', 'such', 'as', 'groups', 'of', 'a', 'prime', 'power', 'exponent', 'have', 'only', 'elements', 'of'... | [-0.2060447157404962, 0.21657150554338364, -0.109099530014646, 0.0647160034416066, -0.07760234684835832, -0.186104693566449, 0.0011481005210606824, 0.3740675003223476, -0.2885542805528357, -0.2733251837836135, 0.1381040100629131, -0.3329664340486661, -0.058624898338513004, 0.2420864344818429, -0.05291461657976643, 0.00... |
709.1689 | Seifert surfaces, Commutators and Vassiliev invariants | We show that the Vassiliev invariants of a knot K, are obstructions to
finding a regular Seifert surface, S, whose complement looks "simple" (e.g.
like the complement of a disc) to the lower central series of its fundamental
group.
| math.GT math.QA | we show that the vassiliev invariants of a knot k are obstructions to finding a regular seifert surface s whose complement looks simple eg like the complement of a disc to the lower central series of its fundamental group | [['we', 'show', 'that', 'the', 'vassiliev', 'invariants', 'of', 'a', 'knot', 'k', 'are', 'obstructions', 'to', 'finding', 'a', 'regular', 'seifert', 'surface', 's', 'whose', 'complement', 'looks', 'simple', 'eg', 'like', 'the', 'complement', 'of', 'a', 'disc', 'to', 'the', 'lower', 'central', 'series', 'of', 'its', 'fu... | [-0.24483740420486683, 0.05120690226650391, -0.16512043210558403, 0.060331072276219345, -0.1519460049099647, -0.14876144885634765, 0.05542948476982136, 0.3080450993699905, -0.321044362985935, -0.29238111990241283, 0.1060736163949164, -0.26460654011521584, -0.16953904105302614, 0.21616881263131896, -0.12588655564169854,... |
709.169 | Equilibrium and dynamics of a trapped superfluid Fermi gas with unequal
masses | Interacting Fermi gases with equal populations but unequal masses are
investigated at zero temperature using local density approximation and the
hydrodynamic theory of superfluids in the presence of harmonic trapping.
We derive the conditions of energetic stability of the superfluid
configuration with respect to ph... | cond-mat.soft cond-mat.supr-con | interacting fermi gases with equal populations but unequal masses are investigated at zero temperature using local density approximation and the hydrodynamic theory of superfluids in the presence of harmonic trapping we derive the conditions of energetic stability of the superfluid configuration with respect to phase s... | [['interacting', 'fermi', 'gases', 'with', 'equal', 'populations', 'but', 'unequal', 'masses', 'are', 'investigated', 'at', 'zero', 'temperature', 'using', 'local', 'density', 'approximation', 'and', 'the', 'hydrodynamic', 'theory', 'of', 'superfluids', 'in', 'the', 'presence', 'of', 'harmonic', 'trapping', 'we', 'deri... | [-0.17354861315254957, 0.2432422000733283, -0.05511323385871947, 0.04610552243844969, 0.04877821067387585, -0.13935347702906672, 0.05643585859896552, 0.33711588838121903, -0.2108418004591239, -0.2734883014666177, 0.03246161719523686, -0.301543093724492, -0.04472886879486426, 0.15454096772700107, 0.06140192875824079, 0.... |
709.1691 | Microwave response of a cylindrical cavity made of bulk MgB2
superconductor | We report on the microwave properties of a resonant cylindrical cavity made
of bulk MgB2 superconductor, produced by the reactive liquid Mg infiltration
process. The frequency response of the cavity has been measured in the range
5-13GHz. Among the various modes, the TE011, resonating at 9.79GHz, exhibits
the highest... | cond-mat.supr-con | we report on the microwave properties of a resonant cylindrical cavity made of bulk mgb2 superconductor produced by the reactive liquid mg infiltration process the frequency response of the cavity has been measured in the range 513ghz among the various modes the te011 resonating at 979ghz exhibits the highest quality f... | [['we', 'report', 'on', 'the', 'microwave', 'properties', 'of', 'a', 'resonant', 'cylindrical', 'cavity', 'made', 'of', 'bulk', 'mgb2', 'superconductor', 'produced', 'by', 'the', 'reactive', 'liquid', 'mg', 'infiltration', 'process', 'the', 'frequency', 'response', 'of', 'the', 'cavity', 'has', 'been', 'measured', 'in'... | [-0.10672069656097197, 0.15438502133474685, -0.04626520509814976, -0.08148200116704629, 0.007569610989386482, -0.07840733132824036, 0.06365981925773667, 0.3776374854080911, -0.20891179615032993, -0.35267544561065733, 0.037637823520136796, -0.2972369167421545, -0.0037356476469929995, 0.2400260150898248, 0.02949950947160... |
709.1692 | Precision photometric redshift calibration for galaxy-galaxy weak
lensing | Accurate photometric redshifts are among the key requirements for precision
weak lensing measurements. Both the large size of the Sloan Digital Sky Survey
(SDSS) and the existence of large spectroscopic redshift samples that are
flux-limited beyond its depth have made it the optimal data source for
developing methods... | astro-ph | accurate photometric redshifts are among the key requirements for precision weak lensing measurements both the large size of the sloan digital sky survey sdss and the existence of large spectroscopic redshift samples that are fluxlimited beyond its depth have made it the optimal data source for developing methods to pr... | [['accurate', 'photometric', 'redshifts', 'are', 'among', 'the', 'key', 'requirements', 'for', 'precision', 'weak', 'lensing', 'measurements', 'both', 'the', 'large', 'size', 'of', 'the', 'sloan', 'digital', 'sky', 'survey', 'sdss', 'and', 'the', 'existence', 'of', 'large', 'spectroscopic', 'redshift', 'samples', 'that... | [-0.035378848237938076, 0.02780242345363128, -0.06866356161575297, 0.13488351126792822, -0.10940693397722968, -0.06818717141625093, 0.05439140492857225, 0.4396860133856535, -0.2130746865545899, -0.3506876247626917, 0.1059043344952159, -0.3158763679275165, -0.06567062820775342, 0.25026770170066265, -0.05278654097660866,... |
709.1693 | Discovery of the accretion-powered millisecond pulsar SWIFT J1756.9-2508
with a low-mass companion | We report on the discovery by the Swift Gamma-Ray Burst Explorer of the
eighth known transient accretion-powered millisecond pulsar, SWIFT
J1756.9-2508, as part of routine observations with the Swift Burst Alert
Telescope hard X-ray transient monitor. The pulsar was subsequently observed by
both the X-Ray Telescope o... | astro-ph | we report on the discovery by the swift gammaray burst explorer of the eighth known transient accretionpowered millisecond pulsar swift j175692508 as part of routine observations with the swift burst alert telescope hard xray transient monitor the pulsar was subsequently observed by both the xray telescope on swift and... | [['we', 'report', 'on', 'the', 'discovery', 'by', 'the', 'swift', 'gammaray', 'burst', 'explorer', 'of', 'the', 'eighth', 'known', 'transient', 'accretionpowered', 'millisecond', 'pulsar', 'swift', 'j175692508', 'as', 'part', 'of', 'routine', 'observations', 'with', 'the', 'swift', 'burst', 'alert', 'telescope', 'hard'... | [-0.0938705899498864, 0.20834191968107155, -0.026877131317146554, 0.12662767060913233, -0.14950995025668987, -0.09511190570544364, 0.11703644544197528, 0.41342560833639486, -0.11494585816737611, -0.4158248312386879, 0.1505852167969732, -0.39048463192790056, -0.010966744613671286, 0.2821615822356043, -0.0584670576851728... |
709.1694 | Successful ToO triggers on the extragalactic sources with the MAGIC
telescope | The MAGIC collaboration has been performing Target of Opportunity (ToO)
observations whenever alerted that known or potential very high energy
gamma-ray emitting extragalactic sources were in a high flux state in the
optical, X-ray band or/and in the TeV energy range. Here we report on MAGIC
observations performed af... | astro-ph | the magic collaboration has been performing target of opportunity too observations whenever alerted that known or potential very high energy gammaray emitting extragalactic sources were in a high flux state in the optical xray band orand in the tev energy range here we report on magic observations performed after such ... | [['the', 'magic', 'collaboration', 'has', 'been', 'performing', 'target', 'of', 'opportunity', 'too', 'observations', 'whenever', 'alerted', 'that', 'known', 'or', 'potential', 'very', 'high', 'energy', 'gammaray', 'emitting', 'extragalactic', 'sources', 'were', 'in', 'a', 'high', 'flux', 'state', 'in', 'the', 'optical... | [-0.051375436061061916, 0.15234140565735288, -0.04144158865092322, 0.14778672018437647, -0.08437264214735478, -0.12993313611368648, 0.07287073238985613, 0.5273048037663102, -0.11225778406951577, -0.44971999172121285, 0.12370167674380354, -0.33331567092100156, -0.020226607492077164, 0.21321110541175586, 0.01718041049316... |
709.1695 | Dynamics of surface solitons at the edge of chirped optical lattices | We address soliton formation at the edge of chirped optical lattices
imprinted in Kerr-type nonlinear media. We find families of power thresholdless
surface waves that do not exist at other types of lattice interfaces. Such
solitons form due to combined action of internal reflection at the interface,
distributed Brag... | physics.optics nlin.PS | we address soliton formation at the edge of chirped optical lattices imprinted in kerrtype nonlinear media we find families of power thresholdless surface waves that do not exist at other types of lattice interfaces such solitons form due to combined action of internal reflection at the interface distributed braggtype ... | [['we', 'address', 'soliton', 'formation', 'at', 'the', 'edge', 'of', 'chirped', 'optical', 'lattices', 'imprinted', 'in', 'kerrtype', 'nonlinear', 'media', 'we', 'find', 'families', 'of', 'power', 'thresholdless', 'surface', 'waves', 'that', 'do', 'not', 'exist', 'at', 'other', 'types', 'of', 'lattice', 'interfaces', ... | [-0.18551141062535617, 0.18819451912057092, -0.056010324655600435, 0.038628143829111825, -0.0994333161450014, -0.19660955101887628, 0.013198464393343141, 0.48105575252188054, -0.2826542567075571, -0.23169160295823, 0.08959333368480524, -0.305726666968861, -0.14790698019333365, 0.17922151173470632, 0.022960451795015394,... |
709.1696 | A Generic Rate Equation for modeling Enzymatic Reactions under Living
Conditions | Based on our experience in kinetic modeling of coupled multiple metabolic
pathways we propose a generic rate equation for the dynamical modeling of
metabolic kinetics. Its symmetric form makes the kinetic parameters (or
functions) easy to relate to values in database and to use in computation. In
addition, such form ... | q-bio.MN q-bio.QM | based on our experience in kinetic modeling of coupled multiple metabolic pathways we propose a generic rate equation for the dynamical modeling of metabolic kinetics its symmetric form makes the kinetic parameters or functions easy to relate to values in database and to use in computation in addition such form is work... | [['based', 'on', 'our', 'experience', 'in', 'kinetic', 'modeling', 'of', 'coupled', 'multiple', 'metabolic', 'pathways', 'we', 'propose', 'a', 'generic', 'rate', 'equation', 'for', 'the', 'dynamical', 'modeling', 'of', 'metabolic', 'kinetics', 'its', 'symmetric', 'form', 'makes', 'the', 'kinetic', 'parameters', 'or', '... | [-0.09867343862330721, 0.11353064608016622, -0.046565448234633225, 0.07182989592359762, -0.07141446730782909, -0.12658744073762077, 0.05272816767495486, 0.3539018455306969, -0.314286618838988, -0.27887934458351904, 0.029157782085202335, -0.23974878177227033, -0.20446857235736154, 0.20899990163630836, -0.015920712664909... |
709.1697 | Enhanced soliton interactions by inhomogeneous nonlocality and
nonlinearity | We address the interactions between optical solitons in the system with
longitudinally varying nonlocality degree and nonlinearity strength. We
consider a physical model describing light propagation in nematic liquid
crystals featuring a strongly nonlocal nonlinear response. We reveal that the
variation of the nonloc... | nlin.PS physics.optics | we address the interactions between optical solitons in the system with longitudinally varying nonlocality degree and nonlinearity strength we consider a physical model describing light propagation in nematic liquid crystals featuring a strongly nonlocal nonlinear response we reveal that the variation of the nonlocalit... | [['we', 'address', 'the', 'interactions', 'between', 'optical', 'solitons', 'in', 'the', 'system', 'with', 'longitudinally', 'varying', 'nonlocality', 'degree', 'and', 'nonlinearity', 'strength', 'we', 'consider', 'a', 'physical', 'model', 'describing', 'light', 'propagation', 'in', 'nematic', 'liquid', 'crystals', 'fe... | [-0.2186886623856567, 0.17555276697412842, -0.06649981452695404, 0.04476355604738707, -0.08855150629367148, -0.18893059719620006, -0.01543473658107576, 0.38559345184337523, -0.3093759207853249, -0.25455944264041525, 0.04254025963711597, -0.29407184298726774, -0.1588508616157231, 0.14362609232554124, 0.02652391570487192... |
709.1698 | Observation of the Semileptonic Decays B --> D* tau nubar and Evidence
for B --> D tau nubar | We present measurements of the semileptonic decays B- --> D0 tau- nubar, B-
--> D*0 tau- nubar, B0bar --> D+ tau- nubar, and B0bar --> D*+ tau- nubar,
which are potentially sensitive to non--Standard Model amplitudes. The data
sample comprises 232x10^6 Upsilon(4S) --> BBbar decays collected with the BaBar
detector. F... | hep-ex | we present measurements of the semileptonic decays b d0 tau nubar b d0 tau nubar b0bar d tau nubar and b0bar d tau nubar which are potentially sensitive to nonstandard model amplitudes the data sample comprises 232x106 upsilon4s bbbar decays collected with the babar detector from a combined fit to b and b0bar channels ... | [['we', 'present', 'measurements', 'of', 'the', 'semileptonic', 'decays', 'b', 'd0', 'tau', 'nubar', 'b', 'd0', 'tau', 'nubar', 'b0bar', 'd', 'tau', 'nubar', 'and', 'b0bar', 'd', 'tau', 'nubar', 'which', 'are', 'potentially', 'sensitive', 'to', 'nonstandard', 'model', 'amplitudes', 'the', 'data', 'sample', 'comprises',... | [-0.09651224200423786, 0.2803572617770954, -0.0068156331370788055, 0.0674323143715831, -0.027313015964310402, -0.23659761234497032, 0.19512303254631316, 0.20515627547263585, -0.21505822380469447, -0.26046962470843876, -0.07480706215632715, -0.5349542147041052, 0.17900490806834107, 0.13132756217329325, 0.086323403036114... |
709.1699 | Efficient Tabling Mechanisms for Transaction Logic Programs | In this paper we present efficient evaluation algorithms for the Horn
Transaction Logic (a generalization of the regular Horn logic programs with
state updates). We present two complementary methods for optimizing the
implementation of Transaction Logic. The first method is based on tabling and
we modified the proof ... | cs.LO cs.AI | in this paper we present efficient evaluation algorithms for the horn transaction logic a generalization of the regular horn logic programs with state updates we present two complementary methods for optimizing the implementation of transaction logic the first method is based on tabling and we modified the proof theory... | [['in', 'this', 'paper', 'we', 'present', 'efficient', 'evaluation', 'algorithms', 'for', 'the', 'horn', 'transaction', 'logic', 'a', 'generalization', 'of', 'the', 'regular', 'horn', 'logic', 'programs', 'with', 'state', 'updates', 'we', 'present', 'two', 'complementary', 'methods', 'for', 'optimizing', 'the', 'implem... | [-0.10810655043261118, 0.046373921472548436, -0.09745172858926747, 0.06179309131465272, -0.11207053647376597, -0.135767529941443, 0.09774301470083398, 0.35428637216875064, -0.2723723182999185, -0.2997451875993442, 0.1345528572089318, -0.27713482770597714, -0.13139488689392145, 0.1815829148945482, -0.06880899489420586, ... |
709.17 | Finite temperature Mott transition in Hubbard model on anisotropic
triangular lattice | We investigate the Hubbard model on the anisotropic triangular lattice by
means of the cellular dynamical mean field theory. The phase diagram determined
in the Hubbard interaction versus temperature plane shows novel reentrant
behavior in the Mott transition due to the competition between Fermi-liquid
formation and ... | cond-mat.str-el | we investigate the hubbard model on the anisotropic triangular lattice by means of the cellular dynamical mean field theory the phase diagram determined in the hubbard interaction versus temperature plane shows novel reentrant behavior in the mott transition due to the competition between fermiliquid formation and magn... | [['we', 'investigate', 'the', 'hubbard', 'model', 'on', 'the', 'anisotropic', 'triangular', 'lattice', 'by', 'means', 'of', 'the', 'cellular', 'dynamical', 'mean', 'field', 'theory', 'the', 'phase', 'diagram', 'determined', 'in', 'the', 'hubbard', 'interaction', 'versus', 'temperature', 'plane', 'shows', 'novel', 'reen... | [-0.1904126941517461, 0.22983545017150508, -0.07126247145646772, 0.06552321428293967, -0.03341590654854844, -0.1467497703731181, 0.07476532631462997, 0.37379151014248274, -0.26056860718730984, -0.26478961061734657, -0.006635615242306481, -0.3036971011186962, -0.22557480662287055, 0.10159222387055589, 0.0399977058027084... |
709.1701 | Enrichment of Qualitative Beliefs for Reasoning under Uncertainty | This paper deals with enriched qualitative belief functions for reasoning
under uncertainty and for combining information expressed in natural language
through linguistic labels. In this work, two possible enrichments (quantitative
and/or qualitative) of linguistic labels are considered and operators
(addition, multi... | cs.AI | this paper deals with enriched qualitative belief functions for reasoning under uncertainty and for combining information expressed in natural language through linguistic labels in this work two possible enrichments quantitative andor qualitative of linguistic labels are considered and operators addition multiplication... | [['this', 'paper', 'deals', 'with', 'enriched', 'qualitative', 'belief', 'functions', 'for', 'reasoning', 'under', 'uncertainty', 'and', 'for', 'combining', 'information', 'expressed', 'in', 'natural', 'language', 'through', 'linguistic', 'labels', 'in', 'this', 'work', 'two', 'possible', 'enrichments', 'quantitative',... | [-0.076998895235275, 0.09252842964999604, -0.05884249151656122, 0.13250919351297796, -0.14352684912243577, -0.12390923157553048, 0.059111284287505304, 0.4266716978879589, -0.25410230383841376, -0.2882919971012708, 0.023542046649945955, -0.2799141235126599, -0.14791950459281603, 0.1667797981909561, -0.134664986267065, 0... |
709.1702 | High-spin structure and Band Termination in $^{103}$Cd | Excited states of the neutron deficient $^{103}$Cd nucleus have been
investigated via the $^{72}$Ge($^{35}$Cl, p3n) reaction at beam energy of 135
MeV by use of in-beam spectroscopic methods. Gamma rays depopulating the
excited states were detected using the Gammasphere spectrometer with high-fold
$\gamma$-ray coinci... | nucl-ex | excited states of the neutron deficient 103cd nucleus have been investigated via the 72ge35cl p3n reaction at beam energy of 135 mev by use of inbeam spectroscopic methods gamma rays depopulating the excited states were detected using the gammasphere spectrometer with highfold gammaray coincidences a quadrupole gammara... | [['excited', 'states', 'of', 'the', 'neutron', 'deficient', '103cd', 'nucleus', 'have', 'been', 'investigated', 'via', 'the', '72ge35cl', 'p3n', 'reaction', 'at', 'beam', 'energy', 'of', '135', 'mev', 'by', 'use', 'of', 'inbeam', 'spectroscopic', 'methods', 'gamma', 'rays', 'depopulating', 'the', 'excited', 'states', '... | [-0.07033800511436432, 0.18286227186447676, -0.04654016777153314, 0.11304839003213195, 0.00876280809415844, -0.13286444277695889, 0.07606201360087092, 0.4179510567454422, -0.1784999587883552, -0.34719928796988847, -0.0168833832546436, -0.3114557005875047, 0.019648729322724184, 0.1439189761928312, 0.08750876245299741, 0... |
709.1703 | Existence, uniqueness and approximation of a stochastic Schr\"odinger
equation: the diffusive case | Recent developments in quantum physics make heavy use of so-called "quantum
trajectories." Mathematically, this theory gives rise to "stochastic
Schr\"odinger equations", that is, perturbation of Schr\"odinger-type equations
under the form of stochastic differential equations. But such equations are in
general not of... | math.PR math-ph math.MP quant-ph | recent developments in quantum physics make heavy use of socalled quantum trajectories mathematically this theory gives rise to stochastic schrodinger equations that is perturbation of schrodingertype equations under the form of stochastic differential equations but such equations are in general not of the usual type a... | [['recent', 'developments', 'in', 'quantum', 'physics', 'make', 'heavy', 'use', 'of', 'socalled', 'quantum', 'trajectories', 'mathematically', 'this', 'theory', 'gives', 'rise', 'to', 'stochastic', 'schrodinger', 'equations', 'that', 'is', 'perturbation', 'of', 'schrodingertype', 'equations', 'under', 'the', 'form', 'o... | [-0.1428065332338002, 0.06231704620053855, -0.09329216487561845, 0.09133625547950558, -0.08774952925135934, -0.1334805441603852, 0.000365167531578582, 0.2525282743258205, -0.27173696681894965, -0.22941926303433208, 0.10626880554160542, -0.2679287249722132, -0.18143768848215297, 0.19777230432302487, -0.0829122923996027,... |
709.1704 | Quantum simulation of the single-particle Schrodinger equation | The working of a quantum computer is described in the concrete example of a
quantum simulator of the single-particle Schrodinger equation. We show that a
register of 6-10 qubits is sufficient to realize a useful quantum simulator
capable of solving in an efficient way standard quantum mechanical problems.
| quant-ph physics.gen-ph | the working of a quantum computer is described in the concrete example of a quantum simulator of the singleparticle schrodinger equation we show that a register of 610 qubits is sufficient to realize a useful quantum simulator capable of solving in an efficient way standard quantum mechanical problems | [['the', 'working', 'of', 'a', 'quantum', 'computer', 'is', 'described', 'in', 'the', 'concrete', 'example', 'of', 'a', 'quantum', 'simulator', 'of', 'the', 'singleparticle', 'schrodinger', 'equation', 'we', 'show', 'that', 'a', 'register', 'of', '610', 'qubits', 'is', 'sufficient', 'to', 'realize', 'a', 'useful', 'qua... | [-0.1413082127692178, 0.15581349703794936, -0.09613429832582672, 0.07233505240583327, -0.0358569478460898, -0.2371822177277257, -0.01437017943438453, 0.32245154327635345, -0.23782990337349474, -0.2898664418219899, 0.022867428483247448, -0.21665262317886422, -0.18268826697021723, 0.32071512565016747, -0.0404880430238942... |
709.1705 | Charge-transfer exciton in La2CuO4 probed with resonant inelastic x-ray
scattering | We report a high-resolution resonant inelastic x-ray scattering study of
La2CuO4. A number of spectral features are identified that were not clearly
visible in earlier lower-resolution data. The momentum dependence of the
spectral weight and the dispersion of the lowest energy excitation across the
insulating gap hav... | cond-mat.str-el cond-mat.dis-nn | we report a highresolution resonant inelastic xray scattering study of la2cuo4 a number of spectral features are identified that were not clearly visible in earlier lowerresolution data the momentum dependence of the spectral weight and the dispersion of the lowest energy excitation across the insulating gap have been ... | [['we', 'report', 'a', 'highresolution', 'resonant', 'inelastic', 'xray', 'scattering', 'study', 'of', 'la2cuo4', 'a', 'number', 'of', 'spectral', 'features', 'are', 'identified', 'that', 'were', 'not', 'clearly', 'visible', 'in', 'earlier', 'lowerresolution', 'data', 'the', 'momentum', 'dependence', 'of', 'the', 'spec... | [-0.13688219598400483, 0.15579989222156038, -0.08602904515563074, 0.04080104216967428, -0.03863139407188042, -0.07885969820680148, 0.03070764005859169, 0.44910137520231513, -0.26074634953786474, -0.33304711610694, 0.02462440223428805, -0.33498420270689583, -0.0757363207997122, 0.12681832102580218, 0.056629582301824605,... |
709.1706 | Substrate-induced band gap opening in epitaxial graphene | Graphene has shown great application potentials as the host material for next
generation electronic devices. However, despite its intriguing properties, one
of the biggest hurdles for graphene to be useful as an electronic material is
its lacking of an energy gap in the electronic spectra. This, for example,
prevents... | cond-mat.mtrl-sci cond-mat.mes-hall cond-mat.str-el | graphene has shown great application potentials as the host material for next generation electronic devices however despite its intriguing properties one of the biggest hurdles for graphene to be useful as an electronic material is its lacking of an energy gap in the electronic spectra this for example prevents the use... | [['graphene', 'has', 'shown', 'great', 'application', 'potentials', 'as', 'the', 'host', 'material', 'for', 'next', 'generation', 'electronic', 'devices', 'however', 'despite', 'its', 'intriguing', 'properties', 'one', 'of', 'the', 'biggest', 'hurdles', 'for', 'graphene', 'to', 'be', 'useful', 'as', 'an', 'electronic',... | [-0.14982566567681108, 0.1042462885567996, -0.031652884132539236, -0.01528423909835207, -0.042317447721337276, -0.12914725281298162, 0.08761760042980313, 0.44672648660217723, -0.3015008794143796, -0.32497030570559826, 0.05015223245446881, -0.31971065036952495, -0.1705687768602123, 0.20658497141053278, -0.01500260964967... |
709.1707 | Magnetic Behavior of Single La$_{0.67}$Ca$_{0.33}$MnO$_3$ Nanotubes:
Surface and Shape Effects | We report magnetization experiments in two magnetically isolated
ferromagnetic nanotubes of perovskite La$_{0.67}$Ca$_{0.33}$MnO$_3$. The
results show that the magnetic anisotropy is determined by the sample shape
although the coercive field is reduced by incoherent magnetization reversal
modes. The temperature depen... | cond-mat.mes-hall cond-mat.mtrl-sci | we report magnetization experiments in two magnetically isolated ferromagnetic nanotubes of perovskite la_067ca_033mno_3 the results show that the magnetic anisotropy is determined by the sample shape although the coercive field is reduced by incoherent magnetization reversal modes the temperature dependence of the mag... | [['we', 'report', 'magnetization', 'experiments', 'in', 'two', 'magnetically', 'isolated', 'ferromagnetic', 'nanotubes', 'of', 'perovskite', 'la_067ca_033mno_3', 'the', 'results', 'show', 'that', 'the', 'magnetic', 'anisotropy', 'is', 'determined', 'by', 'the', 'sample', 'shape', 'although', 'the', 'coercive', 'field',... | [-0.15930422599080438, 0.22807930798415899, -0.048047677787276456, -0.012389543978725652, -0.04505573140055526, -0.09982660268981229, 0.0446183026275214, 0.4311734791114634, -0.22260037252642945, -0.34371380705167265, 0.06091434505138108, -0.29645962308060525, -0.06176784849159565, 0.2575395545493081, 0.059437992653864... |
709.1708 | Symplectic symmetries of 4-manifolds | A study of symplectic actions of a finite group $G$ on smooth 4-manifolds is
initiated. The central new idea is the use of $G$-equivariant
Seiberg-Witten-Taubes theory in studying the structure of the fixed-point set
of these symmetries. The main result in this paper is a complete description of
the fixed-point set s... | math.GT math.SG | a study of symplectic actions of a finite group g on smooth 4manifolds is initiated the central new idea is the use of gequivariant seibergwittentaubes theory in studying the structure of the fixedpoint set of these symmetries the main result in this paper is a complete description of the fixedpoint set structure and t... | [['a', 'study', 'of', 'symplectic', 'actions', 'of', 'a', 'finite', 'group', 'g', 'on', 'smooth', '4manifolds', 'is', 'initiated', 'the', 'central', 'new', 'idea', 'is', 'the', 'use', 'of', 'gequivariant', 'seibergwittentaubes', 'theory', 'in', 'studying', 'the', 'structure', 'of', 'the', 'fixedpoint', 'set', 'of', 'th... | [-0.20988615635963184, 0.08127101021916554, -0.10159335316353436, 0.046166409070276894, -0.10933196827692827, -0.07536411042492003, 0.016434796887741826, 0.3358540613961809, -0.2760128488229004, -0.26149607270455627, 0.11686503684752857, -0.25389596345876136, -0.19184382560527397, 0.20123455731837608, -0.15165694636890... |
709.1709 | HST Observations of Chromospheres in Metal Deficient Field Giants | HST high resolution spectra of metal-deficient field giants more than double
the stars in previous studies, span about 3 magnitudes on the red giant branch,
and sample an abundance range [Fe/H]= -1 to -3. These stars, in spite of their
age and low metallicity, possess chromospheric fluxes of Mg II (2800 Angstrom)
tha... | astro-ph | hst high resolution spectra of metaldeficient field giants more than double the stars in previous studies span about 3 magnitudes on the red giant branch and sample an abundance range feh 1 to 3 these stars in spite of their age and low metallicity possess chromospheric fluxes of mg ii 2800 angstrom that are within a f... | [['hst', 'high', 'resolution', 'spectra', 'of', 'metaldeficient', 'field', 'giants', 'more', 'than', 'double', 'the', 'stars', 'in', 'previous', 'studies', 'span', 'about', '3', 'magnitudes', 'on', 'the', 'red', 'giant', 'branch', 'and', 'sample', 'an', 'abundance', 'range', 'feh', '1', 'to', '3', 'these', 'stars', 'in... | [-0.02492961758554618, 0.15539124920169564, 0.024854704865436183, 0.10155495031873082, -0.07890964400203523, -0.09844486290168744, 0.06846516766221966, 0.4928157071003736, -0.06355269924416661, -0.38192259363557507, 0.0013980603068442334, -0.3050060986719384, 0.02748401622251017, 0.21228318376446756, -0.040507447717018... |
709.171 | Symmetries and exotic smooth structures on a $K3$ surface | Smooth and symplectic symmetries of an infinite family of distinct exotic
$K3$ surfaces are studied, and comparison with the corresponding symmetries of
the standard $K3$ is made. The action on the $K3$ lattice induced by a smooth
finite group action is shown to be strongly restricted, and as a result,
nonsmoothabili... | math.GT math.SG | smooth and symplectic symmetries of an infinite family of distinct exotic k3 surfaces are studied and comparison with the corresponding symmetries of the standard k3 is made the action on the k3 lattice induced by a smooth finite group action is shown to be strongly restricted and as a result nonsmoothability of action... | [['smooth', 'and', 'symplectic', 'symmetries', 'of', 'an', 'infinite', 'family', 'of', 'distinct', 'exotic', 'k3', 'surfaces', 'are', 'studied', 'and', 'comparison', 'with', 'the', 'corresponding', 'symmetries', 'of', 'the', 'standard', 'k3', 'is', 'made', 'the', 'action', 'on', 'the', 'k3', 'lattice', 'induced', 'by',... | [-0.23454899774589696, 0.16044678599546308, -0.08672693985888463, 0.05303207071175656, -0.1130474485958425, -0.14013882845035222, -0.023581961169838905, 0.34633962367462295, -0.2892276411716882, -0.2615469695570377, 0.12328292492331348, -0.27203971472306127, -0.15339463867613265, 0.1785674096825413, -0.0960520895150227... |
709.1711 | A Hyperelliptic View on Teichmuller Space. I | We explicitly describe the Teichmuller space TH_n of hyperelliptic surfaces
in terms of natural and effective coordinates as the space of certain
(2n-6)-tuples of distinct points on the ideal boundary of the Poincare disc. We
essentially use the concept of a simple earthquake which is a particular case
of a Fenchel-N... | math.GT | we explicitly describe the teichmuller space th_n of hyperelliptic surfaces in terms of natural and effective coordinates as the space of certain 2n6tuples of distinct points on the ideal boundary of the poincare disc we essentially use the concept of a simple earthquake which is a particular case of a fenchelnielsen t... | [['we', 'explicitly', 'describe', 'the', 'teichmuller', 'space', 'th_n', 'of', 'hyperelliptic', 'surfaces', 'in', 'terms', 'of', 'natural', 'and', 'effective', 'coordinates', 'as', 'the', 'space', 'of', 'certain', '2n6tuples', 'of', 'distinct', 'points', 'on', 'the', 'ideal', 'boundary', 'of', 'the', 'poincare', 'disc'... | [-0.16610682400129442, 0.12020692888628282, -0.1335045517870348, 0.07134468021653241, -0.11278550762027127, -0.07825302882354308, 0.005887915913320187, 0.32750949148621716, -0.29526000024762544, -0.23939003094843347, 0.1210469446396133, -0.22937444122156725, -0.20160641353438263, 0.24538679862447646, -0.136281992271729... |
709.1712 | Dissipation in intercluster plasma | We discuss dissipative processes in strongly gyrotropic, nearly collisionless
plasma in clusters of galaxies (ICM). First, we point out that Braginsky
theory, which assumes that collisions are more frequent that the system's
dynamical time scale, is inapplicable to fast, sub-viscous ICM motion. Most
importantly, the ... | astro-ph | we discuss dissipative processes in strongly gyrotropic nearly collisionless plasma in clusters of galaxies icm first we point out that braginsky theory which assumes that collisions are more frequent that the systems dynamical time scale is inapplicable to fast subviscous icm motion most importantly the electron contr... | [['we', 'discuss', 'dissipative', 'processes', 'in', 'strongly', 'gyrotropic', 'nearly', 'collisionless', 'plasma', 'in', 'clusters', 'of', 'galaxies', 'icm', 'first', 'we', 'point', 'out', 'that', 'braginsky', 'theory', 'which', 'assumes', 'that', 'collisions', 'are', 'more', 'frequent', 'that', 'the', 'systems', 'dyn... | [-0.1663249611205152, 0.2721392609100475, -0.05787236197341054, 0.0868934153625461, -0.05435250904719648, -0.0871833833123849, -0.012375852340658432, 0.35348186810207777, -0.2812948149007588, -0.2435139584052096, 0.0224404635121036, -0.2665629697828946, -0.020254800839529158, 0.20570255809250365, 0.037829931794542325, ... |
709.1713 | Millimeter Interferometric HCN(1-0) and HCO+(1-0) Observations of
Luminous Infrared Galaxies | We present the results on millimeter interferometric observations of four
luminous infrared galaxies (LIRGs), Arp 220, Mrk 231, IRAS 08572+3915, and VV
114, and one Wolf-Rayet galaxy, He 2-10, using the Nobeyama Millimeter Array
(NMA). Both the HCN(1-0) and HCO+(1-0) molecular lines were observed
simultaneously and t... | astro-ph | we present the results on millimeter interferometric observations of four luminous infrared galaxies lirgs arp 220 mrk 231 iras 085723915 and vv 114 and one wolfrayet galaxy he 210 using the nobeyama millimeter array nma both the hcn10 and hco10 molecular lines were observed simultaneously and their brightnesstemperatu... | [['we', 'present', 'the', 'results', 'on', 'millimeter', 'interferometric', 'observations', 'of', 'four', 'luminous', 'infrared', 'galaxies', 'lirgs', 'arp', '220', 'mrk', '231', 'iras', '085723915', 'and', 'vv', '114', 'and', 'one', 'wolfrayet', 'galaxy', 'he', '210', 'using', 'the', 'nobeyama', 'millimeter', 'array',... | [0.0009477084326631898, 0.03657650421130463, -0.003539939953374084, 0.11252362475087549, -0.034314474226531194, -0.08614140387825583, 0.011217326825399969, 0.5482593375173482, -0.008167154581645842, -0.33424190150849015, 0.026773844610116528, -0.3468924725893885, -0.0036998019125100905, 0.14761292311558546, 0.024163586... |
709.1714 | A GIM Mechanism from Extra Dimensions | We explore how to protect extra dimensional models from large flavor changing
neutral currents by using bulk and brane flavor symmetries. We show that a GIM
mechanism can be built in to warped space models such as Randall-Sundrum or
composite Higgs models if flavor mixing is introduced via UV brane kinetic
mixings fo... | hep-ph | we explore how to protect extra dimensional models from large flavor changing neutral currents by using bulk and brane flavor symmetries we show that a gim mechanism can be built in to warped space models such as randallsundrum or composite higgs models if flavor mixing is introduced via uv brane kinetic mixings for ri... | [['we', 'explore', 'how', 'to', 'protect', 'extra', 'dimensional', 'models', 'from', 'large', 'flavor', 'changing', 'neutral', 'currents', 'by', 'using', 'bulk', 'and', 'brane', 'flavor', 'symmetries', 'we', 'show', 'that', 'a', 'gim', 'mechanism', 'can', 'be', 'built', 'in', 'to', 'warped', 'space', 'models', 'such', ... | [-0.0583435828704387, 0.25433121927082536, 0.018644214803352953, 0.16261547429137863, -0.13660065305419267, -0.24319874686188997, 0.07094757300568745, 0.32794235308188946, -0.23001161676365883, -0.2781204061210156, 0.10421533785411156, -0.22962587997782977, -0.05572646715387236, 0.09525216647423804, -0.0320218411041423... |
709.1715 | Magnetically asymmetric interfaces in a (LaMnO$_3$)/(SrMnO$_3$)
superlattice due to structural asymmetries | Polarized neutron reflectivity measurements of a ferromagnetic
[(LaMnO$_3$)$_{11.8}$/(SrMnO$_3$)$_{4.4}$]$_6$ superlattice reveal a modulated
magnetic structure with an enhanced magnetization at the interfaces where
LaMnO$_3$ was deposited on SrMnO$_3$ (LMO/SMO). However, the opposite
interfaces (SMO/LMO) are found t... | cond-mat.mtrl-sci cond-mat.str-el | polarized neutron reflectivity measurements of a ferromagnetic lamno_3_118srmno_3_44_6 superlattice reveal a modulated magnetic structure with an enhanced magnetization at the interfaces where lamno_3 was deposited on srmno_3 lmosmo however the opposite interfaces smolmo are found to have a reduced ferromagnetic moment... | [['polarized', 'neutron', 'reflectivity', 'measurements', 'of', 'a', 'ferromagnetic', 'lamno_3_118srmno_3_44_6', 'superlattice', 'reveal', 'a', 'modulated', 'magnetic', 'structure', 'with', 'an', 'enhanced', 'magnetization', 'at', 'the', 'interfaces', 'where', 'lamno_3', 'was', 'deposited', 'on', 'srmno_3', 'lmosmo', '... | [-0.20094217564694064, 0.20744199545794778, -0.040334748277483984, 0.004967085934558147, -0.014202289256202273, -0.14896737047211203, 0.014362995393660873, 0.4644008661555343, -0.32537414098894873, -0.32005126494914293, -0.03818332531955093, -0.33341505378484726, -0.11441602689473955, 0.2134335093243524, 0.070293282104... |
709.1716 | Consistent Determination of Particle Production in p-A, d-A and A-A
Collisions using Color Glass Condensate | The success of nonviscous hydrodynamics in describing the collective flow
properties of bulk low $p_\perp$ observables at RHIC has led to the claim that
a novel form of {\it strongly coupled} Quark Gluon Plasma (sQGP) is created in
200 AGeV Au+Au collisions. This success depends strongly, however, on the
initial cond... | nucl-th | the success of nonviscous hydrodynamics in describing the collective flow properties of bulk low p_perp observables at rhic has led to the claim that a novel form of it strongly coupled quark gluon plasma sqgp is created in 200 agev auau collisions this success depends strongly however on the initial conditions assumed... | [['the', 'success', 'of', 'nonviscous', 'hydrodynamics', 'in', 'describing', 'the', 'collective', 'flow', 'properties', 'of', 'bulk', 'low', 'p_perp', 'observables', 'at', 'rhic', 'has', 'led', 'to', 'the', 'claim', 'that', 'a', 'novel', 'form', 'of', 'it', 'strongly', 'coupled', 'quark', 'gluon', 'plasma', 'sqgp', 'is... | [-0.07064725899767568, 0.2172312884215738, -0.18726380792162245, 0.09473192693651927, -0.016826330963522197, -0.10431359235799927, -0.07638993953998365, 0.3600234561928493, -0.17587104061180178, -0.2845820153186865, -0.03578019595485838, -0.3039717319804956, 0.038500654070145066, 0.1315639789962648, -0.0023001435265006... |
709.1717 | Lattice and Schroder paths with periodic boundaries | We consider paths in the plane with $(1,0),$ $(0,1),$ and $(a,b)$-steps that
start at the origin, end at height $n,$ and stay to the left of a given
non-decreasing right boundary. We show that if the boundary is periodic and has
slope at most $b/a,$ then the ordinary generating function for the number of
such paths e... | math.CO | we consider paths in the plane with 10 01 and absteps that start at the origin end at height n and stay to the left of a given nondecreasing right boundary we show that if the boundary is periodic and has slope at most ba then the ordinary generating function for the number of such paths ending at height n is algebraic... | [['we', 'consider', 'paths', 'in', 'the', 'plane', 'with', '10', '01', 'and', 'absteps', 'that', 'start', 'at', 'the', 'origin', 'end', 'at', 'height', 'n', 'and', 'stay', 'to', 'the', 'left', 'of', 'a', 'given', 'nondecreasing', 'right', 'boundary', 'we', 'show', 'that', 'if', 'the', 'boundary', 'is', 'periodic', 'and... | [-0.1322643964306662, 0.1253250993334265, -0.08458971973834899, 0.0498621183393156, -0.07678775792180077, -0.09961439985577969, 0.010597001635435506, 0.33060671282374726, -0.3429145944979463, -0.26222002945405287, 0.07868972396559633, -0.31372423610398475, -0.14993735573961514, 0.1918482792913832, -0.017426481038794246... |
709.1718 | A short-loop algorithm for quantum Monte Carlo simulations | We present an algorithmic framework for a variant of the quantum Monte Carlo
operator-loop algorithm, where non-local cluster updates are constructed in a
way that makes each individual loop smaller. The algorithm is designed to
increase simulation efficiency in cases where conventional loops become very
large, do no... | cond-mat.stat-mech cond-mat.dis-nn cond-mat.mes-hall cond-mat.mtrl-sci cond-mat.other cond-mat.soft | we present an algorithmic framework for a variant of the quantum monte carlo operatorloop algorithm where nonlocal cluster updates are constructed in a way that makes each individual loop smaller the algorithm is designed to increase simulation efficiency in cases where conventional loops become very large do not close... | [['we', 'present', 'an', 'algorithmic', 'framework', 'for', 'a', 'variant', 'of', 'the', 'quantum', 'monte', 'carlo', 'operatorloop', 'algorithm', 'where', 'nonlocal', 'cluster', 'updates', 'are', 'constructed', 'in', 'a', 'way', 'that', 'makes', 'each', 'individual', 'loop', 'smaller', 'the', 'algorithm', 'is', 'desig... | [-0.11523860270273872, 0.11027600199580774, -0.06276143524330109, 0.08478071716846898, -0.05934070563409478, -0.18911523021291943, 0.044629185500089076, 0.40697814341634514, -0.22945600470062344, -0.29897984423441815, 0.08979894560819958, -0.26247911490965636, -0.1588671132433228, 0.2293947124236729, -0.033168654209002... |
709.1719 | Mean-field conditions for percolation on finite graphs | Let G_n be a sequence of finite transitive graphs with vertex degree d=d(n)
and |G_n|=n. Denote by p^t(v,v) the return probability after t steps of the
non-backtracking random walk on G_n. We show that if p^t(v,v) has quasi-random
properties, then critical bond-percolation on G_n has a scaling window of width
n^{-1/3... | math.PR math.CO | let g_n be a sequence of finite transitive graphs with vertex degree ddn and g_nn denote by ptvv the return probability after t steps of the nonbacktracking random walk on g_n we show that if ptvv has quasirandom properties then critical bondpercolation on g_n has a scaling window of width n13 as it would on a random g... | [['let', 'g_n', 'be', 'a', 'sequence', 'of', 'finite', 'transitive', 'graphs', 'with', 'vertex', 'degree', 'ddn', 'and', 'g_nn', 'denote', 'by', 'ptvv', 'the', 'return', 'probability', 'after', 't', 'steps', 'of', 'the', 'nonbacktracking', 'random', 'walk', 'on', 'g_n', 'we', 'show', 'that', 'if', 'ptvv', 'has', 'quasi... | [-0.13525128431589992, 0.19225231098243967, -0.0811322589941097, 0.004207772176331756, -0.04099289661583801, -0.1667724561764661, 0.05432232794665844, 0.36639718683154293, -0.25421605185979523, -0.24365914770213282, 0.09639167435163858, -0.3550930167689468, -0.13794182939013946, 0.12803401449822227, -0.0906265173142663... |
709.172 | Environmentally-Driven Evolution of Simulated Cluster Galaxies | Galaxies in clusters are gas-deficient and a number of possible explanations
for this observation have been advanced, including galaxy-cluster tidal
interactions, galaxy harassment, and ISM-ICM gas stripping. In this paper, we
use a cosmological simulation of cluster formation and evolution in order to
examine this i... | astro-ph | galaxies in clusters are gasdeficient and a number of possible explanations for this observation have been advanced including galaxycluster tidal interactions galaxy harassment and ismicm gas stripping in this paper we use a cosmological simulation of cluster formation and evolution in order to examine this issue from ... | [['galaxies', 'in', 'clusters', 'are', 'gasdeficient', 'and', 'a', 'number', 'of', 'possible', 'explanations', 'for', 'this', 'observation', 'have', 'been', 'advanced', 'including', 'galaxycluster', 'tidal', 'interactions', 'galaxy', 'harassment', 'and', 'ismicm', 'gas', 'stripping', 'in', 'this', 'paper', 'we', 'use',... | [-0.10195073437153399, 0.09519092218475884, -0.09452904112934929, 0.08482037864764695, -0.09120298869104362, -0.02183619141350409, 0.02871167777002305, 0.3966821603403956, -0.21098197337214872, -0.32758061113475145, 0.05502680843632084, -0.27431423530238225, -0.06902414617840857, 0.16140835857995803, -0.019456221699097... |
709.1721 | Parallel marginalization Monte Carlo with applications to conditional
path sampling | Monte Carlo sampling methods often suffer from long correlation times.
Consequently, these methods must be run for many steps to generate an
independent sample. In this paper a method is proposed to overcome this
difficulty. The method utilizes information from rapidly equilibrating coarse
Markov chains that sample m... | stat.CO | monte carlo sampling methods often suffer from long correlation times consequently these methods must be run for many steps to generate an independent sample in this paper a method is proposed to overcome this difficulty the method utilizes information from rapidly equilibrating coarse markov chains that sample margina... | [['monte', 'carlo', 'sampling', 'methods', 'often', 'suffer', 'from', 'long', 'correlation', 'times', 'consequently', 'these', 'methods', 'must', 'be', 'run', 'for', 'many', 'steps', 'to', 'generate', 'an', 'independent', 'sample', 'in', 'this', 'paper', 'a', 'method', 'is', 'proposed', 'to', 'overcome', 'this', 'diffi... | [-0.047262054002460314, 0.1042748975692495, -0.10317512570935138, 0.09722026995766689, -0.033584953263840256, -0.12257165400420918, 0.050593809982049556, 0.4221782814930467, -0.3291047620751402, -0.32627214455210113, 0.14031574427122798, -0.2643064192824942, -0.07757795418968753, 0.21570857669062474, -0.046562185801346... |
709.1722 | Evolution of massive black holes | Supermassive black holes are nowadays believed to reside in most local
galaxies. Accretion of gas and black hole mergers play a fundamental role in
determining the two parameters defining a black hole: mass and spin. I briefly
review here some of the physical processes that are conducive to the evolution
of the massi... | astro-ph | supermassive black holes are nowadays believed to reside in most local galaxies accretion of gas and black hole mergers play a fundamental role in determining the two parameters defining a black hole mass and spin i briefly review here some of the physical processes that are conducive to the evolution of the massive bl... | [['supermassive', 'black', 'holes', 'are', 'nowadays', 'believed', 'to', 'reside', 'in', 'most', 'local', 'galaxies', 'accretion', 'of', 'gas', 'and', 'black', 'hole', 'mergers', 'play', 'a', 'fundamental', 'role', 'in', 'determining', 'the', 'two', 'parameters', 'defining', 'a', 'black', 'hole', 'mass', 'and', 'spin',... | [-0.123146695244233, 0.12713651470839976, -0.048653776716201795, 0.22026685163177348, -0.0934036747225233, -0.07983541408100643, 0.008389287640818872, 0.33619506808148847, -0.09209888277864839, -0.3423479330700797, 0.08634811861415369, -0.3554929232249993, -0.021751287293846944, 0.20516978867251326, -0.0359124919978549... |
709.1723 | Statistical properties of one-dimensional maps with critical points and
singularities | We prove that a class of one-dimensional maps with an arbitrary number of
non-degenerate critical and singular points admits an induced Markov tower with
exponential return time asymptotics. In particular the map has an absolutely
continuous invariant probability measure with exponential decay of correlations
for H\"... | math.DS | we prove that a class of onedimensional maps with an arbitrary number of nondegenerate critical and singular points admits an induced markov tower with exponential return time asymptotics in particular the map has an absolutely continuous invariant probability measure with exponential decay of correlations for holder o... | [['we', 'prove', 'that', 'a', 'class', 'of', 'onedimensional', 'maps', 'with', 'an', 'arbitrary', 'number', 'of', 'nondegenerate', 'critical', 'and', 'singular', 'points', 'admits', 'an', 'induced', 'markov', 'tower', 'with', 'exponential', 'return', 'time', 'asymptotics', 'in', 'particular', 'the', 'map', 'has', 'an',... | [-0.1533248223403984, 0.1761092651580297, -0.11449553590624574, 0.0557926430347118, -0.008386233009080937, -0.16092109320526746, 0.001287126398467003, 0.36394915630684255, -0.2918822540247694, -0.1597614057480972, 0.10167993386920066, -0.299305112120953, -0.10032710277950986, 0.17449019831466547, -0.05159411779505775, ... |
709.1724 | Effective interaction of exhausted regions in kinetics of nucleation | An effect of overlapping of exhausted regions around droplets of a new phase
is analyzed. Several approximation to take overlapping into account are
suggested. The small parameter responsible for convergence is extracted. The
multi particle effects of overlapping are described.
| cond-mat.stat-mech | an effect of overlapping of exhausted regions around droplets of a new phase is analyzed several approximation to take overlapping into account are suggested the small parameter responsible for convergence is extracted the multi particle effects of overlapping are described | [['an', 'effect', 'of', 'overlapping', 'of', 'exhausted', 'regions', 'around', 'droplets', 'of', 'a', 'new', 'phase', 'is', 'analyzed', 'several', 'approximation', 'to', 'take', 'overlapping', 'into', 'account', 'are', 'suggested', 'the', 'small', 'parameter', 'responsible', 'for', 'convergence', 'is', 'extracted', 'th... | [-0.15394146232865752, 0.18716286075396055, -0.10261598858051002, 0.11048406509798951, -0.03713612619321793, -0.10389798119431362, 0.019004068279173225, 0.32334573450498283, -0.24728145950939506, -0.31037966990843413, 0.07158508215798065, -0.23189150771941058, -0.05176992188207805, 0.1531777481228346, 0.008560854499228... |
709.1725 | Volatility return intervals analysis of the Japanese market | We investigate scaling and memory effects in return intervals between price
volatilities above a certain threshold $q$ for the Japanese stock market using
daily and intraday data sets. We find that the distribution of return intervals
can be approximated by a scaling function that depends only on the ratio
between th... | q-fin.ST cond-mat.stat-mech physics.soc-ph | we investigate scaling and memory effects in return intervals between price volatilities above a certain threshold q for the japanese stock market using daily and intraday data sets we find that the distribution of return intervals can be approximated by a scaling function that depends only on the ratio between the ret... | [['we', 'investigate', 'scaling', 'and', 'memory', 'effects', 'in', 'return', 'intervals', 'between', 'price', 'volatilities', 'above', 'a', 'certain', 'threshold', 'q', 'for', 'the', 'japanese', 'stock', 'market', 'using', 'daily', 'and', 'intraday', 'data', 'sets', 'we', 'find', 'that', 'the', 'distribution', 'of', '... | [-0.08394142980968593, 0.1346288423847732, -0.12207758399476641, 0.1650958185915479, -0.022752917815474855, -0.08601065846035044, 0.111669925891563, 0.4119188083810794, -0.2745358987692619, -0.3029873419006905, 0.14978090726657953, -0.31793683322909094, -0.11931044420214908, 0.22087842478079334, -0.07017024390511965, 0... |
709.1726 | A Haar-like Construction for the Ornstein Uhlenbeck Process | The classical Haar construction of Brownian motion uses a binary tree of
triangular wedge-shaped functions. This basis has compactness properties which
make it especially suited for certain classes of numerical algorithms. We
present a similar basis for the Ornstein-Uhlenbeck process, in which the basis
elements appr... | math.PR | the classical haar construction of brownian motion uses a binary tree of triangular wedgeshaped functions this basis has compactness properties which make it especially suited for certain classes of numerical algorithms we present a similar basis for the ornsteinuhlenbeck process in which the basis elements approach as... | [['the', 'classical', 'haar', 'construction', 'of', 'brownian', 'motion', 'uses', 'a', 'binary', 'tree', 'of', 'triangular', 'wedgeshaped', 'functions', 'this', 'basis', 'has', 'compactness', 'properties', 'which', 'make', 'it', 'especially', 'suited', 'for', 'certain', 'classes', 'of', 'numerical', 'algorithms', 'we',... | [-0.10776694416872239, 0.13913058197281877, -0.11064668430959525, 0.06520648083969967, -0.06851381999089651, -0.07361201344421515, 0.050364245104042124, 0.37327828962508947, -0.2689430055731576, -0.1978682166679877, 0.1337819294095014, -0.254929854075284, -0.1279214284285482, 0.20164799054228216, -0.02692780649761529, ... |
709.1727 | Foundations of a quantum gravity at large scales of length and its
consequences for the dynamics of cosmological expansion | We attempt to find new symmetries in the space-time structure, leading to a
modified gravitation at large length scales, which provides the foundations of
a quantum gravity at very low energies. This search begins by considering a
unified model for electrodynamics and gravitation, so that the influence of the
gravita... | gr-qc | we attempt to find new symmetries in the spacetime structure leading to a modified gravitation at large length scales which provides the foundations of a quantum gravity at very low energies this search begins by considering a unified model for electrodynamics and gravitation so that the influence of the gravitational ... | [['we', 'attempt', 'to', 'find', 'new', 'symmetries', 'in', 'the', 'spacetime', 'structure', 'leading', 'to', 'a', 'modified', 'gravitation', 'at', 'large', 'length', 'scales', 'which', 'provides', 'the', 'foundations', 'of', 'a', 'quantum', 'gravity', 'at', 'very', 'low', 'energies', 'this', 'search', 'begins', 'by', ... | [-0.14579762927754675, 0.15996060240382054, -0.10270369027866694, 0.06964386272552792, -0.061333236440676876, -0.09524745497646807, 0.019558429449991605, 0.28122214443238036, -0.24975558814715393, -0.3207875387959702, 0.04831691805269685, -0.24482746047415416, -0.05854802163495581, 0.16164819651568496, -0.0073009887592... |
709.1728 | Trouble with Physics? | This is a review of Lee Smolin's "The Trouble with Physics". The main gist of
the review is that the physics of the past three decades has been rich with new
discoveries in a large number of domains. The Standard Model, while providing a
successful framework for the electroweak and strong interactions still needs to
... | physics.hist-ph hep-th physics.gen-ph physics.pop-ph | this is a review of lee smolins the trouble with physics the main gist of the review is that the physics of the past three decades has been rich with new discoveries in a large number of domains the standard model while providing a successful framework for the electroweak and strong interactions still needs to be devel... | [['this', 'is', 'a', 'review', 'of', 'lee', 'smolins', 'the', 'trouble', 'with', 'physics', 'the', 'main', 'gist', 'of', 'the', 'review', 'is', 'that', 'the', 'physics', 'of', 'the', 'past', 'three', 'decades', 'has', 'been', 'rich', 'with', 'new', 'discoveries', 'in', 'a', 'large', 'number', 'of', 'domains', 'the', 's... | [-0.08513970579668062, 0.16842196848195204, -0.10210939304279902, 0.06481658159996519, -0.11120882509531817, -0.14765730749804346, 0.02559929704023866, 0.30770923028041314, -0.24553751159834153, -0.35407300223028515, 0.1222894921275594, -0.25153717486806804, -0.1144946078612276, 0.19001556439296818, -0.0575240390835239... |
709.1729 | Phase transition of computational power in the resource states for
one-way quantum computation | We study how heralded qubit losses during the preparation of a
two-dimensional cluster state, a universal resource state for one-way quantum
computation, affect its computational power. Above the percolation threshold we
present a polynomial-time algorithm that concentrates a universal cluster
state, using resources ... | quant-ph cond-mat.stat-mech | we study how heralded qubit losses during the preparation of a twodimensional cluster state a universal resource state for oneway quantum computation affect its computational power above the percolation threshold we present a polynomialtime algorithm that concentrates a universal cluster state using resources that scal... | [['we', 'study', 'how', 'heralded', 'qubit', 'losses', 'during', 'the', 'preparation', 'of', 'a', 'twodimensional', 'cluster', 'state', 'a', 'universal', 'resource', 'state', 'for', 'oneway', 'quantum', 'computation', 'affect', 'its', 'computational', 'power', 'above', 'the', 'percolation', 'threshold', 'we', 'present'... | [-0.12545434016466953, 0.20669160773147746, -0.06130913349495518, 0.034350123496191334, -0.01496957804970812, -0.17575988504749787, 0.1743824917564888, 0.3837011167318514, -0.29827599641452035, -0.2624505565036088, 0.0913132442562555, -0.25545744537975235, -0.10949701874858082, 0.18396797902550144, -0.02863525714936186... |
709.173 | Spin-Dependent Tunneling of Single Electrons into an Empty Quantum Dot | Using real-time charge sensing and gate pulsing techniques we measure the
ratio of the rates for tunneling into the excited and ground spin states of a
single-electron AlGaAs/GaAs quantum dot in a parallel magnetic field. We find
that the ratio decreases with increasing magnetic field until tunneling into
the excited... | cond-mat.mes-hall | using realtime charge sensing and gate pulsing techniques we measure the ratio of the rates for tunneling into the excited and ground spin states of a singleelectron algaasgaas quantum dot in a parallel magnetic field we find that the ratio decreases with increasing magnetic field until tunneling into the excited spin ... | [['using', 'realtime', 'charge', 'sensing', 'and', 'gate', 'pulsing', 'techniques', 'we', 'measure', 'the', 'ratio', 'of', 'the', 'rates', 'for', 'tunneling', 'into', 'the', 'excited', 'and', 'ground', 'spin', 'states', 'of', 'a', 'singleelectron', 'algaasgaas', 'quantum', 'dot', 'in', 'a', 'parallel', 'magnetic', 'fie... | [-0.1837169227267926, 0.25835358299082145, -0.014205328867925951, 0.01250786878275297, 0.05631810594544125, -0.17898985736246686, 0.10560744332663792, 0.39117320417426527, -0.2454638712273057, -0.30571961695871624, 0.021338177130625507, -0.281779710756382, -0.05287993595508548, 0.19154089465155266, 0.019978424621513113... |
709.1731 | Electronic transport in locally gated graphene nanoconstrictions | We have developed the combination of an etching and deposition technique that
enables the fabrication of locally gated graphene nanostructures of arbitrary
design. Employing this method, we have fabricated graphene nanoconstrictions
with local tunable transmission and characterized their electronic properties.
An ord... | cond-mat.mes-hall | we have developed the combination of an etching and deposition technique that enables the fabrication of locally gated graphene nanostructures of arbitrary design employing this method we have fabricated graphene nanoconstrictions with local tunable transmission and characterized their electronic properties an order of... | [['we', 'have', 'developed', 'the', 'combination', 'of', 'an', 'etching', 'and', 'deposition', 'technique', 'that', 'enables', 'the', 'fabrication', 'of', 'locally', 'gated', 'graphene', 'nanostructures', 'of', 'arbitrary', 'design', 'employing', 'this', 'method', 'we', 'have', 'fabricated', 'graphene', 'nanoconstricti... | [-0.16768346327880862, 0.12054607483820291, -0.05760542718693614, -0.0778206522052642, 0.022020318508148194, -0.22184906949289143, 0.07352974733803422, 0.4822501859348267, -0.2633597381785512, -0.3300218783505261, -0.027179388218792157, -0.2348136428114958, -0.17155614658724516, 0.24019546002149583, -0.0386680093221366... |
709.1732 | Many-pole model of inelastic losses in x-ray absorption spectra | Inelastic losses are crucial to a quantitative analysis of x-ray absorption
spectra. However, current treatments are semi-phenomenological in nature. Here
a first-principles, many-pole generalization of the plasmon-pole model is
developed for improved calculations of inelastic losses. The method is based on
the GW ap... | cond-mat.mtrl-sci cond-mat.other | inelastic losses are crucial to a quantitative analysis of xray absorption spectra however current treatments are semiphenomenological in nature here a firstprinciples manypole generalization of the plasmonpole model is developed for improved calculations of inelastic losses the method is based on the gw approximation ... | [['inelastic', 'losses', 'are', 'crucial', 'to', 'a', 'quantitative', 'analysis', 'of', 'xray', 'absorption', 'spectra', 'however', 'current', 'treatments', 'are', 'semiphenomenological', 'in', 'nature', 'here', 'a', 'firstprinciples', 'manypole', 'generalization', 'of', 'the', 'plasmonpole', 'model', 'is', 'developed'... | [-0.08291808036189989, 0.08062411694835028, -0.08998809039021713, 0.12151767599930048, -0.041001010937684206, -0.07697643751931126, 0.06082967924545553, 0.4080285082170128, -0.2281617332202294, -0.2873611709470079, -0.008310033124871552, -0.3424980013094244, -0.1262109217499077, 0.2261967611155833, 0.049650562808162324... |
709.1733 | Isolated Eigenvalues of the Ferromagnetic Spin-J XXZ Chain with Kink
Boundary Conditions | We investigate the low-lying excited states of the spin J ferromagnetic XXZ
chain with Ising anisotropy Delta and kink boundary conditions. Since the third
component of the total magnetization, M, is conserved, it is meaningful to
study the spectrum for each fixed value of M. We prove that for J>= 3/2 the
lowest exci... | math-ph cond-mat.stat-mech math.MP quant-ph | we investigate the lowlying excited states of the spin j ferromagnetic xxz chain with ising anisotropy delta and kink boundary conditions since the third component of the total magnetization m is conserved it is meaningful to study the spectrum for each fixed value of m we prove that for j 32 the lowest excited eigenva... | [['we', 'investigate', 'the', 'lowlying', 'excited', 'states', 'of', 'the', 'spin', 'j', 'ferromagnetic', 'xxz', 'chain', 'with', 'ising', 'anisotropy', 'delta', 'and', 'kink', 'boundary', 'conditions', 'since', 'the', 'third', 'component', 'of', 'the', 'total', 'magnetization', 'm', 'is', 'conserved', 'it', 'is', 'mea... | [-0.19881421749505535, 0.22716512002201247, 0.004219824341513838, 0.04226603275189215, -0.002055793156614527, -0.11177266497785847, 0.03367868988425471, 0.3398060703572507, -0.23919029543564344, -0.2824627905113933, 0.07683700109434237, -0.3316610615584068, -0.020970636901135247, 0.12415634622933187, 0.0934432420229616... |
709.1734 | Residual Velocities in Steady Free Boundary Value Problems of Vector
Laplacian Type | This paper describes a technique to determine the linear well-posedness of a
general class of vector elliptic problems that include a steady interface, to
be determined as part of the problem, that separates two subdomains. The
interface satisfies mixed Dirichlet and Neumann conditions. We consider ``2+2''
models, me... | math.NA | this paper describes a technique to determine the linear wellposedness of a general class of vector elliptic problems that include a steady interface to be determined as part of the problem that separates two subdomains the interface satisfies mixed dirichlet and neumann conditions we consider 22 models meaning two ind... | [['this', 'paper', 'describes', 'a', 'technique', 'to', 'determine', 'the', 'linear', 'wellposedness', 'of', 'a', 'general', 'class', 'of', 'vector', 'elliptic', 'problems', 'that', 'include', 'a', 'steady', 'interface', 'to', 'be', 'determined', 'as', 'part', 'of', 'the', 'problem', 'that', 'separates', 'two', 'subdom... | [-0.11216674786243987, 0.08393566158396684, -0.1084429571970499, 0.03517164596944765, -0.1032351563044358, -0.15848693481530063, -0.028550072955113137, 0.35338872658446363, -0.31129440721101026, -0.2544996010871858, 0.15600305258859798, -0.24565439369221817, -0.10648053355440165, 0.20334034844979346, -0.058098575545175... |
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