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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708.3249 | On the Khovanov and knot Floer homologies of quasi-alternating links | Quasi-alternating links are a natural generalization of alternating links. In
this paper, we show that quasi-alternating links are "homologically thin" for
both Khovanov homology and knot Floer homology. In particular, their bigraded
homology groups are determined by the signature of the link, together with the
Euler... | math.GT math.SG | quasialternating links are a natural generalization of alternating links in this paper we show that quasialternating links are homologically thin for both khovanov homology and knot floer homology in particular their bigraded homology groups are determined by the signature of the link together with the euler characteri... | [['quasialternating', 'links', 'are', 'a', 'natural', 'generalization', 'of', 'alternating', 'links', 'in', 'this', 'paper', 'we', 'show', 'that', 'quasialternating', 'links', 'are', 'homologically', 'thin', 'for', 'both', 'khovanov', 'homology', 'and', 'knot', 'floer', 'homology', 'in', 'particular', 'their', 'bigrade... | [-0.32271227407836706, 0.048826860589906575, -0.11567434861208312, 0.114267658481549, -0.09223562843399122, -0.191000717447605, -0.011968104674451752, 0.3578295505139977, -0.37273840147536247, -0.29888899805373514, 0.10263441964343656, -0.22021874726924578, -0.2110858233209001, 0.1390822260727873, -0.15517532634403325,... |
708.325 | Topological estimation of percolation thresholds | Global physical properties of random media change qualitatively at a
percolation threshold, where isolated clusters merge to form one infinite
connected component. The precise knowledge of percolation thresholds is thus of
paramount importance. For two dimensional lattice graphs, we use the universal
scaling form of ... | cond-mat.stat-mech | global physical properties of random media change qualitatively at a percolation threshold where isolated clusters merge to form one infinite connected component the precise knowledge of percolation thresholds is thus of paramount importance for two dimensional lattice graphs we use the universal scaling form of the cl... | [['global', 'physical', 'properties', 'of', 'random', 'media', 'change', 'qualitatively', 'at', 'a', 'percolation', 'threshold', 'where', 'isolated', 'clusters', 'merge', 'to', 'form', 'one', 'infinite', 'connected', 'component', 'the', 'precise', 'knowledge', 'of', 'percolation', 'thresholds', 'is', 'thus', 'of', 'par... | [-0.11173628364223986, 0.16019275477388872, -0.11972563190851361, 0.12853361897286958, -0.07228006778517738, -0.1341845396021381, 0.12683203465072437, 0.36757901556789874, -0.2320822275080718, -0.25261226477101445, 0.06435255065909587, -0.2720889142830856, -0.17579429999750573, 0.12592269147979096, 0.03479036540724337,... |
708.3251 | Supplementary material: Topological estimation of percolation thresholds | This is supplementary material for the article arxiv:0708.3250. We provide an
alternative introduction of the mean Euler Characteristic, additional examples
and the percolation thresholds for 2-uniform lattices.
| cond-mat.stat-mech | this is supplementary material for the article arxiv07083250 we provide an alternative introduction of the mean euler characteristic additional examples and the percolation thresholds for 2uniform lattices | [['this', 'is', 'supplementary', 'material', 'for', 'the', 'article', 'arxiv07083250', 'we', 'provide', 'an', 'alternative', 'introduction', 'of', 'the', 'mean', 'euler', 'characteristic', 'additional', 'examples', 'and', 'the', 'percolation', 'thresholds', 'for', '2uniform', 'lattices']] | [-0.1468832339339245, 0.10825641813761859, -0.07957909719194643, 0.10858718463434623, -0.09426399578268711, -0.13212378967839938, 0.0060816354906329745, 0.3998124696887456, -0.26555826633165663, -0.24149123572099668, 0.13101028749504343, -0.2570507807854133, -0.1977839175826655, 0.1688603308195105, -0.04537757364316629... |
708.3252 | Generalized Relativistic Chapman-Enskog Solution of the Boltzmann
Equation | The Chapman-Enskog method of solution of the relativistic Boltzmann equation
is generalized in order to admit a time-derivative term associated to a
thermodynamic force in its first order solution. Both existence and uniqueness
of such a solution are proved based on the standard theory of integral
equations. The math... | gr-qc | the chapmanenskog method of solution of the relativistic boltzmann equation is generalized in order to admit a timederivative term associated to a thermodynamic force in its first order solution both existence and uniqueness of such a solution are proved based on the standard theory of integral equations the mathematic... | [['the', 'chapmanenskog', 'method', 'of', 'solution', 'of', 'the', 'relativistic', 'boltzmann', 'equation', 'is', 'generalized', 'in', 'order', 'to', 'admit', 'a', 'timederivative', 'term', 'associated', 'to', 'a', 'thermodynamic', 'force', 'in', 'its', 'first', 'order', 'solution', 'both', 'existence', 'and', 'uniquen... | [-0.1257792541100197, 0.028226602624795618, -0.1120441505902332, 0.09108280596699668, -0.08715249886353539, -0.07660552073423177, -0.007405918898469169, 0.2398366811047372, -0.30334839189093404, -0.25290996053141274, 0.11503323449032407, -0.27809906806414053, -0.1699241477332703, 0.18630252820631005, -0.022194387085021... |
708.3253 | Complex X-ray morphology of Abell 3128: A distant cluster behind a
disturbed cluster | We present here the results of a detailed study of the X-ray properties of
the cluster of galaxies Abell 3128 (z=0.06), based on the analysis of deep (100
ks) XMM-Newton data. The most obvious feature of the X-ray morphology of A3128
is the presence of two X-ray peaks separated by ~12'. By detecting the
redshifted Fe... | astro-ph | we present here the results of a detailed study of the xray properties of the cluster of galaxies abell 3128 z006 based on the analysis of deep 100 ks xmmnewton data the most obvious feature of the xray morphology of a3128 is the presence of two xray peaks separated by 12 by detecting the redshifted fe k line we find t... | [['we', 'present', 'here', 'the', 'results', 'of', 'a', 'detailed', 'study', 'of', 'the', 'xray', 'properties', 'of', 'the', 'cluster', 'of', 'galaxies', 'abell', '3128', 'z006', 'based', 'on', 'the', 'analysis', 'of', 'deep', '100', 'ks', 'xmmnewton', 'data', 'the', 'most', 'obvious', 'feature', 'of', 'the', 'xray', '... | [-0.08106255831491083, 0.03919711738760357, -0.11923560369914374, 0.0480388924020586, -0.07303926815216998, -0.01602769069010353, 0.05310447338311083, 0.4362342274627992, -0.18012900409700264, -0.30555095220626144, 0.048048273076716795, -0.3238242236410434, -0.044191876944169955, 0.1812684223082498, 0.04381722225351123... |
708.3254 | Applications of Wallis Theorem | In this paper we present theorems and applications of Wallis theorem related
to trigonometric integrals.
| math.GM | in this paper we present theorems and applications of wallis theorem related to trigonometric integrals | [['in', 'this', 'paper', 'we', 'present', 'theorems', 'and', 'applications', 'of', 'wallis', 'theorem', 'related', 'to', 'trigonometric', 'integrals']] | [-0.13692115557690462, -0.039020962578554946, -0.13036533507208029, 0.0738628476470088, -0.08109455928206444, -0.04707406175633271, 0.1143119443130369, 0.3047295778989792, -0.2763807972272237, -0.2019689771036307, 0.16857074771542102, -0.25063352833191554, -0.24308801020185153, 0.3201449568072955, -0.2673429522663355, ... |
708.3255 | New H2 Jets in Monoceros R2 | We are presenting a wide-field image of the Mon R2 star forming region
obtained with WFCAM on UKIRT in the 2.12 micron filter centered on the H2 1--0
S(1) emission line. We report the discovery of 15 new H2 jets in Mon R2 and two
in L 1646 and confirm most of these discoveries using archival Spitzer IRAC 4.5
and 8.0 ... | astro-ph | we are presenting a widefield image of the mon r2 star forming region obtained with wfcam on ukirt in the 212 micron filter centered on the h2 10 s1 emission line we report the discovery of 15 new h2 jets in mon r2 and two in l 1646 and confirm most of these discoveries using archival spitzer irac 45 and 80 micron imag... | [['we', 'are', 'presenting', 'a', 'widefield', 'image', 'of', 'the', 'mon', 'r2', 'star', 'forming', 'region', 'obtained', 'with', 'wfcam', 'on', 'ukirt', 'in', 'the', '212', 'micron', 'filter', 'centered', 'on', 'the', 'h2', '10', 's1', 'emission', 'line', 'we', 'report', 'the', 'discovery', 'of', '15', 'new', 'h2', '... | [-0.08171412235875007, 0.07331912262473624, -0.012202014586469833, 0.0225894000689985, -0.06398315256650465, -0.09513164713533352, 0.011232920730000606, 0.4769070217844801, -0.17477447488024642, -0.30560483072169015, 0.10810202248715053, -0.2908832444201993, -0.05621393381590969, 0.16159101035800236, -0.050954379207341... |
708.3256 | The width difference of rho vector mesons | We compute the difference in decay widths of charged and neutral \rho(770)
vector mesons. The isospin breaking arising from mass differences of neutral
and charged \pi and \rho mesons, radiative corrections to \rho -> \pi\pi, and
the \rho -> \pi\pi\gamma decays are taken into account. It is found that the
width diffe... | hep-ph | we compute the difference in decay widths of charged and neutral rho770 vector mesons the isospin breaking arising from mass differences of neutral and charged pi and rho mesons radiative corrections to rho pipi and the rho pipigamma decays are taken into account it is found that the width difference delta gamma_rho is... | [['we', 'compute', 'the', 'difference', 'in', 'decay', 'widths', 'of', 'charged', 'and', 'neutral', 'rho770', 'vector', 'mesons', 'the', 'isospin', 'breaking', 'arising', 'from', 'mass', 'differences', 'of', 'neutral', 'and', 'charged', 'pi', 'and', 'rho', 'mesons', 'radiative', 'corrections', 'to', 'rho', 'pipi', 'and... | [-0.09599309578148085, 0.28111735892720346, -0.0857942927111655, 0.17323975789842608, -0.0188415105790333, -0.169666534300547, 0.05505309957702276, 0.3189366065821242, -0.23458655900863368, -0.25347627287860525, -0.06196129146075353, -0.37254760604958204, 0.03522199898048542, 0.07099650108233788, 0.11674175263100932, 0... |
708.3257 | Tong's spectrum for Rosen continued fractions | The Rosen fractions are an infinite set of continued fraction algorithms,
each giving expansions of real numbers in terms of certain algebraic integers.
For each, we give a best possible upper bound for the minimum in appropriate
consecutive blocks of approximation coefficients (in the sense of Diophantine
approximat... | math.NT | the rosen fractions are an infinite set of continued fraction algorithms each giving expansions of real numbers in terms of certain algebraic integers for each we give a best possible upper bound for the minimum in appropriate consecutive blocks of approximation coefficients in the sense of diophantine approximation by... | [['the', 'rosen', 'fractions', 'are', 'an', 'infinite', 'set', 'of', 'continued', 'fraction', 'algorithms', 'each', 'giving', 'expansions', 'of', 'real', 'numbers', 'in', 'terms', 'of', 'certain', 'algebraic', 'integers', 'for', 'each', 'we', 'give', 'a', 'best', 'possible', 'upper', 'bound', 'for', 'the', 'minimum', '... | [-0.22322574427853975, 0.10276521841597204, -0.05141406904699074, 0.07657507765624258, -0.04076773997041441, -0.06527108367207268, 0.15896729362152873, 0.2586038785225283, -0.23471292285692125, -0.2675949651156626, 0.09412290598820186, -0.2728407953880609, -0.1470628837567, 0.21557069266961504, -0.05952618612597386, 0.... |
708.3258 | The XMM Cluster Survey: The Dynamical State of XMMXCS J2215.9-1738 at
z=1.457 | We present new spectroscopic observations of the most distant X-ray selected
galaxy cluster currently known, XMMXCS J2215.9-1738 at z=1.457, obtained with
the DEIMOS instrument at the W. M. Keck Observatory, and the FORS2 instrument
on the ESO Very Large Telescope. Within the cluster virial radius, as estimated
from ... | astro-ph | we present new spectroscopic observations of the most distant xray selected galaxy cluster currently known xmmxcs j221591738 at z1457 obtained with the deimos instrument at the w m keck observatory and the fors2 instrument on the eso very large telescope within the cluster virial radius as estimated from the cluster xr... | [['we', 'present', 'new', 'spectroscopic', 'observations', 'of', 'the', 'most', 'distant', 'xray', 'selected', 'galaxy', 'cluster', 'currently', 'known', 'xmmxcs', 'j221591738', 'at', 'z1457', 'obtained', 'with', 'the', 'deimos', 'instrument', 'at', 'the', 'w', 'm', 'keck', 'observatory', 'and', 'the', 'fors2', 'instru... | [-0.08225758696990039, 0.12186243670055379, -0.09675802968728242, 0.0907164608274966, -0.11828456466238965, -0.04477448134421908, 0.06035362642194347, 0.4202550527141996, -0.1994584234297108, -0.35811235335847685, 0.057324007511996324, -0.31383912421013943, -0.02132756152392301, 0.2170904336519362, 0.015580334221393242... |
708.3259 | Fast evaluation of union-intersection expressions | We show how to represent sets in a linear space data structure such that
expressions involving unions and intersections of sets can be computed in a
worst-case efficient way. This problem has applications in e.g. information
retrieval and database systems. We mainly consider the RAM model of
computation, and sets of ... | cs.DS cs.DB cs.IR | we show how to represent sets in a linear space data structure such that expressions involving unions and intersections of sets can be computed in a worstcase efficient way this problem has applications in eg information retrieval and database systems we mainly consider the ram model of computation and sets of machine ... | [['we', 'show', 'how', 'to', 'represent', 'sets', 'in', 'a', 'linear', 'space', 'data', 'structure', 'such', 'that', 'expressions', 'involving', 'unions', 'and', 'intersections', 'of', 'sets', 'can', 'be', 'computed', 'in', 'a', 'worstcase', 'efficient', 'way', 'this', 'problem', 'has', 'applications', 'in', 'eg', 'inf... | [-0.14662179064699948, 0.08683528537429604, -0.04792997243930586, 0.04562994171006028, -0.039877154212306434, -0.10020764826774775, 0.10052808764157817, 0.35647381472379147, -0.2890882508876357, -0.3362432190555237, 0.09057084848297693, -0.29316511133358636, -0.10648502315355775, 0.22367630879861758, -0.056085366118038... |
708.326 | Asymptotically Optimal Importance Sampling for Jackson Networks with a
Tree Topology | Importance sampling (IS) is a variance reduction method for simulating rare
events. A recent paper by Dupuis, Wang and Sezer (Ann. App. Probab. 17(4):1306-
1346, 2007) exploits connections between IS and stochastic games and optimal
control problems to show how to design and analyze simple and efficient IS
algorithms... | math.PR | importance sampling is is a variance reduction method for simulating rare events a recent paper by dupuis wang and sezer ann app probab 1741306 1346 2007 exploits connections between is and stochastic games and optimal control problems to show how to design and analyze simple and efficient is algorithms for various ove... | [['importance', 'sampling', 'is', 'is', 'a', 'variance', 'reduction', 'method', 'for', 'simulating', 'rare', 'events', 'a', 'recent', 'paper', 'by', 'dupuis', 'wang', 'and', 'sezer', 'ann', 'app', 'probab', '1741306', '1346', '2007', 'exploits', 'connections', 'between', 'is', 'and', 'stochastic', 'games', 'and', 'opti... | [-0.1659339271273289, 0.10565224635389778, -0.016165904453861832, 0.06437247434526294, -0.05149326122509653, -0.21048921842328053, 0.1361651883152745, 0.3832787385822943, -0.2740863227260443, -0.2848890993631626, 0.11338554828305847, -0.30869710054436084, -0.1348110260785676, 0.12417477563073571, -0.11626140522026776, ... |
708.3261 | Complex Structures on Principal Bundles | Holomorphic principal G-bundles over a complex manifold M can be studied
using non-abelian cohomology groups H^1(M,G). On the other hand, if M=\Sigma is
a closed Riemann surface, there is a correspondence between holomorphic
principal G-bundles over \Sigma and coadjoint orbits in the dual of a central
extension of th... | math.DG math.CV | holomorphic principal gbundles over a complex manifold m can be studied using nonabelian cohomology groups h1mg on the other hand if msigma is a closed riemann surface there is a correspondence between holomorphic principal gbundles over sigma and coadjoint orbits in the dual of a central extension of the lie algebra c... | [['holomorphic', 'principal', 'gbundles', 'over', 'a', 'complex', 'manifold', 'm', 'can', 'be', 'studied', 'using', 'nonabelian', 'cohomology', 'groups', 'h1mg', 'on', 'the', 'other', 'hand', 'if', 'msigma', 'is', 'a', 'closed', 'riemann', 'surface', 'there', 'is', 'a', 'correspondence', 'between', 'holomorphic', 'prin... | [-0.24995532370873808, 0.04270719918282272, -0.13603633507959728, 0.057790050857964854, -0.1519169107447436, -0.12295060359548064, -0.03929202655261314, 0.3626853930361477, -0.26863073862307235, -0.19202098061825024, 0.13030761245344938, -0.21651441029008525, -0.17616044072273337, 0.21666607942811592, -0.13578343914281... |
708.3262 | Exciton-Plasmon Coupling in Carbon Nanotubes | We study theoretically the interactions of excitonic states with surface
electromagnetic modes of small-diameter (~1 nm) semiconducting single-walled
carbon nanotubes. We show that these interactions can result in strong
exciton-surface-plasmon coupling. The exciton absorption lineshapes exhibit the
line (Rabi) split... | cond-mat.mes-hall | we study theoretically the interactions of excitonic states with surface electromagnetic modes of smalldiameter 1 nm semiconducting singlewalled carbon nanotubes we show that these interactions can result in strong excitonsurfaceplasmon coupling the exciton absorption lineshapes exhibit the line rabi splitting 0103 ev ... | [['we', 'study', 'theoretically', 'the', 'interactions', 'of', 'excitonic', 'states', 'with', 'surface', 'electromagnetic', 'modes', 'of', 'smalldiameter', '1', 'nm', 'semiconducting', 'singlewalled', 'carbon', 'nanotubes', 'we', 'show', 'that', 'these', 'interactions', 'can', 'result', 'in', 'strong', 'excitonsurfacep... | [-0.18576822174713015, 0.19829858232289552, 0.026451589637435973, 0.025585245167215664, -0.015325194535156092, -0.20069036248450478, 0.1024532762169838, 0.5612297397851944, -0.24726726678510508, -0.28008156157409153, -0.11725704221831014, -0.30565877974033356, -0.13708042862514655, 0.16054298972710968, 0.07001570340245... |
708.3263 | $G$-stable pieces and Lusztig's dimension estimates | We use $G$-stable pieces to construct some equidimensional varieties and as a
consequence, obtain Lusztig's dimension estimates \cite[section 4]{L2}. This is
a generalization of \cite{HL}.
| math.RT | we use gstable pieces to construct some equidimensional varieties and as a consequence obtain lusztigs dimension estimates citesection 4l2 this is a generalization of citehl | [['we', 'use', 'gstable', 'pieces', 'to', 'construct', 'some', 'equidimensional', 'varieties', 'and', 'as', 'a', 'consequence', 'obtain', 'lusztigs', 'dimension', 'estimates', 'citesection', '4l2', 'this', 'is', 'a', 'generalization', 'of', 'citehl']] | [-0.15643642142415046, -0.029172382280230523, -0.16352230720221997, 0.13085870318114756, -0.15914259059354663, -0.1317996161058545, 0.0003238565847277641, 0.272995098978281, -0.3084099464863539, -0.15438406243920327, 0.1158037225343287, -0.22865899935364722, -0.16947179138660431, 0.17961839605122804, -0.266254274249076... |
708.3264 | Fields and Filaments in the Core of the Centaurus Cluster | We present high resolution images of the Faraday Rotation Measure (RM)
structure of the radio galaxy PKS 1246-410, at the center of the Centaurus
cluster. Comparison with Halpha-line and soft X-ray emission reveals a
correspondence between the line-emitting gas, the soft X-ray emitting gas,
regions with an excess in ... | astro-ph | we present high resolution images of the faraday rotation measure rm structure of the radio galaxy pks 1246410 at the center of the centaurus cluster comparison with halphaline and soft xray emission reveals a correspondence between the lineemitting gas the soft xray emitting gas regions with an excess in the rm images... | [['we', 'present', 'high', 'resolution', 'images', 'of', 'the', 'faraday', 'rotation', 'measure', 'rm', 'structure', 'of', 'the', 'radio', 'galaxy', 'pks', '1246410', 'at', 'the', 'center', 'of', 'the', 'centaurus', 'cluster', 'comparison', 'with', 'halphaline', 'and', 'soft', 'xray', 'emission', 'reveals', 'a', 'corre... | [-0.0926692968948969, 0.15298420150758266, -0.031640497752433196, 0.051620832885262265, -0.015592852684444394, -0.04478185652145024, 0.02504009449501233, 0.4551753936142757, -0.20114868311211467, -0.3722621839493513, 0.0512222900231979, -0.2797567184693341, 0.054681855973392195, 0.1576562573298298, 0.03323528143609392,... |
708.3265 | Ground and excited-state fermions in a 1D double-well, exact and
time-dependent density-functional solutions | Two of the most popular quantum mechanical models of interacting fermions are
compared to each other and to potentially exact solutions for a pair of
contact-interacting fermions trapped in a 1D double-well potential, a model of
atoms in a quasi-1D optical lattice or electrons of a Hydrogen molecule in a
strong magne... | cond-mat.other cond-mat.mtrl-sci | two of the most popular quantum mechanical models of interacting fermions are compared to each other and to potentially exact solutions for a pair of contactinteracting fermions trapped in a 1d doublewell potential a model of atoms in a quasi1d optical lattice or electrons of a hydrogen molecule in a strong magnetic fi... | [['two', 'of', 'the', 'most', 'popular', 'quantum', 'mechanical', 'models', 'of', 'interacting', 'fermions', 'are', 'compared', 'to', 'each', 'other', 'and', 'to', 'potentially', 'exact', 'solutions', 'for', 'a', 'pair', 'of', 'contactinteracting', 'fermions', 'trapped', 'in', 'a', '1d', 'doublewell', 'potential', 'a',... | [-0.10452837242036114, 0.10186903117734084, -0.06722388723208712, 0.1423202488788851, 0.0007548169120079489, -0.19758863510391655, 0.05370779100719363, 0.39136242805385246, -0.2127006880837464, -0.2640578034887755, -0.005087434325473884, -0.3084995992859161, -0.09066646530842695, 0.15012110818468757, 0.048104389069606,... |
708.3266 | Convergence of freely decomposable Kleinian groups | We consider a compact orientable hyperbolic 3-manifold with a compressible
boundary. Suppose that we are given a sequence of geometrically finite
hyperbolic metrics whose conformal boundary structures at infinity diverge to a
projective lamination. We prove that if this limit projective lamination is
doubly incompres... | math.GT | we consider a compact orientable hyperbolic 3manifold with a compressible boundary suppose that we are given a sequence of geometrically finite hyperbolic metrics whose conformal boundary structures at infinity diverge to a projective lamination we prove that if this limit projective lamination is doubly incompressible... | [['we', 'consider', 'a', 'compact', 'orientable', 'hyperbolic', '3manifold', 'with', 'a', 'compressible', 'boundary', 'suppose', 'that', 'we', 'are', 'given', 'a', 'sequence', 'of', 'geometrically', 'finite', 'hyperbolic', 'metrics', 'whose', 'conformal', 'boundary', 'structures', 'at', 'infinity', 'diverge', 'to', 'a'... | [-0.20382705642652973, 0.13564542118409598, -0.14898289826295869, 0.07119615646739919, -0.11762571482088517, -0.16959125992237917, -0.014949430851580424, 0.3346820951162561, -0.31873280899850903, -0.14094326165630608, 0.13770767739766301, -0.27365151854118686, -0.14012846855346012, 0.1729847384566391, -0.18448687320877... |
708.3267 | The Friedel-Anderson and Kondo Impurity Problem for Arbitrary s-Band
Density of States and Exchange Interaction | In his renormalization paper of the Kondo effect Wilson replaced the full
band of s-electrons by a small number of ''Wilson states''. He started from a
rather artificial symmetric band with constant density of states and constant
interaction with the impurity. It is shown in the present paper that with a
minor modifi... | cond-mat.str-el | in his renormalization paper of the kondo effect wilson replaced the full band of selectrons by a small number of wilson states he started from a rather artificial symmetric band with constant density of states and constant interaction with the impurity it is shown in the present paper that with a minor modification th... | [['in', 'his', 'renormalization', 'paper', 'of', 'the', 'kondo', 'effect', 'wilson', 'replaced', 'the', 'full', 'band', 'of', 'selectrons', 'by', 'a', 'small', 'number', 'of', 'wilson', 'states', 'he', 'started', 'from', 'a', 'rather', 'artificial', 'symmetric', 'band', 'with', 'constant', 'density', 'of', 'states', 'a... | [-0.15240909874201525, 0.2198691200915768, -0.03572502801474835, 0.06117395134772975, 0.012866784649139101, -0.160653418096082, 0.04830164610655731, 0.3622715703368031, -0.22589439615424906, -0.3193650826017235, 0.01069637506360097, -0.3204763161272488, -0.05868394117659101, 0.11909648989672428, 0.04726834267612312, 0.... |
708.3268 | Ac-cotunneling through an interacting quantum dot under a magnetic field | We analyze inelastic cotunneling through an interacting quantum dot subject
to an ambient magnetic field in the weak tunneling regime under a non-adiabatic
time-dependent bias-voltage. Our results clearly exhibit photon-assisted
satellites and an overall suppression of differential conductance with
increasing driving... | cond-mat.mes-hall | we analyze inelastic cotunneling through an interacting quantum dot subject to an ambient magnetic field in the weak tunneling regime under a nonadiabatic timedependent biasvoltage our results clearly exhibit photonassisted satellites and an overall suppression of differential conductance with increasing driving amplit... | [['we', 'analyze', 'inelastic', 'cotunneling', 'through', 'an', 'interacting', 'quantum', 'dot', 'subject', 'to', 'an', 'ambient', 'magnetic', 'field', 'in', 'the', 'weak', 'tunneling', 'regime', 'under', 'a', 'nonadiabatic', 'timedependent', 'biasvoltage', 'our', 'results', 'clearly', 'exhibit', 'photonassisted', 'sat... | [-0.2303741852579228, 0.17986875318357784, -0.07649442643495434, 0.032088530662280144, 0.003603159860407902, -0.15089770889509532, 0.04856503460856186, 0.3948398267660858, -0.27351592550590886, -0.26009566076415574, -0.06661344749332106, -0.2854244594099158, -0.1834112506643948, 0.2816840708650396, -0.04045897428640874... |
708.3269 | Resonant electromagnetic emission from intrinsic Josephson-junction
stacks with laterally modulated Josephson critical current | Intrinsic Josephson-junction stacks realized in mesas fabricated out of
high-temperature superconductors may be used as sources of coherent
electromagnetic radiation in the terahertz range. The major challenge is to
synchronize Josephson oscillations in all junctions in the stack to get
significant radiation out of t... | cond-mat.supr-con | intrinsic josephsonjunction stacks realized in mesas fabricated out of hightemperature superconductors may be used as sources of coherent electromagnetic radiation in the terahertz range the major challenge is to synchronize josephson oscillations in all junctions in the stack to get significant radiation out of the cr... | [['intrinsic', 'josephsonjunction', 'stacks', 'realized', 'in', 'mesas', 'fabricated', 'out', 'of', 'hightemperature', 'superconductors', 'may', 'be', 'used', 'as', 'sources', 'of', 'coherent', 'electromagnetic', 'radiation', 'in', 'the', 'terahertz', 'range', 'the', 'major', 'challenge', 'is', 'to', 'synchronize', 'jo... | [-0.23046106844031738, 0.15975235289148432, -0.0038486531425622247, 0.03317981228714676, -0.06624236007510695, -0.12837362636318653, 0.049713430467471925, 0.40079498202318237, -0.2657248459318431, -0.2668499852367122, 0.044980368800073244, -0.27133269348719513, -0.09887189207421172, 0.24190783107076727, 0.0232408051531... |
708.327 | Green's matrices of second order elliptic systems with measurable
coefficients in two dimensional domains | We study Green's matrices for divergence form, second order strongly elliptic
systems with bounded measurable coefficients in two dimensional domains. We
establish existence, uniqueness, and pointwise estimates of the Green's
matrices.
| math.AP | we study greens matrices for divergence form second order strongly elliptic systems with bounded measurable coefficients in two dimensional domains we establish existence uniqueness and pointwise estimates of the greens matrices | [['we', 'study', 'greens', 'matrices', 'for', 'divergence', 'form', 'second', 'order', 'strongly', 'elliptic', 'systems', 'with', 'bounded', 'measurable', 'coefficients', 'in', 'two', 'dimensional', 'domains', 'we', 'establish', 'existence', 'uniqueness', 'and', 'pointwise', 'estimates', 'of', 'the', 'greens', 'matrice... | [-0.21897758417312177, 0.06575110769500175, -0.035128149053742806, 0.08728973357187163, -0.07107626280236629, -0.0843157747219647, -0.05728069972246885, 0.3477975637501767, -0.2897483663813722, -0.12230279035265407, 0.16383462415392241, -0.34657909967485934, -0.1469749778869652, 0.18046559609713092, -0.0075529992219901... |
708.3271 | Simulation of Spread and Control of Lesions in Brain | A simulation model for the spread and control of lesions in the brain is
constructed using a planar network (graph) representation for the Central
Nervous System (CNS). The model is inspired by the lesion structures observed
in the case of Multiple Sclerosis (MS), a chronic disease of the CNS. The
initial lesion site... | physics.bio-ph physics.comp-ph q-bio.NC | a simulation model for the spread and control of lesions in the brain is constructed using a planar network graph representation for the central nervous system cns the model is inspired by the lesion structures observed in the case of multiple sclerosis ms a chronic disease of the cns the initial lesion site is at the ... | [['a', 'simulation', 'model', 'for', 'the', 'spread', 'and', 'control', 'of', 'lesions', 'in', 'the', 'brain', 'is', 'constructed', 'using', 'a', 'planar', 'network', 'graph', 'representation', 'for', 'the', 'central', 'nervous', 'system', 'cns', 'the', 'model', 'is', 'inspired', 'by', 'the', 'lesion', 'structures', 'o... | [-0.10002561413036411, 0.12152046137815638, -0.02565013143162771, 0.033460239770045135, 0.0028237392028473366, -0.14438429220644816, 0.07521088946919152, 0.3429805746696486, -0.24842433062393907, -0.2594894452412037, 0.1236930777753294, -0.26001601279446274, -0.18980573089407746, 0.16951318840780977, -0.131221392559729... |
708.3272 | Search for Lepton Flavor Violating tau Decays into Three Leptons | We search for lepton-flavor-violating tau decays into three leptons (electron
or muon) using 535 fb^{-1} of data collected with the Belle detector at the
KEKB asymmetric-energy e+e- collider. No evidence for these decays is observed
and we set 90% confidence level upper limits on the branching fractions between
2.0x1... | hep-ex | we search for leptonflavorviolating tau decays into three leptons electron or muon using 535 fb1 of data collected with the belle detector at the kekb asymmetricenergy ee collider no evidence for these decays is observed and we set 90 confidence level upper limits on the branching fractions between 20x108 and 41x108 th... | [['we', 'search', 'for', 'leptonflavorviolating', 'tau', 'decays', 'into', 'three', 'leptons', 'electron', 'or', 'muon', 'using', '535', 'fb1', 'of', 'data', 'collected', 'with', 'the', 'belle', 'detector', 'at', 'the', 'kekb', 'asymmetricenergy', 'ee', 'collider', 'no', 'evidence', 'for', 'these', 'decays', 'is', 'obs... | [-0.028693587065032316, 0.1802424832148421, -0.014751464184938055, 0.13125338040073542, -0.08335776678568711, -0.12051739820250959, 0.17308075930993777, 0.3054012315009128, -0.09484586729244752, -0.3657533036488475, 0.024596988230548573, -0.4754675548862327, 0.0901624496116049, 0.2437765895579518, 0.13475718987033222, ... |
708.3273 | Path to finding the critical thickness for memory in thin ferroelectric
films | The finite screening length by real metallic electrodes, albeit very small
(<1A), results in finite depolarizing field that tends to split the film into
domains. In very thin ferroelectric films the domain structure reduces to
sinusoidal distribution of polarization considered first in the 1980s. We
discuss the phase... | cond-mat.mtrl-sci cond-mat.stat-mech | the finite screening length by real metallic electrodes albeit very small 1a results in finite depolarizing field that tends to split the film into domains in very thin ferroelectric films the domain structure reduces to sinusoidal distribution of polarization considered first in the 1980s we discuss the phase transiti... | [['the', 'finite', 'screening', 'length', 'by', 'real', 'metallic', 'electrodes', 'albeit', 'very', 'small', '1a', 'results', 'in', 'finite', 'depolarizing', 'field', 'that', 'tends', 'to', 'split', 'the', 'film', 'into', 'domains', 'in', 'very', 'thin', 'ferroelectric', 'films', 'the', 'domain', 'structure', 'reduces'... | [-0.16915186638200358, 0.16344990355487005, -0.08356037863506739, -0.0043332209935834426, -0.06784819210331668, -0.13920686795853643, 0.07939153674504712, 0.4136341839027004, -0.3045309064567418, -0.2511569130226594, 0.08059946962773111, -0.2397109601458832, -0.09479063598266921, 0.18627009614362938, -0.011318710401213... |
708.3274 | Analytic Constructions of General n-Qubit Controlled Gates | In this Letter, we present two analytic expressions that most generally
simulate $n$-qubit controlled-$U$ gates with standard one-qubit gates and CNOT
gates using exponential and polynomial complexity respectively. Explicit
circuits and general expressions of decomposition are derived. The exact
numbers of basic oper... | quant-ph | in this letter we present two analytic expressions that most generally simulate nqubit controlledu gates with standard onequbit gates and cnot gates using exponential and polynomial complexity respectively explicit circuits and general expressions of decomposition are derived the exact numbers of basic operations in th... | [['in', 'this', 'letter', 'we', 'present', 'two', 'analytic', 'expressions', 'that', 'most', 'generally', 'simulate', 'nqubit', 'controlledu', 'gates', 'with', 'standard', 'onequbit', 'gates', 'and', 'cnot', 'gates', 'using', 'exponential', 'and', 'polynomial', 'complexity', 'respectively', 'explicit', 'circuits', 'and... | [-0.1753118653201832, 0.12524990345579837, -0.020524810823910642, 0.06560668690824213, 0.04788110566870222, -0.2803843397787719, 0.09578748741011434, 0.42105153350616403, -0.19099928873793204, -0.31757954159259516, 0.07673505271723459, -0.16831795990748225, -0.19982703822172898, 0.3183767388592351, -0.06126656182953771... |
708.3275 | XMM observation of 1RXS J180431.1-273932: a new M-type X-ray binary with
a 494 s-pulse period neutron star? | Low-mass X-ray binaries are binary systems composed of a compact object and a
low-mass star. Recently, a new class of these systems, known as symbiotic
$X$-ray binaries (with a neutron star with a M-type giant companion), has been
discovered. Here, we present long-duration ${\it XMM}$ observations of the
source 1RXS ... | astro-ph | lowmass xray binaries are binary systems composed of a compact object and a lowmass star recently a new class of these systems known as symbiotic xray binaries with a neutron star with a mtype giant companion has been discovered here we present longduration it xmm observations of the source 1rxs j1804311273932 temporal... | [['lowmass', 'xray', 'binaries', 'are', 'binary', 'systems', 'composed', 'of', 'a', 'compact', 'object', 'and', 'a', 'lowmass', 'star', 'recently', 'a', 'new', 'class', 'of', 'these', 'systems', 'known', 'as', 'symbiotic', 'xray', 'binaries', 'with', 'a', 'neutron', 'star', 'with', 'a', 'mtype', 'giant', 'companion', '... | [-0.10677972211885978, 0.11883810409510225, -0.0662759683679278, 0.10537159421494603, -0.09041006486205494, -0.10214590614332872, 0.07842845716205535, 0.4362296653874949, -0.1497227161104663, -0.36378171960366706, 0.11846792148443296, -0.33189221718902107, -0.012693917053562187, 0.25279590225066334, -0.0396762675217663... |
708.3276 | Search for lepton flavor violating $\tau \to \ell V^0$ decays at Belle | We have searched for neutrinoless $\tau$ lepton decays into $\ell$ and $V^0$,
where $\ell$ stands for an electron or muon, and $V^0$ for a vector meson
($\phi$, $\omega$, $K^{*0}$ or $\bar{K}^{*0}$), using 543 fb$^{-1}$ of data
collected with the Belle detector at the KEKB asymmetric-energy $e^+e^-$
collider. No exce... | hep-ex | we have searched for neutrinoless tau lepton decays into ell and v0 where ell stands for an electron or muon and v0 for a vector meson phi omega k0 or bark0 using 543 fb1 of data collected with the belle detector at the kekb asymmetricenergy ee collider no excess of signal events over the expected background is observe... | [['we', 'have', 'searched', 'for', 'neutrinoless', 'tau', 'lepton', 'decays', 'into', 'ell', 'and', 'v0', 'where', 'ell', 'stands', 'for', 'an', 'electron', 'or', 'muon', 'and', 'v0', 'for', 'a', 'vector', 'meson', 'phi', 'omega', 'k0', 'or', 'bark0', 'using', '543', 'fb1', 'of', 'data', 'collected', 'with', 'the', 'be... | [-0.10330996667065831, 0.2020533817205465, -0.0018567763046419198, 0.09893085424421537, -0.035115426047746326, -0.15061564635139255, 0.10990581990413335, 0.2886070992088819, -0.1355032994683865, -0.3002792823795987, 0.02412966298314421, -0.4269978724403587, 0.08281495688334767, 0.22357027070695715, 0.1297988012243491, ... |
708.3277 | Hadron-quark mixed phase in hyperon stars | We analyze the different possibilities for the hadron-quark phase transition
occurring in beta-stable matter including hyperons in neutron stars. We use a
Brueckner-Hartree-Fock approach including hyperons for the hadronic equation of
state and a generalized MIT bag model for the quark part. We then point out in
deta... | nucl-th | we analyze the different possibilities for the hadronquark phase transition occurring in betastable matter including hyperons in neutron stars we use a bruecknerhartreefock approach including hyperons for the hadronic equation of state and a generalized mit bag model for the quark part we then point out in detail the d... | [['we', 'analyze', 'the', 'different', 'possibilities', 'for', 'the', 'hadronquark', 'phase', 'transition', 'occurring', 'in', 'betastable', 'matter', 'including', 'hyperons', 'in', 'neutron', 'stars', 'we', 'use', 'a', 'bruecknerhartreefock', 'approach', 'including', 'hyperons', 'for', 'the', 'hadronic', 'equation', '... | [-0.0668974658311595, 0.22872163519583721, -0.11069434762041094, 0.13321629948713767, -0.0882752373193701, -0.038574679985001525, 0.09717774702866952, 0.33358074832827816, -0.19918145505731466, -0.28612266748302406, 0.027449104799738815, -0.31326196071321283, -0.08000019661361171, 0.11495214933779851, 0.046983125249064... |
708.3278 | A Review of Procedure to Evolve Quantum Procedures | There exist quantum algorithms that are more efficient than their classical
counterparts; such algorithms were invented by Shor in 1994 and then Grover in
1996. A lack of invention since Grover's algorithm has been commonly attributed
to the non-intuitive nature of quantum algorithms to the classically trained
person... | quant-ph | there exist quantum algorithms that are more efficient than their classical counterparts such algorithms were invented by shor in 1994 and then grover in 1996 a lack of invention since grovers algorithm has been commonly attributed to the nonintuitive nature of quantum algorithms to the classically trained person thus ... | [['there', 'exist', 'quantum', 'algorithms', 'that', 'are', 'more', 'efficient', 'than', 'their', 'classical', 'counterparts', 'such', 'algorithms', 'were', 'invented', 'by', 'shor', 'in', '1994', 'and', 'then', 'grover', 'in', '1996', 'a', 'lack', 'of', 'invention', 'since', 'grovers', 'algorithm', 'has', 'been', 'com... | [-0.04740520763995224, 0.10294333892588634, -0.16255823823560336, 0.08531689995381617, -0.10482165194991835, -0.22226956259473263, 0.017303601125276236, 0.41051641311076353, -0.2447257859534339, -0.3525485753508887, 0.08738834521544159, -0.19518059293242326, -0.22185546340406836, 0.2668149850245467, -0.1140687300095376... |
708.3279 | Which weakly ramified group actions admit a universal formal
deformation? | Consider a formal (mixed-characteristic) deformation functor D of a
representation of a finite group G as automorphisms of a power series ring
k[[t]] over a perfect field k of positive characteristic. Assume that the
action of G is weakly ramified, i.e., the second ramification group is trivial.
Examples of such repr... | math.AG math.NT | consider a formal mixedcharacteristic deformation functor d of a representation of a finite group g as automorphisms of a power series ring kt over a perfect field k of positive characteristic assume that the action of g is weakly ramified ie the second ramification group is trivial examples of such representations are... | [['consider', 'a', 'formal', 'mixedcharacteristic', 'deformation', 'functor', 'd', 'of', 'a', 'representation', 'of', 'a', 'finite', 'group', 'g', 'as', 'automorphisms', 'of', 'a', 'power', 'series', 'ring', 'kt', 'over', 'a', 'perfect', 'field', 'k', 'of', 'positive', 'characteristic', 'assume', 'that', 'the', 'action... | [-0.25429493113607166, 0.0906158965799259, -0.15886077199876308, -0.015050335971172899, -0.12021411663293838, -0.14748593462258577, -0.005573757216334343, 0.3570403999313712, -0.3361794781833887, -0.1961147450990975, 0.09938236159458756, -0.257271574431099, -0.15046454233769327, 0.1944084769319743, -0.0937324105380103,... |
708.328 | Bulk viscosity and deflationary universes | We analyze the conditions that make possible the description of entropy
generation in the new inflationary model by means of a nearequilibrium process.
We show that there are situations in which the bulk viscosity cannot describe
particle production during the coherent field oscillations phase.
| astro-ph | we analyze the conditions that make possible the description of entropy generation in the new inflationary model by means of a nearequilibrium process we show that there are situations in which the bulk viscosity cannot describe particle production during the coherent field oscillations phase | [['we', 'analyze', 'the', 'conditions', 'that', 'make', 'possible', 'the', 'description', 'of', 'entropy', 'generation', 'in', 'the', 'new', 'inflationary', 'model', 'by', 'means', 'of', 'a', 'nearequilibrium', 'process', 'we', 'show', 'that', 'there', 'are', 'situations', 'in', 'which', 'the', 'bulk', 'viscosity', 'ca... | [-0.13329751753675131, 0.22576432016988596, -0.12201883883939849, 0.08542664355954913, -0.012688016410296162, -0.09498449500857128, 0.0231372002305256, 0.3343213031689326, -0.29370884250642526, -0.2485818288806412, 0.0725366869682653, -0.21282088276412753, -0.152280968039607, 0.19737591474679195, -0.05190331181511283, ... |
708.3281 | Chiral violations from one-loop domain wall fermions | We present results from lattice perturbation theory for the residual mass and
other matrix elements measuring the breaking of chiral symmetry in domain-wall
fermions. We have used the exact propagators corresponding to a finite number
of points in the fifth dimensions, and results were obtained for several
choices of... | hep-lat | we present results from lattice perturbation theory for the residual mass and other matrix elements measuring the breaking of chiral symmetry in domainwall fermions we have used the exact propagators corresponding to a finite number of points in the fifth dimensions and results were obtained for several choices of the ... | [['we', 'present', 'results', 'from', 'lattice', 'perturbation', 'theory', 'for', 'the', 'residual', 'mass', 'and', 'other', 'matrix', 'elements', 'measuring', 'the', 'breaking', 'of', 'chiral', 'symmetry', 'in', 'domainwall', 'fermions', 'we', 'have', 'used', 'the', 'exact', 'propagators', 'corresponding', 'to', 'a', ... | [-0.14103407899025255, 0.21214609604570656, -0.06828280887566507, 0.037294601842474476, -0.04227257279070237, -0.06621821350955333, 0.04631679292204073, 0.3649872357312303, -0.18181044726560897, -0.2793935838406189, 0.0984754309980557, -0.3035329073094405, -0.1307878052153123, 0.14229733614215198, 0.03074221911195379, ... |
708.3282 | Modeling Crowd Turbulence by Many-Particle Simulations | A recent study [D. Helbing, A. Johansson and H. Z. Al-Abideen, {\it Phys.
Rev. E} 75, 046109 (2007)] has revealed a "turbulent" state of pedestrian
flows, which is characterized by sudden displacements and causes the falling
and trampling of people. However, turbulent crowd motion is not reproduced well
by current ma... | physics.soc-ph | a recent study d helbing a johansson and h z alabideen it phys rev e 75 046109 2007 has revealed a turbulent state of pedestrian flows which is characterized by sudden displacements and causes the falling and trampling of people however turbulent crowd motion is not reproduced well by current manyparticle models due to... | [['a', 'recent', 'study', 'd', 'helbing', 'a', 'johansson', 'and', 'h', 'z', 'alabideen', 'it', 'phys', 'rev', 'e', '75', '046109', '2007', 'has', 'revealed', 'a', 'turbulent', 'state', 'of', 'pedestrian', 'flows', 'which', 'is', 'characterized', 'by', 'sudden', 'displacements', 'and', 'causes', 'the', 'falling', 'and'... | [-0.11704244210754763, 0.155001027339831, -0.09495151563019696, 0.05363866307863197, -0.03290595762648505, -0.08474704624498136, 0.02758064455163748, 0.34468756523581334, -0.24598588794469833, -0.3371203814454581, 0.031084650173808816, -0.27978646265317314, -0.14842421932877337, 0.16139238462017927, -0.0871760485548691... |
708.3283 | Sigma Model Q-balls and Q-Stars | A new kind of Q-balls is found: Q-balls in a non-linear sigma model. Their
main properties are presented together with those of their self-gravitating
generalization, sigma model Q-stars. A simple special limit of solutions which
are bound by gravity alone (``sigma stars'') is also discussed briefly. The
analysis is ... | gr-qc hep-th | a new kind of qballs is found qballs in a nonlinear sigma model their main properties are presented together with those of their selfgravitating generalization sigma model qstars a simple special limit of solutions which are bound by gravity alone sigma stars is also discussed briefly the analysis is based on calculati... | [['a', 'new', 'kind', 'of', 'qballs', 'is', 'found', 'qballs', 'in', 'a', 'nonlinear', 'sigma', 'model', 'their', 'main', 'properties', 'are', 'presented', 'together', 'with', 'those', 'of', 'their', 'selfgravitating', 'generalization', 'sigma', 'model', 'qstars', 'a', 'simple', 'special', 'limit', 'of', 'solutions', '... | [-0.13065272677936648, 0.1296447554543784, -0.05514206118174795, 0.13902026395585546, -0.06797920092267085, -0.15379821789922216, -0.02073059481055285, 0.3115266072563827, -0.19318768770310535, -0.3129766265727041, 0.10357860990600795, -0.31851954851439784, -0.13067126557503053, 0.18908929865784854, -0.0107783895204718... |
708.3284 | Interacting holographic dark energy in the scalar-Gauss-Bonnet gravity | In this paper we study cosmological application of interacting holographic
dark energy density in the scalar-Gauss-Bonnet framework. We employ the
interacting holographic model of dark energy to obtain the equation of state
for the interacting holographic energy density in spatially flat universe. Our
calculation sho... | hep-th | in this paper we study cosmological application of interacting holographic dark energy density in the scalargaussbonnet framework we employ the interacting holographic model of dark energy to obtain the equation of state for the interacting holographic energy density in spatially flat universe our calculation show taki... | [['in', 'this', 'paper', 'we', 'study', 'cosmological', 'application', 'of', 'interacting', 'holographic', 'dark', 'energy', 'density', 'in', 'the', 'scalargaussbonnet', 'framework', 'we', 'employ', 'the', 'interacting', 'holographic', 'model', 'of', 'dark', 'energy', 'to', 'obtain', 'the', 'equation', 'of', 'state', '... | [-0.12903732655847328, 0.1222261881871902, -0.1725011992248449, 0.10522798638904785, -0.06248985940313086, -0.14789330943467768, -0.06984011926118562, 0.3110796601531353, -0.19553816172868965, -0.3285452791246922, -0.01902860147071051, -0.25096186198928255, -0.0494033536933204, 0.09568383041868343, 0.05113255566461606,... |
708.3285 | Do $c\bar c n\bar n$ bound states exist? | The four--quark system $c\bar c n\bar n$ is studied in the framework of the
constituent quark model. Using different types of quark-quark potentials, we
solve the four--body Schr\"odinger equation by means of the hyperspherical
harmonic formalism. Exploring the low laying $J^{PC}$ states for different
isospin configu... | hep-ph hep-ex | the fourquark system cbar c nbar n is studied in the framework of the constituent quark model using different types of quarkquark potentials we solve the fourbody schrodinger equation by means of the hyperspherical harmonic formalism exploring the low laying jpc states for different isospin configurations no fourquark ... | [['the', 'fourquark', 'system', 'cbar', 'c', 'nbar', 'n', 'is', 'studied', 'in', 'the', 'framework', 'of', 'the', 'constituent', 'quark', 'model', 'using', 'different', 'types', 'of', 'quarkquark', 'potentials', 'we', 'solve', 'the', 'fourbody', 'schrodinger', 'equation', 'by', 'means', 'of', 'the', 'hyperspherical', '... | [-0.12091580133653455, 0.2238643277053009, -0.08464520301569399, 0.1104982374167508, -0.02942861975216325, -0.17274341822200107, 0.07015804061666131, 0.3295100956411083, -0.16450667810425454, -0.22564534138084627, -0.0789050699620252, -0.2849579505307381, -0.07180631770661064, 0.04894176008882841, 0.12415385763982639, ... |
708.3286 | Experiments with a Positivity Preserving Operator | We consider some multivariate rational functions which have (or are
conjectured to have) only positive coefficients in their series expansion. We
consider an operator that preserves positivity of series coefficients, and
apply the inverse of this operator to the rational functions. We obtain new
rational functions wh... | math.CO | we consider some multivariate rational functions which have or are conjectured to have only positive coefficients in their series expansion we consider an operator that preserves positivity of series coefficients and apply the inverse of this operator to the rational functions we obtain new rational functions which see... | [['we', 'consider', 'some', 'multivariate', 'rational', 'functions', 'which', 'have', 'or', 'are', 'conjectured', 'to', 'have', 'only', 'positive', 'coefficients', 'in', 'their', 'series', 'expansion', 'we', 'consider', 'an', 'operator', 'that', 'preserves', 'positivity', 'of', 'series', 'coefficients', 'and', 'apply',... | [-0.1133927478882912, 0.06039235426441018, -0.12505154548263228, 0.055705834247763396, -0.12113878211459599, -0.14301415537232282, -0.0031793270105923955, 0.3499832985973036, -0.31799099012907295, -0.19070206497594513, 0.14995628017995105, -0.2554386947178156, -0.1893722098855604, 0.17595803437792268, -0.06618235231301... |
708.3287 | Combinatorial Bethe ansatz and generalized periodic box-ball system | We reformulate the Kerov-Kirillov-Reshetikhin (KKR) map in the combinatorial
Bethe ansatz from paths to rigged configurations by introducing local energy
distribution in crystal base theory. Combined with an earlier result on the
inverse map, it completes the crystal interpretation of the KKR bijection for
U_q(\hat{s... | math.QA math-ph math.MP nlin.SI | we reformulate the kerovkirillovreshetikhin kkr map in the combinatorial bethe ansatz from paths to rigged configurations by introducing local energy distribution in crystal base theory combined with an earlier result on the inverse map it completes the crystal interpretation of the kkr bijection for u_qhatsl_2 as an a... | [['we', 'reformulate', 'the', 'kerovkirillovreshetikhin', 'kkr', 'map', 'in', 'the', 'combinatorial', 'bethe', 'ansatz', 'from', 'paths', 'to', 'rigged', 'configurations', 'by', 'introducing', 'local', 'energy', 'distribution', 'in', 'crystal', 'base', 'theory', 'combined', 'with', 'an', 'earlier', 'result', 'on', 'the... | [-0.1224000003274448, 0.04323336874915506, -0.07271024841431747, 0.06815022147972793, -0.06609390202690574, -0.07347762476762427, 0.03790155499762691, 0.3165065574966481, -0.35094753626514885, -0.25203838097479414, 0.05670704700956669, -0.24203913518611123, -0.18698712144704427, 0.16694480719811777, -0.0258951143087709... |
708.3288 | The probability of inflation in Loop Quantum Cosmology | The probability of there being sufficient inflation to solve the fine-tuning
associated with the horizon and flatness problems has recently been shown to be
exponentially small, within the context of classical general relativity. Here
this result is extended by considering loop quantum gravity effects, that are
signi... | gr-qc | the probability of there being sufficient inflation to solve the finetuning associated with the horizon and flatness problems has recently been shown to be exponentially small within the context of classical general relativity here this result is extended by considering loop quantum gravity effects that are significant... | [['the', 'probability', 'of', 'there', 'being', 'sufficient', 'inflation', 'to', 'solve', 'the', 'finetuning', 'associated', 'with', 'the', 'horizon', 'and', 'flatness', 'problems', 'has', 'recently', 'been', 'shown', 'to', 'be', 'exponentially', 'small', 'within', 'the', 'context', 'of', 'classical', 'general', 'relat... | [-0.11457334199318818, 0.18973844329205652, -0.09903599635775512, 0.16437190442423646, -0.05883561836866041, -0.18187974674122717, -0.028245913029725973, 0.32171625608073856, -0.2653759417589754, -0.2996096894533063, 0.09099349636041248, -0.21750937087150912, -0.13918967249725636, 0.18359143178289136, -0.11047442469304... |
708.3289 | Optimal stability estimate of the inverse boundary value problem by
partial measurements | In this work we establish log-type stability estimates for the inverse
potential and conductivity problems with partial Dirichlet-to-Neumann map,
where the Dirichlet data is homogeneous on the inaccessible part. This result,
to some extent, improves our former result on the partial data problem in which
log-log-type ... | math.AP | in this work we establish logtype stability estimates for the inverse potential and conductivity problems with partial dirichlettoneumann map where the dirichlet data is homogeneous on the inaccessible part this result to some extent improves our former result on the partial data problem in which loglogtype estimates w... | [['in', 'this', 'work', 'we', 'establish', 'logtype', 'stability', 'estimates', 'for', 'the', 'inverse', 'potential', 'and', 'conductivity', 'problems', 'with', 'partial', 'dirichlettoneumann', 'map', 'where', 'the', 'dirichlet', 'data', 'is', 'homogeneous', 'on', 'the', 'inaccessible', 'part', 'this', 'result', 'to', ... | [-0.06508435092258211, -0.023399512055425013, -0.040939162770400245, 0.04066272553921278, -0.1276524581148156, -0.052455377042749704, 0.04210662461665212, 0.311772562487393, -0.32184579731820495, -0.25939589522170775, 0.20293374432307876, -0.30618890378700225, -0.12098790375439793, 0.2152735979429313, -0.08682917900459... |
708.329 | The Centrality Dependence of Strange Baryon and Meson Production in
Cu+Cu and Au+Au sqrt(s_NN) = 200 GeV collisions | Transverse momentum spectra of Lambda and K0Short particles are presented for
Cu+Cu sqrt(s_NN) = 200 GeV collisions observed at STAR, and compared to Au+Au
measurements at the same energy. For both systems, a number of observables are
shown to increase at mid-rapidity (|y| < 0.5) with increasing centrality. These
are... | nucl-ex | transverse momentum spectra of lambda and k0short particles are presented for cucu sqrts_nn 200 gev collisions observed at star and compared to auau measurements at the same energy for both systems a number of observables are shown to increase at midrapidity y 05 with increasing centrality these are the integrated lamb... | [['transverse', 'momentum', 'spectra', 'of', 'lambda', 'and', 'k0short', 'particles', 'are', 'presented', 'for', 'cucu', 'sqrts_nn', '200', 'gev', 'collisions', 'observed', 'at', 'star', 'and', 'compared', 'to', 'auau', 'measurements', 'at', 'the', 'same', 'energy', 'for', 'both', 'systems', 'a', 'number', 'of', 'obser... | [-0.07205387159830087, 0.25836604270643737, -0.10200488489505102, 0.11605710893574363, 0.0851192025908532, -0.12602498331142745, -0.10675573474700911, 0.35565266448236604, -0.1637500018194204, -0.3660055861047661, -0.12194163286578592, -0.4536699595797153, 0.18227281138293785, 0.1747574819241231, 0.07856074931768288, 0... |
708.3291 | Mass formula for strange baryons in large $N_c$ QCD versus quark model | A previous work establishing a connection between a quark model, with
relativistic kinematics and a $Y$-confinement plus one gluon exchange, and the
$1/N_c$ expansion mass formula is extended to strange baryons. Both methods
predict values for the SU(3)-breaking mass terms which are in good agreement
with each other.... | hep-ph | a previous work establishing a connection between a quark model with relativistic kinematics and a yconfinement plus one gluon exchange and the 1n_c expansion mass formula is extended to strange baryons both methods predict values for the su3breaking mass terms which are in good agreement with each other strange and no... | [['a', 'previous', 'work', 'establishing', 'a', 'connection', 'between', 'a', 'quark', 'model', 'with', 'relativistic', 'kinematics', 'and', 'a', 'yconfinement', 'plus', 'one', 'gluon', 'exchange', 'and', 'the', '1n_c', 'expansion', 'mass', 'formula', 'is', 'extended', 'to', 'strange', 'baryons', 'both', 'methods', 'pr... | [-0.0829687410464976, 0.13786945597064915, -0.16107434288598596, 0.11523440670105628, -0.052746703922748564, -0.1437605335842818, 0.05957363712368533, 0.3222056927718222, -0.13501218191813677, -0.30125199681147935, -0.03596803205669857, -0.3407529692724347, -0.009472141670994461, 0.1266522659990005, 0.00092324146768078... |
708.3292 | New results and Possibilities in K Physics | Several topics in the Kphysics together with the new facility J-Parc are
introduced.
| hep-ex | several topics in the kphysics together with the new facility jparc are introduced | [['several', 'topics', 'in', 'the', 'kphysics', 'together', 'with', 'the', 'new', 'facility', 'jparc', 'are', 'introduced']] | [-0.01664922929679354, 0.24329471495002508, -0.08520935607763629, 0.03703771671280265, -0.14362415857613087, -0.16788767805943886, -0.028759533849855263, 0.35905696265399456, -0.23118817538488656, -0.3325845369448264, 0.09031282795088676, -0.3812648185218374, -0.04551086605836948, 0.2783100452894966, -0.046140615517894... |
708.3293 | Continuous Opinion Dynamics: Insights through Interactive Markov Chains | We reformulate the agent-based opinion dynamics models of Weisbuch-Deffuant
and Hegselmann-Krause as interactive Markov chains. So we switch the scope from
a finite number of n agents to a finite number of n opinion classes. Thus, we
will look at an infinite population distributed to opinion classes instead of
agents... | physics.soc-ph | we reformulate the agentbased opinion dynamics models of weisbuchdeffuant and hegselmannkrause as interactive markov chains so we switch the scope from a finite number of n agents to a finite number of n opinion classes thus we will look at an infinite population distributed to opinion classes instead of agents with re... | [['we', 'reformulate', 'the', 'agentbased', 'opinion', 'dynamics', 'models', 'of', 'weisbuchdeffuant', 'and', 'hegselmannkrause', 'as', 'interactive', 'markov', 'chains', 'so', 'we', 'switch', 'the', 'scope', 'from', 'a', 'finite', 'number', 'of', 'n', 'agents', 'to', 'a', 'finite', 'number', 'of', 'n', 'opinion', 'cla... | [-0.1403184330377441, 0.11966727317698174, -0.12250003333454235, 0.0842813012870745, -0.06095033877421743, -0.1508052552781569, 0.08577873425002998, 0.36658588361281613, -0.27589650833262847, -0.2944820658267977, 0.057023918401234996, -0.2659418481043898, -0.14125541908881412, 0.10349105345264364, -0.031626164956161607... |
708.3294 | Optical colours of AGN in the Extended Chandra Deep Field South:
Obscured black holes in early type galaxies | We investigate the optical colours of X-ray sources from the Extended Chandra
Deep Field South (ECDFS) using photometry from the COMBO-17 survey, aiming to
explore AGN - galaxy feedback models. The X-ray sources populate both the
``blue'' and the ``red sequence'' on the colour-magnitude diagram. However,
sources in t... | astro-ph | we investigate the optical colours of xray sources from the extended chandra deep field south ecdfs using photometry from the combo17 survey aiming to explore agn galaxy feedback models the xray sources populate both the blue and the red sequence on the colourmagnitude diagram however sources in the red sequence appear... | [['we', 'investigate', 'the', 'optical', 'colours', 'of', 'xray', 'sources', 'from', 'the', 'extended', 'chandra', 'deep', 'field', 'south', 'ecdfs', 'using', 'photometry', 'from', 'the', 'combo17', 'survey', 'aiming', 'to', 'explore', 'agn', 'galaxy', 'feedback', 'models', 'the', 'xray', 'sources', 'populate', 'both',... | [-0.02496841188046282, 0.1103441366287843, -0.12010491331608408, 0.12271060129007925, -0.13088952012242763, -0.05371341586303641, 0.0710603602278215, 0.48328407519445643, -0.17755307955300714, -0.31441104861607, 0.08411657905726745, -0.3224996879374183, -0.08601704220228835, 0.17928156699420605, -0.07857339488577068, -... |
708.3295 | Recent progress on the manipulation of single atoms in optical tweezers
for quantum computing | This paper summarizes our recent progress towards using single rubidium atoms
trapped in an optical tweezer to encode quantum information. We demonstrate
single qubit rotations on this system and measure the coherence of the qubit.
We move the quantum bit over distances of tens of microns and show that the
coherence ... | quant-ph | this paper summarizes our recent progress towards using single rubidium atoms trapped in an optical tweezer to encode quantum information we demonstrate single qubit rotations on this system and measure the coherence of the qubit we move the quantum bit over distances of tens of microns and show that the coherence is r... | [['this', 'paper', 'summarizes', 'our', 'recent', 'progress', 'towards', 'using', 'single', 'rubidium', 'atoms', 'trapped', 'in', 'an', 'optical', 'tweezer', 'to', 'encode', 'quantum', 'information', 'we', 'demonstrate', 'single', 'qubit', 'rotations', 'on', 'this', 'system', 'and', 'measure', 'the', 'coherence', 'of',... | [-0.12098593485322506, 0.20724302674523856, -0.019323472297914764, -0.02543954960317077, 0.06567886105793364, -0.17360576761557775, 0.09678796554559513, 0.504134242499576, -0.25193526100586444, -0.25510626966099476, -0.021353329752352747, -0.3114931874853723, -0.08326840286745744, 0.19994630356428816, -0.06133771051420... |
708.3296 | Observation of strong-coupling effects in a diluted magnetic
semiconductor (Ga,Fe)N | A direct observation of the giant Zeeman splitting of the free excitons in
(Ga,Fe)N is reported. The magnetooptical and magnetization data imply the
ferromagnetic sign and a reduced magnitude of the effective p-d exchange energy
governing the interaction between Fe^{3+} ions and holes in GaN, N_0 beta^(app)
= +0.5 +/... | cond-mat.mtrl-sci | a direct observation of the giant zeeman splitting of the free excitons in gafen is reported the magnetooptical and magnetization data imply the ferromagnetic sign and a reduced magnitude of the effective pd exchange energy governing the interaction between fe3 ions and holes in gan n_0 betaapp 05 02 ev this finding co... | [['a', 'direct', 'observation', 'of', 'the', 'giant', 'zeeman', 'splitting', 'of', 'the', 'free', 'excitons', 'in', 'gafen', 'is', 'reported', 'the', 'magnetooptical', 'and', 'magnetization', 'data', 'imply', 'the', 'ferromagnetic', 'sign', 'and', 'a', 'reduced', 'magnitude', 'of', 'the', 'effective', 'pd', 'exchange',... | [-0.1604914477467537, 0.18374299563467503, 0.031779240317021805, 0.07500755038112401, -0.022668483157952626, -0.11957894641906024, 0.12526298185965667, 0.3941122730076313, -0.2450716538478931, -0.3683420493205388, -0.08345168927994867, -0.3554104295372963, -0.05811224600300193, 0.11254800533254941, 0.07707183157404264,... |
708.3297 | Cosmological and phenomenological consequences of string theories | The Standard Model is the low-energy limit of a microscopic theory which
includes extra dimensions and new symmetries. A part of my thesis consisted in
constructing a new class of models with two extra dimensions. We showed that
these models can drive a dynamical symmetry breaking in four dimensions. In
particular, t... | hep-th hep-ph | the standard model is the lowenergy limit of a microscopic theory which includes extra dimensions and new symmetries a part of my thesis consisted in constructing a new class of models with two extra dimensions we showed that these models can drive a dynamical symmetry breaking in four dimensions in particular they are... | [['the', 'standard', 'model', 'is', 'the', 'lowenergy', 'limit', 'of', 'a', 'microscopic', 'theory', 'which', 'includes', 'extra', 'dimensions', 'and', 'new', 'symmetries', 'a', 'part', 'of', 'my', 'thesis', 'consisted', 'in', 'constructing', 'a', 'new', 'class', 'of', 'models', 'with', 'two', 'extra', 'dimensions', 'w... | [-0.12719938405991896, 0.20668920994722756, -0.0698976475758937, 0.09558280726322783, -0.07438905279327562, -0.177485004554172, -0.02434024323736304, 0.3325778136562988, -0.204049998867339, -0.319523454781291, 0.10546898457940425, -0.23127427165383013, -0.14667024853490834, 0.13450781692939717, -0.04423398663546296, 0.... |
708.3298 | Collapse times for attractive Bose-Einstein condensates | We argue that the main mechanism for condensate collapse in an attractive
Bose-Einstein condensate is the loss of coherence between atoms a finite
distance apart, rather than the growth of the occupation number in
noncondensate modes. Since the former mechanism is faster than the latter by a
factor of approximately 3... | cond-mat.other | we argue that the main mechanism for condensate collapse in an attractive boseeinstein condensate is the loss of coherence between atoms a finite distance apart rather than the growth of the occupation number in noncondensate modes since the former mechanism is faster than the latter by a factor of approximately 32 thi... | [['we', 'argue', 'that', 'the', 'main', 'mechanism', 'for', 'condensate', 'collapse', 'in', 'an', 'attractive', 'boseeinstein', 'condensate', 'is', 'the', 'loss', 'of', 'coherence', 'between', 'atoms', 'a', 'finite', 'distance', 'apart', 'rather', 'than', 'the', 'growth', 'of', 'the', 'occupation', 'number', 'in', 'non... | [-0.14693990517158195, 0.19897988386240156, -0.09062287187469857, 0.10544543046271429, 3.446299316627639e-05, -0.09181305548575308, 0.06497859771230391, 0.3196589492194887, -0.2187986780756286, -0.26837734790918016, 0.01353503042067002, -0.2575584520718881, -0.06305335130808609, 0.13400811355427972, 0.00911649651825428... |
708.3299 | The XMM-LSS catalogue: X-ray sources and associated optical data.
Version I | Following the presentation of the XMM-LSS X-ray source detection package by
Pacaud et al., we provide the source lists for the first 5.5 surveyed square
degrees. The catalogues pertain to the [0.5-2] and [2-10] keV bands and contain
in total 3385 point-like or extended sources above a detection likelihood of 15
in ei... | astro-ph | following the presentation of the xmmlss xray source detection package by pacaud et al we provide the source lists for the first 55 surveyed square degrees the catalogues pertain to the 052 and 210 kev bands and contain in total 3385 pointlike or extended sources above a detection likelihood of 15 in either band the ag... | [['following', 'the', 'presentation', 'of', 'the', 'xmmlss', 'xray', 'source', 'detection', 'package', 'by', 'pacaud', 'et', 'al', 'we', 'provide', 'the', 'source', 'lists', 'for', 'the', 'first', '55', 'surveyed', 'square', 'degrees', 'the', 'catalogues', 'pertain', 'to', 'the', '052', 'and', '210', 'kev', 'bands', 'a... | [-0.06830041224559492, 0.02765325274051492, -0.03091760117878252, 0.0944407063861159, -0.09862434918658784, -0.07799379865029528, 0.07524962528942176, 0.4711868882087278, -0.19261300330981612, -0.3925629082814227, 0.12068133513704747, -0.37240064279808677, 0.0007693201280486436, 0.21578167700697382, -0.0354128377368374... |
708.33 | Diffeomorphism Symmetry in the Lagrangian Formulation of Gravity | Starting from a knowledge of certain identities in the Lagrangian
description, the diffeomorphism transformations of metric and connection are
obtained for both the second order (metric) and the first order (Palatini)
formulations of gravity. The transformation laws of the connection and the
metric are derived indepe... | hep-th gr-qc | starting from a knowledge of certain identities in the lagrangian description the diffeomorphism transformations of metric and connection are obtained for both the second order metric and the first order palatini formulations of gravity the transformation laws of the connection and the metric are derived independently ... | [['starting', 'from', 'a', 'knowledge', 'of', 'certain', 'identities', 'in', 'the', 'lagrangian', 'description', 'the', 'diffeomorphism', 'transformations', 'of', 'metric', 'and', 'connection', 'are', 'obtained', 'for', 'both', 'the', 'second', 'order', 'metric', 'and', 'the', 'first', 'order', 'palatini', 'formulation... | [-0.14712232967010802, 0.0756154175388575, -0.12027474139661838, 0.08377346728391583, -0.10831394245097828, -0.08015234289147581, -0.01212424129092445, 0.29730305533545714, -0.2713576417041218, -0.3352443082775507, 0.07019708864552537, -0.2825008323416114, -0.20466498270009956, 0.07419054699130356, -0.07764033208756398... |
708.3301 | Cesaro's integral formula for the Bell numbers (corrected) | M. E. Cesaro (1885) gave a quite remarkable expression for the Bell number
--the number of partitions of an n-element set -- as a definite integral. This
note is an exposition, correcting a typographical error in the original.
| math.HO | m e cesaro 1885 gave a quite remarkable expression for the bell number the number of partitions of an nelement set as a definite integral this note is an exposition correcting a typographical error in the original | [['m', 'e', 'cesaro', '1885', 'gave', 'a', 'quite', 'remarkable', 'expression', 'for', 'the', 'bell', 'number', 'the', 'number', 'of', 'partitions', 'of', 'an', 'nelement', 'set', 'as', 'a', 'definite', 'integral', 'this', 'note', 'is', 'an', 'exposition', 'correcting', 'a', 'typographical', 'error', 'in', 'the', 'orig... | [-0.21286230448734117, 0.04920152236622557, -0.09810376778320484, 0.10118877031915896, -0.0484257722273469, -0.102768611565635, 0.05138243372375901, 0.27139764983911774, -0.21138607665823264, -0.3190690651535988, 0.04994316871995358, -0.29207267516569513, -0.12328627227327309, 0.1980630613397807, -0.18539218108698324, ... |
708.3302 | Universal behaviour of interfaces in 2d and dimensional reduction of
Nambu-Goto strings | We propose a simple effective model for the description of interfaces in 2d
statistical models, based on the first-order treatment of an action
corresponding to the length of the interface. The universal prediction of this
model for the interface free energy agrees with the result of an exact
calculation in the case ... | hep-th cond-mat.stat-mech hep-lat | we propose a simple effective model for the description of interfaces in 2d statistical models based on the firstorder treatment of an action corresponding to the length of the interface the universal prediction of this model for the interface free energy agrees with the result of an exact calculation in the case of th... | [['we', 'propose', 'a', 'simple', 'effective', 'model', 'for', 'the', 'description', 'of', 'interfaces', 'in', '2d', 'statistical', 'models', 'based', 'on', 'the', 'firstorder', 'treatment', 'of', 'an', 'action', 'corresponding', 'to', 'the', 'length', 'of', 'the', 'interface', 'the', 'universal', 'prediction', 'of', '... | [-0.11161288781728171, 0.07602789877402549, -0.07190573115573748, 0.05231692207847498, -0.0022636228064193, -0.12969548611229734, 0.00246339885494377, 0.2989133520499815, -0.2326401028711396, -0.2899389356327585, 0.02105424869245602, -0.24822427561105806, -0.15460143806530705, 0.18442026190636562, -0.002620995939190535... |
708.3303 | Influence of the L21 ordering degree on the magnetic properties in
Co2MnSi Heusler films | We report on the influence of the improved L21 ordering degree on the
magnetic properties of Co2MnSi Heusler films. Different fractions of the L21
phase are obtained by different post-growth annealing temperatures ranging from
350 degC to 500 degC. Room temperature magneto-optical Kerr effect measurements
reveal an i... | cond-mat.mtrl-sci | we report on the influence of the improved l21 ordering degree on the magnetic properties of co2mnsi heusler films different fractions of the l21 phase are obtained by different postgrowth annealing temperatures ranging from 350 degc to 500 degc room temperature magnetooptical kerr effect measurements reveal an increas... | [['we', 'report', 'on', 'the', 'influence', 'of', 'the', 'improved', 'l21', 'ordering', 'degree', 'on', 'the', 'magnetic', 'properties', 'of', 'co2mnsi', 'heusler', 'films', 'different', 'fractions', 'of', 'the', 'l21', 'phase', 'are', 'obtained', 'by', 'different', 'postgrowth', 'annealing', 'temperatures', 'ranging',... | [-0.12941079737025907, 0.2391892076942946, -0.03050937007956363, -0.06774210621777049, -0.00418576098965494, -0.0644453094744651, 0.106673511927231, 0.41248561950218116, -0.26331350772635087, -0.3738091468967341, 0.1003543735161046, -0.34059355457450124, -0.038299989834479936, 0.19038749815590053, 0.039433879641835555,... |
708.3304 | Protected Rabi oscillation induced by natural interactions among
physical qubits | For a system composed of nine qubits, we show that natural interactions among
the qubits induce the time evolution that can be regarded, at discrete times,
as the Rabi oscillation of a logical qubit. Neither fine tuning of the
parameters nor switching of the interactions is necessary. Although
straightforward applica... | quant-ph | for a system composed of nine qubits we show that natural interactions among the qubits induce the time evolution that can be regarded at discrete times as the rabi oscillation of a logical qubit neither fine tuning of the parameters nor switching of the interactions is necessary although straightforward application of... | [['for', 'a', 'system', 'composed', 'of', 'nine', 'qubits', 'we', 'show', 'that', 'natural', 'interactions', 'among', 'the', 'qubits', 'induce', 'the', 'time', 'evolution', 'that', 'can', 'be', 'regarded', 'at', 'discrete', 'times', 'as', 'the', 'rabi', 'oscillation', 'of', 'a', 'logical', 'qubit', 'neither', 'fine', '... | [-0.20087740657160455, 0.19003239469707348, -0.03148525569383892, 0.07288555935642609, -0.010219385214359238, -0.21932720577114084, 0.1019299447096968, 0.36557798518726, -0.2380361274052202, -0.31817695550787983, 0.06270769639254621, -0.17984193021410635, -0.1241202311906859, 0.2383270174516051, -0.048976215962948426, ... |
708.3305 | The role of pressure anisotropy on the maximum mass of cold compact
stars | We study the physical features of a class of exact solutions for cold compact
anisotropic stars. The effect of pressure anisotropy on the maximum mass and
surface redshift is analysed in the Vaidya-Tikekar model. It is shown that
maximum compactness, redshift and mass increase in the presence of anisotropic
pressures... | gr-qc | we study the physical features of a class of exact solutions for cold compact anisotropic stars the effect of pressure anisotropy on the maximum mass and surface redshift is analysed in the vaidyatikekar model it is shown that maximum compactness redshift and mass increase in the presence of anisotropic pressures numer... | [['we', 'study', 'the', 'physical', 'features', 'of', 'a', 'class', 'of', 'exact', 'solutions', 'for', 'cold', 'compact', 'anisotropic', 'stars', 'the', 'effect', 'of', 'pressure', 'anisotropy', 'on', 'the', 'maximum', 'mass', 'and', 'surface', 'redshift', 'is', 'analysed', 'in', 'the', 'vaidyatikekar', 'model', 'it', ... | [-0.1242026792509326, 0.1577998557748894, -0.056451212894171474, 0.0556285488147599, -0.09015090181492269, -0.04188069731462747, -0.009954122112443049, 0.4084079929937919, -0.1751546684342126, -0.32881457495192684, 0.08707943536768047, -0.30233599251757065, -0.05274520406189064, 0.2081718956702389, 0.005487111366043488... |
708.3306 | Carlitz q-Bernoulli numbers and q-Stirling numbers | In this paper we consider carlitz q-Bernoulli numbers and q-stirling numbers
of the first and the second kind. From these numbers we derive many interesting
formulae associated with q-Bernoulli numbers.
| math.NT | in this paper we consider carlitz qbernoulli numbers and qstirling numbers of the first and the second kind from these numbers we derive many interesting formulae associated with qbernoulli numbers | [['in', 'this', 'paper', 'we', 'consider', 'carlitz', 'qbernoulli', 'numbers', 'and', 'qstirling', 'numbers', 'of', 'the', 'first', 'and', 'the', 'second', 'kind', 'from', 'these', 'numbers', 'we', 'derive', 'many', 'interesting', 'formulae', 'associated', 'with', 'qbernoulli', 'numbers']] | [-0.2550255070750912, 0.1427091869576543, -0.04590905165920655, 0.16206289055990056, -0.1075390505294005, -0.07401093378042181, 0.04016225164523348, 0.22592508727684618, -0.31491267568587017, -0.3453182918330034, 0.07031132732129966, -0.259648817156752, -0.2680322880546252, 0.27388652172715716, -0.11034592473879457, 0.... |
708.3307 | A p-adic analogue of a formula of Ramanujan | During his lifetime, Ramanujan provided many formulae relating binomial sums
to special values of the Gamma function. Based on numerical computations, Van
Hamme recently conjectured $p$-adic analogues to such formulae. Using a
combination of ordinary and Gaussian hypergeometric series, we prove one of
these conjectur... | math.NT math.CO | during his lifetime ramanujan provided many formulae relating binomial sums to special values of the gamma function based on numerical computations van hamme recently conjectured padic analogues to such formulae using a combination of ordinary and gaussian hypergeometric series we prove one of these conjectures | [['during', 'his', 'lifetime', 'ramanujan', 'provided', 'many', 'formulae', 'relating', 'binomial', 'sums', 'to', 'special', 'values', 'of', 'the', 'gamma', 'function', 'based', 'on', 'numerical', 'computations', 'van', 'hamme', 'recently', 'conjectured', 'padic', 'analogues', 'to', 'such', 'formulae', 'using', 'a', 'c... | [-0.11882298741774219, 0.00730626870418847, -0.1609756464759509, 0.09982617025832749, -0.117311390551428, -0.13998482783014576, 0.04531329727809255, 0.26399098287026085, -0.28553138189017774, -0.26820114871693984, 0.06684032097044919, -0.28315383477860856, -0.20797880705859925, 0.3241730210267835, -0.06587375951930881,... |
708.3308 | Structure of Ann-categories and Mac Lane - Shukla cohomology | In this paper we study the structure of a class of categories having two
operations which satisfy axioms analoguos to that of rings. Such categories are
called "Ann - categories". We obtain the classification theorems for regular
Ann - categories and Ann - functors by using Mac Lane - Shukla cohomology of
rings. Thes... | math.CT | in this paper we study the structure of a class of categories having two operations which satisfy axioms analoguos to that of rings such categories are called ann categories we obtain the classification theorems for regular ann categories and ann functors by using mac lane shukla cohomology of rings these results give ... | [['in', 'this', 'paper', 'we', 'study', 'the', 'structure', 'of', 'a', 'class', 'of', 'categories', 'having', 'two', 'operations', 'which', 'satisfy', 'axioms', 'analoguos', 'to', 'that', 'of', 'rings', 'such', 'categories', 'are', 'called', 'ann', 'categories', 'we', 'obtain', 'the', 'classification', 'theorems', 'for... | [-0.15443437366334142, -0.056444950485754694, -0.0994740652500606, 0.06425804665243467, -0.021839877040904076, -0.13857662037289778, -0.002777665744718836, 0.3566345498576516, -0.33035384131534423, -0.27328061636109824, 0.11419958357325159, -0.17019215349840824, -0.16884938299228422, 0.1693445450214089, -0.203998723029... |
708.3309 | A combinatorial realization of the Heisenberg action on the space of
conformal blocks | This paper has been withdrawn by the author. Improved versions
(arXiv:1109.5548 and arXiv:0708.4190) are accepted.
| math.GT | this paper has been withdrawn by the author improved versions arxiv11095548 and arxiv07084190 are accepted | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'author', 'improved', 'versions', 'arxiv11095548', 'and', 'arxiv07084190', 'are', 'accepted']] | [-0.09711462904054385, 0.026011533927745543, -0.13960860569316608, 0.038432321538074084, -0.11763299457155742, -0.09331963368906425, -0.06389985712639128, 0.37687546014785767, -0.1961132247860615, -0.383865434389848, 0.15533824666188314, -0.347586807436668, -0.10139533117986642, 0.1074724426636329, -0.30052294668096763... |
708.331 | Stability properties for the higher dimensional catenoid in $\rr^{n+1}$ | This paper concerns some stability properties of higher dimensional catenoids
in $\rr^{n+1}$ with $n\ge 3$. We prove that higher dimensional catenoids have
index one. We use $\delta$-stablity for minimal hypersurfaces and show that the
catenoid is $\frac 2n$-stable and a complete $\frac 2n$-stable minimal
hypersurfac... | math.DG | this paper concerns some stability properties of higher dimensional catenoids in rrn1 with nge 3 we prove that higher dimensional catenoids have index one we use deltastablity for minimal hypersurfaces and show that the catenoid is frac 2nstable and a complete frac 2nstable minimal hypersurface is a catenoid or a hyper... | [['this', 'paper', 'concerns', 'some', 'stability', 'properties', 'of', 'higher', 'dimensional', 'catenoids', 'in', 'rrn1', 'with', 'nge', '3', 'we', 'prove', 'that', 'higher', 'dimensional', 'catenoids', 'have', 'index', 'one', 'we', 'use', 'deltastablity', 'for', 'minimal', 'hypersurfaces', 'and', 'show', 'that', 'th... | [-0.19533183270444474, 0.07651708631269764, -0.042479700000401126, 0.06740613591146509, -0.057656201366498544, -0.2046239538396006, -0.05616028600151798, 0.33200484665780605, -0.19663485727812113, -0.15733274134496847, 0.1620884430941946, -0.3429658304442439, -0.1641387753903441, 0.15563584864548033, -0.140383300959671... |
708.3311 | HST/STIS spectroscopy of the environment in the starburst core of M82 | [Abridged] We present high-resolution optical HST/STIS observations made with
two slits crossing four of the brightest starburst clumps in the vicinity of
the nucleus of M82. These provide H_alpha kinematics, extinction, electron
density and emission measures. From the radial velocity curves we confirm the
presence o... | astro-ph | abridged we present highresolution optical hststis observations made with two slits crossing four of the brightest starburst clumps in the vicinity of the nucleus of m82 these provide h_alpha kinematics extinction electron density and emission measures from the radial velocity curves we confirm the presence of a stella... | [['abridged', 'we', 'present', 'highresolution', 'optical', 'hststis', 'observations', 'made', 'with', 'two', 'slits', 'crossing', 'four', 'of', 'the', 'brightest', 'starburst', 'clumps', 'in', 'the', 'vicinity', 'of', 'the', 'nucleus', 'of', 'm82', 'these', 'provide', 'h_alpha', 'kinematics', 'extinction', 'electron',... | [-0.08627183695674595, 0.11186529429346129, -0.07797302390178697, 0.05604468548645069, -0.038438787394786116, -0.056444452255077306, 0.0442717425853052, 0.4214725595689854, -0.21041850675670368, -0.2868772146743833, 0.04656404967924269, -0.27600991188352103, -0.0214129857149539, 0.15371125103465477, 0.01602203600551318... |
708.3312 | Ab-initio calculation of the vibrational modes of SiH4, H2SiO, Si10H16,
and Si10H14O | We have studied the normal modes of hydrogenated and oxidized silicon
nanocrystals, namely SiH4 (silan), H2SiO (silanon), Si10H16 and Si10H14O. The
small clusters (SiH4 and H2SiO) have been used for convergence tests and their
bondlengths and frequencies have been compared with experimental and
theoretical reference ... | cond-mat.mtrl-sci | we have studied the normal modes of hydrogenated and oxidized silicon nanocrystals namely sih4 silan h2sio silanon si10h16 and si10h14o the small clusters sih4 and h2sio have been used for convergence tests and their bondlengths and frequencies have been compared with experimental and theoretical reference data for the... | [['we', 'have', 'studied', 'the', 'normal', 'modes', 'of', 'hydrogenated', 'and', 'oxidized', 'silicon', 'nanocrystals', 'namely', 'sih4', 'silan', 'h2sio', 'silanon', 'si10h16', 'and', 'si10h14o', 'the', 'small', 'clusters', 'sih4', 'and', 'h2sio', 'have', 'been', 'used', 'for', 'convergence', 'tests', 'and', 'their',... | [-0.026195115880354454, 0.10312200843503601, -0.11395352658276495, 0.03278471646634372, 0.055621150504846714, -0.09522207075435864, 0.05027086828149071, 0.4610299645677993, -0.16833613275697357, -0.27912805482169223, 0.07004111777182276, -0.3543720056743998, -0.0849735935757819, 0.11254681109842893, 0.05680064226402656... |
708.3313 | Observation of $\psi(4415)\to D \bar D{}^{*}_2(2460)$ decay using
initial-state radiation | We report the first observation of the $\psi(4415)$ resonance in the reaction
$\e^+e^-\to D^0 D^-\pi^+$ and a measurement of its cross section in the
center-of-mass energy range $4.0\mathrm{GeV}$ to $5.0\mathrm{GeV}$ with initial
state radiation. From a study of resonant structure in $\psi(4415)$ decay we
conclude th... | hep-ex | we report the first observation of the psi4415 resonance in the reaction eeto d0 dpi and a measurement of its cross section in the centerofmass energy range 40mathrmgev to 50mathrmgev with initial state radiation from a study of resonant structure in psi4415 decay we conclude that the psi4415to d0 dpi decay is dominate... | [['we', 'report', 'the', 'first', 'observation', 'of', 'the', 'psi4415', 'resonance', 'in', 'the', 'reaction', 'eeto', 'd0', 'dpi', 'and', 'a', 'measurement', 'of', 'its', 'cross', 'section', 'in', 'the', 'centerofmass', 'energy', 'range', '40mathrmgev', 'to', '50mathrmgev', 'with', 'initial', 'state', 'radiation', 'fr... | [-0.08310155394341213, 0.13979875353176893, -0.09486395287003468, 0.03112800730425999, -0.004323687951756552, -0.0899485285248024, 0.05644183737192168, 0.3095300492482731, -0.18893330273813153, -0.26538406330418873, -0.024052921681193613, -0.4264137198116226, 0.05066428003630724, 0.13977219357648976, 0.1313018938189888... |
708.3314 | Autocatalytic reaction on low-dimensional substrates | We discuss a model for the autocatalytic reaction $A+B\to 2A$ on substrates
where the reactants perform a compact exploration of the space, i.e., on
lattices whose spectral dimension $\tilde{d}$ is $< 2$. For finite systems, the
total time $\tau$ for the reaction to end scales according to two different
regimes, for ... | cond-mat.stat-mech | we discuss a model for the autocatalytic reaction abto 2a on substrates where the reactants perform a compact exploration of the space ie on lattices whose spectral dimension tilded is 2 for finite systems the total time tau for the reaction to end scales according to two different regimes for high and low concentratio... | [['we', 'discuss', 'a', 'model', 'for', 'the', 'autocatalytic', 'reaction', 'abto', '2a', 'on', 'substrates', 'where', 'the', 'reactants', 'perform', 'a', 'compact', 'exploration', 'of', 'the', 'space', 'ie', 'on', 'lattices', 'whose', 'spectral', 'dimension', 'tilded', 'is', '2', 'for', 'finite', 'systems', 'the', 'to... | [-0.10982989319940893, 0.1917875648203601, -0.03793202970452357, 0.06225637856745956, 0.01809233347686553, -0.12319295566029302, 0.08957988757032492, 0.35410061848020496, -0.24862976061043943, -0.235063464539807, 0.08221611293123626, -0.27105404484290174, -0.07150141505251933, 0.16564437720595246, 0.03911382788877434, ... |
708.3315 | Destruction of Anderson localization by a weak nonlinearity | We study numerically a spreading of an initially localized wave packet in a
one-dimensional discrete nonlinear Schr\"odinger lattice with disorder. We
demonstrate that above a certain critical strength of nonlinearity the Anderson
localization is destroyed and an unlimited subdiffusive spreading of the field
along th... | cond-mat.dis-nn nlin.CD | we study numerically a spreading of an initially localized wave packet in a onedimensional discrete nonlinear schrodinger lattice with disorder we demonstrate that above a certain critical strength of nonlinearity the anderson localization is destroyed and an unlimited subdiffusive spreading of the field along the latt... | [['we', 'study', 'numerically', 'a', 'spreading', 'of', 'an', 'initially', 'localized', 'wave', 'packet', 'in', 'a', 'onedimensional', 'discrete', 'nonlinear', 'schrodinger', 'lattice', 'with', 'disorder', 'we', 'demonstrate', 'that', 'above', 'a', 'certain', 'critical', 'strength', 'of', 'nonlinearity', 'the', 'anders... | [-0.20209896301385016, 0.24186986100721697, -0.011641955806408078, 0.052454325508733746, -0.009909387336665531, -0.16584040569141506, 0.01697271966622793, 0.36404403297929094, -0.29559522778727115, -0.17659846367314458, 0.06180719320109347, -0.3317356074578129, -0.15214863275177776, 0.1609394440543838, 0.02508276476437... |
708.3316 | Anisotropic magnetoresistance in nanocontacts | We present ab initio calculations of the evolution of anisotropic
magnetoresistance (AMR) in Ni nanocontacts from the ballistic to the tunnel
regime. We find an extraordinary enhancement of AMR, compared to bulk, in two
scenarios. In systems without localized states, like chemically pure break
junctions, large AMR on... | cond-mat.mes-hall cond-mat.mtrl-sci | we present ab initio calculations of the evolution of anisotropic magnetoresistance amr in ni nanocontacts from the ballistic to the tunnel regime we find an extraordinary enhancement of amr compared to bulk in two scenarios in systems without localized states like chemically pure break junctions large amr only occurs ... | [['we', 'present', 'ab', 'initio', 'calculations', 'of', 'the', 'evolution', 'of', 'anisotropic', 'magnetoresistance', 'amr', 'in', 'ni', 'nanocontacts', 'from', 'the', 'ballistic', 'to', 'the', 'tunnel', 'regime', 'we', 'find', 'an', 'extraordinary', 'enhancement', 'of', 'amr', 'compared', 'to', 'bulk', 'in', 'two', '... | [-0.2037450541795876, 0.15486843091373606, -0.03915214118583558, 0.024363163381797046, -0.012628746192114284, -0.12290192373061123, 0.029339155220301248, 0.36109184122716004, -0.2816738970046012, -0.3459028226789087, -0.041944296076857984, -0.32634276937012774, -0.06660708619612986, 0.18659879139830501, 0.0509778860487... |
708.3317 | On surface tension for compact stars | In an earlier treatment it was demonstrated that general relativity gives
higher values of surface tension in strange stars with quark matter than
neutron stars.We generate the modified Tolman-Oppenheimer-Volkoff equation to
incorporate anisotropic matter and use this to show that pressure anisotropy
provides for a w... | gr-qc | in an earlier treatment it was demonstrated that general relativity gives higher values of surface tension in strange stars with quark matter than neutron starswe generate the modified tolmanoppenheimervolkoff equation to incorporate anisotropic matter and use this to show that pressure anisotropy provides for a wide r... | [['in', 'an', 'earlier', 'treatment', 'it', 'was', 'demonstrated', 'that', 'general', 'relativity', 'gives', 'higher', 'values', 'of', 'surface', 'tension', 'in', 'strange', 'stars', 'with', 'quark', 'matter', 'than', 'neutron', 'starswe', 'generate', 'the', 'modified', 'tolmanoppenheimervolkoff', 'equation', 'to', 'in... | [-0.08310986405859391, 0.1944335265288828, -0.12665429630627234, 0.07762325706736495, -0.1244829465697209, -0.09211138758187493, -0.01143133624146382, 0.33024644463633496, -0.20182174329335492, -0.3517216608176629, -0.024369951983292896, -0.27477285083072883, -0.06897125959396362, 0.215194181073457, -0.0237427701180179... |
708.3318 | Phase Transitions in Pressurised Semiflexible Polymer Rings | We propose and study a model for the equilibrium statistical mechanics of a
pressurised semiflexible polymer ring. The Hamiltonian has a term which couples
to the algebraic area of the ring and a term which accounts for bending
(semiflexibility). The model allows for self-intersections. Using a combination
of Monte C... | cond-mat.stat-mech | we propose and study a model for the equilibrium statistical mechanics of a pressurised semiflexible polymer ring the hamiltonian has a term which couples to the algebraic area of the ring and a term which accounts for bending semiflexibility the model allows for selfintersections using a combination of monte carlo sim... | [['we', 'propose', 'and', 'study', 'a', 'model', 'for', 'the', 'equilibrium', 'statistical', 'mechanics', 'of', 'a', 'pressurised', 'semiflexible', 'polymer', 'ring', 'the', 'hamiltonian', 'has', 'a', 'term', 'which', 'couples', 'to', 'the', 'algebraic', 'area', 'of', 'the', 'ring', 'and', 'a', 'term', 'which', 'accoun... | [-0.14244020952024367, 0.11950884341959617, -0.11638025508034013, 0.051362571252559296, -0.002055789479702119, -0.11843209080891498, 0.05225243743039538, 0.3366958397557799, -0.27672074881647496, -0.2813765914333577, 0.10487965085784233, -0.27849892429579187, -0.11139246163926772, 0.18659211365376532, 0.011158256310451... |
708.3319 | A construction of Horikawa surface via Q-Gorenstein smoothings | In this article we prove that Fintushel-Stern's construction of Horikawa
surface, which is obtained from an elliptic surface via a rational blow-down
surgery in smooth category, can be performed in complex category. The main
technique involved is Q-Gorenstein smoothings.
| math.AG math.GT | in this article we prove that fintushelsterns construction of horikawa surface which is obtained from an elliptic surface via a rational blowdown surgery in smooth category can be performed in complex category the main technique involved is qgorenstein smoothings | [['in', 'this', 'article', 'we', 'prove', 'that', 'fintushelsterns', 'construction', 'of', 'horikawa', 'surface', 'which', 'is', 'obtained', 'from', 'an', 'elliptic', 'surface', 'via', 'a', 'rational', 'blowdown', 'surgery', 'in', 'smooth', 'category', 'can', 'be', 'performed', 'in', 'complex', 'category', 'the', 'main... | [-0.15299584301045308, 0.028114141290783524, -0.17946023668926686, 0.08313713811684209, -0.08325935470370147, -0.15134639138928974, -0.07067159190773964, 0.3600052859729681, -0.3508556997164702, -0.20135117775927752, 0.10815750659765819, -0.17857213160739496, -0.2443843600459588, 0.28403380431999, -0.2684875405990543, ... |
708.332 | Optical polarizabilities of large molecules measured in near-field
interferometry | We discuss a novel application of matter wave interferometry to characterize
the scalar optical polarizability of molecules at 532 nm. The interferometer
presented here consists of two material absorptive gratings and one central
optical phase grating. The interaction of the molecules with the standing light
wave is ... | quant-ph | we discuss a novel application of matter wave interferometry to characterize the scalar optical polarizability of molecules at 532 nm the interferometer presented here consists of two material absorptive gratings and one central optical phase grating the interaction of the molecules with the standing light wave is dete... | [['we', 'discuss', 'a', 'novel', 'application', 'of', 'matter', 'wave', 'interferometry', 'to', 'characterize', 'the', 'scalar', 'optical', 'polarizability', 'of', 'molecules', 'at', '532', 'nm', 'the', 'interferometer', 'presented', 'here', 'consists', 'of', 'two', 'material', 'absorptive', 'gratings', 'and', 'one', '... | [-0.14051821353073177, 0.15552135043514845, -0.06510790650788535, 0.00330270536773257, -0.023486993227822658, -0.11334546346965636, 0.024643088712826625, 0.4633259883261899, -0.19584766009018525, -0.2942734744367946, 0.009980598419833068, -0.2841249418675772, -0.10588335082866251, 0.18035934685379204, 0.066592453732195... |
708.3321 | CP Violation in Two Zero Texture Neutrino Mass Matrices | It has been shown that the neutrino mass matrices with two texture zeros in
the charged lepton basis predict non-zero 1-3 mixing and are necessarily CP
violating with one possible exception in class C for maximal mixing.
| hep-ph | it has been shown that the neutrino mass matrices with two texture zeros in the charged lepton basis predict nonzero 13 mixing and are necessarily cp violating with one possible exception in class c for maximal mixing | [['it', 'has', 'been', 'shown', 'that', 'the', 'neutrino', 'mass', 'matrices', 'with', 'two', 'texture', 'zeros', 'in', 'the', 'charged', 'lepton', 'basis', 'predict', 'nonzero', '13', 'mixing', 'and', 'are', 'necessarily', 'cp', 'violating', 'with', 'one', 'possible', 'exception', 'in', 'class', 'c', 'for', 'maximal',... | [-0.11121637091304906, 0.2944419902522822, 0.061610004386386356, 0.10220901776306532, -0.04443796950618963, -0.24820168824816072, -0.00922776126881709, 0.32302114546198296, -0.18969605389881777, -0.2993891678775686, 0.08561413346261189, -0.3139964904560632, -0.07411719647210997, 0.09804332578504407, 0.07036887673107353... |
708.3322 | Do we know eventually p(e)? | A quasi-particle model is employed to derive from available lattice QCD
calculations an equation of state useable in hydrodynamical simulations of the
expansion stage of strongly interacting matter created in ultra-relativistic
heavy-ion collisions. Various lattice results give an astonishing agreement of
the pressur... | hep-ph | a quasiparticle model is employed to derive from available lattice qcd calculations an equation of state useable in hydrodynamical simulations of the expansion stage of strongly interacting matter created in ultrarelativistic heavyion collisions various lattice results give an astonishing agreement of the pressure as a... | [['a', 'quasiparticle', 'model', 'is', 'employed', 'to', 'derive', 'from', 'available', 'lattice', 'qcd', 'calculations', 'an', 'equation', 'of', 'state', 'useable', 'in', 'hydrodynamical', 'simulations', 'of', 'the', 'expansion', 'stage', 'of', 'strongly', 'interacting', 'matter', 'created', 'in', 'ultrarelativistic',... | [-0.11028512049504695, 0.19695190542543117, -0.12788227914618502, 0.05978857106832868, -0.02286402474288389, -0.04636971343609487, 0.04684146427294899, 0.3116187969604449, -0.23460073143631358, -0.3101021948831607, 0.04944860229524639, -0.2842648033260929, -0.03268964492328326, 0.12092381607688152, 0.056197783609842074... |
708.3323 | Enhancement of the Gilbert damping constant due to spin pumping in
noncollinear ferromagnet/nonmagnet/ferromagnet trilayer systems | We analyzed the enhancement of the Gilbert damping constant due to spin
pumping in non-collinear ferromagnet / non-magnet / ferromagnet trilayer
systems. We show that the Gilbert damping constant depends both on the
precession angle of the magnetization of the free layer and on the direction of
the magntization of th... | cond-mat.mes-hall cond-mat.other | we analyzed the enhancement of the gilbert damping constant due to spin pumping in noncollinear ferromagnet nonmagnet ferromagnet trilayer systems we show that the gilbert damping constant depends both on the precession angle of the magnetization of the free layer and on the direction of the magntization of the fixed l... | [['we', 'analyzed', 'the', 'enhancement', 'of', 'the', 'gilbert', 'damping', 'constant', 'due', 'to', 'spin', 'pumping', 'in', 'noncollinear', 'ferromagnet', 'nonmagnet', 'ferromagnet', 'trilayer', 'systems', 'we', 'show', 'that', 'the', 'gilbert', 'damping', 'constant', 'depends', 'both', 'on', 'the', 'precession', 'a... | [-0.2788723472675139, 0.1718462461351671, 0.028784228495858384, -0.018939222505485468, -0.11603702303854692, -0.11842403047238335, 0.0393541361431055, 0.36155356173262454, -0.3197958029975945, -0.2767921548731851, 0.016825649644791458, -0.23857628517417293, -0.10335571109317243, 0.23565184735608372, 0.05154864179591337... |
708.3324 | Single-crystal growth and magnetic properties of the metallic molybdate
pyrochlore Sm2Mo2O7 | We have successfully grown cm3-size single crystals of the
metallic-ferromagnet Sm2Mo2O7 by the floating-zone method using an infrared-red
image furnace. The growth difficulties and the remedies found using a 2-mirror
image furnace are discussed. Magnetization studies along the three crystalline
axes of the compound ... | cond-mat.str-el cond-mat.mtrl-sci | we have successfully grown cm3size single crystals of the metallicferromagnet sm2mo2o7 by the floatingzone method using an infraredred image furnace the growth difficulties and the remedies found using a 2mirror image furnace are discussed magnetization studies along the three crystalline axes of the compound are prese... | [['we', 'have', 'successfully', 'grown', 'cm3size', 'single', 'crystals', 'of', 'the', 'metallicferromagnet', 'sm2mo2o7', 'by', 'the', 'floatingzone', 'method', 'using', 'an', 'infraredred', 'image', 'furnace', 'the', 'growth', 'difficulties', 'and', 'the', 'remedies', 'found', 'using', 'a', '2mirror', 'image', 'furnac... | [-0.06952721931797973, 0.12399261899862707, -0.07566358158522743, -0.045470307922480094, -0.03503701161845761, -0.09263407682873688, 0.04191772892313488, 0.4476472405101157, -0.21903709243288486, -0.26576307876887967, 0.1170317764488696, -0.2901666163135383, -0.09158804681215246, 0.2325653048011206, -0.0112927694473478... |
708.3325 | Generalised compact spheres in electric fields | We present exact solutions to the Einstein-Maxwell system of equations in
spherically symmetric gravitational fields with a specified form of the
electric field intensity. The condition of pressure isotropy yields a
difference equation with variable, rational coefficients. In an earlier
treatment this condition was i... | gr-qc | we present exact solutions to the einsteinmaxwell system of equations in spherically symmetric gravitational fields with a specified form of the electric field intensity the condition of pressure isotropy yields a difference equation with variable rational coefficients in an earlier treatment this condition was integra... | [['we', 'present', 'exact', 'solutions', 'to', 'the', 'einsteinmaxwell', 'system', 'of', 'equations', 'in', 'spherically', 'symmetric', 'gravitational', 'fields', 'with', 'a', 'specified', 'form', 'of', 'the', 'electric', 'field', 'intensity', 'the', 'condition', 'of', 'pressure', 'isotropy', 'yields', 'a', 'difference... | [-0.14126646571505738, 0.06544450815485418, -0.09583426680359425, 0.059952322624134594, -0.10029704448287234, -0.13012975880481076, -0.03957406423205152, 0.3147008822045543, -0.18475533742457628, -0.2867698074704168, 0.05389780943832276, -0.2742524544045216, -0.13260576212978592, 0.18394031178093317, 0.0009183787712545... |
708.3326 | On the moduli stack of commutative, 1-parameter formal Lie groups | We attempt to develop a general algebro-geometric study of the moduli stack
of commutative, 1-parameter formal Lie groups. We emphasize the pro-algebraic
structure of this stack: it is the inverse limit, over varying n, of moduli
stacks of n-buds, and these latter stacks are algebraic. Our main results
pertain to asp... | math.AG math.CT | we attempt to develop a general algebrogeometric study of the moduli stack of commutative 1parameter formal lie groups we emphasize the proalgebraic structure of this stack it is the inverse limit over varying n of moduli stacks of nbuds and these latter stacks are algebraic our main results pertain to aspects of the h... | [['we', 'attempt', 'to', 'develop', 'a', 'general', 'algebrogeometric', 'study', 'of', 'the', 'moduli', 'stack', 'of', 'commutative', '1parameter', 'formal', 'lie', 'groups', 'we', 'emphasize', 'the', 'proalgebraic', 'structure', 'of', 'this', 'stack', 'it', 'is', 'the', 'inverse', 'limit', 'over', 'varying', 'n', 'of'... | [-0.19772401974951648, 0.0320423518262624, -0.12475914515958852, 0.0941011875710753, -0.12229724292620926, -0.06650907786405948, 0.04699179576429348, 0.3739773745547576, -0.33387270408222475, -0.25428744988987245, 0.0881158255744748, -0.19434364285903521, -0.13017273456677345, 0.1975358514092773, -0.17183436293446694, ... |
708.3327 | Effects of Unparticles on Running of Gauge Couplings | Unparticles charged under a gauge group can contribute to the running of the
gauge coupling. We show that a scalar unparticle of scaling dimension d
contributes to the \beta function a term that is (2-d) times that from a scalar
particle in the same representation. This result has important implications on
asymptotic... | hep-ph | unparticles charged under a gauge group can contribute to the running of the gauge coupling we show that a scalar unparticle of scaling dimension d contributes to the beta function a term that is 2d times that from a scalar particle in the same representation this result has important implications on asymptotic freedom... | [['unparticles', 'charged', 'under', 'a', 'gauge', 'group', 'can', 'contribute', 'to', 'the', 'running', 'of', 'the', 'gauge', 'coupling', 'we', 'show', 'that', 'a', 'scalar', 'unparticle', 'of', 'scaling', 'dimension', 'd', 'contributes', 'to', 'the', 'beta', 'function', 'a', 'term', 'that', 'is', '2d', 'times', 'that... | [-0.10934488457054473, 0.25470536031173724, -0.08709003714940104, 0.13074462699453132, -0.09519110283790491, -0.16855549089825497, -0.007280541265096802, 0.322518994152928, -0.21500891704971975, -0.3153130126496156, 0.04512075035749242, -0.2741901427531281, -0.0780564817193991, 0.12138456082246146, 0.025261331836764628... |
708.3328 | Electron-electron Relaxation in Disordered Interacting Systems | We study the relaxation of a non-equilibrium carrier distribution under the
influence of the electron-electron interaction in the presence of disorder.
Based on the Anderson model, our Hamiltonian is composed from a single particle
part including the disorder and a two-particle part accounting for the Coulomb
interac... | cond-mat.dis-nn cond-mat.str-el | we study the relaxation of a nonequilibrium carrier distribution under the influence of the electronelectron interaction in the presence of disorder based on the anderson model our hamiltonian is composed from a single particle part including the disorder and a twoparticle part accounting for the coulomb interaction we... | [['we', 'study', 'the', 'relaxation', 'of', 'a', 'nonequilibrium', 'carrier', 'distribution', 'under', 'the', 'influence', 'of', 'the', 'electronelectron', 'interaction', 'in', 'the', 'presence', 'of', 'disorder', 'based', 'on', 'the', 'anderson', 'model', 'our', 'hamiltonian', 'is', 'composed', 'from', 'a', 'single', ... | [-0.15298156986486108, 0.18622818737409064, -0.10241705768128177, 0.048074055457142266, 0.03522215647408591, -0.09680784378008592, 0.03251847111073042, 0.3048606297437338, -0.27745501467558953, -0.26372205684449346, 0.01735429042933642, -0.2915694900226617, -0.12016764177112943, 0.1379540962987535, 0.05575303452473784,... |
708.3329 | Finite dimensional modules and perpendicular subcategories | We explain how, under some hypotheses, one can construct a sequence of finite
dimensional $kG$-modules that lie in certain prescribed additive subcategories,
but whose direct limits do not. We use these to show that many of the
triangulated quotients of $\Mod$ are not generated, as triangulated categories,
by the cor... | math.RT | we explain how under some hypotheses one can construct a sequence of finite dimensional kgmodules that lie in certain prescribed additive subcategories but whose direct limits do not we use these to show that many of the triangulated quotients of mod are not generated as triangulated categories by the corresponding quo... | [['we', 'explain', 'how', 'under', 'some', 'hypotheses', 'one', 'can', 'construct', 'a', 'sequence', 'of', 'finite', 'dimensional', 'kgmodules', 'that', 'lie', 'in', 'certain', 'prescribed', 'additive', 'subcategories', 'but', 'whose', 'direct', 'limits', 'do', 'not', 'we', 'use', 'these', 'to', 'show', 'that', 'many',... | [-0.14442346072033177, 0.06300719402497634, -0.0740985978748007, 0.09156446945692959, -0.08006415643793499, -0.13173991642442756, -0.023527782558913118, 0.4127312975229117, -0.3901959119749994, -0.21758897583289394, 0.12272623853139772, -0.17030442053259448, -0.13104913577212599, 0.199235238971847, -0.21430854682393116... |
708.333 | Swift/XRT monitoring of five orbital cycles of LSI +61 303 | LSI +61 303 is one of the most interesting high-mass X-ray binaries owing to
its spatially resolved radio emission and its TeV emission, generally
attributed to non-thermal particles in an accretion-powered relativistic jet or
in the termination shock of the relativistic wind of a young pulsar. Also, the
nature of th... | astro-ph | lsi 61 303 is one of the most interesting highmass xray binaries owing to its spatially resolved radio emission and its tev emission generally attributed to nonthermal particles in an accretionpowered relativistic jet or in the termination shock of the relativistic wind of a young pulsar also the nature of the compact ... | [['lsi', '61', '303', 'is', 'one', 'of', 'the', 'most', 'interesting', 'highmass', 'xray', 'binaries', 'owing', 'to', 'its', 'spatially', 'resolved', 'radio', 'emission', 'and', 'its', 'tev', 'emission', 'generally', 'attributed', 'to', 'nonthermal', 'particles', 'in', 'an', 'accretionpowered', 'relativistic', 'jet', '... | [-0.10246743025892802, 0.13484748932979826, -0.0751640835026922, 0.14735440010270845, -0.09610395843834839, -0.11926609596476552, 0.06473155191324784, 0.4616179002399466, -0.2129774768691277, -0.3724824908803489, 0.09490940046539958, -0.3376126921327735, -0.005261333264715442, 0.23196308080037947, -0.020819095006641166... |
708.3331 | A radio air shower surface detector as an extension for IceCube and
IceTop | The IceCube neutrino detector is built into the Antarctic ice sheet at the
South Pole to measure high energy neutrinos. For this, 4800 photomultiplier
tubes (PMTs) are being deployed at depths between 1450 and 2450 meters into the
ice to measure neutrino induced charged particles like muons. IceTop is a
surface air s... | astro-ph | the icecube neutrino detector is built into the antarctic ice sheet at the south pole to measure high energy neutrinos for this 4800 photomultiplier tubes pmts are being deployed at depths between 1450 and 2450 meters into the ice to measure neutrino induced charged particles like muons icetop is a surface air shower d... | [['the', 'icecube', 'neutrino', 'detector', 'is', 'built', 'into', 'the', 'antarctic', 'ice', 'sheet', 'at', 'the', 'south', 'pole', 'to', 'measure', 'high', 'energy', 'neutrinos', 'for', 'this', '4800', 'photomultiplier', 'tubes', 'pmts', 'are', 'being', 'deployed', 'at', 'depths', 'between', '1450', 'and', '2450', 'm... | [-0.07858138948686647, 0.35454268430963803, -0.020948391455061898, 0.1266962492784312, -0.030155966831064158, -0.00232309237849172, -0.0736974990276804, 0.436165934244355, -0.15917814720248047, -0.41061003294333326, 0.04738166455769845, -0.41667766795381084, 0.008530844116818856, 0.1707750178558834, 0.04198391127891347... |
708.3332 | Predictions from type II see-saw mechanism in SU(5) | We propose a simple, testable, SU(5) model within the context of the type II
neutrino see-saw mechanism. It is based on requiring renormalizability, the
absence of any other matter fields besides those already present in the
Standard Model and consistency with all experimental data. These "minimal"
requirements, toge... | hep-ph | we propose a simple testable su5 model within the context of the type ii neutrino seesaw mechanism it is based on requiring renormalizability the absence of any other matter fields besides those already present in the standard model and consistency with all experimental data these minimal requirements together with gro... | [['we', 'propose', 'a', 'simple', 'testable', 'su5', 'model', 'within', 'the', 'context', 'of', 'the', 'type', 'ii', 'neutrino', 'seesaw', 'mechanism', 'it', 'is', 'based', 'on', 'requiring', 'renormalizability', 'the', 'absence', 'of', 'any', 'other', 'matter', 'fields', 'besides', 'those', 'already', 'present', 'in',... | [-0.0640156388768113, 0.20474669457387432, -0.05749023424028616, 0.18177103840393308, -0.14188040922474587, -0.2278932730751735, 0.04721833748290394, 0.3444341351901194, -0.21142231071249803, -0.29096316463563227, 0.0517584108624568, -0.22776811868848007, -0.10550259511498078, 0.106876764366154, 0.03316306333142844, 0.... |
708.3333 | Existence and properties of geometric quotients | In this paper, we study quotients of groupoids and coarse moduli spaces of
stacks in a general setting. Geometric quotients are not always categorical,
but we present a natural topological condition under which a geometric quotient
is categorical. We also show the existence of geometric quotients of finite
flat group... | math.AG | in this paper we study quotients of groupoids and coarse moduli spaces of stacks in a general setting geometric quotients are not always categorical but we present a natural topological condition under which a geometric quotient is categorical we also show the existence of geometric quotients of finite flat groupoids a... | [['in', 'this', 'paper', 'we', 'study', 'quotients', 'of', 'groupoids', 'and', 'coarse', 'moduli', 'spaces', 'of', 'stacks', 'in', 'a', 'general', 'setting', 'geometric', 'quotients', 'are', 'not', 'always', 'categorical', 'but', 'we', 'present', 'a', 'natural', 'topological', 'condition', 'under', 'which', 'a', 'geome... | [-0.15041857320776897, 0.04545912802464089, -0.17509889276246132, 0.16033953348699126, -0.1444815111536424, -0.13961272507688952, 0.014153108307051934, 0.36930028667438375, -0.32235623831019816, -0.19787436020018045, 0.1420421276435943, -0.17302556303233696, -0.1313403373927746, 0.21952817865841778, -0.2577271241586185... |
708.3334 | Communication regimes in opinion dynamics: Changing the number of
communicating agents | This article contributes in four ways to the research on time-discrete
continuous opinion dynamics with compromising agents. First, communication
regimes are introduced as an elementary concept of opinion dynamic models.
Second, we develop a model that covers two major models of continuous opinion
dynamics, i.e. the ... | physics.soc-ph | this article contributes in four ways to the research on timediscrete continuous opinion dynamics with compromising agents first communication regimes are introduced as an elementary concept of opinion dynamic models second we develop a model that covers two major models of continuous opinion dynamics ie the basic mode... | [['this', 'article', 'contributes', 'in', 'four', 'ways', 'to', 'the', 'research', 'on', 'timediscrete', 'continuous', 'opinion', 'dynamics', 'with', 'compromising', 'agents', 'first', 'communication', 'regimes', 'are', 'introduced', 'as', 'an', 'elementary', 'concept', 'of', 'opinion', 'dynamic', 'models', 'second', '... | [-0.09082341374148829, 0.11734260226915537, -0.09905055115500895, 0.07126834323773017, -0.09496770651581196, -0.1618506767643759, 0.08942696863176444, 0.3578421463115284, -0.2885592751921369, -0.2975561521087702, 0.08140091935369688, -0.25440718932793693, -0.18064758305643827, 0.14661096659166595, -0.06471577050576273,... |
708.3335 | On the interrelation between monopoles, vortices, topological charge and
chiral symmetry breaking: an analysis using overlap fermions for SU(2) | We study the properties of configurations from which P-vortices on one hand
or Abelian monopoles on the other hand have been removed. We find that the zero
modes and the band of non-zero modes close to zero disappear from the spectrum
of the overlap Dirac operator, confirming the absence of topological charge and
qua... | hep-lat | we study the properties of configurations from which pvortices on one hand or abelian monopoles on the other hand have been removed we find that the zero modes and the band of nonzero modes close to zero disappear from the spectrum of the overlap dirac operator confirming the absence of topological charge and quark con... | [['we', 'study', 'the', 'properties', 'of', 'configurations', 'from', 'which', 'pvortices', 'on', 'one', 'hand', 'or', 'abelian', 'monopoles', 'on', 'the', 'other', 'hand', 'have', 'been', 'removed', 'we', 'find', 'that', 'the', 'zero', 'modes', 'and', 'the', 'band', 'of', 'nonzero', 'modes', 'close', 'to', 'zero', 'di... | [-0.12737483309209346, 0.2500485493391752, -0.0979542289543897, 0.10879291293770074, -0.027813388593494894, -0.11540399309061468, 0.08328123253583908, 0.36149426563084125, -0.18139079865068197, -0.28072110008448364, 0.08326607374753803, -0.33613289131224156, -0.06150068815052509, 0.1225153427850455, 0.01323405245691537... |
708.3336 | Far-field fluorescence microscopy beyond the diffraction limit:
Fluorescence imaging with ultrahigh resolution | Fluorescence microscopy is an important and extensively utilised tool for
imaging biological systems. However, the image resolution that can be obtained
has a limit as defined through the laws of diffraction. Demand for improved
resolution has stimulated research into developing methods to image beyond the
diffractio... | physics.bio-ph | fluorescence microscopy is an important and extensively utilised tool for imaging biological systems however the image resolution that can be obtained has a limit as defined through the laws of diffraction demand for improved resolution has stimulated research into developing methods to image beyond the diffraction lim... | [['fluorescence', 'microscopy', 'is', 'an', 'important', 'and', 'extensively', 'utilised', 'tool', 'for', 'imaging', 'biological', 'systems', 'however', 'the', 'image', 'resolution', 'that', 'can', 'be', 'obtained', 'has', 'a', 'limit', 'as', 'defined', 'through', 'the', 'laws', 'of', 'diffraction', 'demand', 'for', 'i... | [0.0026548676527081393, 0.07545505741993702, -0.09334295630677898, 0.031081438820777286, -0.04170283322962813, -0.10175456358199446, -0.02182307267963536, 0.47486411856535155, -0.27736793930491066, -0.304859299885316, 0.14448922160519367, -0.29199041339815557, -0.15951395996360698, 0.2988225052722244, -0.07296041377350... |
708.3337 | Sterile neutrino signals from supernovae | We investigate the effects of a mixing of active and sterile neutrinos on the
ratios of supernova electron neutrino flux ($F_e$) and antineutrino flux
($F_{\bar e}$) to the total flux of the other neutrino and antineutrino
flavours ($F_a$). We assume that the heaviest (in the normal hierarchy)
Standard Model neutrino... | hep-ph | we investigate the effects of a mixing of active and sterile neutrinos on the ratios of supernova electron neutrino flux f_e and antineutrino flux f_bar e to the total flux of the other neutrino and antineutrino flavours f_a we assume that the heaviest in the normal hierarchy standard model neutrino nu_3 mixes with a s... | [['we', 'investigate', 'the', 'effects', 'of', 'a', 'mixing', 'of', 'active', 'and', 'sterile', 'neutrinos', 'on', 'the', 'ratios', 'of', 'supernova', 'electron', 'neutrino', 'flux', 'f_e', 'and', 'antineutrino', 'flux', 'f_bar', 'e', 'to', 'the', 'total', 'flux', 'of', 'the', 'other', 'neutrino', 'and', 'antineutrino'... | [-0.10335991274889396, 0.31047872696173096, 0.028920151325671568, 0.18093216227286535, 0.0019326062123898578, -0.08639783162785614, 0.11463454651200901, 0.3214857297423093, -0.20859433672512356, -0.32288077078435734, 0.0045838470621358445, -0.2878090031849949, -0.0044601413704778835, 0.1611709699338383, 0.0772366498434... |
708.3338 | Ergodic properties of a class of non-Markovian processes | We study a fairly general class of time-homogeneous stochastic evolutions
driven by noises that are not white in time. As a consequence, the resulting
processes do not have the Markov property. In this setting, we obtain
constructive criteria for the uniqueness of stationary solutions that are very
close in spirit to... | math.PR math.DS | we study a fairly general class of timehomogeneous stochastic evolutions driven by noises that are not white in time as a consequence the resulting processes do not have the markov property in this setting we obtain constructive criteria for the uniqueness of stationary solutions that are very close in spirit to the ex... | [['we', 'study', 'a', 'fairly', 'general', 'class', 'of', 'timehomogeneous', 'stochastic', 'evolutions', 'driven', 'by', 'noises', 'that', 'are', 'not', 'white', 'in', 'time', 'as', 'a', 'consequence', 'the', 'resulting', 'processes', 'do', 'not', 'have', 'the', 'markov', 'property', 'in', 'this', 'setting', 'we', 'obt... | [-0.10204620127326357, 0.13168072919389176, -0.1038836589470662, 0.07055366806821031, -0.0351731118754467, -0.1117015505728206, 0.05410533771406815, 0.4058824646214168, -0.27665681508509166, -0.22595159823219932, 0.14924234571981015, -0.19053303542920572, -0.13209356016390203, 0.22202194966780145, -0.09659586775445653,... |
708.3339 | Crowd turbulence: the physics of crowd disasters | The panic stampede is a serious concern during mass events like soccer
championship games. Despite huge numbers of security forces and crowd control
measures, hundreds of lives are lost in crowd disasters each year. An analysis
of video recordings of the annual pilgrimage in Makkah reveals how high-density
crowds dev... | physics.soc-ph physics.flu-dyn | the panic stampede is a serious concern during mass events like soccer championship games despite huge numbers of security forces and crowd control measures hundreds of lives are lost in crowd disasters each year an analysis of video recordings of the annual pilgrimage in makkah reveals how highdensity crowds develop t... | [['the', 'panic', 'stampede', 'is', 'a', 'serious', 'concern', 'during', 'mass', 'events', 'like', 'soccer', 'championship', 'games', 'despite', 'huge', 'numbers', 'of', 'security', 'forces', 'and', 'crowd', 'control', 'measures', 'hundreds', 'of', 'lives', 'are', 'lost', 'in', 'crowd', 'disasters', 'each', 'year', 'an... | [-0.16400767798672933, 0.1552206115498013, -0.11568540722498151, 0.11828825552947819, -0.07038302385232977, -0.0826237322228243, 0.040022410398929335, 0.3278974997582006, -0.18176081324698495, -0.3711197763742482, 0.13819887050519103, -0.35425936963531324, -0.17050031067223334, 0.17965936352361422, -0.2503904304390804,... |
708.334 | Stability of Metastable Vacua in Gauge Mediated SUSY Breaking Models
with Ultra Light Gravitino | Recently Murayama and Nomura proposed a simple scheme to construct the gauge
mediation models, using metastable supersymmetry breaking vacua. It has a
possibility to predict the ultra light gravitino mass m_{3/2} \lesssim 16 eV,
while such a light gravitino may destabilize the metastable vacua. We
investigate stabili... | hep-ph | recently murayama and nomura proposed a simple scheme to construct the gauge mediation models using metastable supersymmetry breaking vacua it has a possibility to predict the ultra light gravitino mass m_32 lesssim 16 ev while such a light gravitino may destabilize the metastable vacua we investigate stability of the ... | [['recently', 'murayama', 'and', 'nomura', 'proposed', 'a', 'simple', 'scheme', 'to', 'construct', 'the', 'gauge', 'mediation', 'models', 'using', 'metastable', 'supersymmetry', 'breaking', 'vacua', 'it', 'has', 'a', 'possibility', 'to', 'predict', 'the', 'ultra', 'light', 'gravitino', 'mass', 'm_32', 'lesssim', '16', ... | [-0.12655311378635345, 0.3097460430178598, -0.03905370721082774, 0.17298744673532765, -0.05045265359841587, -0.1787902275062797, 0.07263541971934179, 0.31877965675742037, -0.18427344371523377, -0.3377396373919422, 0.08456798916919187, -0.24155869648881978, -0.0028969452926708807, 0.13252192362579668, -0.007916204499891... |
708.3341 | Browsing through 3D representations of unstructured picture collections:
an empirical study | The paper presents a 3D interactive representation of fairly large picture
collections which facilitates browsing through unstructured sets of icons or
pictures. Implementation of this representation implies choosing between two
visualization strategies: users may either manipulate the view (OV) or be
immersed in it ... | cs.HC | the paper presents a 3d interactive representation of fairly large picture collections which facilitates browsing through unstructured sets of icons or pictures implementation of this representation implies choosing between two visualization strategies users may either manipulate the view ov or be immersed in it iv the... | [['the', 'paper', 'presents', 'a', '3d', 'interactive', 'representation', 'of', 'fairly', 'large', 'picture', 'collections', 'which', 'facilitates', 'browsing', 'through', 'unstructured', 'sets', 'of', 'icons', 'or', 'pictures', 'implementation', 'of', 'this', 'representation', 'implies', 'choosing', 'between', 'two', ... | [-0.09104072688757603, 0.04391069685880211, -0.10024246441377006, 0.04984134728498436, -0.1386566685576891, -0.18465209677654865, 0.08381321194284627, 0.4323126556480239, -0.210395465805677, -0.396720691363263, 0.04534570945643595, -0.3092635227688428, -0.13814553201543808, 0.14435278124513168, -0.13553850913163404, -0... |
708.3342 | NMSSM neutralino dark matter | We study the viability of the lightest neutralino as a dark matter candidate
in the Next-to-Minimal Supersymmetric Standard Model. Taking into account
accelerator constraints as well as bounds on low-energy observables, and
imposing consistency with present bounds on the neutralino relic density, we
address the prosp... | hep-ph | we study the viability of the lightest neutralino as a dark matter candidate in the nexttominimal supersymmetric standard model taking into account accelerator constraints as well as bounds on lowenergy observables and imposing consistency with present bounds on the neutralino relic density we address the prospects for... | [['we', 'study', 'the', 'viability', 'of', 'the', 'lightest', 'neutralino', 'as', 'a', 'dark', 'matter', 'candidate', 'in', 'the', 'nexttominimal', 'supersymmetric', 'standard', 'model', 'taking', 'into', 'account', 'accelerator', 'constraints', 'as', 'well', 'as', 'bounds', 'on', 'lowenergy', 'observables', 'and', 'im... | [-0.08820485186419989, 0.22040025149717143, -0.065125996781219, 0.1737931861774996, -0.09813806418035376, -0.15755583129725173, 0.05323988695040737, 0.28651396174621035, -0.19328956847128115, -0.3916146645812612, 0.04634882092206298, -0.26865586611981457, 0.06396785924750331, 0.14770101326468743, 0.052537711952371814, ... |
708.3343 | Thermal gravitational waves | There is a lot of current interest in sources of gravitational waves and
active ongoing projects to detect such radiation, such as the LIGO project.
These are long wavelength, low frequency gravitational waves. LISA would be
sensitive to much longer wavelengths and lower fluxes. However compact stellar
objects can ge... | astro-ph | there is a lot of current interest in sources of gravitational waves and active ongoing projects to detect such radiation such as the ligo project these are long wavelength low frequency gravitational waves lisa would be sensitive to much longer wavelengths and lower fluxes however compact stellar objects can generate ... | [['there', 'is', 'a', 'lot', 'of', 'current', 'interest', 'in', 'sources', 'of', 'gravitational', 'waves', 'and', 'active', 'ongoing', 'projects', 'to', 'detect', 'such', 'radiation', 'such', 'as', 'the', 'ligo', 'project', 'these', 'are', 'long', 'wavelength', 'low', 'frequency', 'gravitational', 'waves', 'lisa', 'wou... | [-0.10264839018774709, 0.24090772653488737, -0.054657688893769915, 0.1500687699786412, -0.13299356673868667, -0.04374668908605695, -0.00473259552994645, 0.3812408575518547, -0.2034989595413208, -0.3225164138810023, 0.09021562499508849, -0.31242673972523527, -0.026932966448427912, 0.2666606732546107, -0.0105697877533537... |
708.3344 | Higgs-mass predictions | A compilation of Higgs-mass predictions is proposed
| hep-ph hep-th | a compilation of higgsmass predictions is proposed | [['a', 'compilation', 'of', 'higgsmass', 'predictions', 'is', 'proposed']] | [-0.09734199515410832, -0.06670423756752696, -0.14187154883984476, 0.013805349041441721, -0.1819510686078242, -0.12672353688893573, 0.05864329769143036, 0.2965493564094816, -0.10652377296771322, -0.3147659754114492, 0.03625461592205933, -0.30197510176471304, -0.0015800301916897297, 0.26469030124800547, -0.0237846224169... |
708.3345 | Transitions involving conical magnetic phases in a model with bilinear
and biquadratic interactions | In a previous work a model was proposed for the phase transitions of crystals
with localized magnetic moments which at low temperature have a "conical"
arrangement that at higher T transforms into a more symmetrical structure
(depending on the compound) before becoming totally disordered. The model
assumes bilinear a... | cond-mat.stat-mech | in a previous work a model was proposed for the phase transitions of crystals with localized magnetic moments which at low temperature have a conical arrangement that at higher t transforms into a more symmetrical structure depending on the compound before becoming totally disordered the model assumes bilinear and biqu... | [['in', 'a', 'previous', 'work', 'a', 'model', 'was', 'proposed', 'for', 'the', 'phase', 'transitions', 'of', 'crystals', 'with', 'localized', 'magnetic', 'moments', 'which', 'at', 'low', 'temperature', 'have', 'a', 'conical', 'arrangement', 'that', 'at', 'higher', 't', 'transforms', 'into', 'a', 'more', 'symmetrical',... | [-0.11088343371366868, 0.1724695567022902, -0.07776049689032491, 0.04544749863287862, -0.021423909043754054, -0.12761794847179334, 0.07539016303831134, 0.37899064877466565, -0.23721504798319576, -0.3058735096222325, 0.03631164142313338, -0.3104712936128008, -0.10803022120153295, 0.16018227458899392, 0.05806719894178383... |
708.3346 | Fluctuations in the Site Disordered Traveling Salesman Problem | We extend a previous statistical mechanical treatment of the traveling
salesman problem by defining a discrete "site disordered'' problem in which
fluctuations about saddle points can be computed. The results clarify the basis
of our original treatment, and illuminate but do not resolve the difficulties
of taking the... | cond-mat.dis-nn | we extend a previous statistical mechanical treatment of the traveling salesman problem by defining a discrete site disordered problem in which fluctuations about saddle points can be computed the results clarify the basis of our original treatment and illuminate but do not resolve the difficulties of taking the zero t... | [['we', 'extend', 'a', 'previous', 'statistical', 'mechanical', 'treatment', 'of', 'the', 'traveling', 'salesman', 'problem', 'by', 'defining', 'a', 'discrete', 'site', 'disordered', 'problem', 'in', 'which', 'fluctuations', 'about', 'saddle', 'points', 'can', 'be', 'computed', 'the', 'results', 'clarify', 'the', 'basi... | [-0.11556960279371456, 0.10261540918976866, -0.12306792308975543, 0.09668884165252425, -0.08937975288634854, -0.12354320003318467, 0.1085838789502824, 0.324298947409261, -0.3042438409424254, -0.27775938908702563, 0.0939836516689476, -0.26028951284076485, -0.10926816160125392, 0.15474401401297655, -0.09150868043070659, ... |
708.3347 | Lens spaces obtainable by surgery on doubly primitive knots | In this paper, we consider which lens spaces are obtainable by Dehn surgery
described by Berge on doubly primitive knots. It is given an algorithm to
decide whether a given lens space is obtainable by such surgery. Also included
is a complete characterization of such surgery yielding lens spaces with Klein
bottles.
| math.GT | in this paper we consider which lens spaces are obtainable by dehn surgery described by berge on doubly primitive knots it is given an algorithm to decide whether a given lens space is obtainable by such surgery also included is a complete characterization of such surgery yielding lens spaces with klein bottles | [['in', 'this', 'paper', 'we', 'consider', 'which', 'lens', 'spaces', 'are', 'obtainable', 'by', 'dehn', 'surgery', 'described', 'by', 'berge', 'on', 'doubly', 'primitive', 'knots', 'it', 'is', 'given', 'an', 'algorithm', 'to', 'decide', 'whether', 'a', 'given', 'lens', 'space', 'is', 'obtainable', 'by', 'such', 'surge... | [-0.17413193619666764, 0.10304234283690815, -0.07491965344748817, 0.09942148477645017, -0.1335734067699657, -0.18533348025252613, -0.030349945271154866, 0.3967791259861909, -0.24687039393645066, -0.32033815009232897, 0.16019153035953282, -0.23199914064473257, -0.2314581246688389, 0.283054260429568, -0.20678412611596286... |
708.3348 | Lorentz violation and the proper-time method | In this paper, we apply the proper-time method to generate the
Lorentz-violating Chern-Simons terms in the four-dimensional Yang-Mills and
non-linearized gravity theories. It is shown that the coefficient of the
induced Chern-Simons term is finite but regularization dependent.
| hep-th | in this paper we apply the propertime method to generate the lorentzviolating chernsimons terms in the fourdimensional yangmills and nonlinearized gravity theories it is shown that the coefficient of the induced chernsimons term is finite but regularization dependent | [['in', 'this', 'paper', 'we', 'apply', 'the', 'propertime', 'method', 'to', 'generate', 'the', 'lorentzviolating', 'chernsimons', 'terms', 'in', 'the', 'fourdimensional', 'yangmills', 'and', 'nonlinearized', 'gravity', 'theories', 'it', 'is', 'shown', 'that', 'the', 'coefficient', 'of', 'the', 'induced', 'chernsimons'... | [-0.14017303568911493, 0.19594899974273225, -0.10807658653510244, 0.08805765198408871, -0.11890626512467861, -0.1398246068213331, -0.09971682396165929, 0.2799959915052903, -0.17965521545786606, -0.23561903845371776, 0.00944143366436229, -0.26783911690213963, -0.2932239156216383, 0.07569762356089134, -0.1124580279482822... |
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