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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710.3553 | Homotopical interpretation of globular complex by multipointed d-space | Globular complexes were introduced by E. Goubault and the author in
arXiv:math/0107060 to model higher dimensional automata. Globular complexes are
topological spaces equipped with a globular decomposition which is the directed
analogue of the cellular decomposition of a CW-complex. We prove that there
exists a combi... | math.AT math.CT | globular complexes were introduced by e goubault and the author in arxivmath0107060 to model higher dimensional automata globular complexes are topological spaces equipped with a globular decomposition which is the directed analogue of the cellular decomposition of a cwcomplex we prove that there exists a combinatorial... | [['globular', 'complexes', 'were', 'introduced', 'by', 'e', 'goubault', 'and', 'the', 'author', 'in', 'arxivmath0107060', 'to', 'model', 'higher', 'dimensional', 'automata', 'globular', 'complexes', 'are', 'topological', 'spaces', 'equipped', 'with', 'a', 'globular', 'decomposition', 'which', 'is', 'the', 'directed', '... | [-0.13261618623144777, 0.05820029043117721, -0.08314146432307323, 0.11394165551633836, -0.09701328335658592, -0.1158041520153775, 0.015526441674606473, 0.3810902242031362, -0.39077528850997195, -0.23320616257310012, 0.03437508005052318, -0.21722960494096494, -0.15236411905646616, 0.15147501811555591, -0.186179385776175... |
710.3554 | Optimization of a Neutrino Factory: Discovery Machine versus Precision
Instrument | We discuss the optimization of a neutrino factory experiment for the purpose
of sin^2(2theta_13), mass hierarchy, and CP violation discoveries. This
includes a review of possible optimization strategies, as well as an
application of these to different sin^2(2theta_13) regions.
| hep-ph | we discuss the optimization of a neutrino factory experiment for the purpose of sin22theta_13 mass hierarchy and cp violation discoveries this includes a review of possible optimization strategies as well as an application of these to different sin22theta_13 regions | [['we', 'discuss', 'the', 'optimization', 'of', 'a', 'neutrino', 'factory', 'experiment', 'for', 'the', 'purpose', 'of', 'sin22theta_13', 'mass', 'hierarchy', 'and', 'cp', 'violation', 'discoveries', 'this', 'includes', 'a', 'review', 'of', 'possible', 'optimization', 'strategies', 'as', 'well', 'as', 'an', 'applicatio... | [-0.10533678321502148, 0.1151657673945943, -0.004248851193831517, 0.14726798803223154, -0.08900616356195548, -0.12538753588421223, 0.1303580571921208, 0.2844713783034912, -0.2458304422788131, -0.3772103671366588, 0.162257179701462, -0.2539036994537291, -0.10371662619022223, 0.21481981491431212, -0.016750746931976233, 0... |
710.3555 | H-> WZ and H->Wgamma in the MSSM | We study the complete one loop contribution to $H^\pm\to W^\pm Z$ and $H^\pm
\to W^\pm \gamma$ in the Minimal Supersymmetric Standard Model (MSSM).
| hep-ph | we study the complete one loop contribution to hpmto wpm z and hpm to wpm gamma in the minimal supersymmetric standard model mssm | [['we', 'study', 'the', 'complete', 'one', 'loop', 'contribution', 'to', 'hpmto', 'wpm', 'z', 'and', 'hpm', 'to', 'wpm', 'gamma', 'in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm']] | [0.014373031849770443, 0.22957895667818579, 0.06630798526432204, 0.2087774118003638, -0.12804577442938866, -0.29622570060841413, 0.06504025067324223, 0.33010227275688364, -0.23347039164408392, -0.13064621437502943, -0.027812252747421357, -0.3294555572995349, 0.03162226060648327, 0.09482142992277184, 0.02565209583743758... |
710.3556 | Graphene Terahertz Plasmon Oscillators | In this paper we propose and discuss coherent terahertz sources based on
charge density wave (plasmon) amplification in two dimensional graphene. The
coupling of the plasmons to interband electron-hole transitions in population
inverted graphene layers can lead to plasmon amplification through stimulated
emission. Pl... | cond-mat.mes-hall cond-mat.mtrl-sci | in this paper we propose and discuss coherent terahertz sources based on charge density wave plasmon amplification in two dimensional graphene the coupling of the plasmons to interband electronhole transitions in population inverted graphene layers can lead to plasmon amplification through stimulated emission plasmon g... | [['in', 'this', 'paper', 'we', 'propose', 'and', 'discuss', 'coherent', 'terahertz', 'sources', 'based', 'on', 'charge', 'density', 'wave', 'plasmon', 'amplification', 'in', 'two', 'dimensional', 'graphene', 'the', 'coupling', 'of', 'the', 'plasmons', 'to', 'interband', 'electronhole', 'transitions', 'in', 'population'... | [-0.16086830417101353, 0.19387911315020545, -0.006358424435594792, 0.011511531422556138, -0.0487060064067509, -0.12928120141528202, 0.08299105440109154, 0.4626640347356828, -0.22380847038411295, -0.268942931814995, -0.05664159714194965, -0.27563111732609025, -0.16062247102759433, 0.22170134169197586, 0.0126304505362070... |
710.3557 | Luminous Red Galaxies in hierarchical cosmologies | Luminous red galaxies (LRGs) are much rarer and more massive than L*
galaxies. Coupled with their extreme colours, LRGs therefore provide a
demanding testing ground for the physics of massive galaxy formation. We
present the first self-consistent predictions for the abundance and properties
of LRGs in hierarchical st... | astro-ph | luminous red galaxies lrgs are much rarer and more massive than l galaxies coupled with their extreme colours lrgs therefore provide a demanding testing ground for the physics of massive galaxy formation we present the first selfconsistent predictions for the abundance and properties of lrgs in hierarchical structure f... | [['luminous', 'red', 'galaxies', 'lrgs', 'are', 'much', 'rarer', 'and', 'more', 'massive', 'than', 'l', 'galaxies', 'coupled', 'with', 'their', 'extreme', 'colours', 'lrgs', 'therefore', 'provide', 'a', 'demanding', 'testing', 'ground', 'for', 'the', 'physics', 'of', 'massive', 'galaxy', 'formation', 'we', 'present', '... | [-0.03491564771884084, 0.09151444683659683, -0.08062884505926418, 0.11374134281186046, -0.10050121584170638, -0.05785323913190879, 0.03436109686370793, 0.3926431294804549, -0.08116773720199146, -0.40969506126761535, 0.002453335384713498, -0.2998033727479648, -0.032870601189214914, 0.18533068265507158, -0.04026800263851... |
710.3558 | Magnetic fields and the dynamics of spiral galaxies | We investigate the dynamics of magnetic fields in spiral galaxies by
performing 3D MHD simulations of galactic discs subject to a spiral potential.
Recent hydrodynamic simulations have demonstrated the formation of inter-arm
spurs as well as spiral arm molecular clouds provided the ISM model includes a
cold HI phase.... | astro-ph | we investigate the dynamics of magnetic fields in spiral galaxies by performing 3d mhd simulations of galactic discs subject to a spiral potential recent hydrodynamic simulations have demonstrated the formation of interarm spurs as well as spiral arm molecular clouds provided the ism model includes a cold hi phase we f... | [['we', 'investigate', 'the', 'dynamics', 'of', 'magnetic', 'fields', 'in', 'spiral', 'galaxies', 'by', 'performing', '3d', 'mhd', 'simulations', 'of', 'galactic', 'discs', 'subject', 'to', 'a', 'spiral', 'potential', 'recent', 'hydrodynamic', 'simulations', 'have', 'demonstrated', 'the', 'formation', 'of', 'interarm',... | [-0.1445217851614241, 0.16775892851177351, -0.046384799771113996, 0.06334137313984733, -0.04044329786631295, -0.025520569827749192, -0.013275857577358201, 0.40561030994034064, -0.22649552914552443, -0.3053488915819984, 0.04554584100367147, -0.2245842496764598, -0.07759496642463554, 0.1632080826723858, 0.050342389048886... |
710.3559 | Separation of Attractors in 1-modulus Quantum Corrected Special Geometry | We study the attractor equations for a quantum corrected prepotential
F=t^3+i\lambda, with \lambda \in R,which is the only correction which preserves
the axion shift symmetry and modifies the geometry.
By performing computations in the ``magnetic'' charge configuration, we find
evidence for interesting phenomena (a... | hep-th | we study the attractor equations for a quantum corrected prepotential ft3ilambda with lambda in rwhich is the only correction which preserves the axion shift symmetry and modifies the geometry by performing computations in the magnetic charge configuration we find evidence for interesting phenomena absent in the classi... | [['we', 'study', 'the', 'attractor', 'equations', 'for', 'a', 'quantum', 'corrected', 'prepotential', 'ft3ilambda', 'with', 'lambda', 'in', 'rwhich', 'is', 'the', 'only', 'correction', 'which', 'preserves', 'the', 'axion', 'shift', 'symmetry', 'and', 'modifies', 'the', 'geometry', 'by', 'performing', 'computations', 'i... | [-0.19528933070635177, 0.13131457218847606, -0.09038843750900957, 0.08670381360845465, -0.028485745387063978, -0.12863970961738028, 0.06537938961882214, 0.24431900564089137, -0.2457984825684074, -0.25900348975270426, 0.07233590906253085, -0.28050310620686636, -0.12831295877398555, 0.16560125650996166, 0.014404162537209... |
710.356 | HE 0515-4414 - an unusual sub-damped Ly alpha system revisited | Using STIS and VLT UVES observations we have examined the ionization,
abundances, and differential dust depletion of metals, the kinematic structure,
and the physical conditions in the molecular hydrogen-bearing sub-damped Ly
alpha system toward HE 0515-4414 at z = 1.15. The velocity interval of
associated metal line... | astro-ph | using stis and vlt uves observations we have examined the ionization abundances and differential dust depletion of metals the kinematic structure and the physical conditions in the molecular hydrogenbearing subdamped ly alpha system toward he 05154414 at z 115 the velocity interval of associated metal lines extends for... | [['using', 'stis', 'and', 'vlt', 'uves', 'observations', 'we', 'have', 'examined', 'the', 'ionization', 'abundances', 'and', 'differential', 'dust', 'depletion', 'of', 'metals', 'the', 'kinematic', 'structure', 'and', 'the', 'physical', 'conditions', 'in', 'the', 'molecular', 'hydrogenbearing', 'subdamped', 'ly', 'alph... | [-0.049027157101737356, 0.1438988125104153, 0.04284374026396094, 0.03464998888169412, 0.0021321584137827445, -0.13047125156062486, 0.03589861109180169, 0.4420515506517613, -0.17687949072748024, -0.3471943979861636, 0.006361312687198964, -0.32674521458124695, 0.0021096399942434384, 0.12735576739301013, -0.02592473231604... |
710.3561 | Stationary probability density of stochastic search processes in global
optimization | A method for the construction of approximate analytical expressions for the
stationary marginal densities of general stochastic search processes is
proposed. By the marginal densities, regions of the search space that with high
probability contain the global optima can be readily defined. The density
estimation proce... | cs.AI cond-mat.stat-mech cs.NE | a method for the construction of approximate analytical expressions for the stationary marginal densities of general stochastic search processes is proposed by the marginal densities regions of the search space that with high probability contain the global optima can be readily defined the density estimation procedure ... | [['a', 'method', 'for', 'the', 'construction', 'of', 'approximate', 'analytical', 'expressions', 'for', 'the', 'stationary', 'marginal', 'densities', 'of', 'general', 'stochastic', 'search', 'processes', 'is', 'proposed', 'by', 'the', 'marginal', 'densities', 'regions', 'of', 'the', 'search', 'space', 'that', 'with', '... | [-0.0982435289483804, 0.10479311576256385, -0.0694193460047245, 0.05301280769591148, -0.01823513826641899, -0.1292069422869155, 0.09554051337047265, 0.32580748641720186, -0.25692773202004343, -0.35074958983952037, 0.1069838028257856, -0.21545469677792145, -0.1245110656063144, 0.1678826234733256, -0.03146437924498549, 0... |
710.3562 | Neutrino induced threshold production of two pions and N^*(1440)
electroweak form factors | We study the threshold production of two pions induced by neutrinos in
nucleon targets. The contribution of nucleon, pion and contact terms are
calculated using a chiral Lagrangian. The contribution of the Roper resonance,
neglected in earlier studies, has also been taken into account. The numerical
results for the c... | hep-ph | we study the threshold production of two pions induced by neutrinos in nucleon targets the contribution of nucleon pion and contact terms are calculated using a chiral lagrangian the contribution of the roper resonance neglected in earlier studies has also been taken into account the numerical results for the cross sec... | [['we', 'study', 'the', 'threshold', 'production', 'of', 'two', 'pions', 'induced', 'by', 'neutrinos', 'in', 'nucleon', 'targets', 'the', 'contribution', 'of', 'nucleon', 'pion', 'and', 'contact', 'terms', 'are', 'calculated', 'using', 'a', 'chiral', 'lagrangian', 'the', 'contribution', 'of', 'the', 'roper', 'resonance... | [-0.07789642879431811, 0.18671587950746538, -0.10485597634089923, 0.12617669800198167, -0.02051397807332217, -0.07674724443328626, -0.0012595303518988124, 0.35329733990611284, -0.15317319683867311, -0.25018368400377006, -0.0021276458074689047, -0.3603524365077872, -0.055906896573414494, 0.15237210539742074, 0.094979172... |
710.3563 | Langmuir wave filamentation instability | A Langmuir wave (LW) model is constructed whose equilibria are consistent
with stimulated Raman scatter optimization, with Hamiltonian dynamics and with
rotational invariance. Linear instability analysis includes terms to all orders
in wave amplitude and fluctuation wavenumber expansions, deltak. Resultant LW
modulat... | physics.plasm-ph | a langmuir wave lw model is constructed whose equilibria are consistent with stimulated raman scatter optimization with hamiltonian dynamics and with rotational invariance linear instability analysis includes terms to all orders in wave amplitude and fluctuation wavenumber expansions deltak resultant lw modulational in... | [['a', 'langmuir', 'wave', 'lw', 'model', 'is', 'constructed', 'whose', 'equilibria', 'are', 'consistent', 'with', 'stimulated', 'raman', 'scatter', 'optimization', 'with', 'hamiltonian', 'dynamics', 'and', 'with', 'rotational', 'invariance', 'linear', 'instability', 'analysis', 'includes', 'terms', 'to', 'all', 'order... | [-0.2200532404658122, 0.2895255187550225, -0.03579331001935479, 0.07947279993767062, -0.08309615137748039, -0.11907888962051426, -0.012481420938573323, 0.28032115321510875, -0.26425441121682525, -0.2313770611818211, 0.06353370919495295, -0.2889424405203989, -0.11259275337514014, 0.1590343239144064, 0.07424645053031735,... |
710.3564 | Some comments on embedding inflation in the AdS/CFT correspondence | The anti-de Sitter space/conformal field theory correspondence (AdS/CFT) can
potentially provide a complete formulation of string theory on a landscape of
stable and metastable vacua that naturally give rise to eternal inflation. As a
model for this process, we consider bubble solutions with de Sitter interiors,
obta... | hep-th | the antide sitter spaceconformal field theory correspondence adscft can potentially provide a complete formulation of string theory on a landscape of stable and metastable vacua that naturally give rise to eternal inflation as a model for this process we consider bubble solutions with de sitter interiors obtained by pa... | [['the', 'antide', 'sitter', 'spaceconformal', 'field', 'theory', 'correspondence', 'adscft', 'can', 'potentially', 'provide', 'a', 'complete', 'formulation', 'of', 'string', 'theory', 'on', 'a', 'landscape', 'of', 'stable', 'and', 'metastable', 'vacua', 'that', 'naturally', 'give', 'rise', 'to', 'eternal', 'inflation'... | [-0.1451048385583015, 0.15436490849681242, -0.16176808589850278, 0.11346988243045576, -0.09282195895930807, -0.15290222911040902, 0.008604856310686207, 0.2600238253448076, -0.19902247294564457, -0.24792782427154153, 0.12145681206140366, -0.26875663428183866, -0.10472529489368967, 0.14366625803214608, -0.099869176461224... |
710.3565 | Robustness of key features of loop quantum cosmology | Loop quantum cosmology of the k=0 FRW model (with a massless scalar field) is
shown to be exactly soluble if the scalar field is used as the internal time
already in the classical Hamiltonian theory. Analytical methods are then used
i) to show that the quantum bounce is generic; ii) to establish that the matter
densi... | gr-qc hep-th | loop quantum cosmology of the k0 frw model with a massless scalar field is shown to be exactly soluble if the scalar field is used as the internal time already in the classical hamiltonian theory analytical methods are then used i to show that the quantum bounce is generic ii to establish that the matter density has an... | [['loop', 'quantum', 'cosmology', 'of', 'the', 'k0', 'frw', 'model', 'with', 'a', 'massless', 'scalar', 'field', 'is', 'shown', 'to', 'be', 'exactly', 'soluble', 'if', 'the', 'scalar', 'field', 'is', 'used', 'as', 'the', 'internal', 'time', 'already', 'in', 'the', 'classical', 'hamiltonian', 'theory', 'analytical', 'me... | [-0.08494377800297746, 0.13031456496818647, -0.1540377226006811, 0.11058219222343338, -0.10556483930376775, -0.18005504352404833, -0.009192042408419624, 0.3413434360787684, -0.22136441850177715, -0.27645914689094925, 0.07759923988987515, -0.2536071668281877, -0.1731639041028277, 0.1777168488268529, -0.05360996074248905... |
710.3566 | Markov Chain Methods For Analyzing Complex Transport Networks | We have developed a steady state theory of complex transport networks used to
model the flow of commodity, information, viruses, opinions, or traffic. Our
approach is based on the use of the Markov chains defined on the graph
representations of transport networks allowing for the effective network
design, network per... | physics.soc-ph physics.data-an | we have developed a steady state theory of complex transport networks used to model the flow of commodity information viruses opinions or traffic our approach is based on the use of the markov chains defined on the graph representations of transport networks allowing for the effective network design network performance... | [['we', 'have', 'developed', 'a', 'steady', 'state', 'theory', 'of', 'complex', 'transport', 'networks', 'used', 'to', 'model', 'the', 'flow', 'of', 'commodity', 'information', 'viruses', 'opinions', 'or', 'traffic', 'our', 'approach', 'is', 'based', 'on', 'the', 'use', 'of', 'the', 'markov', 'chains', 'defined', 'on',... | [-0.1482760454788804, 0.09127436346560716, -0.09824839181639254, 0.07038416428864003, -0.07519408354163169, -0.1698186466023326, 0.03120611030422151, 0.4281557617783546, -0.3076165649534669, -0.2692960339188576, 0.09912951584439725, -0.24708302592486142, -0.21116559492610396, 0.13583788827434182, -0.06501269475743175, ... |
710.3567 | Nonlinear NMR dynamics in hyperpolarized liquid 3He | In a highly polarized liquid (laser-polarized 3He-4He mixtures in our
experiment), dipolar magnetic interactions within the liquid introduce a
significant nonlinear and nonlocal contribution to the Bloch equation that
leads to instabilities during NMR evolution. We have launched a study of these
instabilities using s... | cond-mat.other | in a highly polarized liquid laserpolarized 3he4he mixtures in our experiment dipolar magnetic interactions within the liquid introduce a significant nonlinear and nonlocal contribution to the bloch equation that leads to instabilities during nmr evolution we have launched a study of these instabilities using spin echo... | [['in', 'a', 'highly', 'polarized', 'liquid', 'laserpolarized', '3he4he', 'mixtures', 'in', 'our', 'experiment', 'dipolar', 'magnetic', 'interactions', 'within', 'the', 'liquid', 'introduce', 'a', 'significant', 'nonlinear', 'and', 'nonlocal', 'contribution', 'to', 'the', 'bloch', 'equation', 'that', 'leads', 'to', 'in... | [-0.13356971578587862, 0.2198119945709054, -0.08082099787901495, 0.04044782495316626, -0.04480160079388456, -0.10159353643063117, 0.030592902113725853, 0.41774808123538437, -0.26914824704554946, -0.2893793024292046, 0.06790786284995688, -0.2615276306232607, -0.07693721853535283, 0.2181988716464151, 0.036175392946990376... |
710.3568 | A criterion for an abelian variety to be simple | In this note we give a numerical criterion that expresses the condition that
an abelian variety be simple in terms of an invariant that is closely related
to the s-invariant of Ein-Cutkosky-Lazarsfeld. The criterion yields new
examples where s-invariants are irrational. It may also be viewed as a
statement about the ... | math.AG | in this note we give a numerical criterion that expresses the condition that an abelian variety be simple in terms of an invariant that is closely related to the sinvariant of eincutkoskylazarsfeld the criterion yields new examples where sinvariants are irrational it may also be viewed as a statement about the geometry... | [['in', 'this', 'note', 'we', 'give', 'a', 'numerical', 'criterion', 'that', 'expresses', 'the', 'condition', 'that', 'an', 'abelian', 'variety', 'be', 'simple', 'in', 'terms', 'of', 'an', 'invariant', 'that', 'is', 'closely', 'related', 'to', 'the', 'sinvariant', 'of', 'eincutkoskylazarsfeld', 'the', 'criterion', 'yie... | [-0.1465097089382735, 0.08877136751808311, -0.15008208482626784, 0.11982715336436575, -0.11402925255454399, -0.14374942372299054, -0.0059993204745379365, 0.31897131983529436, -0.3023428509181196, -0.2388750781347467, 0.1327848877122795, -0.20312711372971534, -0.21742084558037195, 0.27269047087227755, -0.172062571685422... |
710.3569 | On the Eisenstein ideal of Drinfeld modular curves | Let $\goth E(\goth p)$ denote the Eisenstein ideal in the Hecke algebra $\Bbb
T(\goth p)$ of the Drinfeld modular curve $X_0(\goth p)$ parameterizing
Drinfeld modules of rank two over $\Bbb F_q[T]$ of general characteristic with
Hecke level $\goth p$-structure, where $\goth p\triangleleft\Bbb F_q[T]$ is a
non-zero pr... | math.NT | let goth egoth p denote the eisenstein ideal in the hecke algebra bbb tgoth p of the drinfeld modular curve x_0goth p parameterizing drinfeld modules of rank two over bbb f_qt of general characteristic with hecke level goth pstructure where goth ptriangleleftbbb f_qt is a nonzero prime ideal we prove that the character... | [['let', 'goth', 'egoth', 'p', 'denote', 'the', 'eisenstein', 'ideal', 'in', 'the', 'hecke', 'algebra', 'bbb', 'tgoth', 'p', 'of', 'the', 'drinfeld', 'modular', 'curve', 'x_0goth', 'p', 'parameterizing', 'drinfeld', 'modules', 'of', 'rank', 'two', 'over', 'bbb', 'f_qt', 'of', 'general', 'characteristic', 'with', 'hecke... | [-0.34763389896267116, 0.06635957340805386, -0.12154571072329791, -0.032285673099044614, -0.08185192447107954, -0.2165714128790662, -0.12384042303818159, 0.21012405212968588, -0.40739609664067244, -0.08036966824259323, -0.0059427764902536115, -0.24352129301629388, -0.06699009320567338, 0.2072105007365537, -0.1310989510... |
710.357 | Muntz type Theorems I | In this paper, we concentrate our attention on the Muntz problem in the
univariate setting and for the uniform norm.
| math.CA | in this paper we concentrate our attention on the muntz problem in the univariate setting and for the uniform norm | [['in', 'this', 'paper', 'we', 'concentrate', 'our', 'attention', 'on', 'the', 'muntz', 'problem', 'in', 'the', 'univariate', 'setting', 'and', 'for', 'the', 'uniform', 'norm']] | [-0.03666154518723488, -0.009477730747312308, -0.03723997568158666, 0.09064808466355316, -0.05719391638413072, -0.03188157482072711, 0.047589234687620774, 0.4103076383471489, -0.27922532372176645, -0.16608145610662178, 0.15419967278139665, -0.23515717815607787, -0.1757545296102762, 0.17007578844204546, -0.1947419556789... |
710.3571 | Group Theoretical Construction of Nucleon Operators using All-to-All
Quark Propagators | We describe a method to construct irreducible baryon operators using
all-to-all quark propagators. It was demonstrated earlier that a large basis of
extended baryon operators on anisotropic, quenched lattices can be used to
reliably extract the masses of 5 or more excited states in the nucleon channel.
All-to-all qua... | hep-lat | we describe a method to construct irreducible baryon operators using alltoall quark propagators it was demonstrated earlier that a large basis of extended baryon operators on anisotropic quenched lattices can be used to reliably extract the masses of 5 or more excited states in the nucleon channel alltoall quark propag... | [['we', 'describe', 'a', 'method', 'to', 'construct', 'irreducible', 'baryon', 'operators', 'using', 'alltoall', 'quark', 'propagators', 'it', 'was', 'demonstrated', 'earlier', 'that', 'a', 'large', 'basis', 'of', 'extended', 'baryon', 'operators', 'on', 'anisotropic', 'quenched', 'lattices', 'can', 'be', 'used', 'to',... | [-0.0752127316557061, 0.2509172525966451, -0.10096750892286956, 0.16946311211007564, -0.06207732628669818, -0.11285206157402104, 0.05319808873816767, 0.3696886818146422, -0.19487619428217512, -0.2502969427059601, 0.06514151069592228, -0.2801272957047232, -0.09830119395723605, 0.1355400266154308, 0.03710921792999278, 0.... |
710.3572 | Theory of semiconductor quantum-wire based single- and two-qubit gates | A GaAs/AlGaAs based two-qubit quantum device that allows the controlled
generation and straightforward detection of entanglement by measuring a
stationary current-voltage characteristic is proposed. We have developed a
two-particle Green's function method of open systems and calculate the
properties of three-dimensio... | cond-mat.mes-hall quant-ph | a gaasalgaas based twoqubit quantum device that allows the controlled generation and straightforward detection of entanglement by measuring a stationary currentvoltage characteristic is proposed we have developed a twoparticle greens function method of open systems and calculate the properties of threedimensional inter... | [['a', 'gaasalgaas', 'based', 'twoqubit', 'quantum', 'device', 'that', 'allows', 'the', 'controlled', 'generation', 'and', 'straightforward', 'detection', 'of', 'entanglement', 'by', 'measuring', 'a', 'stationary', 'currentvoltage', 'characteristic', 'is', 'proposed', 'we', 'have', 'developed', 'a', 'twoparticle', 'gre... | [-0.22448203305786224, 0.20916243267129175, -0.047954444530881754, -0.010001950311286673, 0.05735495089388946, -0.27331476564667806, 0.015751646538147656, 0.38538135890261965, -0.20233798150301857, -0.2776477824106124, -0.039260790821266586, -0.2625003830284446, -0.1236659854047877, 0.26292193505693884, 0.0171287781871... |
710.3573 | On the failure of the Poincar\'e Lemma for de-bar-sub-M II | We obtain very sharp results about the lack of validity of the Poincare lemma
for the tangential Cauchy Riemann equations, acting on tangential forms,
tangential to a CR manifold M of general CR dimension n, and general CR
codimension k. This generalizes the classical nonsolvability example of H.
Lewy. We also discus... | math.DG math.AP math.CV | we obtain very sharp results about the lack of validity of the poincare lemma for the tangential cauchy riemann equations acting on tangential forms tangential to a cr manifold m of general cr dimension n and general cr codimension k this generalizes the classical nonsolvability example of h lewy we also discuss the cr... | [['we', 'obtain', 'very', 'sharp', 'results', 'about', 'the', 'lack', 'of', 'validity', 'of', 'the', 'poincare', 'lemma', 'for', 'the', 'tangential', 'cauchy', 'riemann', 'equations', 'acting', 'on', 'tangential', 'forms', 'tangential', 'to', 'a', 'cr', 'manifold', 'm', 'of', 'general', 'cr', 'dimension', 'n', 'and', '... | [-0.20411691832421824, 0.04616572861320888, -0.016723592353698153, 0.08810509175796491, -0.14141685765785858, -0.12201089468092108, -0.039351403987847075, 0.27994942163917214, -0.2893217821808484, -0.2548436610601269, 0.05277249273748543, -0.21515088200939295, -0.13835140114996392, 0.22034697850139287, -0.0753761981972... |
710.3574 | A graph theoretic expansion formula for cluster algebras of classical
type | In this paper we give a graph theoretic combinatorial interpretation for the
cluster variables that arise in most cluster algebras of finite type. In
particular, we provide a family of graphs such that a weighted enumeration of
their perfect matchings encodes the numerator of the associated Laurent
polynomial while d... | math.CO math.RT | in this paper we give a graph theoretic combinatorial interpretation for the cluster variables that arise in most cluster algebras of finite type in particular we provide a family of graphs such that a weighted enumeration of their perfect matchings encodes the numerator of the associated laurent polynomial while decom... | [['in', 'this', 'paper', 'we', 'give', 'a', 'graph', 'theoretic', 'combinatorial', 'interpretation', 'for', 'the', 'cluster', 'variables', 'that', 'arise', 'in', 'most', 'cluster', 'algebras', 'of', 'finite', 'type', 'in', 'particular', 'we', 'provide', 'a', 'family', 'of', 'graphs', 'such', 'that', 'a', 'weighted', 'e... | [-0.16179320751415455, 0.049311953300938884, -0.08452357176472158, 0.05124478297691573, -0.1179151214659214, -0.0928622316897792, 0.04755968920585206, 0.311262694658602, -0.2942737636608346, -0.24599417362033443, 0.0925275722039206, -0.24734391556943164, -0.1794161919203094, 0.17413776528966776, -0.11804086552275454, -... |
710.3575 | Fundamental Limit to Linear One-Dimensional Slow Light Structures | Using a new general approach to limits in optical structures that counts
orthogonal waves generated by scattering, we derive an upper limit to the
number of bits of delay possible in one-dimensional slow light structures that
are based on linear optical response to the signal field. The limit is
essentially the produ... | physics.optics | using a new general approach to limits in optical structures that counts orthogonal waves generated by scattering we derive an upper limit to the number of bits of delay possible in onedimensional slow light structures that are based on linear optical response to the signal field the limit is essentially the product of... | [['using', 'a', 'new', 'general', 'approach', 'to', 'limits', 'in', 'optical', 'structures', 'that', 'counts', 'orthogonal', 'waves', 'generated', 'by', 'scattering', 'we', 'derive', 'an', 'upper', 'limit', 'to', 'the', 'number', 'of', 'bits', 'of', 'delay', 'possible', 'in', 'onedimensional', 'slow', 'light', 'structu... | [-0.15812209521918075, 0.13787343780671202, -0.0729058171333424, -0.0047963113350400315, -0.09255775873517168, -0.09415683329079284, 0.054544044963630106, 0.4168789950359998, -0.26973546607668736, -0.2826461494771828, 0.11677997443194758, -0.23525854215379163, -0.14049565670650516, 0.21406199891874889, -0.0281993452909... |
710.3576 | Entanglement between charge qubits induced by a common dissipative
environment | We study entanglement generation between two charge qubits due to the strong
coupling with a common bosonic environment (Ohmic bath). The coupling to the
boson bath is a source of both quantum noise (leading to decoherence) and an
indirect interaction between qubits. As a result, two effects compete as a
function of ... | cond-mat.mes-hall | we study entanglement generation between two charge qubits due to the strong coupling with a common bosonic environment ohmic bath the coupling to the boson bath is a source of both quantum noise leading to decoherence and an indirect interaction between qubits as a result two effects compete as a function of the coupl... | [['we', 'study', 'entanglement', 'generation', 'between', 'two', 'charge', 'qubits', 'due', 'to', 'the', 'strong', 'coupling', 'with', 'a', 'common', 'bosonic', 'environment', 'ohmic', 'bath', 'the', 'coupling', 'to', 'the', 'boson', 'bath', 'is', 'a', 'source', 'of', 'both', 'quantum', 'noise', 'leading', 'to', 'decoh... | [-0.1819085138623865, 0.25369847176886995, -0.0164123523745288, 0.03280615538485276, 0.012719181999202493, -0.20396839436686154, 0.05197011985707558, 0.34306818972007164, -0.23446070684970005, -0.2955665757554104, -0.011695103104976774, -0.3328491164714966, -0.08828787166552926, 0.1806309572014126, 0.05840268813399146,... |
710.3577 | External Momentum, Volume Effects, and the Nucleon Magnetic Moment | We analyze the determination of volume effects for correlation functions that
depend on an external momentum. As a specific example, we consider finite
volume nucleon current correlators, and focus on the nucleon magnetic moment.
Because the multipole decomposition relies on SO(3) rotational invariance, the
structure... | hep-lat hep-ph nucl-th | we analyze the determination of volume effects for correlation functions that depend on an external momentum as a specific example we consider finite volume nucleon current correlators and focus on the nucleon magnetic moment because the multipole decomposition relies on so3 rotational invariance the structure of such ... | [['we', 'analyze', 'the', 'determination', 'of', 'volume', 'effects', 'for', 'correlation', 'functions', 'that', 'depend', 'on', 'an', 'external', 'momentum', 'as', 'a', 'specific', 'example', 'we', 'consider', 'finite', 'volume', 'nucleon', 'current', 'correlators', 'and', 'focus', 'on', 'the', 'nucleon', 'magnetic', ... | [-0.1460907418081046, 0.21575953769648992, -0.06600724792145696, 0.13219850620560072, -0.10076254779611386, -0.053681042743846774, 0.018718918548295955, 0.33105658126894283, -0.23990814317319845, -0.26200066389188775, 0.054757467347568506, -0.3216369193160554, -0.03160515427117463, 0.12425723890113216, 0.01952382957726... |
710.3578 | Creation of macroscopic quantum superposition states by a measurement | We propose a novel protocol for the creation of macroscopic quantum
superposition (MQS) states based on a measurement of a non-monotonous function
of a quantum collective variable. The main advantage of this protocol is that
it does not require switching on and off nonlinear interactions in the system.
We predict thi... | quant-ph | we propose a novel protocol for the creation of macroscopic quantum superposition mqs states based on a measurement of a nonmonotonous function of a quantum collective variable the main advantage of this protocol is that it does not require switching on and off nonlinear interactions in the system we predict this proto... | [['we', 'propose', 'a', 'novel', 'protocol', 'for', 'the', 'creation', 'of', 'macroscopic', 'quantum', 'superposition', 'mqs', 'states', 'based', 'on', 'a', 'measurement', 'of', 'a', 'nonmonotonous', 'function', 'of', 'a', 'quantum', 'collective', 'variable', 'the', 'main', 'advantage', 'of', 'this', 'protocol', 'is', ... | [-0.17307390578167692, 0.22409886831085976, -0.13991960730445124, 0.014257773688407487, -0.018221155013123602, -0.18254180226398453, 0.10612113324746694, 0.3281445064365047, -0.22317795544760685, -0.270789018028403, -0.029340631578895836, -0.2357104517621537, -0.11344334171855286, 0.1896956072903353, 9.009546970259653e... |
710.3579 | Holomorphic correspondences between CR manifolds | It is proved that a germ of a real analytic CR map from a smooth
real-analytic minimal CR manifold M to an essentially finite real-algebraic
generic submanifold M' of P^N of the same CR-dimension extends as a holomorphic
correspondence along M. Applications are given for pseudoconcave submanifolds
of P^N.
| math.CV math.AG math.DG | it is proved that a germ of a real analytic cr map from a smooth realanalytic minimal cr manifold m to an essentially finite realalgebraic generic submanifold m of pn of the same crdimension extends as a holomorphic correspondence along m applications are given for pseudoconcave submanifolds of pn | [['it', 'is', 'proved', 'that', 'a', 'germ', 'of', 'a', 'real', 'analytic', 'cr', 'map', 'from', 'a', 'smooth', 'realanalytic', 'minimal', 'cr', 'manifold', 'm', 'to', 'an', 'essentially', 'finite', 'realalgebraic', 'generic', 'submanifold', 'm', 'of', 'pn', 'of', 'the', 'same', 'crdimension', 'extends', 'as', 'a', 'ho... | [-0.294621967463469, -0.0327200478068149, -0.06233708840813868, 0.05761614135152907, -0.0792226625454365, -0.16633985298020498, -0.06964243442884513, 0.3098979160398701, -0.24948099673706658, -0.15652434660920075, 0.012795660711292709, -0.25833926638778376, -0.16753412629192582, 0.2361807154957205, -0.12399032221612882... |
710.358 | Computer Based Analytical Simulations of the Chiral Hadronic Processes | The availability of computational modeling tools for subatomic physics (Form,
FeynArts, FormCalc, and FeynCalc) has made it possible to perform sophisticated
calculations in perturbative quantum field theory. We have adapted these
packages in order to apply them to the effective chiral field theory of
hadronic intera... | physics.comp-ph hep-ph | the availability of computational modeling tools for subatomic physics form feynarts formcalc and feyncalc has made it possible to perform sophisticated calculations in perturbative quantum field theory we have adapted these packages in order to apply them to the effective chiral field theory of hadronic interactions a... | [['the', 'availability', 'of', 'computational', 'modeling', 'tools', 'for', 'subatomic', 'physics', 'form', 'feynarts', 'formcalc', 'and', 'feyncalc', 'has', 'made', 'it', 'possible', 'to', 'perform', 'sophisticated', 'calculations', 'in', 'perturbative', 'quantum', 'field', 'theory', 'we', 'have', 'adapted', 'these', ... | [-0.0523816342007552, 0.09156910268986812, -0.1376761934294396, 0.10180008704545068, -0.10982157610601088, -0.13831725329557648, 0.009738654287562508, 0.38022798529566554, -0.21358456132937315, -0.34712575535580026, 0.008716327592455705, -0.2685472591642718, -0.09166907018325368, 0.1566587619666682, 0.04346853293875446... |
710.3581 | Discrimination between evolution operators | Under broad conditions, evolutions due to two different Hamiltonians are
shown to lead at some moment to orthogonal states. For two spin-1/2 systems
subject to precession by different magnetic fields the achievement of
orthogonalization is demonstrated for every scenario but a special one. This
discrimination between... | quant-ph | under broad conditions evolutions due to two different hamiltonians are shown to lead at some moment to orthogonal states for two spin12 systems subject to precession by different magnetic fields the achievement of orthogonalization is demonstrated for every scenario but a special one this discrimination between evolut... | [['under', 'broad', 'conditions', 'evolutions', 'due', 'to', 'two', 'different', 'hamiltonians', 'are', 'shown', 'to', 'lead', 'at', 'some', 'moment', 'to', 'orthogonal', 'states', 'for', 'two', 'spin12', 'systems', 'subject', 'to', 'precession', 'by', 'different', 'magnetic', 'fields', 'the', 'achievement', 'of', 'ort... | [-0.15253035227041914, 0.15432006502912068, -0.06931310572240147, 0.06714370499997001, -0.037087092239831, -0.176136805177001, 0.003364276604510711, 0.3871797009238175, -0.21485956079725707, -0.30040820021392955, 0.09741137427737981, -0.19963602393787974, -0.0961358096239911, 0.26185880494692054, -0.01458983086714787, ... |
710.3582 | Earth's extensive entropy bound | The possibility of planetary mass black hole production by crossing entropy
limits is addressed. Such a possibility is given by pointing out that two
geophysical quantities have comparable values: first, Earth's total negative
entropy flux integrated over geological time and, second, its extensive entropy
bound, whic... | gr-qc | the possibility of planetary mass black hole production by crossing entropy limits is addressed such a possibility is given by pointing out that two geophysical quantities have comparable values first earths total negative entropy flux integrated over geological time and second its extensive entropy bound which follows... | [['the', 'possibility', 'of', 'planetary', 'mass', 'black', 'hole', 'production', 'by', 'crossing', 'entropy', 'limits', 'is', 'addressed', 'such', 'a', 'possibility', 'is', 'given', 'by', 'pointing', 'out', 'that', 'two', 'geophysical', 'quantities', 'have', 'comparable', 'values', 'first', 'earths', 'total', 'negativ... | [-0.12232820054897192, 0.17251287865021203, -0.08467500702139329, 0.15242793246659198, -0.047228656000119044, -0.084311782640659, 0.09335316837849943, 0.26220000106841324, -0.2002225577661937, -0.3331124514002692, 0.10004228469386528, -0.3173937378874557, -0.08969691541596231, 0.24466435485942797, -0.024203594723208384... |
710.3583 | Off-center impurity in alkali halides: reorientation, electric
polarization and pairing to F center. IV. Reorientational rate | This last Part IV is aimed at deriving relaxation rates (times) of an
off-center Li+ impurity. We follow Christov's reaction rate method to define
general rate equations in terms of the exact Mathieu eigenvalues, as well as of
harmonic-oscillator eigenvalues approximating for the energy spectrum near the
bottom of th... | physics.chem-ph physics.comp-ph | this last part iv is aimed at deriving relaxation rates times of an offcenter li impurity we follow christovs reaction rate method to define general rate equations in terms of the exact mathieu eigenvalues as well as of harmonicoscillator eigenvalues approximating for the energy spectrum near the bottom of the reorient... | [['this', 'last', 'part', 'iv', 'is', 'aimed', 'at', 'deriving', 'relaxation', 'rates', 'times', 'of', 'an', 'offcenter', 'li', 'impurity', 'we', 'follow', 'christovs', 'reaction', 'rate', 'method', 'to', 'define', 'general', 'rate', 'equations', 'in', 'terms', 'of', 'the', 'exact', 'mathieu', 'eigenvalues', 'as', 'wel... | [-0.08840168739729763, 0.11207683910454405, 0.005843433923196837, 0.0638944664527156, 0.03555002172841974, -0.14754741517421993, 0.034621441402756005, 0.3437986211527301, -0.22560703168046134, -0.23742046169481118, 0.04467191468321961, -0.2912365026346853, -0.10415428546611624, 0.20420586860374265, 0.002059850295114776... |
710.3584 | Boundary of central tiles associated with Pisot beta-numeration and
purely periodic expansions | This paper studies tilings related to the beta-transformation when beta is a
Pisot number (that is not supposed to be a unit). Then it applies the obtained
results to study the set of rational numbers having a purely periodic
beta-expansion. Special focus is given to some quadratic examples.
| math.DS math.NT | this paper studies tilings related to the betatransformation when beta is a pisot number that is not supposed to be a unit then it applies the obtained results to study the set of rational numbers having a purely periodic betaexpansion special focus is given to some quadratic examples | [['this', 'paper', 'studies', 'tilings', 'related', 'to', 'the', 'betatransformation', 'when', 'beta', 'is', 'a', 'pisot', 'number', 'that', 'is', 'not', 'supposed', 'to', 'be', 'a', 'unit', 'then', 'it', 'applies', 'the', 'obtained', 'results', 'to', 'study', 'the', 'set', 'of', 'rational', 'numbers', 'having', 'a', '... | [-0.16140592913143337, 0.11448677727215302, -0.04568680659091721, 0.07943407656178654, -0.1514812294044532, -0.16699502654955722, 0.05671972042910056, 0.3105142548835526, -0.3046963968469451, -0.18870390920589367, 0.1318114531750325, -0.3090800848682799, -0.2079438865184784, 0.23460729517197856, -0.1328829368285369, 0.... |
710.3585 | (Extra)Ordinary Gauge Mediation | We study models of "(extra)ordinary gauge mediation," which consist of taking
ordinary gauge mediation and extending the messenger superpotential to include
all renormalizable couplings consistent with SM gauge invariance and an
R-symmetry. We classify all such models and find that their phenomenology can
differ sign... | hep-ph hep-th | we study models of extraordinary gauge mediation which consist of taking ordinary gauge mediation and extending the messenger superpotential to include all renormalizable couplings consistent with sm gauge invariance and an rsymmetry we classify all such models and find that their phenomenology can differ significantly... | [['we', 'study', 'models', 'of', 'extraordinary', 'gauge', 'mediation', 'which', 'consist', 'of', 'taking', 'ordinary', 'gauge', 'mediation', 'and', 'extending', 'the', 'messenger', 'superpotential', 'to', 'include', 'all', 'renormalizable', 'couplings', 'consistent', 'with', 'sm', 'gauge', 'invariance', 'and', 'an', '... | [-0.1368635598038513, 0.28418235431862604, -0.026991978180553534, 0.17748245501280885, -0.14845928052374352, -0.20600295802413493, 0.006297073574773803, 0.32417465452376787, -0.20942966403456126, -0.3595847272174021, 0.06451088603713706, -0.23366370508694542, -0.16463530523933273, 0.10002982485380056, -0.00817565407204... |
710.3586 | Baryon oscillations in galaxy and matter power-spectrum covariance
matrices | We investigate large-amplitude baryon acoustic oscillations (BAO's) in
off-diagonal entries of cosmological power-spectrum covariance matrices. These
covariance-matrix BAO's describe the increased attenuation of power-spectrum
BAO's caused by upward fluctuations in large-scale power. We derive an analytic
approximati... | astro-ph | we investigate largeamplitude baryon acoustic oscillations baos in offdiagonal entries of cosmological powerspectrum covariance matrices these covariancematrix baos describe the increased attenuation of powerspectrum baos caused by upward fluctuations in largescale power we derive an analytic approximation to covarianc... | [['we', 'investigate', 'largeamplitude', 'baryon', 'acoustic', 'oscillations', 'baos', 'in', 'offdiagonal', 'entries', 'of', 'cosmological', 'powerspectrum', 'covariance', 'matrices', 'these', 'covariancematrix', 'baos', 'describe', 'the', 'increased', 'attenuation', 'of', 'powerspectrum', 'baos', 'caused', 'by', 'upwa... | [-0.10846798256824405, 0.1127207440698, -0.050024736402360916, 0.17226506820782186, -0.1255372596605049, -0.04993878791134779, 0.0012134951539337635, 0.3284533950988646, -0.20329436455149907, -0.31174305661653096, 0.05435610545792623, -0.331947110600773, -0.10107004132864254, 0.21683631805455558, -0.008134971545370934,... |
710.3587 | Star Formation History up to z = 7.4: Implications for Gamma-Ray Bursts
and the Cosmic Metallicity Evolution | The current Swift sample of gamma-ray bursts (GRBs) with measured redshifts
allows to test the assumption that GRBs trace the star formation in the
Universe. Some authors have claimed that the rate of GRBs increases with cosmic
redshift faster than the star formation rate, whose cause is not known yet. In
this paper,... | astro-ph | the current swift sample of gammaray bursts grbs with measured redshifts allows to test the assumption that grbs trace the star formation in the universe some authors have claimed that the rate of grbs increases with cosmic redshift faster than the star formation rate whose cause is not known yet in this paper i invest... | [['the', 'current', 'swift', 'sample', 'of', 'gammaray', 'bursts', 'grbs', 'with', 'measured', 'redshifts', 'allows', 'to', 'test', 'the', 'assumption', 'that', 'grbs', 'trace', 'the', 'star', 'formation', 'in', 'the', 'universe', 'some', 'authors', 'have', 'claimed', 'that', 'the', 'rate', 'of', 'grbs', 'increases', '... | [-0.027653946141988316, 0.11767180622690056, -0.06127765533272867, 0.1284542823404384, -0.11071916959093263, -0.03890648612200662, 0.06559320567434447, 0.42789149922491226, -0.1788720992402415, -0.3508307487824587, 0.024459471975246238, -0.2793365430509935, -0.009712382509692193, 0.2128828817312347, -0.0417026156335379... |
710.3588 | A Comparison of Weak Lensing Measurements From Ground- and Space-Based
Facilities | We assess the relative merits of weak lensing surveys, using overlapping
imaging data from the ground-based Subaru telescope and the Hubble Space
Telescope (HST). Our tests complement similar studies undertaken with simulated
data. From observations of 230,000 matched objects in the 2 square degree
COSMOS field, we i... | astro-ph | we assess the relative merits of weak lensing surveys using overlapping imaging data from the groundbased subaru telescope and the hubble space telescope hst our tests complement similar studies undertaken with simulated data from observations of 230000 matched objects in the 2 square degree cosmos field we identify th... | [['we', 'assess', 'the', 'relative', 'merits', 'of', 'weak', 'lensing', 'surveys', 'using', 'overlapping', 'imaging', 'data', 'from', 'the', 'groundbased', 'subaru', 'telescope', 'and', 'the', 'hubble', 'space', 'telescope', 'hst', 'our', 'tests', 'complement', 'similar', 'studies', 'undertaken', 'with', 'simulated', '... | [-0.023917187836974167, 0.06018339530734053, -0.06252355811207794, 0.09218836959104898, -0.10897092834808106, -0.05732591961440089, 0.04416852195836539, 0.41351129722369967, -0.13785597912339104, -0.4139289908219389, 0.08443160561714755, -0.35381000750633174, 0.008400022424757481, 0.2606193166605175, -0.033443148377849... |
710.3589 | Threshold singularities in the dynamic response of gapless integrable
models | We develop a method of an asymptotically exact treatment of threshold
singularities in dynamic response functions of gapless integrable models. The
method utilizes the integrability to recast the original problem in terms of
the low-energy properties of a certain deformed Hamiltonian. The deformed
Hamiltonian is loca... | cond-mat.str-el cond-mat.mes-hall | we develop a method of an asymptotically exact treatment of threshold singularities in dynamic response functions of gapless integrable models the method utilizes the integrability to recast the original problem in terms of the lowenergy properties of a certain deformed hamiltonian the deformed hamiltonian is local hen... | [['we', 'develop', 'a', 'method', 'of', 'an', 'asymptotically', 'exact', 'treatment', 'of', 'threshold', 'singularities', 'in', 'dynamic', 'response', 'functions', 'of', 'gapless', 'integrable', 'models', 'the', 'method', 'utilizes', 'the', 'integrability', 'to', 'recast', 'the', 'original', 'problem', 'in', 'terms', '... | [-0.13471797200099353, 0.10272039167449042, -0.12210555645603552, 0.1058884200777477, -0.043403943229876236, -0.14599354754774327, 0.0281489013921447, 0.32875278661678353, -0.2657906640186367, -0.23508563500840263, 0.037781413511305775, -0.2640455296622163, -0.19878318600625877, 0.12124653187501862, -0.0128093548455690... |
710.359 | Protoplanetary disk fragmentation with varying radiative physics,
initial conditions and numerical techniques | We review recent results of SPH simulations of gravitational instability in
gaseous protoplanetary disks,emphasizing the role of thermodynamics in both
isolated and binary systems. Contradictory results appeared in the literature
regarding disk fragmentation at tens of AU from the central star are likely due
to the d... | astro-ph | we review recent results of sph simulations of gravitational instability in gaseous protoplanetary disksemphasizing the role of thermodynamics in both isolated and binary systems contradictory results appeared in the literature regarding disk fragmentation at tens of au from the central star are likely due to the diffe... | [['we', 'review', 'recent', 'results', 'of', 'sph', 'simulations', 'of', 'gravitational', 'instability', 'in', 'gaseous', 'protoplanetary', 'disksemphasizing', 'the', 'role', 'of', 'thermodynamics', 'in', 'both', 'isolated', 'and', 'binary', 'systems', 'contradictory', 'results', 'appeared', 'in', 'the', 'literature', ... | [-0.09374523025707625, 0.08031973695202468, -0.09643413001540145, 0.08927993833175593, -0.034111571372055866, -0.1084241775163995, -0.03934701421864265, 0.3732562396954335, -0.22130906038470402, -0.35157244870775595, 0.09248880480594589, -0.2503171381930357, -0.059616343372620416, 0.19686500886214142, -0.03607866489266... |
710.3591 | Detection of methane on Kuiper Belt Object (50000) Quaoar | The near-infrared spectrum of (50000) Quaoar obtained at the Keck Observatory
shows distinct absorption features of crystalline water ice, solid methane and
ethane, and possibly other higher order hydrocarbons. Quaoar is only the fifth
Kuiper belt object on which volatile ices have been detected. The small amount
of ... | astro-ph | the nearinfrared spectrum of 50000 quaoar obtained at the keck observatory shows distinct absorption features of crystalline water ice solid methane and ethane and possibly other higher order hydrocarbons quaoar is only the fifth kuiper belt object on which volatile ices have been detected the small amount of methane o... | [['the', 'nearinfrared', 'spectrum', 'of', '50000', 'quaoar', 'obtained', 'at', 'the', 'keck', 'observatory', 'shows', 'distinct', 'absorption', 'features', 'of', 'crystalline', 'water', 'ice', 'solid', 'methane', 'and', 'ethane', 'and', 'possibly', 'other', 'higher', 'order', 'hydrocarbons', 'quaoar', 'is', 'only', 't... | [-0.05511432272348418, 0.2025015857956072, -0.07384353228816651, 0.0454103700782969, -0.04768617188625307, -0.05626134564875659, -0.028728239832962132, 0.3437803957992828, -0.19000754805551057, -0.37775108825796877, 0.09553525187299554, -0.33623091937098876, -0.07308865006149085, 0.1411310731018164, -0.1083913115077618... |
710.3592 | Numerical Study of a Three-Dimensional Mixed Ising Ferrimagnet in the
Presence of an External Field | We present a numerical study based on Monte Carlo algorithm of the magnetic
properties of a mixed Ising ferrimagnetic model on a cubic lattice where spins
$\sigma =\pm 1/2$ and spins $S=0,\pm 1$ are in alternating sites on the
lattice. We carried out exact ground state calculations and employ a Monte
Carlo simulation... | cond-mat.stat-mech | we present a numerical study based on monte carlo algorithm of the magnetic properties of a mixed ising ferrimagnetic model on a cubic lattice where spins sigma pm 12 and spins s0pm 1 are in alternating sites on the lattice we carried out exact ground state calculations and employ a monte carlo simulation to obtain the... | [['we', 'present', 'a', 'numerical', 'study', 'based', 'on', 'monte', 'carlo', 'algorithm', 'of', 'the', 'magnetic', 'properties', 'of', 'a', 'mixed', 'ising', 'ferrimagnetic', 'model', 'on', 'a', 'cubic', 'lattice', 'where', 'spins', 'sigma', 'pm', '12', 'and', 'spins', 's0pm', '1', 'are', 'in', 'alternating', 'sites'... | [-0.17335292689986234, 0.1732294275729017, -0.06111302481474736, 0.030689817262945448, -0.027523456680346427, -0.10628976917818306, 0.09959557164995748, 0.3894539614241042, -0.22865073910115039, -0.31962887571728604, 0.07516891826274182, -0.31947770109766815, -0.06241703571707714, 0.15161648818189058, 0.097863632892295... |
710.3593 | HE 1113-0641: The Smallest Separation Gravitational Lens Identified by a
Ground-based Optical Telescope | The Hamburg/ESO quasar HE 1113-0641 is found to be a quadruple gravitational
lens, based on observations with the twin 6.5m Magellan telescopes at the Las
Campanas Observatory, and subsequently with the Hubble Space Telescope. The
z_S=1.235 quasar appears in a cross configuration, with i' band magnitudes
ranging from... | astro-ph | the hamburgeso quasar he 11130641 is found to be a quadruple gravitational lens based on observations with the twin 65m magellan telescopes at the las campanas observatory and subsequently with the hubble space telescope the z_s1235 quasar appears in a cross configuration with i band magnitudes ranging from 180 to 188 ... | [['the', 'hamburgeso', 'quasar', 'he', '11130641', 'is', 'found', 'to', 'be', 'a', 'quadruple', 'gravitational', 'lens', 'based', 'on', 'observations', 'with', 'the', 'twin', '65m', 'magellan', 'telescopes', 'at', 'the', 'las', 'campanas', 'observatory', 'and', 'subsequently', 'with', 'the', 'hubble', 'space', 'telesco... | [-0.09126019317522276, 0.0714969299412493, -0.11127388377449123, 0.07650019481440942, -0.13363262305742707, -0.09228227141730744, 0.022544905220575888, 0.4278723738605863, -0.13742710827560775, -0.39729389587481473, 0.06993474403139333, -0.3367031396976833, -0.0694656958646976, 0.21314102932489637, -0.05012844975652366... |
710.3594 | Influence of Impact Parameter Fluctuations on Transverse Momentum
Fluctuations | The preliminary NA49 results on the energy dependence of transverse momentum
fluctuations over the whole SPS energy range exhibit an unexpected effect. The
$\Phi_{p_{T}}$ fluctuation measure - used by the NA49 experiment - manifests a
different behavior for different charge combinations. Whereas the
$\Phi_{p_{T}}$ is... | nucl-ex hep-ph nucl-th | the preliminary na49 results on the energy dependence of transverse momentum fluctuations over the whole sps energy range exhibit an unexpected effect the phi_p_t fluctuation measure used by the na49 experiment manifests a different behavior for different charge combinations whereas the phi_p_t is consistent with zero ... | [['the', 'preliminary', 'na49', 'results', 'on', 'the', 'energy', 'dependence', 'of', 'transverse', 'momentum', 'fluctuations', 'over', 'the', 'whole', 'sps', 'energy', 'range', 'exhibit', 'an', 'unexpected', 'effect', 'the', 'phi_p_t', 'fluctuation', 'measure', 'used', 'by', 'the', 'na49', 'experiment', 'manifests', '... | [-0.076255125274176, 0.31065824009871806, -0.10115868253170611, 0.13241088919642363, 0.030242968839448617, -0.09518685970333932, -0.08263698362699068, 0.3266061332354449, -0.17530768257652565, -0.3219814983468433, -0.033407264286420824, -0.36806939497752034, 0.013047321190513808, 0.1861299971937092, 0.05397178511198911... |
710.3595 | On gradient Ricci solitons with Symmetry | We study gradient Ricci solitons with maximal symmetry. First we show that
there are no non-trivial homogeneous gradient Ricci solitons. Thus the most
symmetry one can expect is an isometric cohomogeneity one group action. Many
examples of cohomogeneity one gradient solitons have been constructed. However,
we apply t... | math.DG | we study gradient ricci solitons with maximal symmetry first we show that there are no nontrivial homogeneous gradient ricci solitons thus the most symmetry one can expect is an isometric cohomogeneity one group action many examples of cohomogeneity one gradient solitons have been constructed however we apply the main ... | [['we', 'study', 'gradient', 'ricci', 'solitons', 'with', 'maximal', 'symmetry', 'first', 'we', 'show', 'that', 'there', 'are', 'no', 'nontrivial', 'homogeneous', 'gradient', 'ricci', 'solitons', 'thus', 'the', 'most', 'symmetry', 'one', 'can', 'expect', 'is', 'an', 'isometric', 'cohomogeneity', 'one', 'group', 'action... | [-0.2154369167983532, 0.11040316880158346, -0.1105223258778657, 0.06352453375369158, -0.1851198050410372, -0.2113835353863566, -0.17774220744677346, 0.4911221584738934, -0.20050570641306217, -0.1527648081377863, 0.1791760740683682, -0.3306042450824625, -0.1871198001572837, 0.14517023326663223, -0.11429391788599426, -0.... |
710.3596 | Surface Enhanced Raman Scattering Investigation of Uranium Hydride and
Uranium Oxide | The present approach to SERS does not rely on a hihj electrical conductivity
substrate or admixture to enable the SERS process. The novelty of our method is
to create an artificial periodic electron distribution on a surface by
illumination with ultraviolet radiation whose photon energy is above the
photoelectric wor... | cond-mat.mtrl-sci | the present approach to sers does not rely on a hihj electrical conductivity substrate or admixture to enable the sers process the novelty of our method is to create an artificial periodic electron distribution on a surface by illumination with ultraviolet radiation whose photon energy is above the photoelectric work f... | [['the', 'present', 'approach', 'to', 'sers', 'does', 'not', 'rely', 'on', 'a', 'hihj', 'electrical', 'conductivity', 'substrate', 'or', 'admixture', 'to', 'enable', 'the', 'sers', 'process', 'the', 'novelty', 'of', 'our', 'method', 'is', 'to', 'create', 'an', 'artificial', 'periodic', 'electron', 'distribution', 'on',... | [-0.037418530972779925, 0.09943476998722751, -0.09978016686432485, -0.03301661394690663, -0.0805688917742304, -0.10601115717007867, 0.07085987599786231, 0.44816691667403813, -0.22370512838879564, -0.3360557628549495, 0.021426657930824836, -0.29846336149593006, -0.1594882094925094, 0.23817040675917184, -0.09846304952746... |
710.3597 | Electromagnetic reactions on light nuclei using chiral effective theory | I describe the use of chiral effective theory (ChiET) to compute
electromagnetic reactions in two- and three-nucleon systems. I first explain
how chiral perturbation theory can be extended to the few-nucleon sector. I
then explain the predictions of the resulting ChiET for electron-deuteron
scattering, and how they w... | nucl-th | i describe the use of chiral effective theory chiet to compute electromagnetic reactions in two and threenucleon systems i first explain how chiral perturbation theory can be extended to the fewnucleon sector i then explain the predictions of the resulting chiet for electrondeuteron scattering and how they will be test... | [['i', 'describe', 'the', 'use', 'of', 'chiral', 'effective', 'theory', 'chiet', 'to', 'compute', 'electromagnetic', 'reactions', 'in', 'two', 'and', 'threenucleon', 'systems', 'i', 'first', 'explain', 'how', 'chiral', 'perturbation', 'theory', 'can', 'be', 'extended', 'to', 'the', 'fewnucleon', 'sector', 'i', 'then', ... | [-0.011275876398977577, 0.18467362854886343, -0.12418332758682724, 0.13143425910942713, -0.06591321072275085, -0.11074147184322379, 0.0035101600936899074, 0.35100510524471806, -0.23262901391301835, -0.27737185032800676, 0.03551839546024876, -0.32904668106716506, -0.09447469483414779, 0.14755552748636325, 0.051405798130... |
710.3598 | Scalar field exact solutions for non-flat FLRW cosmology: A technique
from non-linear Schr\"odinger-type formulation | We report a method of solving for canonical scalar field exact solution in a
non-flat FLRW universe with barotropic fluid using non-linear Schr\"{o}dinger
(NLS)-type formulation in comparison to the method in the standard Friedmann
framework. We consider phantom and non-phantom scalar field cases with
exponential and... | gr-qc astro-ph hep-th quant-ph | we report a method of solving for canonical scalar field exact solution in a nonflat flrw universe with barotropic fluid using nonlinear schrodinger nlstype formulation in comparison to the method in the standard friedmann framework we consider phantom and nonphantom scalar field cases with exponential and powerlaw acc... | [['we', 'report', 'a', 'method', 'of', 'solving', 'for', 'canonical', 'scalar', 'field', 'exact', 'solution', 'in', 'a', 'nonflat', 'flrw', 'universe', 'with', 'barotropic', 'fluid', 'using', 'nonlinear', 'schrodinger', 'nlstype', 'formulation', 'in', 'comparison', 'to', 'the', 'method', 'in', 'the', 'standard', 'fried... | [-0.10683069079665534, -0.0037995176165398345, -0.12458325786718044, 0.05902067781566272, -0.12524251503791345, -0.18935213530862546, -0.047071397753365066, 0.33383646912603493, -0.17593627153749924, -0.29321384376072024, 0.0783122327257262, -0.2573785184242998, -0.1358859595135752, 0.1745618551475815, 0.03497971614531... |
710.3599 | Hamilton relativity group for noninertial states in quantum mechanics | Physical states in quantum mechanics are rays in a Hilbert space. Projective
representations of a relativity group transform between the quantum physical
states that are in the admissible class. The physical observables of position,
time, energy and momentum are the Hermitian representation of the
Weyl-Heisenberg alg... | math-ph math.MP | physical states in quantum mechanics are rays in a hilbert space projective representations of a relativity group transform between the quantum physical states that are in the admissible class the physical observables of position time energy and momentum are the hermitian representation of the weylheisenberg algebra we... | [['physical', 'states', 'in', 'quantum', 'mechanics', 'are', 'rays', 'in', 'a', 'hilbert', 'space', 'projective', 'representations', 'of', 'a', 'relativity', 'group', 'transform', 'between', 'the', 'quantum', 'physical', 'states', 'that', 'are', 'in', 'the', 'admissible', 'class', 'the', 'physical', 'observables', 'of'... | [-0.18301073020244607, 0.1651449662927118, -0.15906392415792386, 0.05994737601523833, -0.0954546665903408, -0.09839018115705651, -0.06303729852888643, 0.3514316457851858, -0.29711041986806, -0.24041705311946115, 0.06926848943751282, -0.24624010583771982, -0.12332495750657782, 0.17550085781982577, -0.11047700260163898, ... |
710.36 | Statistical Methods for Investigating the Cosmic Ray Energy Spectrum | Two separate statistical tests are described and developed in order to test
un-binned data sets for adherence to the power-law form. The first test employs
the TP-statistic, a function defined to deviate from zero when the sample
deviates from the power-law form, regardless of the value of the power index.
The second... | astro-ph math.ST stat.TH | two separate statistical tests are described and developed in order to test unbinned data sets for adherence to the powerlaw form the first test employs the tpstatistic a function defined to deviate from zero when the sample deviates from the powerlaw form regardless of the value of the power index the second test empl... | [['two', 'separate', 'statistical', 'tests', 'are', 'described', 'and', 'developed', 'in', 'order', 'to', 'test', 'unbinned', 'data', 'sets', 'for', 'adherence', 'to', 'the', 'powerlaw', 'form', 'the', 'first', 'test', 'employs', 'the', 'tpstatistic', 'a', 'function', 'defined', 'to', 'deviate', 'from', 'zero', 'when',... | [-0.028139445290435106, 0.04429154581804243, -0.16480082461041295, 0.08872444361137848, -0.07418901372713865, -0.17080880786266384, 0.07289489753828901, 0.2801619044168749, -0.19792799346355927, -0.37141503227434847, 0.04594517960665851, -0.320676638563681, -0.023188720321437966, 0.17506119494727398, -0.005734154010295... |
710.3601 | A Possible Orbital Solution For The Triple Star WDS 18253+4846 | We present here the orbital elements for the pair BC of visual binary star
WDS 18253+4846 (ADS 11344 = HD 170109) and ephemerides for the period
2008-2014. As the orbital elements of pair AB already existed we analyzed mass
ratio between these two pairs and concluded that components C is the biggest
one in this tripl... | astro-ph | we present here the orbital elements for the pair bc of visual binary star wds 182534846 ads 11344 hd 170109 and ephemerides for the period 20082014 as the orbital elements of pair ab already existed we analyzed mass ratio between these two pairs and concluded that components c is the biggest one in this triple system | [['we', 'present', 'here', 'the', 'orbital', 'elements', 'for', 'the', 'pair', 'bc', 'of', 'visual', 'binary', 'star', 'wds', '182534846', 'ads', '11344', 'hd', '170109', 'and', 'ephemerides', 'for', 'the', 'period', '20082014', 'as', 'the', 'orbital', 'elements', 'of', 'pair', 'ab', 'already', 'existed', 'we', 'analyz... | [-0.22165110782843153, 0.1165612019457907, -0.013540540136537462, 0.048310770916770086, -0.0182373002962262, -0.10579797302214604, 0.07731748071393736, 0.3857502448636125, -0.21224369154364434, -0.2902276305973811, 0.04548300903527734, -0.31361262429997605, -0.09577642933834556, 0.18568597885094723, -0.0177211462309197... |
710.3602 | Multichannel chiral approach for kaonic hydrogen | We present an exact solution to the $K^{-}$-proton bound state problem
formulated in the momentum space. The 1s level characteristics of the kaonic
hydrogen are described together with the available low energy $\bar{K}N$ data.
| nucl-th | we present an exact solution to the kproton bound state problem formulated in the momentum space the 1s level characteristics of the kaonic hydrogen are described together with the available low energy barkn data | [['we', 'present', 'an', 'exact', 'solution', 'to', 'the', 'kproton', 'bound', 'state', 'problem', 'formulated', 'in', 'the', 'momentum', 'space', 'the', '1s', 'level', 'characteristics', 'of', 'the', 'kaonic', 'hydrogen', 'are', 'described', 'together', 'with', 'the', 'available', 'low', 'energy', 'barkn', 'data']] | [-0.12546024816658566, 0.11574872343857458, -0.03803179729455972, 0.12632804670754602, -0.019087611622286633, -0.10777257169213365, 0.08426477367688409, 0.3291301190414849, -0.2427892858052955, -0.3308450081659591, 0.025930440926458687, -0.3298376807121231, 0.011511417078402112, 0.09647340308327008, 0.03259829056504018... |
710.3603 | On a Clique-Based Integer Programming Formulation of Vertex Colouring
with Applications in Course Timetabling | Vertex colouring is a well-known problem in combinatorial optimisation, whose
alternative integer programming formulations have recently attracted
considerable attention. This paper briefly surveys seven known formulations of
vertex colouring and introduces a formulation of vertex colouring using a
suitable clique pa... | cs.DM cs.DS math.CO | vertex colouring is a wellknown problem in combinatorial optimisation whose alternative integer programming formulations have recently attracted considerable attention this paper briefly surveys seven known formulations of vertex colouring and introduces a formulation of vertex colouring using a suitable clique partiti... | [['vertex', 'colouring', 'is', 'a', 'wellknown', 'problem', 'in', 'combinatorial', 'optimisation', 'whose', 'alternative', 'integer', 'programming', 'formulations', 'have', 'recently', 'attracted', 'considerable', 'attention', 'this', 'paper', 'briefly', 'surveys', 'seven', 'known', 'formulations', 'of', 'vertex', 'col... | [-0.10923448537696938, 0.021777313153602575, -0.06465902195001642, 0.051716261728168386, -0.20273233946870295, -0.16876796098720087, 0.03508434183446266, 0.37237271709008174, -0.26657218761382656, -0.35665001025782866, 0.13587068394643434, -0.25463808478232014, -0.2104508077517446, 0.13077307120782503, -0.1719328113994... |
710.3604 | On the existence of Lyapounov variables for Schroedinger evolution | The theory of (classical and) quantum mechanical microscopic irreversibility
developed by B. Misra, I. Prigogine and M. Courbage (MPC) and various other
contributors is based on the central notion of a Lyapounov variable - i.e., a
dynamical variable whose value varies monotonically as time increases.
Incompatibility ... | math-ph math.MP | the theory of classical and quantum mechanical microscopic irreversibility developed by b misra i prigogine and m courbage mpc and various other contributors is based on the central notion of a lyapounov variable ie a dynamical variable whose value varies monotonically as time increases incompatibility between certain ... | [['the', 'theory', 'of', 'classical', 'and', 'quantum', 'mechanical', 'microscopic', 'irreversibility', 'developed', 'by', 'b', 'misra', 'i', 'prigogine', 'and', 'm', 'courbage', 'mpc', 'and', 'various', 'other', 'contributors', 'is', 'based', 'on', 'the', 'central', 'notion', 'of', 'a', 'lyapounov', 'variable', 'ie', ... | [-0.12778306485290222, 0.13258465558590551, -0.13071441459041303, 0.0734015616431736, -0.060522673274229825, -0.1363970929784861, 0.042684893580769115, 0.29441368269423646, -0.3084983794425411, -0.24781370741561398, 0.09272261585266832, -0.23689188632107844, -0.14839470648774128, 0.17848598413388833, -0.065611717128596... |
710.3605 | A Kolmogorov Extension Theorem for POVMs | We prove a theorem about positive-operator-valued measures (POVMs) that is an
analog of the Kolmogorov extension theorem, a standard theorem of probability
theory. According to our theorem, if a sequence of POVMs G_n on $\mathbb{R}^n$
satisfies the consistency (or projectivity) condition $G_{n+1}(A\times
\mathbb{R}) ... | math-ph math.MP quant-ph | we prove a theorem about positiveoperatorvalued measures povms that is an analog of the kolmogorov extension theorem a standard theorem of probability theory according to our theorem if a sequence of povms g_n on mathbbrn satisfies the consistency or projectivity condition g_n1atimes mathbbr g_na then there is a povm g... | [['we', 'prove', 'a', 'theorem', 'about', 'positiveoperatorvalued', 'measures', 'povms', 'that', 'is', 'an', 'analog', 'of', 'the', 'kolmogorov', 'extension', 'theorem', 'a', 'standard', 'theorem', 'of', 'probability', 'theory', 'according', 'to', 'our', 'theorem', 'if', 'a', 'sequence', 'of', 'povms', 'g_n', 'on', 'ma... | [-0.13192134036515385, 0.10447017165857594, -0.1488622824112192, 0.0886315218775939, -0.021882812779110212, -0.11765753297517315, 0.0664282174518284, 0.32430986394413197, -0.27058939535457355, -0.17006081631645942, 0.10831656058778605, -0.3016023171038773, -0.1485124067701877, 0.18448244302402225, -0.16021884207386905,... |
710.3606 | Distributional Limits for the Symmetric Exclusion Process | Strong negative dependence properties have recently been proved for the
symmetric exclusion process. In this paper, we apply these results to prove
convergence to the Poisson and normal distributions for various functionals of
the process.
| math.PR math-ph math.MP | strong negative dependence properties have recently been proved for the symmetric exclusion process in this paper we apply these results to prove convergence to the poisson and normal distributions for various functionals of the process | [['strong', 'negative', 'dependence', 'properties', 'have', 'recently', 'been', 'proved', 'for', 'the', 'symmetric', 'exclusion', 'process', 'in', 'this', 'paper', 'we', 'apply', 'these', 'results', 'to', 'prove', 'convergence', 'to', 'the', 'poisson', 'and', 'normal', 'distributions', 'for', 'various', 'functionals', ... | [-0.0233650322205254, 0.059616901286478556, -0.14816538582422903, 0.11187934042671778, -0.06502219348081521, -0.07290506844541857, 0.013415843597613275, 0.41279531794467145, -0.2854542433151177, -0.25266835520576153, 0.08904153085646353, -0.2520389787054488, -0.16387678155941623, 0.18225193369601453, -0.053068164150629... |
710.3607 | Vector bundles on contractible smooth schemes | We discuss algebraic vector bundles on smooth k-schemes X contractible from
the standpoint of A^1-homotopy theory; when k = C, the smooth manifolds X(C)
are contractible as topological spaces. The integral algebraic K-theory and
integral motivic cohomology of such schemes are that of Spec k. One might hope
that furth... | math.AG math.KT | we discuss algebraic vector bundles on smooth kschemes x contractible from the standpoint of a1homotopy theory when k c the smooth manifolds xc are contractible as topological spaces the integral algebraic ktheory and integral motivic cohomology of such schemes are that of spec k one might hope that furthermore and in ... | [['we', 'discuss', 'algebraic', 'vector', 'bundles', 'on', 'smooth', 'kschemes', 'x', 'contractible', 'from', 'the', 'standpoint', 'of', 'a1homotopy', 'theory', 'when', 'k', 'c', 'the', 'smooth', 'manifolds', 'xc', 'are', 'contractible', 'as', 'topological', 'spaces', 'the', 'integral', 'algebraic', 'ktheory', 'and', '... | [-0.244866586239479, 0.10674040549851925, -0.05834081928307181, 0.07220561901694826, -0.11386488873138079, -0.2248251593605554, -0.026034046687199948, 0.41686816213813227, -0.3237552919997101, -0.146267012891544, 0.12193200552214391, -0.22667642780000505, -0.19323207649667062, 0.21729685654060035, -0.15643939577683635,... |
710.3608 | Embedding Bratteli-Vershik systems in cellular automata | Many dynamical systems can be naturally represented as `Bratteli-Vershik' (or
`adic') systems, which provide an appealing combinatorial description of their
dynamics. If an adic system X satisfies two technical conditions (`focus' and
`bounded width') then we show how to represent X using a two-dimensional
subshift o... | math.DS | many dynamical systems can be naturally represented as brattelivershik or adic systems which provide an appealing combinatorial description of their dynamics if an adic system x satisfies two technical conditions focus and bounded width then we show how to represent x using a twodimensional subshift of finite type y ea... | [['many', 'dynamical', 'systems', 'can', 'be', 'naturally', 'represented', 'as', 'brattelivershik', 'or', 'adic', 'systems', 'which', 'provide', 'an', 'appealing', 'combinatorial', 'description', 'of', 'their', 'dynamics', 'if', 'an', 'adic', 'system', 'x', 'satisfies', 'two', 'technical', 'conditions', 'focus', 'and',... | [-0.18378085823744975, 0.1407073148296805, -0.07495190570304214, 0.038100968410131025, -0.03254751058100441, -0.17826387820162543, 0.05910733618318688, 0.3985674713211235, -0.37013912986054326, -0.1744983827897398, 0.07909652477314393, -0.2547490169662376, -0.1471016721875775, 0.16818392877611368, -0.13149309773341022,... |
710.3609 | CARS polarized microscopy of three-dimensional director structures in
liquid crystals | We demonstrate three-dimensional vibrational imaging of director structures
in liquid crystals using coherent anti-Stokes Raman scattering (CARS) polarized
microscopy. Spatial mapping of the structures is based on sensitivity of a
polarized CARS signal to orientation of anisotropic molecules in liquid
crystals. As an... | cond-mat.soft cond-mat.mtrl-sci physics.bio-ph physics.chem-ph physics.optics | we demonstrate threedimensional vibrational imaging of director structures in liquid crystals using coherent antistokes raman scattering cars polarized microscopy spatial mapping of the structures is based on sensitivity of a polarized cars signal to orientation of anisotropic molecules in liquid crystals as an example... | [['we', 'demonstrate', 'threedimensional', 'vibrational', 'imaging', 'of', 'director', 'structures', 'in', 'liquid', 'crystals', 'using', 'coherent', 'antistokes', 'raman', 'scattering', 'cars', 'polarized', 'microscopy', 'spatial', 'mapping', 'of', 'the', 'structures', 'is', 'based', 'on', 'sensitivity', 'of', 'a', 'p... | [-0.10615851977726797, 0.1765732958024396, -0.09612876889799293, -0.03066446099625397, -0.02416284435202141, -0.11274969071854611, 0.007097485210161304, 0.5362329462895522, -0.2986810564793445, -0.23118416184081217, 0.019421369157498702, -0.3277871397235808, -0.1696636734744282, 0.1915471450318708, 0.037848865809988835... |
710.361 | Effects of a tungsten addition on the morphological evolution, spatial
correlations, and temporal evolution of a model Ni-Al-Cr superalloy | The effect of adding 2 at.% W to a model Ni-Al-Cr superalloy on the
morphological evolution, spatial correlations and temporal evolution of
g'(L12)-precipitates at 1073 K is studied with scanning electron microscopy and
atomic force microscopy. Adding W yields a larger microhardness, earlier onset
of spheroidal-to-cu... | cond-mat.mtrl-sci | the effect of adding 2 at w to a model nialcr superalloy on the morphological evolution spatial correlations and temporal evolution of gl12precipitates at 1073 k is studied with scanning electron microscopy and atomic force microscopy adding w yields a larger microhardness earlier onset of spheroidaltocuboidal precipit... | [['the', 'effect', 'of', 'adding', '2', 'at', 'w', 'to', 'a', 'model', 'nialcr', 'superalloy', 'on', 'the', 'morphological', 'evolution', 'spatial', 'correlations', 'and', 'temporal', 'evolution', 'of', 'gl12precipitates', 'at', '1073', 'k', 'is', 'studied', 'with', 'scanning', 'electron', 'microscopy', 'and', 'atomic'... | [-0.07274003308982803, 0.21360764457868078, -0.0825898610562898, 0.02210123473345541, 0.005029923688524809, -0.15248112655423868, 0.045660189485016205, 0.3683175985725262, -0.27561599396479625, -0.345345174316884, 0.0009615546023735824, -0.3582046060130382, -0.054225900302975416, 0.14175674598365545, 0.0358081088604357... |
710.3611 | Speeding up HMC with better integrators | We discuss how dynamical fermion computations may be made yet cheaper by
using symplectic integrators that conserve energy much more accurately without
decreasing the integration step size. We first explain why symplectic
integrators exactly conserve a ``shadow'' Hamiltonian close to the desired one,
and how this Ham... | hep-lat | we discuss how dynamical fermion computations may be made yet cheaper by using symplectic integrators that conserve energy much more accurately without decreasing the integration step size we first explain why symplectic integrators exactly conserve a shadow hamiltonian close to the desired one and how this hamiltonian... | [['we', 'discuss', 'how', 'dynamical', 'fermion', 'computations', 'may', 'be', 'made', 'yet', 'cheaper', 'by', 'using', 'symplectic', 'integrators', 'that', 'conserve', 'energy', 'much', 'more', 'accurately', 'without', 'decreasing', 'the', 'integration', 'step', 'size', 'we', 'first', 'explain', 'why', 'symplectic', '... | [-0.11858150627835863, 0.12406713739867763, -0.10455509496838317, 0.1244908822510868, -0.13623699575460466, -0.13750513340707493, 0.028973905333541623, 0.369913367464301, -0.3101198745858964, -0.3345408268316194, 0.09705945950492408, -0.19964575173347726, -0.18757148590047173, 0.18629159883762053, -0.09601731443698265,... |
710.3612 | Adaptive Multigrid Algorithm for the QCD Dirac-Wilson Operator | We present a new multigrid solver that is suitable for the Dirac operator in
the presence of disordered gauge fields. The key behind the success of the
algorithm is an adaptive projection onto the coarse grids that preserves the
near null space. The resulting algorithm has weak dependence on the gauge
coupling and ex... | hep-lat | we present a new multigrid solver that is suitable for the dirac operator in the presence of disordered gauge fields the key behind the success of the algorithm is an adaptive projection onto the coarse grids that preserves the near null space the resulting algorithm has weak dependence on the gauge coupling and exhibi... | [['we', 'present', 'a', 'new', 'multigrid', 'solver', 'that', 'is', 'suitable', 'for', 'the', 'dirac', 'operator', 'in', 'the', 'presence', 'of', 'disordered', 'gauge', 'fields', 'the', 'key', 'behind', 'the', 'success', 'of', 'the', 'algorithm', 'is', 'an', 'adaptive', 'projection', 'onto', 'the', 'coarse', 'grids', '... | [-0.15074491574379958, 0.1469966301613711, -0.08801877302558798, 0.04571266889290296, -0.06352738590028725, -0.12850853677618465, 0.00422672501238259, 0.36449857830609145, -0.22677445808719648, -0.22322122879191547, 0.08647499380841557, -0.25668671157358114, -0.15513903566783196, 0.15425455864016457, -0.017982170935475... |
710.3613 | FFLO state in thin superconducting films | We present the analysis of the inhomogeneous Fulde-Ferrell-Larkin-Ovchinnikov
(FFLO) superconducting state in thin superconducting films in the parallel
magnetic field. For the tetragonal crystal symmetry (relevant to CeCoIn$_{5}$ -
the most probable candidate for the FFLO state formation) we predict a very
peculiar ... | cond-mat.supr-con cond-mat.str-el | we present the analysis of the inhomogeneous fuldeferrelllarkinovchinnikov fflo superconducting state in thin superconducting films in the parallel magnetic field for the tetragonal crystal symmetry relevant to cecoin_5 the most probable candidate for the fflo state formation we predict a very peculiar inplane angular ... | [['we', 'present', 'the', 'analysis', 'of', 'the', 'inhomogeneous', 'fuldeferrelllarkinovchinnikov', 'fflo', 'superconducting', 'state', 'in', 'thin', 'superconducting', 'films', 'in', 'the', 'parallel', 'magnetic', 'field', 'for', 'the', 'tetragonal', 'crystal', 'symmetry', 'relevant', 'to', 'cecoin_5', 'the', 'most',... | [-0.2669645307700165, 0.23432769149688298, -0.06830278522379342, 0.04457785717270795, -0.10705819600335663, -0.11168217157117194, 0.0744226845701979, 0.3285519225552442, -0.2357007552535155, -0.26203005962140324, -0.005675165087080723, -0.23180632433661866, -0.02278410268962265, 0.17812678415793926, 0.10071631792991881... |
710.3614 | Star Clusters in the Nearby Late-Type Galaxy NGC 1311 | Ultraviolet, optical and near infrared images of the nearby (D ~ 5.5 Mpc) SBm
galaxy NGC 1311, obtained with the Hubble Space Telescope, reveal a small
population of 13 candidate star clusters. We identify candidate star clusters
based on a combination of their luminosity, extent and spectral energy
distribution. The... | astro-ph | ultraviolet optical and near infrared images of the nearby d 55 mpc sbm galaxy ngc 1311 obtained with the hubble space telescope reveal a small population of 13 candidate star clusters we identify candidate star clusters based on a combination of their luminosity extent and spectral energy distribution the masses of th... | [['ultraviolet', 'optical', 'and', 'near', 'infrared', 'images', 'of', 'the', 'nearby', 'd', '55', 'mpc', 'sbm', 'galaxy', 'ngc', '1311', 'obtained', 'with', 'the', 'hubble', 'space', 'telescope', 'reveal', 'a', 'small', 'population', 'of', '13', 'candidate', 'star', 'clusters', 'we', 'identify', 'candidate', 'star', '... | [-0.05723741055540317, 0.15343704549353812, -0.0669095580580995, 0.10309707189913138, -0.07915316532855829, -0.03800399414892611, 0.09374089784279176, 0.43324553538355737, -0.15440411279098942, -0.4238066733814776, 0.05157492016200218, -0.2824833218632689, 0.007070077398743529, 0.1752377569345854, -0.024304357747390093... |
710.3615 | Paramagnonlike excitations and spin diffusion in magnetic resonance
studies of copper oxide superconductors | The relaxation function theory for a doped two-dimensional Heisenberg
antiferromagnetic system in the paramagnetic state for all wave vectors through
the Brillouin zone is presented in view of low frequency response of high-$T_c$
copper oxide superconductors. We deduced the regions of long lifetime [$T
\lesssim 400(1... | cond-mat.supr-con cond-mat.str-el | the relaxation function theory for a doped twodimensional heisenberg antiferromagnetic system in the paramagnetic state for all wave vectors through the brillouin zone is presented in view of low frequency response of hight_c copper oxide superconductors we deduced the regions of long lifetime t lesssim 40014x k and ov... | [['the', 'relaxation', 'function', 'theory', 'for', 'a', 'doped', 'twodimensional', 'heisenberg', 'antiferromagnetic', 'system', 'in', 'the', 'paramagnetic', 'state', 'for', 'all', 'wave', 'vectors', 'through', 'the', 'brillouin', 'zone', 'is', 'presented', 'in', 'view', 'of', 'low', 'frequency', 'response', 'of', 'hig... | [-0.19665423150698857, 0.2646183699166038, -8.144066936668309e-05, 0.0023126409659376262, -0.02007952141147321, -0.12611477193757142, 0.15061533528556725, 0.3727016604623233, -0.2723940709477355, -0.1985137925805101, -0.0029071234568054305, -0.3652221820820337, -0.028374807919835907, 0.2018459639993721, 0.1021132582755... |
710.3616 | Coincidences of Dark Energy with Dark Matter -- Clues for a Simple
Alternative? | A rare coincidence of scales in standard particle physics is needed to
explain why $\Lambda$ or the negative pressure of cosmological dark energy (DE)
coincides with the positive pressure $P_0$ of random motion of dark matter (DM)
in bright galaxies. Recently Zlosnik et al. (2007) propose to modify the
Einsteinian cu... | astro-ph gr-qc hep-ph | a rare coincidence of scales in standard particle physics is needed to explain why lambda or the negative pressure of cosmological dark energy de coincides with the positive pressure p_0 of random motion of dark matter dm in bright galaxies recently zlosnik et al 2007 propose to modify the einsteinian curvature by addi... | [['a', 'rare', 'coincidence', 'of', 'scales', 'in', 'standard', 'particle', 'physics', 'is', 'needed', 'to', 'explain', 'why', 'lambda', 'or', 'the', 'negative', 'pressure', 'of', 'cosmological', 'dark', 'energy', 'de', 'coincides', 'with', 'the', 'positive', 'pressure', 'p_0', 'of', 'random', 'motion', 'of', 'dark', '... | [-0.12354928719380881, 0.18753976172261072, -0.1232017377957876, 0.09426004733081515, -0.13082256328181108, -0.1351036475181623, -0.039906620943907935, 0.3150760321006484, -0.22390575366563092, -0.3316569774689382, 0.010846333496533987, -0.24361520183234536, -0.06107919803025386, 0.12540755856153146, -0.017559635037643... |
710.3617 | Top physics at the Tevatron Collider | The top quark has been discovered in 1995 at the CDF and DO experiments
located in the Tevatron ring at the Fermilab laboratory. After more than a
decade the Tevatron collider, with its center-of-mass energy collisions of 1.96
TeV, is still the only machine capable of producing such exceptionally heavy
particle. Here... | hep-ex | the top quark has been discovered in 1995 at the cdf and do experiments located in the tevatron ring at the fermilab laboratory after more than a decade the tevatron collider with its centerofmass energy collisions of 196 tev is still the only machine capable of producing such exceptionally heavy particle here i presen... | [['the', 'top', 'quark', 'has', 'been', 'discovered', 'in', '1995', 'at', 'the', 'cdf', 'and', 'do', 'experiments', 'located', 'in', 'the', 'tevatron', 'ring', 'at', 'the', 'fermilab', 'laboratory', 'after', 'more', 'than', 'a', 'decade', 'the', 'tevatron', 'collider', 'with', 'its', 'centerofmass', 'energy', 'collisio... | [-0.028877021671062937, 0.1646389491252706, -0.11803947294025983, 0.08237322512522183, -0.06593310919550943, -0.15164204202198855, -0.010131194305435662, 0.368405927654723, -0.1550343342889494, -0.3404478872011245, 0.0363663311122956, -0.38640114937869596, 0.10216547939664042, 0.18544670494607793, 0.0821632271448911, 0... |
710.3618 | Fast algorithms for matching CCD images to a stellar catalogue | Two new algorithms are described for matching two dimensional coordinate
lists of point sources that are signifcantly faster than previous methods. By
matching rarely occurring triangles (or more complex shapes) in the two lists,
and by ordering searches by decreasing probability of success, it is
demonstrated that v... | astro-ph | two new algorithms are described for matching two dimensional coordinate lists of point sources that are signifcantly faster than previous methods by matching rarely occurring triangles or more complex shapes in the two lists and by ordering searches by decreasing probability of success it is demonstrated that very few... | [['two', 'new', 'algorithms', 'are', 'described', 'for', 'matching', 'two', 'dimensional', 'coordinate', 'lists', 'of', 'point', 'sources', 'that', 'are', 'signifcantly', 'faster', 'than', 'previous', 'methods', 'by', 'matching', 'rarely', 'occurring', 'triangles', 'or', 'more', 'complex', 'shapes', 'in', 'the', 'two',... | [-0.11314589159363615, 0.1120754686766007, -0.026832869508047114, 0.059115163225558306, -0.05361117634860495, -0.15015396746041784, 0.082808425402915, 0.43498147638248547, -0.20953669847103254, -0.4015536196957513, 0.12838491768224583, -0.2630623017143154, -0.07206537659227734, 0.22429098777487227, -0.03776417777259425... |
710.3619 | Eternally inflating cosmologies from intersecting spacelike branes | Intersecting spacelike braneworld cosmologies are investigated. The time axis
is set on the scale parameter of extra space, which may include more than one
timelike metric. Obtained are eternally inflating (i.e. undergoing late-time
inflation) Robertson-Walker spacetime and extra space with a constant scale
factor. I... | hep-th | intersecting spacelike braneworld cosmologies are investigated the time axis is set on the scale parameter of extra space which may include more than one timelike metric obtained are eternally inflating ie undergoing latetime inflation robertsonwalker spacetime and extra space with a constant scale factor in the case o... | [['intersecting', 'spacelike', 'braneworld', 'cosmologies', 'are', 'investigated', 'the', 'time', 'axis', 'is', 'set', 'on', 'the', 'scale', 'parameter', 'of', 'extra', 'space', 'which', 'may', 'include', 'more', 'than', 'one', 'timelike', 'metric', 'obtained', 'are', 'eternally', 'inflating', 'ie', 'undergoing', 'late... | [-0.2229627477026019, 0.18521364537016966, -0.02948996560791364, 0.11243201344041154, -0.14478236011778697, -0.19676258931091675, -0.07447406946299359, 0.33253067512160694, -0.14519405578716826, -0.268125001532145, 0.16538396749633533, -0.277002184281651, -0.06132145235852267, 0.11783439629018688, -0.06058414101164836,... |
710.362 | Nonlinear completion of massive gravity of the Fierz-Pauli type | A possible nonlinear completion of massive gravity of the Fierz-Pauli type is
proposed. The theory describes a system consisting of a massive tensor field of
the Fierz-Pauli type and an additional massive vector field. Massless limit as
well as flat-spacetime limit can be taken smoothly. Constructing a nonlinear
vers... | hep-th | a possible nonlinear completion of massive gravity of the fierzpauli type is proposed the theory describes a system consisting of a massive tensor field of the fierzpauli type and an additional massive vector field massless limit as well as flatspacetime limit can be taken smoothly constructing a nonlinear version of t... | [['a', 'possible', 'nonlinear', 'completion', 'of', 'massive', 'gravity', 'of', 'the', 'fierzpauli', 'type', 'is', 'proposed', 'the', 'theory', 'describes', 'a', 'system', 'consisting', 'of', 'a', 'massive', 'tensor', 'field', 'of', 'the', 'fierzpauli', 'type', 'and', 'an', 'additional', 'massive', 'vector', 'field', '... | [-0.17688853327328197, 0.16023657197678964, -0.07413798243953632, 0.08482007197677516, -0.12620942082542638, -0.15826735702844766, -0.053320953488134995, 0.21936688938966165, -0.2127137733480105, -0.2877278829423281, 0.10958135922511036, -0.21864590518749677, -0.17521827799053147, 0.1027162888732094, -0.052495016157627... |
710.3621 | Numerical removal of water-vapor effects from THz-TDS measurements | One source of disturbance in a pulsed T-ray signal is attributed to ambient
water vapor. Water molecules in the gas phase selectively absorb T-rays at
discrete frequencies corresponding to their molecular rotational transitions.
This results in prominent resonances spread over the T-ray spectrum, and in the
time doma... | cs.CE physics.comp-ph | one source of disturbance in a pulsed tray signal is attributed to ambient water vapor water molecules in the gas phase selectively absorb trays at discrete frequencies corresponding to their molecular rotational transitions this results in prominent resonances spread over the tray spectrum and in the time domain the t... | [['one', 'source', 'of', 'disturbance', 'in', 'a', 'pulsed', 'tray', 'signal', 'is', 'attributed', 'to', 'ambient', 'water', 'vapor', 'water', 'molecules', 'in', 'the', 'gas', 'phase', 'selectively', 'absorb', 'trays', 'at', 'discrete', 'frequencies', 'corresponding', 'to', 'their', 'molecular', 'rotational', 'transiti... | [-0.09303590331253138, 0.16104949198115878, -0.07147854693473606, 0.008007659725245763, -0.051082524511832414, -0.11440006720054655, 0.07152061535206171, 0.4122066726684788, -0.28031973933463383, -0.2879907425754426, 0.12567140479716446, -0.2717016593768256, -0.09532011235514057, 0.17981406427070237, -0.072430662805356... |
710.3622 | Hyperon-nucleon potentials from lattice QCD | We calculate $p\Xi^0$ potentials from the equal-time Bethe-Salpeter amplitude
measured in the quenched QCD simulation with the spatial lattice volume, (4.4
fm)$^3$. The standard Wilson gauge action with the gauge coupling $\beta=5.7$
on $32^4$ lattice together with the standard Wilson quark action are used. The
hoppi... | hep-lat | we calculate pxi0 potentials from the equaltime bethesalpeter amplitude measured in the quenched qcd simulation with the spatial lattice volume 44 fm3 the standard wilson gauge action with the gauge coupling beta57 on 324 lattice together with the standard wilson quark action are used the hopping parameter kappa_ud0167... | [['we', 'calculate', 'pxi0', 'potentials', 'from', 'the', 'equaltime', 'bethesalpeter', 'amplitude', 'measured', 'in', 'the', 'quenched', 'qcd', 'simulation', 'with', 'the', 'spatial', 'lattice', 'volume', '44', 'fm3', 'the', 'standard', 'wilson', 'gauge', 'action', 'with', 'the', 'gauge', 'coupling', 'beta57', 'on', '... | [-0.13868559457459093, 0.2733396366877737, -0.05935635602746914, 0.08872294700567555, -0.011265558610652007, -0.1591504722638847, 0.07283341608259802, 0.3807939569788431, -0.17104431813935828, -0.23116483686497935, -0.005706890979994795, -0.2970672935442208, 0.021388235404551807, 0.060917871909861275, 0.094822495407082... |
710.3623 | Subsonic Flows for the Full Euler Equations in Half Plane | We study the subsonic flows governed by full Euler equations in the half
plane bounded below by a piecewise smooth curve asymptotically approaching
x1-axis. Nonconstant conditions in the far field are prescribed to ensure the
real Euler flows. The Euler system is reduced to a single elliptic equation for
the stream f... | math.AP | we study the subsonic flows governed by full euler equations in the half plane bounded below by a piecewise smooth curve asymptotically approaching x1axis nonconstant conditions in the far field are prescribed to ensure the real euler flows the euler system is reduced to a single elliptic equation for the stream functi... | [['we', 'study', 'the', 'subsonic', 'flows', 'governed', 'by', 'full', 'euler', 'equations', 'in', 'the', 'half', 'plane', 'bounded', 'below', 'by', 'a', 'piecewise', 'smooth', 'curve', 'asymptotically', 'approaching', 'x1axis', 'nonconstant', 'conditions', 'in', 'the', 'far', 'field', 'are', 'prescribed', 'to', 'ensur... | [-0.20955101882089983, 0.07460162474527815, -0.1127545594958202, 0.07832435599554612, -0.06163522015097288, -0.12495392883407339, -0.002491085245361868, 0.2621106241460679, -0.2943813618017747, -0.22852039340672628, 0.17005843813377344, -0.2832073147830395, -0.09930933409651636, 0.24438019815551223, -0.0474105477508790... |
710.3624 | Cosmology of Gravitino LSP Scenario with Right-Handed Sneutrino NLSP | We consider supersymmetric model with right-handed (s)neutrinos where the
neutrino masses are purely Dirac-type. We discuss cosmology based on such a
scenario, paying particular attention to the case that the gravitino is the
lightest superparticles (LSP) while the right-handed sneutrino is the next-LSP.
It will be s... | hep-ph | we consider supersymmetric model with righthanded sneutrinos where the neutrino masses are purely diractype we discuss cosmology based on such a scenario paying particular attention to the case that the gravitino is the lightest superparticles lsp while the righthanded sneutrino is the nextlsp it will be shown that the... | [['we', 'consider', 'supersymmetric', 'model', 'with', 'righthanded', 'sneutrinos', 'where', 'the', 'neutrino', 'masses', 'are', 'purely', 'diractype', 'we', 'discuss', 'cosmology', 'based', 'on', 'such', 'a', 'scenario', 'paying', 'particular', 'attention', 'to', 'the', 'case', 'that', 'the', 'gravitino', 'is', 'the',... | [-0.1077608672392671, 0.22516636665677653, -0.013259022776037455, 0.19952627906168346, -0.11935031667235307, -0.1612779440009035, -0.015413201175397262, 0.34454768743889874, -0.2403204868431203, -0.27702664844691754, 0.09925201484584249, -0.2781980304396711, -0.07160237338393927, 0.15481383250735234, -0.027415317698614... |
710.3625 | Lattice calculation of the QGP viscosities - Present results and next
project - | The shear and bulk viscosities of gluon plasma are calculated by accumulating
a large amount of data for the Matsubara Green function ($G_{\beta}(t_m)$) on
isotropic $24^3 \times 8$ and $16^3 \times 8$ lattices. In the case of
Iwasaki's improved action, the calculations of $G_{\beta}(t_m)$ are carried out
on roughly ... | hep-lat | the shear and bulk viscosities of gluon plasma are calculated by accumulating a large amount of data for the matsubara green function g_betat_m on isotropic 243 times 8 and 163 times 8 lattices in the case of iwasakis improved action the calculations of g_betat_m are carried out on roughly 6 million configurations whil... | [['the', 'shear', 'and', 'bulk', 'viscosities', 'of', 'gluon', 'plasma', 'are', 'calculated', 'by', 'accumulating', 'a', 'large', 'amount', 'of', 'data', 'for', 'the', 'matsubara', 'green', 'function', 'g_betat_m', 'on', 'isotropic', '243', 'times', '8', 'and', '163', 'times', '8', 'lattices', 'in', 'the', 'case', 'of'... | [-0.10843763605482253, 0.17418962836708918, -0.07032148916651762, 0.05676344652339151, -0.0128128267024615, -0.06727354650873904, 0.03716250941863013, 0.36401393166066265, -0.2274015276935895, -0.30683405645856315, 0.09953442533471774, -0.3049845760442021, -0.06834374478349405, 0.20077079160463082, 0.001114621990009535... |
710.3626 | Twenty Years of Searching for (and Finding) Globular Cluster Pulsars | Globular clusters produce orders of magnitude more millisecond pulsars per
unit mass than the Galactic disk. Since the first cluster pulsar was uncovered
twenty years ago, at least 138 have been identified - most of which are binary
millisecond pulsars. Because of their origins involving stellar encounters,
many of t... | astro-ph | globular clusters produce orders of magnitude more millisecond pulsars per unit mass than the galactic disk since the first cluster pulsar was uncovered twenty years ago at least 138 have been identified most of which are binary millisecond pulsars because of their origins involving stellar encounters many of these sys... | [['globular', 'clusters', 'produce', 'orders', 'of', 'magnitude', 'more', 'millisecond', 'pulsars', 'per', 'unit', 'mass', 'than', 'the', 'galactic', 'disk', 'since', 'the', 'first', 'cluster', 'pulsar', 'was', 'uncovered', 'twenty', 'years', 'ago', 'at', 'least', '138', 'have', 'been', 'identified', 'most', 'of', 'whi... | [-0.1254936641936573, 0.19844228134856426, -0.06312801060058908, 0.136165727252124, -0.13681397992019942, -0.038616950099822134, 0.03799981667387848, 0.37858206492715646, -0.18131194033880352, -0.378162446964, 0.06276428533497633, -0.3235233381523618, -0.00498454793289836, 0.3074765011136021, -0.00161511663048129, 0.00... |
710.3627 | Homotopy on spatial graphs and generalized Sato-Levine invariants | Edge-homotopy and vertex-homotopy are equivalence relations on spatial graphs
which are generalizations of Milnor's link-homotopy. Fleming and the author
introduced some edge (resp. vertex)-homotopy invariants of spatial graphs by
applying the Sato-Levine invariant for the constituent 2-component
algebraically split ... | math.GT | edgehomotopy and vertexhomotopy are equivalence relations on spatial graphs which are generalizations of milnors linkhomotopy fleming and the author introduced some edge resp vertexhomotopy invariants of spatial graphs by applying the satolevine invariant for the constituent 2component algebraically split links in this... | [['edgehomotopy', 'and', 'vertexhomotopy', 'are', 'equivalence', 'relations', 'on', 'spatial', 'graphs', 'which', 'are', 'generalizations', 'of', 'milnors', 'linkhomotopy', 'fleming', 'and', 'the', 'author', 'introduced', 'some', 'edge', 'resp', 'vertexhomotopy', 'invariants', 'of', 'spatial', 'graphs', 'by', 'applying... | [-0.2535138035350492, 0.14566721129034396, -0.06519335900551416, 0.11397612025849783, -0.1333878152859463, -0.17949642965071638, 0.005517274851281144, 0.30805887874793, -0.2842938569702313, -0.31394400665352884, 0.06989910190393754, -0.2483758919898578, -0.17891295705462845, 0.09984387268482799, -0.09823968329034011, 0... |
710.3628 | Universal Baxterization for $\mathbb{Z}$-graded Hopf algebras | We present a method for Baxterizing solutions of the constant Yang-Baxter
equation associated with $\mathbb{Z}$-graded Hopf algebras. To demonstrate the
approach, we provide examples for the Taft algebras and the quantum group
$U_q[sl(2)]$.
| math.QA | we present a method for baxterizing solutions of the constant yangbaxter equation associated with mathbbzgraded hopf algebras to demonstrate the approach we provide examples for the taft algebras and the quantum group u_qsl2 | [['we', 'present', 'a', 'method', 'for', 'baxterizing', 'solutions', 'of', 'the', 'constant', 'yangbaxter', 'equation', 'associated', 'with', 'mathbbzgraded', 'hopf', 'algebras', 'to', 'demonstrate', 'the', 'approach', 'we', 'provide', 'examples', 'for', 'the', 'taft', 'algebras', 'and', 'the', 'quantum', 'group', 'u_q... | [-0.15243614744395018, -0.008947754802647978, -0.06295970274368301, 0.04296530535793863, -0.13903408165788278, -0.19262720584811177, -0.03750040843442548, 0.3660751553834416, -0.36827147426083684, -0.17228850786341354, 0.13554218427452724, -0.27278967830352485, -0.22888706100638956, 0.24081038375152275, -0.081495417078... |
710.3629 | Dynamical quark recombination in ultrarelativistic heavy-ion collisions
and the proton to pion ratio | We study quark thermal recombination as a function of energy density during
the evolution of a heavy-ion collision in a numerical model that reproduces
aspects of QCD phenomenology. We show that starting with a set of free quarks
(or quarks and antiquarks) the probability to form colorless clusters of three
quarks di... | hep-ph nucl-th | we study quark thermal recombination as a function of energy density during the evolution of a heavyion collision in a numerical model that reproduces aspects of qcd phenomenology we show that starting with a set of free quarks or quarks and antiquarks the probability to form colorless clusters of three quarks differs ... | [['we', 'study', 'quark', 'thermal', 'recombination', 'as', 'a', 'function', 'of', 'energy', 'density', 'during', 'the', 'evolution', 'of', 'a', 'heavyion', 'collision', 'in', 'a', 'numerical', 'model', 'that', 'reproduces', 'aspects', 'of', 'qcd', 'phenomenology', 'we', 'show', 'that', 'starting', 'with', 'a', 'set', ... | [-0.051621967395558285, 0.19836237098828083, -0.14974866261224398, 0.10299530542936972, -0.008498375977682516, -0.0527131772342431, 0.07065677382130427, 0.3517259298614488, -0.20624601700489692, -0.27533669959690965, -0.005086454554340604, -0.30619092605840625, -0.0007513150339946151, 0.11802747179597115, 0.04120063947... |
710.363 | Scattering for the non-radial 3D cubic nonlinear Schroedinger equation | Scattering of radial $H^1$ solutions to the 3D focusing cubic nonlinear
Schr\"odinger equation below a mass-energy threshold $M[u]E[u] < M[Q]E[Q]$ and
satisfying an initial mass-gradient bound $\|u_0\|_{L^2} \|\nabla u_0 \|_{L^2}
< \|Q\|_{L^2} \|\nabla Q\|_{L^2}$, where $Q$ is the ground state, was
established in Hol... | math.AP | scattering of radial h1 solutions to the 3d focusing cubic nonlinear schrodinger equation below a massenergy threshold mueu mqeq and satisfying an initial massgradient bound u_0_l2 nabla u_0 _l2 q_l2 nabla q_l2 where q is the ground state was established in holmerroudenko 2007 in this note we extend the result in holme... | [['scattering', 'of', 'radial', 'h1', 'solutions', 'to', 'the', '3d', 'focusing', 'cubic', 'nonlinear', 'schrodinger', 'equation', 'below', 'a', 'massenergy', 'threshold', 'mueu', 'mqeq', 'and', 'satisfying', 'an', 'initial', 'massgradient', 'bound', 'u_0_l2', 'nabla', 'u_0', '_l2', 'q_l2', 'nabla', 'q_l2', 'where', 'q... | [-0.14503289743359865, 0.06868981003130362, -0.09103950977857624, 0.07789909818218023, -0.10994743865947905, -0.10411488908097713, 0.0020046245024007347, 0.2874861182312348, -0.2727178376486076, -0.24147601291354345, 0.09292024410803736, -0.2780270784527862, -0.08028706650449229, 0.15818672929058916, -0.065112297281822... |
710.3631 | The Interaction of Stellar Objects within a Common Envelope | We use high-resolution, three-dimensional hydrodynamic simulations to study
the hydrodynamic and gravitational interaction between stellar companions
embedded within a differentially rotating common envelope. Specifically, we
evaluate the contributions of the nonaxisymmetric gravitational tides and ram
pressure force... | astro-ph | we use highresolution threedimensional hydrodynamic simulations to study the hydrodynamic and gravitational interaction between stellar companions embedded within a differentially rotating common envelope specifically we evaluate the contributions of the nonaxisymmetric gravitational tides and ram pressure forces to th... | [['we', 'use', 'highresolution', 'threedimensional', 'hydrodynamic', 'simulations', 'to', 'study', 'the', 'hydrodynamic', 'and', 'gravitational', 'interaction', 'between', 'stellar', 'companions', 'embedded', 'within', 'a', 'differentially', 'rotating', 'common', 'envelope', 'specifically', 'we', 'evaluate', 'the', 'co... | [-0.1574521164277669, 0.1429053865306471, -0.10061063290718389, 0.10200484724152153, -0.0881932873870372, -0.005151247470387937, 0.014581905339680915, 0.30474492153026966, -0.21608355148645067, -0.2895207736213264, 0.03427849210424323, -0.22985888171211086, -0.09946677365617172, 0.24130425093431226, -0.0209070558886270... |
710.3632 | 2-pile Nim with a Restricted Number of Move-size Imitations | We study a variation of the combinatorial game of 2-pile Nim. Move as in
2-pile Nim but with the following constraint:
Suppose the previous player has just removed say $x>0$ tokens from the
shorter pile (either pile in case they have the same height). If the next
player now removes $x$ tokens from the larger pile, ... | math.CO | we study a variation of the combinatorial game of 2pile nim move as in 2pile nim but with the following constraint suppose the previous player has just removed say x0 tokens from the shorter pile either pile in case they have the same height if the next player now removes x tokens from the larger pile then he imitates ... | [['we', 'study', 'a', 'variation', 'of', 'the', 'combinatorial', 'game', 'of', '2pile', 'nim', 'move', 'as', 'in', '2pile', 'nim', 'but', 'with', 'the', 'following', 'constraint', 'suppose', 'the', 'previous', 'player', 'has', 'just', 'removed', 'say', 'x0', 'tokens', 'from', 'the', 'shorter', 'pile', 'either', 'pile',... | [-0.07135782003187255, 0.12462730330179199, -0.13747858000411425, 0.06095962828188551, -0.10615349686774078, -0.24297877491118192, 0.1321097819635005, 0.36740106804324174, -0.296409684661563, -0.270277125080448, 0.041346413448258346, -0.30071779286294287, -0.11791471889548337, 0.06494524047028885, -0.17532264774164824,... |
710.3633 | Dynamics in Thompson's Group F | We describe an explicit relationship between strand diagrams and
piecewise-linear functions for elements of Thompson's group F. Using this
correspondence, we investigate the dynamics of elements of F, and we show that
conjugacy of one-bump functions can be described by a Mather-type invariant.
| math.GR math.DS | we describe an explicit relationship between strand diagrams and piecewiselinear functions for elements of thompsons group f using this correspondence we investigate the dynamics of elements of f and we show that conjugacy of onebump functions can be described by a mathertype invariant | [['we', 'describe', 'an', 'explicit', 'relationship', 'between', 'strand', 'diagrams', 'and', 'piecewiselinear', 'functions', 'for', 'elements', 'of', 'thompsons', 'group', 'f', 'using', 'this', 'correspondence', 'we', 'investigate', 'the', 'dynamics', 'of', 'elements', 'of', 'f', 'and', 'we', 'show', 'that', 'conjugac... | [-0.17471638869312478, 0.11659985811132995, -0.11213756236815597, 0.08437597151368675, -0.013517030264909675, -0.06723707792826178, 0.0595064804684825, 0.4217637359369092, -0.34764654643651915, -0.24058189642865482, 0.01599932317735582, -0.2413600457082616, -0.23744431883096695, 0.17697187926529384, -0.0727795180296752... |
710.3634 | Neutrino Emission From Inhomogeneous Pion Condensed Quark Matter | It is believed that quark matter can exist in neutron star interior if the
baryon density is high enough. When there is a large isospin density, quark
matter could be in a pion condensed phase. We compute neutrino emission from
direct Urca processes in such a phase, particularly in the inhomogeneous
Larkin-Ovchinniko... | hep-ph astro-ph nucl-th | it is believed that quark matter can exist in neutron star interior if the baryon density is high enough when there is a large isospin density quark matter could be in a pion condensed phase we compute neutrino emission from direct urca processes in such a phase particularly in the inhomogeneous larkinovchinnikovfuldef... | [['it', 'is', 'believed', 'that', 'quark', 'matter', 'can', 'exist', 'in', 'neutron', 'star', 'interior', 'if', 'the', 'baryon', 'density', 'is', 'high', 'enough', 'when', 'there', 'is', 'a', 'large', 'isospin', 'density', 'quark', 'matter', 'could', 'be', 'in', 'a', 'pion', 'condensed', 'phase', 'we', 'compute', 'neut... | [-0.07474217326312825, 0.35655068661477685, -0.11065840261880362, 0.16365342917244718, -0.07390070892870426, -0.07873111723692737, 0.07182375563011653, 0.3461434764490611, -0.2040258091536985, -0.2355622169494197, 0.057125767787405544, -0.3060559244704959, -0.011137329892295858, 0.1394872194243784, 0.05546288242887543,... |
710.3635 | Spectral beam combining of Yb-doped fiber lasers using wavelength
dependent polarization rotators and polarization beam combiners | We propose a robust spectral beam combining scheme using wavelength dependent
polarisation rotators and polarization beam combiners. We successfully
demonstrated the concept for two Yb-doped fiber lasers at 1064nm and 1092nm up
to a total input power of 90W. The results reveal a very good combining
efficiency and the... | physics.optics | we propose a robust spectral beam combining scheme using wavelength dependent polarisation rotators and polarization beam combiners we successfully demonstrated the concept for two ybdoped fiber lasers at 1064nm and 1092nm up to a total input power of 90w the results reveal a very good combining efficiency and the pote... | [['we', 'propose', 'a', 'robust', 'spectral', 'beam', 'combining', 'scheme', 'using', 'wavelength', 'dependent', 'polarisation', 'rotators', 'and', 'polarization', 'beam', 'combiners', 'we', 'successfully', 'demonstrated', 'the', 'concept', 'for', 'two', 'ybdoped', 'fiber', 'lasers', 'at', '1064nm', 'and', '1092nm', 'u... | [-0.11367656489213308, 0.07729006981632362, -0.10986608022358268, -0.020251167171712343, -0.004782677783320348, -0.19565481019672007, 0.0801736255234573, 0.5007310084998607, -0.23509450567265353, -0.3059647768735886, 0.048794620854702465, -0.22727525077449778, -0.06430249245216449, 0.2940450470816965, -0.04813552050230... |
710.3636 | The evolution of the peculiar Type Ia supernova SN 2005hk over 400 days | $UBVRI$ photometry and medium resolution optical spectroscopy of peculiar
Type Ia supernova SN 2005hk are presented and analysed, covering the
pre-maximum phase to around 400 days after explosion. The supernova is found to
be underluminous compared to "normal" Type Ia supernovae. The photometric and
spectroscopic evo... | astro-ph | ubvri photometry and medium resolution optical spectroscopy of peculiar type ia supernova sn 2005hk are presented and analysed covering the premaximum phase to around 400 days after explosion the supernova is found to be underluminous compared to normal type ia supernovae the photometric and spectroscopic evolution of ... | [['ubvri', 'photometry', 'and', 'medium', 'resolution', 'optical', 'spectroscopy', 'of', 'peculiar', 'type', 'ia', 'supernova', 'sn', '2005hk', 'are', 'presented', 'and', 'analysed', 'covering', 'the', 'premaximum', 'phase', 'to', 'around', '400', 'days', 'after', 'explosion', 'the', 'supernova', 'is', 'found', 'to', '... | [-0.01768883875920437, 0.09759133416718166, -0.04042596099162964, 0.1407393014818234, -0.14487264588242396, -0.1601273911171838, 0.039370142939917155, 0.442242793738842, -0.1708114116942804, -0.3117715594799895, 0.05714159160300991, -0.32678505921687345, 0.03414296871541362, 0.20832665295303357, -0.051827337742418565, ... |
710.3637 | A Rigidity Theorem for Affine K\"ahler-Ricci Flat Graph | It is shown that any smooth strictly convex global solution of
$$\det(\frac{\partial^{2}u}{\partial \xi_{i}\partial \xi_{j}}) = \exp
\left\{-\sum_{i=1}^n d_i \frac{\partial u}{\partial \xi_{i}} - d_0\right\},$$
where $d_0$, $d_1$,...,$d_n$ are constants, must be a quadratic polynomial.
This extends a well-known theor... | math.DG math.AP | it is shown that any smooth strictly convex global solution of detfracpartial2upartial xi_ipartial xi_j exp leftsum_i1n d_i fracpartial upartial xi_i d_0right where d_0 d_1d_n are constants must be a quadratic polynomial this extends a wellknown theorem of jorgenscalabipogorelov | [['it', 'is', 'shown', 'that', 'any', 'smooth', 'strictly', 'convex', 'global', 'solution', 'of', 'detfracpartial2upartial', 'xi_ipartial', 'xi_j', 'exp', 'leftsum_i1n', 'd_i', 'fracpartial', 'upartial', 'xi_i', 'd_0right', 'where', 'd_0', 'd_1d_n', 'are', 'constants', 'must', 'be', 'a', 'quadratic', 'polynomial', 'thi... | [-0.20784898348467643, 0.10713494536192979, -0.03958750680527266, -0.007760584409184316, -0.11307401874321787, -0.3061092988697483, -0.097701286082156, 0.27642270561088533, -0.38605919693980145, -0.03783924654400086, 0.11718170081867892, -0.3741317967172055, -0.14501034660155282, 0.13936020658515832, -0.102132319637081... |
710.3638 | Nonparametric estimation of correlation functions in longitudinal and
spatial data, with application to colon carcinogenesis experiments | In longitudinal and spatial studies, observations often demonstrate strong
correlations that are stationary in time or distance lags, and the times or
locations of these data being sampled may not be homogeneous. We propose a
nonparametric estimator of the correlation function in such data, using kernel
methods. We d... | math.ST stat.TH | in longitudinal and spatial studies observations often demonstrate strong correlations that are stationary in time or distance lags and the times or locations of these data being sampled may not be homogeneous we propose a nonparametric estimator of the correlation function in such data using kernel methods we develop ... | [['in', 'longitudinal', 'and', 'spatial', 'studies', 'observations', 'often', 'demonstrate', 'strong', 'correlations', 'that', 'are', 'stationary', 'in', 'time', 'or', 'distance', 'lags', 'and', 'the', 'times', 'or', 'locations', 'of', 'these', 'data', 'being', 'sampled', 'may', 'not', 'be', 'homogeneous', 'we', 'propo... | [-0.06507375040142746, 0.06231193083082901, -0.09964621364353941, 0.06481734836527792, -0.015086373286117073, -0.10369512450319694, 0.060819910952417115, 0.3895011478523304, -0.25621236748174653, -0.2658013473316045, 0.12133878558697589, -0.29128668018217596, -0.1561899764749866, 0.17237318994907233, -0.053269358776550... |
710.3639 | Radiative Corrections to High Energy Lepton Bremsstrahlung on Heavy
Nuclei | One-loop radiative corrections to the leptonic tensor in high energy
bremsstrahlung on heavy nuclei are calculated. Virtual and real photon
radiation is taken into account. Double bremsstrahlung is simulated by means of
Monte Carlo. Numerical results are presented for the case of muon
bremsstrahlung in conditions of ... | hep-ph | oneloop radiative corrections to the leptonic tensor in high energy bremsstrahlung on heavy nuclei are calculated virtual and real photon radiation is taken into account double bremsstrahlung is simulated by means of monte carlo numerical results are presented for the case of muon bremsstrahlung in conditions of the co... | [['oneloop', 'radiative', 'corrections', 'to', 'the', 'leptonic', 'tensor', 'in', 'high', 'energy', 'bremsstrahlung', 'on', 'heavy', 'nuclei', 'are', 'calculated', 'virtual', 'and', 'real', 'photon', 'radiation', 'is', 'taken', 'into', 'account', 'double', 'bremsstrahlung', 'is', 'simulated', 'by', 'means', 'of', 'mont... | [-0.0074918542573309075, 0.27196287918083656, -0.05307351898115415, 0.21295875610443404, 0.013952768107768722, -0.08668270972199164, -0.04020868965352957, 0.4163423025120909, -0.17203577240714088, -0.2974347564248511, -0.03263410211701949, -0.36463892601358777, 0.08220064897949879, 0.2613204659249347, 0.120686379915031... |
710.364 | A dynamic look-ahead Monte Carlo algorithm for pricing Bermudan options | Under the assumption of no-arbitrage, the pricing of American and Bermudan
options can be casted into optimal stopping problems. We propose a new adaptive
simulation based algorithm for the numerical solution of optimal stopping
problems in discrete time. Our approach is to recursively compute the so-called
continuat... | math.PR | under the assumption of noarbitrage the pricing of american and bermudan options can be casted into optimal stopping problems we propose a new adaptive simulation based algorithm for the numerical solution of optimal stopping problems in discrete time our approach is to recursively compute the socalled continuation val... | [['under', 'the', 'assumption', 'of', 'noarbitrage', 'the', 'pricing', 'of', 'american', 'and', 'bermudan', 'options', 'can', 'be', 'casted', 'into', 'optimal', 'stopping', 'problems', 'we', 'propose', 'a', 'new', 'adaptive', 'simulation', 'based', 'algorithm', 'for', 'the', 'numerical', 'solution', 'of', 'optimal', 's... | [-0.07083542858329571, -0.01932928220861975, -0.15624054692369077, 0.11682952337887519, -0.10777764008806567, -0.1313154687283232, 0.1270775251087483, 0.4235916610052383, -0.3178205363957662, -0.2572046558835294, 0.20704073970072165, -0.22585568870391143, -0.1371700524404231, 0.22784407967031975, -0.11012226270262176, ... |
710.3641 | The Euler Characteristic Formula for Logarithmic Minimal Degenerations
of Surfaces with Kodaira Dimension Zero and its application to Calabi-Yau
Threefolds with a pencil | In this paper, the Euler characteristic formula for projective logarithmic
minimal degenerations of surfaces with Kodaira dimension zero over a
1-dimensional complex disk is proved under a reasonable assumption and as its
application, the singularity of logarithmic minimal degenerations are
determined in the abelian ... | math.AG | in this paper the euler characteristic formula for projective logarithmic minimal degenerations of surfaces with kodaira dimension zero over a 1dimensional complex disk is proved under a reasonable assumption and as its application the singularity of logarithmic minimal degenerations are determined in the abelian or hy... | [['in', 'this', 'paper', 'the', 'euler', 'characteristic', 'formula', 'for', 'projective', 'logarithmic', 'minimal', 'degenerations', 'of', 'surfaces', 'with', 'kodaira', 'dimension', 'zero', 'over', 'a', '1dimensional', 'complex', 'disk', 'is', 'proved', 'under', 'a', 'reasonable', 'assumption', 'and', 'as', 'its', 'a... | [-0.1875136481316457, 0.02498823621076448, -0.09357584415133609, 0.10630453643686853, -0.0969217941543997, -0.19631704128737193, -0.004300813091144529, 0.2830450546949409, -0.26284668310870263, -0.21129216834209685, 0.0979130636808614, -0.2243080974291187, -0.16094951789966935, 0.23640955078989528, -0.1889676470309496,... |
710.3642 | On the Complexity of Spill Everywhere under SSA Form | Compilation for embedded processors can be either aggressive (time consuming
cross-compilation) or just in time (embedded and usually dynamic). The
heuristics used in dynamic compilation are highly constrained by limited
resources, time and memory in particular. Recent results on the SSA form open
promising direction... | cs.DS cs.CC | compilation for embedded processors can be either aggressive time consuming crosscompilation or just in time embedded and usually dynamic the heuristics used in dynamic compilation are highly constrained by limited resources time and memory in particular recent results on the ssa form open promising directions for the ... | [['compilation', 'for', 'embedded', 'processors', 'can', 'be', 'either', 'aggressive', 'time', 'consuming', 'crosscompilation', 'or', 'just', 'in', 'time', 'embedded', 'and', 'usually', 'dynamic', 'the', 'heuristics', 'used', 'in', 'dynamic', 'compilation', 'are', 'highly', 'constrained', 'by', 'limited', 'resources', ... | [-0.12833067977658305, 0.048210196419265064, -0.035425830137178385, 0.07179957975578263, -0.106415915917982, -0.1864165103202955, 0.08296235173609581, 0.38894392515538057, -0.28208947165820725, -0.3402250896778625, 0.1714898759211182, -0.2279116792895029, -0.09668705432751146, 0.2557634650312386, -0.09817516163524477, ... |
710.3643 | Stabilizing a purely dipolar quantum gas against collapse | We report on the experimental observation of the dipolar collapse of a
quantum gas which sets in when we reduce the contact interaction below some
critical value using a Feshbach resonance. Due to the anisotropy of the
dipole-dipole interaction, the stability of a dipolar Bose-Einstein condensate
depends not only on ... | cond-mat.other | we report on the experimental observation of the dipolar collapse of a quantum gas which sets in when we reduce the contact interaction below some critical value using a feshbach resonance due to the anisotropy of the dipoledipole interaction the stability of a dipolar boseeinstein condensate depends not only on the st... | [['we', 'report', 'on', 'the', 'experimental', 'observation', 'of', 'the', 'dipolar', 'collapse', 'of', 'a', 'quantum', 'gas', 'which', 'sets', 'in', 'when', 'we', 'reduce', 'the', 'contact', 'interaction', 'below', 'some', 'critical', 'value', 'using', 'a', 'feshbach', 'resonance', 'due', 'to', 'the', 'anisotropy', 'o... | [-0.18992024328275295, 0.17795386452194864, -0.06647466108268868, 0.04668190938923343, -0.04317591927813745, -0.1346667124292261, 0.06333735653207498, 0.36816944828075643, -0.24270840654298004, -0.24893478086152304, 0.01915778184569218, -0.2642703431007345, -0.09855839416829754, 0.18399261766673783, 0.05489734028655607... |
710.3644 | Heavy-fermion metals with hybridization nodes: Unconventional Fermi
liquids and competing phases | Microscopic models for heavy-fermion materials often assume a local, i.e.,
momentum-independent, hybridization between the conduction band and the
local-moment f electrons. Motivated by recent experiments, we consider
situations where this neglect of momentum dependence is inappropriate, namely
when the hybridization... | cond-mat.str-el cond-mat.stat-mech | microscopic models for heavyfermion materials often assume a local ie momentumindependent hybridization between the conduction band and the localmoment f electrons motivated by recent experiments we consider situations where this neglect of momentum dependence is inappropriate namely when the hybridization function has... | [['microscopic', 'models', 'for', 'heavyfermion', 'materials', 'often', 'assume', 'a', 'local', 'ie', 'momentumindependent', 'hybridization', 'between', 'the', 'conduction', 'band', 'and', 'the', 'localmoment', 'f', 'electrons', 'motivated', 'by', 'recent', 'experiments', 'we', 'consider', 'situations', 'where', 'this'... | [-0.17570523963389328, 0.24585929195674863, -0.04212552487350455, 0.10258266646784117, -0.0745909563208953, -0.1592185615686836, 0.10248354744242799, 0.3403379012427361, -0.2769142571473267, -0.273366921132703, -0.04071709971943098, -0.3578843981930532, -0.14570663182246613, 0.1475324397679509, 0.05337241407350365, -0.... |
710.3645 | The k-generalized distribution: A new descriptive model for the size
distribution of incomes | This paper proposes the k-generalized distribution as a model for describing
the distribution and dispersion of income within a population. Formulas for the
shape, moments and standard tools for inequality measurement - such as the
Lorenz curve and the Gini coefficient - are given. A method for parameter
estimation i... | q-fin.GN physics.soc-ph | this paper proposes the kgeneralized distribution as a model for describing the distribution and dispersion of income within a population formulas for the shape moments and standard tools for inequality measurement such as the lorenz curve and the gini coefficient are given a method for parameter estimation is also dis... | [['this', 'paper', 'proposes', 'the', 'kgeneralized', 'distribution', 'as', 'a', 'model', 'for', 'describing', 'the', 'distribution', 'and', 'dispersion', 'of', 'income', 'within', 'a', 'population', 'formulas', 'for', 'the', 'shape', 'moments', 'and', 'standard', 'tools', 'for', 'inequality', 'measurement', 'such', 'a... | [-0.018620862411002494, 0.057439928927591866, -0.12540311790736658, 0.13823959387040563, -0.03339512595640762, -0.13325315634720028, 0.040366557228844614, 0.3313062878857766, -0.2340574167003589, -0.33550558228577887, 0.12517103220702017, -0.31290096201534784, -0.12954007903380052, 0.22315927926850107, -0.0986449301132... |
710.3646 | Thermodynamic time asymmetry in nonequilibrium fluctuations | We here present the complete analysis of experiments on driven Brownian
motion and electric noise in a $RC$ circuit, showing that thermodynamic entropy
production can be related to the breaking of time-reversal symmetry in the
statistical description of these nonequilibrium systems. The symmetry breaking
can be expre... | cond-mat.stat-mech | we here present the complete analysis of experiments on driven brownian motion and electric noise in a rc circuit showing that thermodynamic entropy production can be related to the breaking of timereversal symmetry in the statistical description of these nonequilibrium systems the symmetry breaking can be expressed in... | [['we', 'here', 'present', 'the', 'complete', 'analysis', 'of', 'experiments', 'on', 'driven', 'brownian', 'motion', 'and', 'electric', 'noise', 'in', 'a', 'rc', 'circuit', 'showing', 'that', 'thermodynamic', 'entropy', 'production', 'can', 'be', 'related', 'to', 'the', 'breaking', 'of', 'timereversal', 'symmetry', 'in... | [-0.1776913838877686, 0.17801851649327496, -0.10815580660607993, 0.06547170121079385, 0.03481573318212963, -0.11735661309763887, 0.06892710491982207, 0.32422031991575895, -0.3237509809704007, -0.24611144043962685, 0.06260002632993028, -0.2911803993118698, -0.07858435831669915, 0.15092469537794068, -0.0356711947426543, ... |
710.3647 | Asymptotic approximation of nonparametric regression experiments with
unknown variances | Asymptotic equivalence results for nonparametric regression experiments have
always assumed that the variances of the observations are known. In practice,
however the variance of each observation is generally considered to be an
unknown nuisance parameter. We establish an asymptotic approximation to the
nonparametric... | math.ST stat.TH | asymptotic equivalence results for nonparametric regression experiments have always assumed that the variances of the observations are known in practice however the variance of each observation is generally considered to be an unknown nuisance parameter we establish an asymptotic approximation to the nonparametric regr... | [['asymptotic', 'equivalence', 'results', 'for', 'nonparametric', 'regression', 'experiments', 'have', 'always', 'assumed', 'that', 'the', 'variances', 'of', 'the', 'observations', 'are', 'known', 'in', 'practice', 'however', 'the', 'variance', 'of', 'each', 'observation', 'is', 'generally', 'considered', 'to', 'be', '... | [-0.07244349505245976, 0.08309467295645306, -0.11971568064854561, 0.0950275840818683, -0.10036867099714655, -0.13989870381333586, 0.007040834004620036, 0.3734601606859021, -0.2648351130808152, -0.2994966069733706, 0.19014518415822096, -0.2925039140001229, -0.09919402697033168, 0.16983523465539282, -0.08778430029605198,... |
710.3648 | Hydrodynamic stability and mode coupling in Keplerian flows: local
strato-rotational analysis | Aims. Qualitative analysis of key (but yet unappreciated) linear phenomena in
stratified hydrodynamic Keplerian flows: (i) the occurrence of a vortex mode,
as a consequence of strato-rotational balance, with its transient dynamics;
(ii) the generation of spiral-density waves (also called inertia-gravity or
$g\Omega$ ... | astro-ph | aims qualitative analysis of key but yet unappreciated linear phenomena in stratified hydrodynamic keplerian flows i the occurrence of a vortex mode as a consequence of stratorotational balance with its transient dynamics ii the generation of spiraldensity waves also called inertiagravity or gomega waves by the vortex ... | [['aims', 'qualitative', 'analysis', 'of', 'key', 'but', 'yet', 'unappreciated', 'linear', 'phenomena', 'in', 'stratified', 'hydrodynamic', 'keplerian', 'flows', 'i', 'the', 'occurrence', 'of', 'a', 'vortex', 'mode', 'as', 'a', 'consequence', 'of', 'stratorotational', 'balance', 'with', 'its', 'transient', 'dynamics', ... | [-0.19545365782390695, 0.19329219542023743, -0.10321899892068377, 0.04389163682365096, -0.09489580460769288, -0.09650951798676569, -0.047988414402832004, 0.2825587323738956, -0.2995455267008248, -0.24172250796839886, 0.10146294489466384, -0.23734059059289375, -0.13889052564958476, 0.18860640179858926, 0.010297012343710... |
710.3649 | CMB Temperature Polarization Correlation and Primordial Gravitational
Waves | We examine the use of the CMB's TE cross correlation power spectrum as a
complementary test to detect primordial gravitational waves (PGWs). The first
method used is based on the determination of the lowest multipole, $\ell_0$,
where the TE power spectrum, $C_{\ell}^{TE}$, first changes sign. The second
method uses W... | astro-ph | we examine the use of the cmbs te cross correlation power spectrum as a complementary test to detect primordial gravitational waves pgws the first method used is based on the determination of the lowest multipole ell_0 where the te power spectrum c_ellte first changes sign the second method uses wiener filtering on the... | [['we', 'examine', 'the', 'use', 'of', 'the', 'cmbs', 'te', 'cross', 'correlation', 'power', 'spectrum', 'as', 'a', 'complementary', 'test', 'to', 'detect', 'primordial', 'gravitational', 'waves', 'pgws', 'the', 'first', 'method', 'used', 'is', 'based', 'on', 'the', 'determination', 'of', 'the', 'lowest', 'multipole', ... | [-0.11086881362642043, 0.08171399033170205, -0.06378118844272998, 0.1051199455273887, -0.08882159710599062, -0.10613753823563457, 0.004469105988764801, 0.3170643771019502, -0.24071941161289429, -0.30858018416433763, 0.0533933526585595, -0.34388756546645594, -0.08356613099861604, 0.1880697270568747, 0.04047601191470256,... |
710.365 | Linearization of holomorphic germs with quasi-Brjuno fixed points | Let $f$ be a germ of holomorphic diffeomorphism of $\C^n$ fixing the origin
$O$, with $df_O$ diagonalizable. We prove that, under certain arithmetic
conditions on the eigenvalues of $df_O$ and some restrictions on the
resonances, $f$ is locally holomorphically linearizable if and only if there
exists a particular $f$... | math.DS math.CV | let f be a germ of holomorphic diffeomorphism of cn fixing the origin o with df_o diagonalizable we prove that under certain arithmetic conditions on the eigenvalues of df_o and some restrictions on the resonances f is locally holomorphically linearizable if and only if there exists a particular finvariant complex mani... | [['let', 'f', 'be', 'a', 'germ', 'of', 'holomorphic', 'diffeomorphism', 'of', 'cn', 'fixing', 'the', 'origin', 'o', 'with', 'df_o', 'diagonalizable', 'we', 'prove', 'that', 'under', 'certain', 'arithmetic', 'conditions', 'on', 'the', 'eigenvalues', 'of', 'df_o', 'and', 'some', 'restrictions', 'on', 'the', 'resonances',... | [-0.2155064855487301, 0.07188263587796917, -0.08883038610219955, 0.011148961097933351, -0.1030519098150902, -0.18874255652324512, 0.007076417081631147, 0.34579891447837535, -0.2834973696565542, -0.16139122216174237, 0.11801824663013506, -0.2369061420743282, -0.1840822856586713, 0.2003755788390453, -0.11827228070738224,... |
710.3651 | CMB Temperature Polarization Correlation and Primordial Gravitational
Waves II: Wiener Filtering and Tests Based on Monte Carlo Simulations | In this paper we continue our study of CMB TE cross correlation as a source
of information about primordial gravitational waves. In an accompanying paper,
we considered the zero multipole method. In this paper we use Wiener filtering
of the CMB TE data to remove the density perturbation contribution to the TE
power s... | astro-ph | in this paper we continue our study of cmb te cross correlation as a source of information about primordial gravitational waves in an accompanying paper we considered the zero multipole method in this paper we use wiener filtering of the cmb te data to remove the density perturbation contribution to the te power spectr... | [['in', 'this', 'paper', 'we', 'continue', 'our', 'study', 'of', 'cmb', 'te', 'cross', 'correlation', 'as', 'a', 'source', 'of', 'information', 'about', 'primordial', 'gravitational', 'waves', 'in', 'an', 'accompanying', 'paper', 'we', 'considered', 'the', 'zero', 'multipole', 'method', 'in', 'this', 'paper', 'we', 'us... | [-0.08670974621323595, 0.06584208089651378, -0.0504658375547765, 0.10193745765001003, -0.04633194679547459, -0.1294671549455403, 0.038002607190171386, 0.3533671759643069, -0.20559989551898755, -0.3237021181585701, 0.07152853594783515, -0.343381735129435, -0.08898290088846769, 0.17668683918062214, 0.03695834144768114, 0... |
710.3652 | Time-Frequency Analysis of Fourier Integral Operators | We use time-frequency methods for the study of Fourier Integral operators
(FIOs). In this paper we shall show that Gabor frames provide very efficient
representations for a large class of FIOs. Indeed, similarly to the case of
shearlets and curvelets frames, the matrix representation of a Fourier Integral
Operator wi... | math.AP math.NA | we use timefrequency methods for the study of fourier integral operators fios in this paper we shall show that gabor frames provide very efficient representations for a large class of fios indeed similarly to the case of shearlets and curvelets frames the matrix representation of a fourier integral operator with respec... | [['we', 'use', 'timefrequency', 'methods', 'for', 'the', 'study', 'of', 'fourier', 'integral', 'operators', 'fios', 'in', 'this', 'paper', 'we', 'shall', 'show', 'that', 'gabor', 'frames', 'provide', 'very', 'efficient', 'representations', 'for', 'a', 'large', 'class', 'of', 'fios', 'indeed', 'similarly', 'to', 'the', ... | [-0.0993098587995129, 0.05275062854135675, -0.11634132831668652, 0.15650610085956904, -0.12911621546990484, -0.08277812937265072, -0.029521420131180892, 0.4244898750009585, -0.2916748207870263, -0.12608249866871676, 0.1648881695024213, -0.26395152656275933, -0.20772181929336214, 0.2492134312110744, -0.15588144477152702... |
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