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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710.1353 | Exact Numerical Study of Pair Formation with Imbalanced Fermion
Populations | We present an exact Quantum Monte Carlo study of the attractive 1-dimensional
Hubbard model with imbalanced fermion population. The pair-pair correlation
function, which decays monotonically in the absence of polarization P, develops
oscillations when P is nonzero, characteristic of
Fulde-Ferrell-Larkin-Ovchinnikov p... | cond-mat.str-el | we present an exact quantum monte carlo study of the attractive 1dimensional hubbard model with imbalanced fermion population the pairpair correlation function which decays monotonically in the absence of polarization p develops oscillations when p is nonzero characteristic of fuldeferrelllarkinovchinnikov phase the pa... | [['we', 'present', 'an', 'exact', 'quantum', 'monte', 'carlo', 'study', 'of', 'the', 'attractive', '1dimensional', 'hubbard', 'model', 'with', 'imbalanced', 'fermion', 'population', 'the', 'pairpair', 'correlation', 'function', 'which', 'decays', 'monotonically', 'in', 'the', 'absence', 'of', 'polarization', 'p', 'deve... | [-0.18530211471119434, 0.24433780233965816, -0.09590323491090345, 0.10964323915733418, 0.0002686015539589005, -0.15777286596664594, 0.047694578477386555, 0.34554282497238675, -0.26167078241235964, -0.2746799321772548, -0.06301426718122574, -0.3337922932648467, -0.04390225283493963, 0.1074452874989787, 0.069095144560987... |
710.1354 | On the Newman sum over multiples of a prime with a primitive or
semiprimitive root 2 | We obtain a simple relations for the Newman sum over multiples of a prime
with a primitive or semiprimitive root 2. We consider the case of p=17 as well.
| math.NT | we obtain a simple relations for the newman sum over multiples of a prime with a primitive or semiprimitive root 2 we consider the case of p17 as well | [['we', 'obtain', 'a', 'simple', 'relations', 'for', 'the', 'newman', 'sum', 'over', 'multiples', 'of', 'a', 'prime', 'with', 'a', 'primitive', 'or', 'semiprimitive', 'root', '2', 'we', 'consider', 'the', 'case', 'of', 'p17', 'as', 'well']] | [-0.1990952935262487, 0.07098641689738323, -0.027436366368984354, 0.06802751258786383, -0.06616681435241781, -0.11763740531650596, 0.05521178239121519, 0.2782353197770386, -0.2970093556776129, -0.25840851953574295, 0.10804736938584468, -0.2853659810177211, -0.1699662788947723, 0.20820569313645107, -0.03669947665184736,... |
710.1355 | Studies on the Lorenz model | We study the Lorenz model from the viewpoint of its accessible singularities
and local index.
| math.AG | we study the lorenz model from the viewpoint of its accessible singularities and local index | [['we', 'study', 'the', 'lorenz', 'model', 'from', 'the', 'viewpoint', 'of', 'its', 'accessible', 'singularities', 'and', 'local', 'index']] | [-0.1229328453540802, 0.03751682893683513, -0.18357228549818197, 0.09878820814192295, -0.024069479232033095, -0.1521287159062922, 0.07537579257041216, 0.26122774680455524, -0.327221777352194, -0.2859433966378371, 0.09746229794497291, -0.29899392450849216, -0.2527820974588394, 0.17850221667128305, -0.0688661802560091, 0... |
710.1356 | Quantum Monte Carlo Study of a Dynamic Hubbard Model | The `dynamic' Hubbard Hamiltonian describes interacting fermions on a lattice
whose on-site repulsion is modulated by a coupling to a fluctuating bosonic
field. We investigate one such model, introduced by Hirsch, using the
determinant Quantum Monte Carlo method. Our key result is that the extended
s-wave pairing ver... | cond-mat.supr-con cond-mat.str-el | the dynamic hubbard hamiltonian describes interacting fermions on a lattice whose onsite repulsion is modulated by a coupling to a fluctuating bosonic field we investigate one such model introduced by hirsch using the determinant quantum monte carlo method our key result is that the extended swave pairing vertex repuls... | [['the', 'dynamic', 'hubbard', 'hamiltonian', 'describes', 'interacting', 'fermions', 'on', 'a', 'lattice', 'whose', 'onsite', 'repulsion', 'is', 'modulated', 'by', 'a', 'coupling', 'to', 'a', 'fluctuating', 'bosonic', 'field', 'we', 'investigate', 'one', 'such', 'model', 'introduced', 'by', 'hirsch', 'using', 'the', '... | [-0.1946500812093688, 0.2264186044413393, -0.08411606186179116, 0.1049058603439793, -0.04380956858185222, -0.20839147858259058, 0.07809115515556186, 0.32833535552901383, -0.258954295786802, -0.25906398991013274, -0.002315470973272346, -0.3218308769072555, -0.13135656683525743, 0.08426400967541017, 0.07967503845863858, ... |
710.1357 | Does Sex Induce a Phase Transition? | We discovered a dynamic phase transition induced by sexual reproduction. The
dynamics is a pure Darwinian rule with both fundamental ingredients to drive
evolution: 1) random mutations and crossings which act in the sense of
increasing the entropy (or diversity); and 2) selection which acts in the
opposite sense by l... | q-bio.PE cond-mat.stat-mech physics.bio-ph | we discovered a dynamic phase transition induced by sexual reproduction the dynamics is a pure darwinian rule with both fundamental ingredients to drive evolution 1 random mutations and crossings which act in the sense of increasing the entropy or diversity and 2 selection which acts in the opposite sense by limiting t... | [['we', 'discovered', 'a', 'dynamic', 'phase', 'transition', 'induced', 'by', 'sexual', 'reproduction', 'the', 'dynamics', 'is', 'a', 'pure', 'darwinian', 'rule', 'with', 'both', 'fundamental', 'ingredients', 'to', 'drive', 'evolution', '1', 'random', 'mutations', 'and', 'crossings', 'which', 'act', 'in', 'the', 'sense... | [-0.12869502462993335, 0.22609461087685423, -0.05608934594682701, 0.10114222284679747, -0.05169244340782904, -0.18414771179466144, 0.13260450100566706, 0.3526896690706844, -0.276577577456508, -0.27083721487256496, 0.07238343407237983, -0.2662416877204795, -0.12525339369540628, 0.12733919089406973, -0.0776846203499783, ... |
710.1358 | Nodal solutions to quasilinear elliptic equations on compact Riemannian
manifolds | We show the existence of nodal solutions to perturbed quasilinear elliptic
equations with critical Sobolev exponent on compact Riemannian manifolds. A
nonexistence result is also given.
| math.AP | we show the existence of nodal solutions to perturbed quasilinear elliptic equations with critical sobolev exponent on compact riemannian manifolds a nonexistence result is also given | [['we', 'show', 'the', 'existence', 'of', 'nodal', 'solutions', 'to', 'perturbed', 'quasilinear', 'elliptic', 'equations', 'with', 'critical', 'sobolev', 'exponent', 'on', 'compact', 'riemannian', 'manifolds', 'a', 'nonexistence', 'result', 'is', 'also', 'given']] | [-0.2821357766023049, 0.022115271628046267, -0.07616851027481832, 0.10456341553855544, -0.16403321016696282, -0.174537548992353, -0.09259782917797565, 0.23528981655209252, -0.26009107287973166, -0.1984017305613424, 0.14934229669877544, -0.3897029786155774, -0.13323325885889623, 0.2573473464446859, -0.11362477846873495,... |
710.1359 | The Fractal Density Structure in Supersonic Isothermal Turbulence:
Solenoidal versus Compressive Energy Injection | In a systematic study, we compare the density statistics in high resolution
numerical experiments of supersonic isothermal turbulence, driven by the
usually adopted solenoidal (divergence-free) forcing and by compressive
(curl-free) forcing. We find that for the same rms Mach number, compressive
forcing produces much... | astro-ph | in a systematic study we compare the density statistics in high resolution numerical experiments of supersonic isothermal turbulence driven by the usually adopted solenoidal divergencefree forcing and by compressive curlfree forcing we find that for the same rms mach number compressive forcing produces much stronger de... | [['in', 'a', 'systematic', 'study', 'we', 'compare', 'the', 'density', 'statistics', 'in', 'high', 'resolution', 'numerical', 'experiments', 'of', 'supersonic', 'isothermal', 'turbulence', 'driven', 'by', 'the', 'usually', 'adopted', 'solenoidal', 'divergencefree', 'forcing', 'and', 'by', 'compressive', 'curlfree', 'fo... | [-0.08900268628875713, 0.16052326191139454, -0.1084999661454888, 0.04397161578607192, -0.04250925059928151, -0.06719124434335579, -0.009452227719797654, 0.3262884953640796, -0.2346670985085598, -0.2932568404411528, 0.08048696470798813, -0.2341407644498046, -0.06197025017031739, 0.25405518681321654, -0.03919414811003696... |
710.136 | Complementary self-similarity | A few aspects of self-similarity related to complementary components of
closed subsets of R^n are briefly discussed.
| math.CA | a few aspects of selfsimilarity related to complementary components of closed subsets of rn are briefly discussed | [['a', 'few', 'aspects', 'of', 'selfsimilarity', 'related', 'to', 'complementary', 'components', 'of', 'closed', 'subsets', 'of', 'rn', 'are', 'briefly', 'discussed']] | [-0.17494214413797154, 0.13810619821443276, 0.019928028697476667, 0.11521676642929807, -0.09235107559053336, -0.1255030401105828, -0.058056395720033085, 0.32760971916072507, -0.32718121808241396, -0.12927142355371923, 0.161755619899315, -0.330314421094954, -0.1157162512981278, 0.22134233561947064, -0.08770235217012026,... |
710.1361 | Blow-up rate for a semi-linear accretive wave equation | In this paper we consider the semi-linear wave equation: $u_{tt}-\Delta
u=u_t|u_t|^{p-1}$ in $\mathbb{R}^N$. We provide an associated energy. With this
energy we give the blow-up rate for blowing up solutions in the case of bounded
below energy.
| math-ph math.MP | in this paper we consider the semilinear wave equation u_ttdelta uu_tu_tp1 in mathbbrn we provide an associated energy with this energy we give the blowup rate for blowing up solutions in the case of bounded below energy | [['in', 'this', 'paper', 'we', 'consider', 'the', 'semilinear', 'wave', 'equation', 'u_ttdelta', 'uu_tu_tp1', 'in', 'mathbbrn', 'we', 'provide', 'an', 'associated', 'energy', 'with', 'this', 'energy', 'we', 'give', 'the', 'blowup', 'rate', 'for', 'blowing', 'up', 'solutions', 'in', 'the', 'case', 'of', 'bounded', 'belo... | [-0.20450112766896686, 0.06310726952223275, 0.03656813314753688, 0.020194383098795596, -0.04713438772079018, -0.05702576320618391, 0.00332744207763527, 0.28437345361130106, -0.308941802320381, -0.20422513384578955, 0.11786754462001328, -0.33338364368925494, -0.07185000610641307, 0.20097060643860865, -0.0538883605558011... |
710.1362 | Smeared BTZ Black Hole from Space Noncommutativity | We study a novel phenomena of smearing of black hole horizons from the effect
of space noncommutativity. We present an explicit example in $AdS_3$ space,
using the Chern-Simons formulation of gravity. This produces a smeared BTZ
black hole which goes beyond the classical spacetime unexpectedly and there is
{\it no} r... | hep-th gr-qc | we study a novel phenomena of smearing of black hole horizons from the effect of space noncommutativity we present an explicit example in ads_3 space using the chernsimons formulation of gravity this produces a smeared btz black hole which goes beyond the classical spacetime unexpectedly and there is it no reality prob... | [['we', 'study', 'a', 'novel', 'phenomena', 'of', 'smearing', 'of', 'black', 'hole', 'horizons', 'from', 'the', 'effect', 'of', 'space', 'noncommutativity', 'we', 'present', 'an', 'explicit', 'example', 'in', 'ads_3', 'space', 'using', 'the', 'chernsimons', 'formulation', 'of', 'gravity', 'this', 'produces', 'a', 'smea... | [-0.13919355244314696, 0.1552718273190498, -0.12471697056574411, 0.134391189580198, -0.08714078230366029, -0.14618252442839244, 0.012989976671091764, 0.3345976430780249, -0.19922446162068372, -0.26782954098463385, 0.11089084326220254, -0.29332148309420447, -0.12001807540985934, 0.15541848564352534, -0.08368232628267609... |
710.1363 | The influence of the structure imperfectness of a crystalline undulator
on the emission spectrum | We study the influence of an imperfect structure of a crystalline undulator
on the spectrum of the undulator radiation. The main attention is paid to the
undulators in which the periodic bending in the bulk appears as a result of a
regular (periodic) surface deformations. We demonstrate that this method of
preparatio... | physics.acc-ph | we study the influence of an imperfect structure of a crystalline undulator on the spectrum of the undulator radiation the main attention is paid to the undulators in which the periodic bending in the bulk appears as a result of a regular periodic surface deformations we demonstrate that this method of preparation of a... | [['we', 'study', 'the', 'influence', 'of', 'an', 'imperfect', 'structure', 'of', 'a', 'crystalline', 'undulator', 'on', 'the', 'spectrum', 'of', 'the', 'undulator', 'radiation', 'the', 'main', 'attention', 'is', 'paid', 'to', 'the', 'undulators', 'in', 'which', 'the', 'periodic', 'bending', 'in', 'the', 'bulk', 'appear... | [-0.18614656557529283, 0.16474113176387148, -0.11347036294749267, -0.00522850281609002, -0.05651762787132494, -0.05691173901501041, 0.0006743811924631397, 0.39365487432567986, -0.27151644105712575, -0.2801233063331775, 0.045789531119147776, -0.23226684563723143, -0.10521871169843781, 0.21431788322465714, -0.05107898035... |
710.1364 | Boltzmann distribution of free energies in a finite-connectivity
spin-glass system and the cavity approach | At sufficiently low temperatures, the configurational phase space of a large
spin-glass system breaks into many separated domains, each of which is referred
to as a macroscopic state. The system is able to visit all spin configurations
of the same macroscopic state, while it can not spontaneously jump between two
dif... | cond-mat.dis-nn | at sufficiently low temperatures the configurational phase space of a large spinglass system breaks into many separated domains each of which is referred to as a macroscopic state the system is able to visit all spin configurations of the same macroscopic state while it can not spontaneously jump between two different ... | [['at', 'sufficiently', 'low', 'temperatures', 'the', 'configurational', 'phase', 'space', 'of', 'a', 'large', 'spinglass', 'system', 'breaks', 'into', 'many', 'separated', 'domains', 'each', 'of', 'which', 'is', 'referred', 'to', 'as', 'a', 'macroscopic', 'state', 'the', 'system', 'is', 'able', 'to', 'visit', 'all', '... | [-0.13483724573914038, 0.24013349450861557, -0.08881926406033788, 0.004900604061713055, 0.002953759788516721, -0.15119239912754057, 0.08098109859580438, 0.3202577630067338, -0.24129621023806094, -0.3212076366474532, 0.06972799153358798, -0.26419200713868546, -0.053114481044538094, 0.12698280065663797, -0.03014616692683... |
710.1365 | Distribution of equilibrium free energies in a thermodynamic system with
broken ergodicity | At low temperatures the configurational phase space of a macroscopic complex
system (e.g., a spin-glass) of $N\sim 10^{23}$ interacting particles may split
into an exponential number $\Omega_s \sim \exp({\rm const} \times N)$ of
ergodic sub-spaces (thermodynamic states). Previous theoretical studies assumed
that the ... | cond-mat.dis-nn | at low temperatures the configurational phase space of a macroscopic complex system eg a spinglass of nsim 1023 interacting particles may split into an exponential number omega_s sim exprm const times n of ergodic subspaces thermodynamic states previous theoretical studies assumed that the equilibrium collective behavi... | [['at', 'low', 'temperatures', 'the', 'configurational', 'phase', 'space', 'of', 'a', 'macroscopic', 'complex', 'system', 'eg', 'a', 'spinglass', 'of', 'nsim', '1023', 'interacting', 'particles', 'may', 'split', 'into', 'an', 'exponential', 'number', 'omega_s', 'sim', 'exprm', 'const', 'times', 'n', 'of', 'ergodic', 's... | [-0.14627775058827616, 0.2518970590302188, -0.12660541959727803, 0.07707901081691186, 0.019128867211596418, -0.12714114597166012, 0.06889205083787216, 0.3172450174161261, -0.2374187290569711, -0.28116949923534057, 0.041682363076798734, -0.29079707747212413, -0.06843648625671807, 0.12737611967322388, 0.02226279507863871... |
710.1366 | Matrices Totally Positive Relative to a Tree | It is known that for a totally positive (TP) matrix, the eigenvalues are
positive and distinct and the eigenvector associated with the smallest
eigenvalue is totally nonzero and has an alternating sign pattern. Here, a
certain weakening of the TP hypothesis is shown to yield a similar conclusion.
| math.CO | it is known that for a totally positive tp matrix the eigenvalues are positive and distinct and the eigenvector associated with the smallest eigenvalue is totally nonzero and has an alternating sign pattern here a certain weakening of the tp hypothesis is shown to yield a similar conclusion | [['it', 'is', 'known', 'that', 'for', 'a', 'totally', 'positive', 'tp', 'matrix', 'the', 'eigenvalues', 'are', 'positive', 'and', 'distinct', 'and', 'the', 'eigenvector', 'associated', 'with', 'the', 'smallest', 'eigenvalue', 'is', 'totally', 'nonzero', 'and', 'has', 'an', 'alternating', 'sign', 'pattern', 'here', 'a',... | [-0.1837393271186253, 0.1808779170511722, -0.09166798659134656, 0.049387353460285034, -0.09612156408062826, -0.15403514016846506, -0.01667949561184893, 0.3522853859855483, -0.28101365695086616, -0.2021585524538144, 0.12749867136396156, -0.3254146886223073, -0.20653975225559407, 0.12700846147102615, -0.00114009735989384... |
710.1367 | Faster than Light Quantum Communication | Faster than light communication might be possible using the collapse of the
quantum wave-function without any accompanying paradoxes.
| physics.gen-ph | faster than light communication might be possible using the collapse of the quantum wavefunction without any accompanying paradoxes | [['faster', 'than', 'light', 'communication', 'might', 'be', 'possible', 'using', 'the', 'collapse', 'of', 'the', 'quantum', 'wavefunction', 'without', 'any', 'accompanying', 'paradoxes']] | [-0.14076867510771585, 0.20227091593874824, -0.13972115402834284, 0.14800215202073255, -0.14211207711034352, -0.21431611444697612, 0.06827342115704799, 0.33017312238613766, -0.20234812144190073, -0.2958567027623455, 0.08893748859150542, -0.25901702051568365, -0.07221769127580854, 0.23151512506107488, -0.015940712040497... |
710.1368 | Measurement of the Tau Lepton Polarisation at LEP2 | A first measurement of the average polarisation P_tau of tau leptons produced
in e+e- annihilation at energies significantly above the Z resonance is
presented. The polarisation is determined from the kinematic spectra of tau
hadronic decays. The measured value P_tau = -0.164 +/- 0.125 is consistent with
the Standard... | hep-ex | a first measurement of the average polarisation p_tau of tau leptons produced in ee annihilation at energies significantly above the z resonance is presented the polarisation is determined from the kinematic spectra of tau hadronic decays the measured value p_tau 0164 0125 is consistent with the standard model predicti... | [['a', 'first', 'measurement', 'of', 'the', 'average', 'polarisation', 'p_tau', 'of', 'tau', 'leptons', 'produced', 'in', 'ee', 'annihilation', 'at', 'energies', 'significantly', 'above', 'the', 'z', 'resonance', 'is', 'presented', 'the', 'polarisation', 'is', 'determined', 'from', 'the', 'kinematic', 'spectra', 'of', ... | [-0.03338462903098971, 0.2268015391912246, -0.06990073415810209, 0.12352005846332759, 0.02494318933601965, -0.1096806256917485, 0.024561278189107645, 0.3290040206425546, -0.24632162433281019, -0.3083702473852195, -0.047364144726950476, -0.3619985643839627, 0.1606179190832272, 0.17778289304707168, 0.11591769950954538, 0... |
710.1369 | Consequence of doping in spatiotemporal rock-paper-scissors games | What determines species diversity is dramatic concern in science. Here we
report the effect of doping on diversity in spatiotemporal rock-paper-scissors
(RPS) games, which can be observed directly in ecological, biological and
social systems in nature. Doping means that there exists some buffer patches
which do not i... | nlin.AO q-bio.PE | what determines species diversity is dramatic concern in science here we report the effect of doping on diversity in spatiotemporal rockpaperscissors rps games which can be observed directly in ecological biological and social systems in nature doping means that there exists some buffer patches which do not involve the... | [['what', 'determines', 'species', 'diversity', 'is', 'dramatic', 'concern', 'in', 'science', 'here', 'we', 'report', 'the', 'effect', 'of', 'doping', 'on', 'diversity', 'in', 'spatiotemporal', 'rockpaperscissors', 'rps', 'games', 'which', 'can', 'be', 'observed', 'directly', 'in', 'ecological', 'biological', 'and', 's... | [-0.13346740316764194, 0.14992007665207674, -0.040776954272537136, 0.08759089555141741, -0.04104305234063288, -0.16998237607807948, 0.11148085946313523, 0.40605230241500095, -0.27628558622352006, -0.29676239817114225, 0.04691113229311104, -0.26826115428181047, -0.17533347250187192, 0.16473732050588547, -0.0749906201782... |
710.137 | A problem of enumeration of two-color bracelets with several variations | We consider the problem of enumeration of incongruent two-color bracelets of
$n$ beads, $k$ of which are black, and study several natural variations of this
problem. We also give recursion formulas for enumeration of $t$-color
bracelets, $t\geq3.
| math.CO | we consider the problem of enumeration of incongruent twocolor bracelets of n beads k of which are black and study several natural variations of this problem we also give recursion formulas for enumeration of tcolor bracelets tgeq3 | [['we', 'consider', 'the', 'problem', 'of', 'enumeration', 'of', 'incongruent', 'twocolor', 'bracelets', 'of', 'n', 'beads', 'k', 'of', 'which', 'are', 'black', 'and', 'study', 'several', 'natural', 'variations', 'of', 'this', 'problem', 'we', 'also', 'give', 'recursion', 'formulas', 'for', 'enumeration', 'of', 'tcolor... | [-0.18431621820137306, 0.13212647852865425, -0.02775877095897355, 0.0801312505437464, -0.058153418169633764, -0.10664458854778393, 0.085243945941329, 0.337379105640827, -0.2543099811552344, -0.32660067504322204, 0.10196586680674069, -0.2976405456460811, -0.15922738053533878, 0.16895098717430154, -0.08127109946587086, 0... |
710.1371 | Study of the Exclusive Initial-State-Radiation Production of the DDbar
System | A search for charmonium and other new states is performed in a study of
exclusive initial-state-radiation production of D Dbar events from
electron-positron annihilations at a center-of-mass energy of 10.58 GeV. The
data sample corresponds to an integrated luminosity of 384 fb-1 and was
recorded by the BABAR experime... | hep-ex | a search for charmonium and other new states is performed in a study of exclusive initialstateradiation production of d dbar events from electronpositron annihilations at a centerofmass energy of 1058 gev the data sample corresponds to an integrated luminosity of 384 fb1 and was recorded by the babar experiment at the ... | [['a', 'search', 'for', 'charmonium', 'and', 'other', 'new', 'states', 'is', 'performed', 'in', 'a', 'study', 'of', 'exclusive', 'initialstateradiation', 'production', 'of', 'd', 'dbar', 'events', 'from', 'electronpositron', 'annihilations', 'at', 'a', 'centerofmass', 'energy', 'of', '1058', 'gev', 'the', 'data', 'samp... | [-0.10381155141590874, 0.14466139121423954, -0.10269210602819305, 0.14207454792166263, -0.0037880450122288823, -0.12180136667910157, 0.09848195273121915, 0.2863202925613054, -0.12674736476607726, -0.3135743232386321, -0.05252188026122557, -0.4465531091945073, 0.10016222863899756, 0.14139920891653843, 0.1144388357475015... |
710.1372 | The average kinetic energy density of Cooper pairs above T_c in
YBa_2Cu_3O_{7-x}}, Bi_2Sr_2CaCu_2O_{8+\delta}, and Nb} | We have obtained isofield curves for the square root of the average kinetic
energy density of the superconducting state for three single crystals of
underdoped YBa_2Cu_3O_{7-x}, an optimally doped single crystal of
Bi_2Sr_2CaCu_2O_{8+\delta}, and Nb. These curves, determined from isofield
magnetization versus tempera... | cond-mat.supr-con | we have obtained isofield curves for the square root of the average kinetic energy density of the superconducting state for three single crystals of underdoped yba_2cu_3o_7x an optimally doped single crystal of bi_2sr_2cacu_2o_8delta and nb these curves determined from isofield magnetization versus temperature measurem... | [['we', 'have', 'obtained', 'isofield', 'curves', 'for', 'the', 'square', 'root', 'of', 'the', 'average', 'kinetic', 'energy', 'density', 'of', 'the', 'superconducting', 'state', 'for', 'three', 'single', 'crystals', 'of', 'underdoped', 'yba_2cu_3o_7x', 'an', 'optimally', 'doped', 'single', 'crystal', 'of', 'bi_2sr_2ca... | [-0.1597247640495242, 0.20331009855141313, -0.04501435101760187, 0.022886279317411197, 0.0004133242343006463, -0.126546337499401, 0.1595830731950272, 0.33100569289948406, -0.22670875814604177, -0.2950323735856874, 0.008339935511580786, -0.390828769247251, -0.021632090039636898, 0.2584734872497361, 0.06070495668755865, ... |
710.1373 | Generalized parton distributions from domain wall valence quarks and
staggered sea quarks | Moments of the generalized parton distributions of the nucleon, calculated
with a mixed action of domain wall valence quarks and asqtad staggered sea
quarks, are presented for pion masses extending down to 359 MeV. Results for
the moments of the unpolarized, helicity, and transversity distributions are
given and comp... | hep-lat | moments of the generalized parton distributions of the nucleon calculated with a mixed action of domain wall valence quarks and asqtad staggered sea quarks are presented for pion masses extending down to 359 mev results for the moments of the unpolarized helicity and transversity distributions are given and compared to... | [['moments', 'of', 'the', 'generalized', 'parton', 'distributions', 'of', 'the', 'nucleon', 'calculated', 'with', 'a', 'mixed', 'action', 'of', 'domain', 'wall', 'valence', 'quarks', 'and', 'asqtad', 'staggered', 'sea', 'quarks', 'are', 'presented', 'for', 'pion', 'masses', 'extending', 'down', 'to', '359', 'mev', 'res... | [-0.06307522502456962, 0.26602564130111467, -0.08322347143940552, 0.12855435338712354, -0.06624255226645856, -0.022453562332773392, 0.06227917044556567, 0.40717719141774034, -0.14172409793685134, -0.2481932610235348, 0.030745500075032135, -0.308204211375429, 0.014742916278845193, 0.13054746136601483, 0.0757829137431571... |
710.1374 | Nanosecond electro-optical switching with a repetition rate above 20MHz | We describe an electro-optical switch based on a commercial electro-optic
modulator (modified for high-speed operation) and a 340V pulser having a rise
time of 2.2ns (at 250V). It can produce arbitrary pulse patterns with an
average repetition rate beyond 20MHz. It uses a grounded-grid triode driven by
transmitting p... | physics.optics physics.ins-det | we describe an electrooptical switch based on a commercial electrooptic modulator modified for highspeed operation and a 340v pulser having a rise time of 22ns at 250v it can produce arbitrary pulse patterns with an average repetition rate beyond 20mhz it uses a groundedgrid triode driven by transmitting power transist... | [['we', 'describe', 'an', 'electrooptical', 'switch', 'based', 'on', 'a', 'commercial', 'electrooptic', 'modulator', 'modified', 'for', 'highspeed', 'operation', 'and', 'a', '340v', 'pulser', 'having', 'a', 'rise', 'time', 'of', '22ns', 'at', '250v', 'it', 'can', 'produce', 'arbitrary', 'pulse', 'patterns', 'with', 'an... | [-0.17656618377692263, 0.1310666949249653, -0.07645391227520058, -0.051034663043076724, -0.06582489649069981, -0.25533857123113013, 0.07872236663029647, 0.46749502574880675, -0.24705051688451163, -0.2835195565950388, 0.09349907131072029, -0.2137451402902026, -0.1530375740471178, 0.3231027569510305, -0.10430648171303558... |
710.1375 | Dynamic Models of Learning and Education Measurement | Pre-post testing is a commonly used method in physics education community for
evaluating students' achievement and or the effectiveness of teaching through a
specific period of instruction. A popular method to analyze pre-post testing
results is the normalized gain first brought to the physics education community
in ... | physics.ed-ph physics.data-an | prepost testing is a commonly used method in physics education community for evaluating students achievement and or the effectiveness of teaching through a specific period of instruction a popular method to analyze prepost testing results is the normalized gain first brought to the physics education community in wide u... | [['prepost', 'testing', 'is', 'a', 'commonly', 'used', 'method', 'in', 'physics', 'education', 'community', 'for', 'evaluating', 'students', 'achievement', 'and', 'or', 'the', 'effectiveness', 'of', 'teaching', 'through', 'a', 'specific', 'period', 'of', 'instruction', 'a', 'popular', 'method', 'to', 'analyze', 'prepos... | [-0.009852674069491864, 0.05105608577550351, -0.12282785543889271, 0.1096926898623859, -0.0818985587063858, -0.17254496050331786, 0.07570948847161846, 0.4068228856058871, -0.20927002405972447, -0.3734271095069995, 0.050921409059810685, -0.2871608373198064, -0.1490205935694473, 0.18639644268417283, -0.10240662017119649,... |
710.1376 | Emergent Symmetry and Dimensional Reduction at a Quantum Critical Point | We show that the spatial dimensionality of the quantum critical point
associated with Bose--Einstein condensation at T=0 is reduced when the
underlying lattice comprises a set of layers coupled by a frustrating
interaction. For this purpose, we use an heuristic mean field approach that is
complemented and justified b... | cond-mat.str-el | we show that the spatial dimensionality of the quantum critical point associated with boseeinstein condensation at t0 is reduced when the underlying lattice comprises a set of layers coupled by a frustrating interaction for this purpose we use an heuristic mean field approach that is complemented and justified by a mor... | [['we', 'show', 'that', 'the', 'spatial', 'dimensionality', 'of', 'the', 'quantum', 'critical', 'point', 'associated', 'with', 'boseeinstein', 'condensation', 'at', 't0', 'is', 'reduced', 'when', 'the', 'underlying', 'lattice', 'comprises', 'a', 'set', 'of', 'layers', 'coupled', 'by', 'a', 'frustrating', 'interaction',... | [-0.15350974864887598, 0.17465349079261963, -0.08435575037191693, 0.01974448749823416, -0.01604351514361353, -0.15040479067506063, 0.05335409126172845, 0.34830067839282447, -0.22996682381161895, -0.24304934659511104, 0.06138716424958637, -0.2957144360551531, -0.15933425832364675, 0.12944655226042065, 0.0356022379824764... |
710.1377 | Entropy of Stars, Black Holes and Dark Energy | When a star collapses to form a black hole, its entropy increases
considerably, for a solar mass black hole, there is a factor of 1019 increase
in entropy. This corresponds to a tremendous loss of information as only the
total mass, angular momentum or electric charge (if any) of the matter going
inside the horizon c... | astro-ph | when a star collapses to form a black hole its entropy increases considerably for a solar mass black hole there is a factor of 1019 increase in entropy this corresponds to a tremendous loss of information as only the total mass angular momentum or electric charge if any of the matter going inside the horizon can be mea... | [['when', 'a', 'star', 'collapses', 'to', 'form', 'a', 'black', 'hole', 'its', 'entropy', 'increases', 'considerably', 'for', 'a', 'solar', 'mass', 'black', 'hole', 'there', 'is', 'a', 'factor', 'of', '1019', 'increase', 'in', 'entropy', 'this', 'corresponds', 'to', 'a', 'tremendous', 'loss', 'of', 'information', 'as',... | [-0.13129129595795852, 0.18620839766279257, -0.06038765044003311, 0.10528718293385787, -0.06282469606311578, -0.10289362390499769, 0.049286287109781474, 0.27129329257230794, -0.2255936189968553, -0.3500703312909334, 0.08480520325085511, -0.3685072644406723, -0.003225847771520623, 0.19027086105132993, -0.074483767885895... |
710.1378 | Generation and detection of gravitational waves at microwave frequencies
by means of a superconducting two-body system | The 2-body system of a superconducting sphere levitated in the magnetic field
generated by a persistent current in a superconducting ring, can possibly
convert gravitational waves into electromagnetic waves, and vice versa.
Faraday's law of induction implies that the time-varying distance between the
sphere and the r... | gr-qc | the 2body system of a superconducting sphere levitated in the magnetic field generated by a persistent current in a superconducting ring can possibly convert gravitational waves into electromagnetic waves and vice versa faradays law of induction implies that the timevarying distance between the sphere and the ring caus... | [['the', '2body', 'system', 'of', 'a', 'superconducting', 'sphere', 'levitated', 'in', 'the', 'magnetic', 'field', 'generated', 'by', 'a', 'persistent', 'current', 'in', 'a', 'superconducting', 'ring', 'can', 'possibly', 'convert', 'gravitational', 'waves', 'into', 'electromagnetic', 'waves', 'and', 'vice', 'versa', 'f... | [-0.21206965881973766, 0.23676575177980635, -0.05183584003460182, 0.0287798429213623, -0.10357176121676254, -0.08518238533504827, 0.02802514375409458, 0.33531930556298817, -0.28730508813439587, -0.29466113557519263, 0.06663083400831796, -0.2683976701309168, -0.0891208436643315, 0.20042795843314812, 0.04775313355521364,... |
710.1379 | 5D Differential Calculus and Noether Analysis of Translation Symmetries
in kappa-Minkowski Noncommutative Spacetime | We perform a Noether analysis for a description of translation
transformations in 4D kappa-Minkowski noncommutative spacetime which is based
on the structure of a 5D differential calculus. Taking properly into account
the properties of the differential calculus we arrive at an explicit formula
for the conserved charg... | hep-th | we perform a noether analysis for a description of translation transformations in 4d kappaminkowski noncommutative spacetime which is based on the structure of a 5d differential calculus taking properly into account the properties of the differential calculus we arrive at an explicit formula for the conserved charges w... | [['we', 'perform', 'a', 'noether', 'analysis', 'for', 'a', 'description', 'of', 'translation', 'transformations', 'in', '4d', 'kappaminkowski', 'noncommutative', 'spacetime', 'which', 'is', 'based', 'on', 'the', 'structure', 'of', 'a', '5d', 'differential', 'calculus', 'taking', 'properly', 'into', 'account', 'the', 'p... | [-0.11292214171766345, 0.04929843924830167, -0.15333737799230573, 0.10757942099659357, -0.1423827230825207, -0.087327598302222, -0.011958533944909587, 0.33011439993087927, -0.24203187412123628, -0.26765289026965844, 0.028843232463530974, -0.23480568851914202, -0.14240989614444882, 0.1280124416790291, -0.083412073472681... |
710.138 | Mirror duality and noncommutative tori | In this paper, we study a mirror duality on a generalized complex torus and a
noncommutative complex torus. First, we derive a symplectic version of Riemann
condition using mirror duality on ordinary complex tori. Based on this we will
find a mirror correspondence on generalized complex tori and generalize the
mirror... | hep-th math-ph math.MP | in this paper we study a mirror duality on a generalized complex torus and a noncommutative complex torus first we derive a symplectic version of riemann condition using mirror duality on ordinary complex tori based on this we will find a mirror correspondence on generalized complex tori and generalize the mirror duali... | [['in', 'this', 'paper', 'we', 'study', 'a', 'mirror', 'duality', 'on', 'a', 'generalized', 'complex', 'torus', 'and', 'a', 'noncommutative', 'complex', 'torus', 'first', 'we', 'derive', 'a', 'symplectic', 'version', 'of', 'riemann', 'condition', 'using', 'mirror', 'duality', 'on', 'ordinary', 'complex', 'tori', 'based... | [-0.18998074895071407, 0.041831256566388954, -0.11329208356478522, 0.17105105721707187, -0.11679833817986711, -0.1355586517226672, -0.02246222059024618, 0.3261302839363775, -0.22511094543827517, -0.20671698351901385, 0.1453649359323355, -0.1665380379755891, -0.2762867987396256, 0.2207999602147949, -0.19506571061849112,... |
710.1381 | On the symplectic phase space of KdV | We prove that the Birkhoff map $\Om$ for KdV constructed on $H^{-1}_0(\T)$
can be interpolated between $H^{-1}_0(\T)$ and $L^2_0(\T)$. In particular, the
symplectic phase space $H^{1/2}_0(\T)$ can be described in terms of Birkhoff
coordinates. As an application, we characterize the regularity of a potential
$q\in H^{... | math.FA math.AP | we prove that the birkhoff map om for kdv constructed on h1_0t can be interpolated between h1_0t and l2_0t in particular the symplectic phase space h12_0t can be described in terms of birkhoff coordinates as an application we characterize the regularity of a potential qin h1t in terms of the decay of the gap lengths of... | [['we', 'prove', 'that', 'the', 'birkhoff', 'map', 'om', 'for', 'kdv', 'constructed', 'on', 'h1_0t', 'can', 'be', 'interpolated', 'between', 'h1_0t', 'and', 'l2_0t', 'in', 'particular', 'the', 'symplectic', 'phase', 'space', 'h12_0t', 'can', 'be', 'described', 'in', 'terms', 'of', 'birkhoff', 'coordinates', 'as', 'an',... | [-0.1635956926752002, 0.07410145754904314, -0.09097956771391534, 0.0758502138177714, 0.001957168652405662, -0.04754917617256363, 0.014156429431281023, 0.33242318070223253, -0.33279097584947465, -0.21334105288429606, 0.1278777961795699, -0.2613499408978368, -0.13763753421634675, 0.2161640421217007, -0.0945275379344821, ... |
710.1382 | Global anisotropy of arrival directions of ultra-high-energy cosmic
rays: capabilities of space-based detectors | Planned space-based ultra-high-energy cosmic-ray detectors (TUS, JEM-EUSO and
S-EUSO) are best suited for searches of global anisotropies in the distribution
of arrival directions of cosmic-ray particles because they will be able to
observe the full sky with a single instrument. We calculate quantitatively the
streng... | astro-ph | planned spacebased ultrahighenergy cosmicray detectors tus jemeuso and seuso are best suited for searches of global anisotropies in the distribution of arrival directions of cosmicray particles because they will be able to observe the full sky with a single instrument we calculate quantitatively the strength of anisotr... | [['planned', 'spacebased', 'ultrahighenergy', 'cosmicray', 'detectors', 'tus', 'jemeuso', 'and', 'seuso', 'are', 'best', 'suited', 'for', 'searches', 'of', 'global', 'anisotropies', 'in', 'the', 'distribution', 'of', 'arrival', 'directions', 'of', 'cosmicray', 'particles', 'because', 'they', 'will', 'be', 'able', 'to',... | [-0.066468993875952, 0.18479845292334046, -0.11281278956504096, 0.16854292501562407, -0.07139098900592043, -0.030453976815832513, -0.0039856869173014444, 0.3846008305393514, -0.19836795933189846, -0.36753069818729445, 0.0018445467365728247, -0.3418905803312858, -0.008414290630857328, 0.1969870358018116, 0.0638495723938... |
710.1383 | Log-concavity property of the error probability with application to
local bounds for wireless communications | A clear understanding the behavior of the error probability (EP) as a
function of signal-to-noise ratio (SNR) and other system parameters is
fundamental for assessing the design of digital wireless communication
systems.We propose an analytical framework based on the log-concavity property
of the EP which we prove fo... | cs.IT math.IT | a clear understanding the behavior of the error probability ep as a function of signaltonoise ratio snr and other system parameters is fundamental for assessing the design of digital wireless communication systemswe propose an analytical framework based on the logconcavity property of the ep which we prove for a wide f... | [['a', 'clear', 'understanding', 'the', 'behavior', 'of', 'the', 'error', 'probability', 'ep', 'as', 'a', 'function', 'of', 'signaltonoise', 'ratio', 'snr', 'and', 'other', 'system', 'parameters', 'is', 'fundamental', 'for', 'assessing', 'the', 'design', 'of', 'digital', 'wireless', 'communication', 'systemswe', 'propo... | [-0.1402040287481483, 0.03856981008532414, -0.05822325927596309, 0.08251821453737693, -0.0626520136124052, -0.13750378260630425, 0.0829193006092855, 0.3547562388473271, -0.25134556663037927, -0.27645718007934866, 0.12743548257132692, -0.18670186152635718, -0.18506760644312534, 0.24804507244958968, -0.07978343525610399,... |
710.1384 | Traffic of molecular motors: from theory to experiments | Intracellular transport along microtubules or actin filaments, powered by
molecular motors such as kinesins, dyneins or myosins, has been recently
modeled using one-dimensional driven lattice gases. We discuss some
generalizations of these models, that include extended particles and defects.
We investigate the feasib... | physics.bio-ph q-bio.BM | intracellular transport along microtubules or actin filaments powered by molecular motors such as kinesins dyneins or myosins has been recently modeled using onedimensional driven lattice gases we discuss some generalizations of these models that include extended particles and defects we investigate the feasibility of ... | [['intracellular', 'transport', 'along', 'microtubules', 'or', 'actin', 'filaments', 'powered', 'by', 'molecular', 'motors', 'such', 'as', 'kinesins', 'dyneins', 'or', 'myosins', 'has', 'been', 'recently', 'modeled', 'using', 'onedimensional', 'driven', 'lattice', 'gases', 'we', 'discuss', 'some', 'generalizations', 'o... | [-0.1337548712544958, 0.18351146553177386, -0.004092486132867635, 0.00034220347879454494, -0.0025651259176811434, -0.16553926348569803, 0.07778267720714212, 0.44727437205146997, -0.22813884874340146, -0.248690950544551, 0.0536076843898627, -0.2813027008785866, -0.18115616754075745, 0.15300938859727467, -0.0172103415447... |
710.1385 | Cognitive Medium Access: Exploration, Exploitation and Competition | This paper establishes the equivalence between cognitive medium access and
the competitive multi-armed bandit problem. First, the scenario in which a
single cognitive user wishes to opportunistically exploit the availability of
empty frequency bands in the spectrum with multiple bands is considered. In
this scenario,... | cs.IT cs.NI math.IT | this paper establishes the equivalence between cognitive medium access and the competitive multiarmed bandit problem first the scenario in which a single cognitive user wishes to opportunistically exploit the availability of empty frequency bands in the spectrum with multiple bands is considered in this scenario the av... | [['this', 'paper', 'establishes', 'the', 'equivalence', 'between', 'cognitive', 'medium', 'access', 'and', 'the', 'competitive', 'multiarmed', 'bandit', 'problem', 'first', 'the', 'scenario', 'in', 'which', 'a', 'single', 'cognitive', 'user', 'wishes', 'to', 'opportunistically', 'exploit', 'the', 'availability', 'of', ... | [-0.15976324537288897, 0.030836216892960684, -0.06333948516397324, 0.0851530733628717, -0.1335997479444504, -0.22929108133731582, 0.164026426281612, 0.40811835553919534, -0.31127756137938534, -0.32428608428129985, 0.07593858373572224, -0.2043045937496516, -0.1549830605844804, 0.12511127083994372, -0.10048360494085462, ... |
710.1386 | Quasi-socle ideals in Gorenstein numerical semigroup rings | Quasi-socle ideals, that is the ideals $I$ of the form $I= Q :
\mathfrak{m}^q$ in Gorenstein numerical semigroup rings over fields are
explored, where $Q$ is a parameter ideal, and $\mathfrak{m}$ is the maximal
ideal in the base local ring, and $q \geq 1$ is an integer. The problems of
when $I$ is integral over $Q$ a... | math.AC | quasisocle ideals that is the ideals i of the form i q mathfrakmq in gorenstein numerical semigroup rings over fields are explored where q is a parameter ideal and mathfrakm is the maximal ideal in the base local ring and q geq 1 is an integer the problems of when i is integral over q and of when the associated graded ... | [['quasisocle', 'ideals', 'that', 'is', 'the', 'ideals', 'i', 'of', 'the', 'form', 'i', 'q', 'mathfrakmq', 'in', 'gorenstein', 'numerical', 'semigroup', 'rings', 'over', 'fields', 'are', 'explored', 'where', 'q', 'is', 'a', 'parameter', 'ideal', 'and', 'mathfrakm', 'is', 'the', 'maximal', 'ideal', 'in', 'the', 'base', ... | [-0.22140941393936608, 0.07868332757675785, -0.006088544239665007, 0.01690895907133334, -0.04728863781995394, -0.21820145525497855, -0.13747924885579518, 0.3695775740719461, -0.38102772415845426, -0.11768853630531918, 0.14012539428779736, -0.3133334926293268, -0.06786759345272145, 0.19008542568265618, -0.10816240304621... |
710.1387 | Quasi-socle ideals in local rings with Gorenstein tangent cones | Quasi-socle ideals, that is the ideals $I$ of the form $I= Q :
\mathfrak{m}^q$ in a Noetherian local ring $(A, \mathfrak{m})$ with the
Gorenstein tangent cone $\mathrm{G}(\mathfrak{m}) = \bigoplus_{n \geq
0}{\mathfrak{m}}^n/{\mathfrak{m}}^{n+1}$ are explored, where $q \geq 1$ is an
integer and $Q$ is a parameter idea... | math.AC | quasisocle ideals that is the ideals i of the form i q mathfrakmq in a noetherian local ring a mathfrakm with the gorenstein tangent cone mathrmgmathfrakm bigoplus_n geq 0mathfrakmnmathfrakmn1 are explored where q geq 1 is an integer and q is a parameter ideal of a generated by monomials of a system x_1 x_2 x_d of elem... | [['quasisocle', 'ideals', 'that', 'is', 'the', 'ideals', 'i', 'of', 'the', 'form', 'i', 'q', 'mathfrakmq', 'in', 'a', 'noetherian', 'local', 'ring', 'a', 'mathfrakm', 'with', 'the', 'gorenstein', 'tangent', 'cone', 'mathrmgmathfrakm', 'bigoplus_n', 'geq', '0mathfrakmnmathfrakmn1', 'are', 'explored', 'where', 'q', 'geq'... | [-0.2482544759149167, 0.0986129743337825, -0.03764879534665112, -0.009729381375423868, -0.010817554461656609, -0.25382263532395816, -0.1164386777955795, 0.39006081769225476, -0.4024158706105201, -0.07937824894090957, 0.09716010916320973, -0.3430719001340532, -0.028042343749760466, 0.14175479564920207, -0.12189583830692... |
710.1388 | Interference-induced splitting of resonances in spontaneous emission | We study the resonance fluorescence from a coherently driven four-level atom
in the Y-type configuration. The effects of quantum interference induced by
spontaneous emission on the fluorescence properties of the atom are
investigated. It is found that the quantum interference resulting from cascade
emission decays of... | quant-ph | we study the resonance fluorescence from a coherently driven fourlevel atom in the ytype configuration the effects of quantum interference induced by spontaneous emission on the fluorescence properties of the atom are investigated it is found that the quantum interference resulting from cascade emission decays of the a... | [['we', 'study', 'the', 'resonance', 'fluorescence', 'from', 'a', 'coherently', 'driven', 'fourlevel', 'atom', 'in', 'the', 'ytype', 'configuration', 'the', 'effects', 'of', 'quantum', 'interference', 'induced', 'by', 'spontaneous', 'emission', 'on', 'the', 'fluorescence', 'properties', 'of', 'the', 'atom', 'are', 'inv... | [-0.13281741339116565, 0.20984779191610303, -0.05878061667374037, 0.07087516196601057, 0.02764296311900942, -0.11180979134605347, 0.061415938210664586, 0.3866659767419389, -0.24416101704921248, -0.27303793192705483, -0.046426502534513844, -0.31553495810954896, -0.1132690687166545, 0.18302584431378296, 0.053869595353319... |
710.1389 | Comparison of two experiments on radiative neutron decay | Over 10 years ago we proposed an experiment on measuring the characteristics
of radiative neutron decay in papers [1, 2]. At the same time we had published
the theoretical spectrum of radiative gamma quanta, calculated within the
framework of the electroweak interactions, on the basis of which we proposed
the methodo... | nucl-ex | over 10 years ago we proposed an experiment on measuring the characteristics of radiative neutron decay in papers 1 2 at the same time we had published the theoretical spectrum of radiative gamma quanta calculated within the framework of the electroweak interactions on the basis of which we proposed the methodology for... | [['over', '10', 'years', 'ago', 'we', 'proposed', 'an', 'experiment', 'on', 'measuring', 'the', 'characteristics', 'of', 'radiative', 'neutron', 'decay', 'in', 'papers', '1', '2', 'at', 'the', 'same', 'time', 'we', 'had', 'published', 'the', 'theoretical', 'spectrum', 'of', 'radiative', 'gamma', 'quanta', 'calculated',... | [-0.05585230938158929, 0.15579743650903563, -0.06619762760638777, 0.06337712984687338, -0.04415591555337111, -0.08216980716627505, 0.09916594446533256, 0.33579048841363857, -0.18567257386114863, -0.37356498968477053, 0.06639558715435366, -0.3290793659703599, -0.02245055733869473, 0.2343780132258932, 0.01718590787197980... |
710.139 | The Stationary Phase Method for a Wave Packet in a Semiconductor Layered
System. The applicability of the method | Using the formal analysis made by Bohm in his book, {\em "Quantum theory"},
Dover Publications Inc. New York (1979), to calculate approximately the phase
time for a transmitted and the reflected wave packets through a potential
barrier, we calculate the phase time for a semiconductor system formed by
different mesosc... | cond-mat.mes-hall cond-mat.mtrl-sci | using the formal analysis made by bohm in his book em quantum theory dover publications inc new york 1979 to calculate approximately the phase time for a transmitted and the reflected wave packets through a potential barrier we calculate the phase time for a semiconductor system formed by different mesoscopic layers th... | [['using', 'the', 'formal', 'analysis', 'made', 'by', 'bohm', 'in', 'his', 'book', 'em', 'quantum', 'theory', 'dover', 'publications', 'inc', 'new', 'york', '1979', 'to', 'calculate', 'approximately', 'the', 'phase', 'time', 'for', 'a', 'transmitted', 'and', 'the', 'reflected', 'wave', 'packets', 'through', 'a', 'poten... | [-0.17137921344220927, 0.11137028793351264, -0.07287003539605581, 0.03409197059607405, -0.028170725806901727, -0.11204601552608849, 0.06512172479971064, 0.3063165878820884, -0.28284938464259457, -0.27274223417043686, 0.09441868046909364, -0.26755466430106356, -0.1565186303230611, 0.19885438414122067, -0.002895524531097... |
710.1391 | Integrablility of a Classical $N= 2$ Super Sinh-Gordon Model with Jump
Defects | The Lagrangian formalism for the N=2 supersymmetric sinh-Gordon model with a
jump defect is considered. The modified conserved momentum and energy are
constructed in terms of border functions. The supersymmetric Backlund
transformation is given and an one-soliton solution is obtained.
The Lax formulation based on t... | hep-th | the lagrangian formalism for the n2 supersymmetric sinhgordon model with a jump defect is considered the modified conserved momentum and energy are constructed in terms of border functions the supersymmetric backlund transformation is given and an onesoliton solution is obtained the lax formulation based on the affine ... | [['the', 'lagrangian', 'formalism', 'for', 'the', 'n2', 'supersymmetric', 'sinhgordon', 'model', 'with', 'a', 'jump', 'defect', 'is', 'considered', 'the', 'modified', 'conserved', 'momentum', 'and', 'energy', 'are', 'constructed', 'in', 'terms', 'of', 'border', 'functions', 'the', 'supersymmetric', 'backlund', 'transfo... | [-0.1260727609221179, 0.0904569332342362, -0.0394840612828445, 0.07285749238694851, -0.0834581542115372, -0.12871840526349843, -0.0485273755964441, 0.29822924826294184, -0.2656489118265036, -0.24569900505817854, 0.09962453257191019, -0.2475751217048711, -0.1350289823439641, 0.11203045240985468, -0.03571393978722298, 0.... |
710.1392 | Patching over fields | We develop a new form of patching that is both far-reaching and more
elementary than the previous versions that have been used in inverse Galois
theory for function fields of curves. A key point of our approach is to work
with fields and vector spaces, rather than rings and modules. After presenting
a self-contained ... | math.AG math.RA | we develop a new form of patching that is both farreaching and more elementary than the previous versions that have been used in inverse galois theory for function fields of curves a key point of our approach is to work with fields and vector spaces rather than rings and modules after presenting a selfcontained develop... | [['we', 'develop', 'a', 'new', 'form', 'of', 'patching', 'that', 'is', 'both', 'farreaching', 'and', 'more', 'elementary', 'than', 'the', 'previous', 'versions', 'that', 'have', 'been', 'used', 'in', 'inverse', 'galois', 'theory', 'for', 'function', 'fields', 'of', 'curves', 'a', 'key', 'point', 'of', 'our', 'approach'... | [-0.11226722425685506, 0.05555613876052507, -0.1470136325168487, 0.08406513678197022, -0.11931674162002459, -0.10678994816995852, -0.01610425264695787, 0.35084533609118157, -0.27277461411941745, -0.2724687097823783, 0.12282721351749225, -0.22073753563406534, -0.19578109479793157, 0.27242943851200685, -0.094216334091320... |
710.1393 | A Measurement of Proper Motions of SiO Maser Sources in the Galactic
Center with the VLBA | We report on the high-precision astrometric observations of maser sources
around the Galactic Center in the SiO J=1--0 v=1 and 2 lines with the VLBA
during 2001 -- 2004. With phase-referencing interferometry referred to the
radio continuum source Sgr A*, accurate positions of masers were obtained for
three detected o... | astro-ph | we report on the highprecision astrometric observations of maser sources around the galactic center in the sio j10 v1 and 2 lines with the vlba during 2001 2004 with phasereferencing interferometry referred to the radio continuum source sgr a accurate positions of masers were obtained for three detected objects irs 10 ... | [['we', 'report', 'on', 'the', 'highprecision', 'astrometric', 'observations', 'of', 'maser', 'sources', 'around', 'the', 'galactic', 'center', 'in', 'the', 'sio', 'j10', 'v1', 'and', '2', 'lines', 'with', 'the', 'vlba', 'during', '2001', '2004', 'with', 'phasereferencing', 'interferometry', 'referred', 'to', 'the', 'r... | [-0.08367555676380822, 0.04559109277610623, -0.04365698693798216, -0.0332483684467758, -0.10899282439705535, -0.0679412845456036, 0.0209925186699091, 0.5020279502992094, -0.16103891423523162, -0.3215390949481795, 0.08390243465050548, -0.282731633842785, 0.026262202366260735, 0.1691642272449374, -0.055566462442918116, -... |
710.1394 | Bosonized supersymmetry from the Majorana-Dirac-Staunton theory and
massive higher-spin fields | We propose a (3+1)D linear set of covariant vector equations, which unify the
spin 0 ``new Dirac equation'' with its spin 1/2 counterpart, proposed by
Staunton. Our equations describe a spin (0,1/2) supermultiplet with different
numbers of degrees of freedom in the bosonic and fermionic sectors. The
translation-invar... | hep-th math-ph math.MP | we propose a 31d linear set of covariant vector equations which unify the spin 0 new dirac equation with its spin 12 counterpart proposed by staunton our equations describe a spin 012 supermultiplet with different numbers of degrees of freedom in the bosonic and fermionic sectors the translationinvariant spin deegres o... | [['we', 'propose', 'a', '31d', 'linear', 'set', 'of', 'covariant', 'vector', 'equations', 'which', 'unify', 'the', 'spin', '0', 'new', 'dirac', 'equation', 'with', 'its', 'spin', '12', 'counterpart', 'proposed', 'by', 'staunton', 'our', 'equations', 'describe', 'a', 'spin', '012', 'supermultiplet', 'with', 'different',... | [-0.17549947790731676, 0.22023055164993274, -0.05734178438037634, 0.007440790552645921, -0.12325283905863763, -0.14458217773586513, -0.030582472175359726, 0.2659480434656143, -0.24388556337356568, -0.2656752657443285, 0.040033255663700404, -0.2676524606888415, -0.13556754259578885, 0.0853133119624108, -0.00814523165300... |
710.1395 | Mapping the Spatial Distribution of Charge Carriers in LaAlO3/SrTiO3
Heterostructures | At the interface between complex insulating oxides, novel phases with
interesting properties may occur, such as the metallic state reported in the
LaAlO3/SrTiO3 system. While this state has been predicted and reported to be
confined at the interface, some works indicate a much broader spatial
extension, thereby quest... | cond-mat.mtrl-sci cond-mat.str-el | at the interface between complex insulating oxides novel phases with interesting properties may occur such as the metallic state reported in the laalo3srtio3 system while this state has been predicted and reported to be confined at the interface some works indicate a much broader spatial extension thereby questioning i... | [['at', 'the', 'interface', 'between', 'complex', 'insulating', 'oxides', 'novel', 'phases', 'with', 'interesting', 'properties', 'may', 'occur', 'such', 'as', 'the', 'metallic', 'state', 'reported', 'in', 'the', 'laalo3srtio3', 'system', 'while', 'this', 'state', 'has', 'been', 'predicted', 'and', 'reported', 'to', 'b... | [-0.106178932148808, 0.10482560510747135, -0.08834312814132621, 0.010634015600662678, -0.05004057943510513, -0.1729954171584298, 0.08628521005312602, 0.39236132748114566, -0.25744413990837833, -0.33597990742574135, 0.06120734834500278, -0.28898735457720853, -0.11255371855727087, 0.20551278680873414, 0.01267594681742290... |
710.1396 | The isoperimetric profile of a compact Riemannian Manifold for small
volumes | We show that, the solutions of the isoperimetric problem for small volumes
are $C^{2,\alpha}$-close to small spheres. On the way, we define a class of
submanifolds called pseudo balls, defined by an equation weaker than constancy
of mean curvature. We show that in a neighborhood of each point of a compact
riemannian ... | math.DG | we show that the solutions of the isoperimetric problem for small volumes are c2alphaclose to small spheres on the way we define a class of submanifolds called pseudo balls defined by an equation weaker than constancy of mean curvature we show that in a neighborhood of each point of a compact riemannian manifold there ... | [['we', 'show', 'that', 'the', 'solutions', 'of', 'the', 'isoperimetric', 'problem', 'for', 'small', 'volumes', 'are', 'c2alphaclose', 'to', 'small', 'spheres', 'on', 'the', 'way', 'we', 'define', 'a', 'class', 'of', 'submanifolds', 'called', 'pseudo', 'balls', 'defined', 'by', 'an', 'equation', 'weaker', 'than', 'cons... | [-0.1609170346238305, 0.09925193894014228, -0.06586508310577843, 0.11608654320281878, -0.08779374366688929, -0.09611218304927932, 0.002587921980224299, 0.34530961015418676, -0.27992121634607237, -0.2406421098962761, 0.08902206648536173, -0.307967972306154, -0.12671535031011935, 0.1562516321532763, -0.16492105025295797,... |
710.1397 | From conformal embeddings to quantum symmetries: an exceptional SU(4)
example | We briefly discuss several algebraic tools that are used to describe the
quantum symmetries of Boundary Conformal Field Theories on a torus. The
starting point is a fusion category, together with an action on another
category described by a quantum graph. For known examples, the corresponding
modular invariant partit... | math-ph hep-th math.MP math.QA | we briefly discuss several algebraic tools that are used to describe the quantum symmetries of boundary conformal field theories on a torus the starting point is a fusion category together with an action on another category described by a quantum graph for known examples the corresponding modular invariant partition fu... | [['we', 'briefly', 'discuss', 'several', 'algebraic', 'tools', 'that', 'are', 'used', 'to', 'describe', 'the', 'quantum', 'symmetries', 'of', 'boundary', 'conformal', 'field', 'theories', 'on', 'a', 'torus', 'the', 'starting', 'point', 'is', 'a', 'fusion', 'category', 'together', 'with', 'an', 'action', 'on', 'another'... | [-0.1002636597321559, 0.09738273401660169, -0.09766887193695913, 0.10051767178811133, -0.08881682046358624, -0.15666158670579555, -0.017848036469771497, 0.34576294456999146, -0.29185873635553866, -0.24242121606103836, 0.12692852743891297, -0.2782562500496785, -0.17277881192664304, 0.15564167977470944, -0.07405317232253... |
710.1398 | Logic of Simultaneity | A logical model of spatiotemporal structures is pictured as a succession of
processes in time. One usual way to formalize time structure is to assume the
global existence of time points and then collect some of them to form time
intervals of processes. Under this set-theoretic approach, the logic that
governs the pro... | math.LO | a logical model of spatiotemporal structures is pictured as a succession of processes in time one usual way to formalize time structure is to assume the global existence of time points and then collect some of them to form time intervals of processes under this settheoretic approach the logic that governs the processes... | [['a', 'logical', 'model', 'of', 'spatiotemporal', 'structures', 'is', 'pictured', 'as', 'a', 'succession', 'of', 'processes', 'in', 'time', 'one', 'usual', 'way', 'to', 'formalize', 'time', 'structure', 'is', 'to', 'assume', 'the', 'global', 'existence', 'of', 'time', 'points', 'and', 'then', 'collect', 'some', 'of', ... | [-0.16167913784530746, 0.09879191802091165, -0.1277663015228297, 0.08453131698643444, -0.09671514861734717, -0.11502696098926078, 0.08187084564997349, 0.3601190039293475, -0.3438015785203398, -0.25584273676421226, 0.07277811846870463, -0.20542087144401325, -0.12600829473272565, 0.15194777639200246, -0.03801384032703936... |
710.1399 | Percolation in the Sherrington-Kirkpatrick Spin Glass | We present extended versions and give detailed proofs of results concerning
percolation (using various sets of two-replica bond occupation variables) in
Sherrington-Kirkpatrick spin glasses (with zero external field) that were first
given in an earlier paper by the same authors. We also explain how
ultrametricity is ... | cond-mat.dis-nn cond-mat.stat-mech math.PR | we present extended versions and give detailed proofs of results concerning percolation using various sets of tworeplica bond occupation variables in sherringtonkirkpatrick spin glasses with zero external field that were first given in an earlier paper by the same authors we also explain how ultrametricity is manifeste... | [['we', 'present', 'extended', 'versions', 'and', 'give', 'detailed', 'proofs', 'of', 'results', 'concerning', 'percolation', 'using', 'various', 'sets', 'of', 'tworeplica', 'bond', 'occupation', 'variables', 'in', 'sherringtonkirkpatrick', 'spin', 'glasses', 'with', 'zero', 'external', 'field', 'that', 'were', 'first'... | [-0.12783399859478525, 0.2260579244722074, -0.08633622608906708, 0.08400534682891511, -0.021313752237503893, -0.09047161920794419, 0.0820037407943384, 0.3458813852826212, -0.2094723513553373, -0.29221143097295854, 0.07916134021180377, -0.2874799175892307, -0.13916857288015552, 0.10694377538317643, -0.009429111325440286... |
710.14 | A new isotropic cell for studying the thermo-mechanical behavior of
unsaturated expansive clays | This paper presents a new suction-temperature controlled isotropic cell that
can be used to study the thermo-mechanical behavior of unsaturated expansive
clays. The vapor equilibrium technique is used to control the soil suction; the
temperature of the cell is controlled using a thermostat bath. The isotropic
pressur... | physics.class-ph | this paper presents a new suctiontemperature controlled isotropic cell that can be used to study the thermomechanical behavior of unsaturated expansive clays the vapor equilibrium technique is used to control the soil suction the temperature of the cell is controlled using a thermostat bath the isotropic pressure is ap... | [['this', 'paper', 'presents', 'a', 'new', 'suctiontemperature', 'controlled', 'isotropic', 'cell', 'that', 'can', 'be', 'used', 'to', 'study', 'the', 'thermomechanical', 'behavior', 'of', 'unsaturated', 'expansive', 'clays', 'the', 'vapor', 'equilibrium', 'technique', 'is', 'used', 'to', 'control', 'the', 'soil', 'suc... | [-0.08433369138239794, 0.16808864584651917, -0.12287273118910316, -0.033892832072898234, -0.04389166599777464, -0.13594586060905497, 0.0854489896845149, 0.3669243081383509, -0.2657120460261629, -0.22942384313281677, 0.10376344640318254, -0.2350593448221071, -0.15584806359232697, 0.21614878632332366, -0.1176709480302995... |
710.1401 | Analysis of the B --> \pi \ell^+ \ell^- Decay in the Standard Model with
Fourth Generation | We investigate the influence of the fourth generation quarks on the branching
ratio and the CP-asymmetry in B -->\pi \ell^+ \ell^- decay. Taking the
|V_{t'd}V_{t'b}| ~ 0.001 with phase about 10 degree, which is consistent with
the sin2\phi_1 of the CKM and the B_d mixing parameter \Delta m_{B_d}, we
obtain that for b... | hep-ph | we investigate the influence of the fourth generation quarks on the branching ratio and the cpasymmetry in b pi ell ell decay taking the v_tdv_tb 0001 with phase about 10 degree which is consistent with the sin2phi_1 of the ckm and the b_d mixing parameter delta m_b_d we obtain that for both muon and tau channels the b... | [['we', 'investigate', 'the', 'influence', 'of', 'the', 'fourth', 'generation', 'quarks', 'on', 'the', 'branching', 'ratio', 'and', 'the', 'cpasymmetry', 'in', 'b', 'pi', 'ell', 'ell', 'decay', 'taking', 'the', 'v_tdv_tb', '0001', 'with', 'phase', 'about', '10', 'degree', 'which', 'is', 'consistent', 'with', 'the', 'si... | [-0.11199268603928074, 0.24919280317986262, 0.003864072289352662, 0.10987598775933871, -0.06743082343209013, -0.11848979834119015, 0.11420593698395887, 0.27788992701359444, -0.2579933682578468, -0.31597123110545017, 0.04441945995943986, -0.2922130610106217, -0.02113572095094301, 0.16992709881878484, 0.09349435088268229... |
710.1402 | Covering an uncountable square by countably many continuous functions | We prove that there exists a countable family of continuous real functions
whose graphs together with their inverses cover an uncountable square, i.e. a
set of the form $X\times X$, where $X$ is an uncountable subset of the real
line. This extends Sierpi\'nski's theorem from 1919, saying that $S\times S$
can be cover... | math.LO math.GN | we prove that there exists a countable family of continuous real functions whose graphs together with their inverses cover an uncountable square ie a set of the form xtimes x where x is an uncountable subset of the real line this extends sierpinskis theorem from 1919 saying that stimes s can be covered by countably man... | [['we', 'prove', 'that', 'there', 'exists', 'a', 'countable', 'family', 'of', 'continuous', 'real', 'functions', 'whose', 'graphs', 'together', 'with', 'their', 'inverses', 'cover', 'an', 'uncountable', 'square', 'ie', 'a', 'set', 'of', 'the', 'form', 'xtimes', 'x', 'where', 'x', 'is', 'an', 'uncountable', 'subset', 'o... | [-0.1402171908463869, 0.13798924426114859, -0.03355650396293236, 0.01570290820285057, -0.09315910171200004, -0.11439487999305128, 0.0658606272798756, 0.3775097961847981, -0.30678589180525806, -0.17728689812227255, 0.1223844417784777, -0.3259405226653649, -0.09395993721619662, 0.2134626544759764, -0.12912169023184106, -... |
710.1403 | Decays in Quantum Hierarchical Models | We study the dynamics of a simple model for quantum decay, where a single
state is coupled to a set of discrete states, the pseudo continuum, each
coupled to a real continuum of states. We find that for constant matrix
elements between the single state and the pseudo continuum the decay occurs via
one state in a cert... | quant-ph cond-mat.dis-nn | we study the dynamics of a simple model for quantum decay where a single state is coupled to a set of discrete states the pseudo continuum each coupled to a real continuum of states we find that for constant matrix elements between the single state and the pseudo continuum the decay occurs via one state in a certain re... | [['we', 'study', 'the', 'dynamics', 'of', 'a', 'simple', 'model', 'for', 'quantum', 'decay', 'where', 'a', 'single', 'state', 'is', 'coupled', 'to', 'a', 'set', 'of', 'discrete', 'states', 'the', 'pseudo', 'continuum', 'each', 'coupled', 'to', 'a', 'real', 'continuum', 'of', 'states', 'we', 'find', 'that', 'for', 'cons... | [-0.13160646281650532, 0.21573899043858916, -0.02429742272268387, 0.06528609563626916, 0.002515284665117877, -0.1398905024263144, 0.04933825867466521, 0.3458307007921563, -0.29411737503740343, -0.219064365748478, 0.1018898813728837, -0.2883748827110706, -0.09234119378843521, 0.1512369769068597, 0.01643918923492901, 0.0... |
710.1404 | Performance Comparison of Persistence Frameworks | One of the essential and most complex components in the software development
process is the database. The complexity increases when the "orientation" of the
interacting components differs. A persistence framework moves the program data
in its most natural form to and from a permanent data store, the database. Thus
a ... | cs.DB cs.IR | one of the essential and most complex components in the software development process is the database the complexity increases when the orientation of the interacting components differs a persistence framework moves the program data in its most natural form to and from a permanent data store the database thus a persiste... | [['one', 'of', 'the', 'essential', 'and', 'most', 'complex', 'components', 'in', 'the', 'software', 'development', 'process', 'is', 'the', 'database', 'the', 'complexity', 'increases', 'when', 'the', 'orientation', 'of', 'the', 'interacting', 'components', 'differs', 'a', 'persistence', 'framework', 'moves', 'the', 'pr... | [-0.12672600327596717, 0.021103196717318026, -0.06792712585389694, 0.04738998129004778, -0.03816250408248555, -0.09270238672052661, 0.034232152697269716, 0.337946926233589, -0.29184403599199826, -0.33097600360070506, 0.12263018399682296, -0.30902605367103414, -0.13503119796614654, 0.20490004098223102, -0.06089455198736... |
710.1405 | Quiet Sun internetwork magnetic fields from the inversion of Hinode
measurements | We analyze Fe I 630 nm observations of the quiet Sun at disk center taken
with the spectropolarimeter of the Solar Optical Telescope aboard the Hinode
satellite. A significant fraction of the scanned area, including granules,
turns out to be covered by magnetic fields. We derive field strength and
inclination probabi... | astro-ph | we analyze fe i 630 nm observations of the quiet sun at disk center taken with the spectropolarimeter of the solar optical telescope aboard the hinode satellite a significant fraction of the scanned area including granules turns out to be covered by magnetic fields we derive field strength and inclination probability d... | [['we', 'analyze', 'fe', 'i', '630', 'nm', 'observations', 'of', 'the', 'quiet', 'sun', 'at', 'disk', 'center', 'taken', 'with', 'the', 'spectropolarimeter', 'of', 'the', 'solar', 'optical', 'telescope', 'aboard', 'the', 'hinode', 'satellite', 'a', 'significant', 'fraction', 'of', 'the', 'scanned', 'area', 'including',... | [-0.10886303677928642, 0.13984688975596388, -0.013195022013257084, 0.03813212657473529, -0.04575832447507114, -0.07942284187127914, 0.01755816206579732, 0.43252630148814103, -0.18422553842130038, -0.3847032517029373, 0.06468849734671928, -0.2853687134197104, -0.07039290705747972, 0.20186372132858732, -0.041467457844344... |
710.1406 | Limits from Weak Gravity Conjecture on Dark Energy Models | The weak gravity conjecture has been proposed as a criterion to distinguish
the landscape from the swampland in string theory. As an application in
cosmology of this conjecture, we use it to impose theoretical constraint on
parameters of two types of dark energy models. Our analysis indicates that the
Chaplygin-gas-t... | astro-ph | the weak gravity conjecture has been proposed as a criterion to distinguish the landscape from the swampland in string theory as an application in cosmology of this conjecture we use it to impose theoretical constraint on parameters of two types of dark energy models our analysis indicates that the chaplygingastype mod... | [['the', 'weak', 'gravity', 'conjecture', 'has', 'been', 'proposed', 'as', 'a', 'criterion', 'to', 'distinguish', 'the', 'landscape', 'from', 'the', 'swampland', 'in', 'string', 'theory', 'as', 'an', 'application', 'in', 'cosmology', 'of', 'this', 'conjecture', 'we', 'use', 'it', 'to', 'impose', 'theoretical', 'constra... | [-0.116484960819951, 0.10879646100978407, -0.13966147219302294, 0.1323909616416872, -0.08578198950415776, -0.18835478225998856, -0.0093434991841032, 0.2986837394512546, -0.24346619612180892, -0.3574767287613617, 0.09041652189464205, -0.19594297437629674, -0.10586405516728575, 0.18935906632090516, -0.04805400527231855, ... |
710.1407 | Strong influence of precursor powder on the critical current density of
Fe-sheathed MgB2 tapes | The effect of the quality of starting powders on the microstructure and
superconducting properties of in-situ processed Fe-sheathed MgB2 tapes has been
investigated. Three different types of commercial atomized spherical magnesium
powder and two different purities of amorphous boron powder were employed. When
using t... | cond-mat.supr-con | the effect of the quality of starting powders on the microstructure and superconducting properties of insitu processed fesheathed mgb2 tapes has been investigated three different types of commercial atomized spherical magnesium powder and two different purities of amorphous boron powder were employed when using the 10m... | [['the', 'effect', 'of', 'the', 'quality', 'of', 'starting', 'powders', 'on', 'the', 'microstructure', 'and', 'superconducting', 'properties', 'of', 'insitu', 'processed', 'fesheathed', 'mgb2', 'tapes', 'has', 'been', 'investigated', 'three', 'different', 'types', 'of', 'commercial', 'atomized', 'spherical', 'magnesium... | [-0.023617611245856627, 0.22688156033600895, 0.011865766413682541, -0.09077454850213318, 0.026723356428710338, -0.16968252025051228, 0.11177296526051614, 0.4545360412695353, -0.14408121213612968, -0.3954128490033134, 0.029516287598240848, -0.358631247414017, 0.06978179420504892, 0.24685398335352737, 0.00242455844846029... |
710.1408 | Exact L_2-small ball asymptotics of Gaussian processes and the spectrum
of boundary value problems with "non-separated" boundary conditions | We sharpen a classical result on the spectral asymptotics of the boundary
value problems for self-adjoint ordinary differential operator. Using this
result we obtain the exact $L_2$-small ball asymptotics for a new class of zero
mean Gaussian processes. This class includes, in particular, integrated
generalized Slepi... | math.PR math-ph math.MP | we sharpen a classical result on the spectral asymptotics of the boundary value problems for selfadjoint ordinary differential operator using this result we obtain the exact l_2small ball asymptotics for a new class of zero mean gaussian processes this class includes in particular integrated generalized slepian process... | [['we', 'sharpen', 'a', 'classical', 'result', 'on', 'the', 'spectral', 'asymptotics', 'of', 'the', 'boundary', 'value', 'problems', 'for', 'selfadjoint', 'ordinary', 'differential', 'operator', 'using', 'this', 'result', 'we', 'obtain', 'the', 'exact', 'l_2small', 'ball', 'asymptotics', 'for', 'a', 'new', 'class', 'of... | [-0.04080395116138139, 0.027292443580725894, -0.12282274661785257, 0.10416869312582223, -0.10985209194145032, -0.10994862264487892, 0.027658450018082346, 0.34539204709497945, -0.2899339132210506, -0.1850892738771758, 0.13024240271520934, -0.26991115661803633, -0.13392685762872653, 0.1736667593275862, -0.101485862662749... |
710.1409 | Ejecta and progenitor of the low-luminosity Type IIP supernova 2003Z | The origin of low-luminosity Type IIP supernovae is unclear: they have been
proposed to originate either from massive (about 25 Msun) or low-mass (about 9
Msun) stars. We wish to determine parameters of the low-luminosity Type IIP
supernova 2003Z, to estimate a mass-loss rate of the presupernova, and to
recover a pro... | astro-ph | the origin of lowluminosity type iip supernovae is unclear they have been proposed to originate either from massive about 25 msun or lowmass about 9 msun stars we wish to determine parameters of the lowluminosity type iip supernova 2003z to estimate a massloss rate of the presupernova and to recover a progenitor mass w... | [['the', 'origin', 'of', 'lowluminosity', 'type', 'iip', 'supernovae', 'is', 'unclear', 'they', 'have', 'been', 'proposed', 'to', 'originate', 'either', 'from', 'massive', 'about', '25', 'msun', 'or', 'lowmass', 'about', '9', 'msun', 'stars', 'we', 'wish', 'to', 'determine', 'parameters', 'of', 'the', 'lowluminosity', ... | [-0.03706647751045991, 0.11854990120496198, -0.014582532686823657, 0.15449234756444388, -0.11612963181486803, -0.06799246624898936, 0.07841531590333786, 0.38011992515610726, -0.0943841012997617, -0.34893702520739994, 0.07254052936031226, -0.29088867330072643, 0.05431663893727216, 0.1828536780426632, -0.0729136829092473... |
710.141 | Equivariant representable K-theory | We interpret certain equivariant Kasparov groups as equivariant representable
K-theory groups. We compute these groups via a classifying space and as
K-theory groups of suitable sigma-C*-algebras. We also relate equivariant
vector bundles to these sigma-C*-algebras and provide sufficient conditions for
equivariant ve... | math.KT | we interpret certain equivariant kasparov groups as equivariant representable ktheory groups we compute these groups via a classifying space and as ktheory groups of suitable sigmacalgebras we also relate equivariant vector bundles to these sigmacalgebras and provide sufficient conditions for equivariant vector bundles... | [['we', 'interpret', 'certain', 'equivariant', 'kasparov', 'groups', 'as', 'equivariant', 'representable', 'ktheory', 'groups', 'we', 'compute', 'these', 'groups', 'via', 'a', 'classifying', 'space', 'and', 'as', 'ktheory', 'groups', 'of', 'suitable', 'sigmacalgebras', 'we', 'also', 'relate', 'equivariant', 'vector', '... | [-0.19203879029179613, 0.06699935972962218, -0.07701858648409446, 0.17842282236864168, -0.13262788410841797, -0.136550952331163, 0.0027431615628302096, 0.47887068952744205, -0.3943111283627028, -0.17334599716899296, 0.13328014652361161, -0.1276320894200277, -0.19182766446222863, 0.2002900545174877, -0.2542752380638073,... |
710.1411 | MOND, dark matter, and conservation of energy | The MOND equation $m \vec a \mu(a) = \vec F$ could be transformed to the
equivalent form $m \vec a = \vec{F'}$, where $\Vec{F'}$ is a transformed force.
Using this transformation we argue that MOND could not avoid introducing dark
matter, and introduces nonconservative terms to the equations of motion.
| gr-qc astro-ph hep-th | the mond equation m vec a mua vec f could be transformed to the equivalent form m vec a vecf where vecf is a transformed force using this transformation we argue that mond could not avoid introducing dark matter and introduces nonconservative terms to the equations of motion | [['the', 'mond', 'equation', 'm', 'vec', 'a', 'mua', 'vec', 'f', 'could', 'be', 'transformed', 'to', 'the', 'equivalent', 'form', 'm', 'vec', 'a', 'vecf', 'where', 'vecf', 'is', 'a', 'transformed', 'force', 'using', 'this', 'transformation', 'we', 'argue', 'that', 'mond', 'could', 'not', 'avoid', 'introducing', 'dark',... | [-0.23693128011655062, 0.1716225691488944, -0.16233604944621524, 0.05183146566074962, -0.16994561587731974, -0.15536357971723191, -0.07260330545250326, 0.2702260770990203, -0.32116343911426765, -0.26797039613787393, -0.04022092850451978, -0.20856684640360376, -0.11557367506126563, 0.1141654067420556, -0.076731129918092... |
710.1412 | Conjugation-invariant norms on groups of geometric origin | A group is said to be bounded if it has a finite diameter with respect to any
bi-invariant metric. In the present paper we discuss boundedness of various
groups of diffeomorphisms.
| math.GR math.GT | a group is said to be bounded if it has a finite diameter with respect to any biinvariant metric in the present paper we discuss boundedness of various groups of diffeomorphisms | [['a', 'group', 'is', 'said', 'to', 'be', 'bounded', 'if', 'it', 'has', 'a', 'finite', 'diameter', 'with', 'respect', 'to', 'any', 'biinvariant', 'metric', 'in', 'the', 'present', 'paper', 'we', 'discuss', 'boundedness', 'of', 'various', 'groups', 'of', 'diffeomorphisms']] | [-0.1823167698457837, 0.14748268609776372, -0.12870297535893419, -0.004728086994990947, -0.15521437794931472, -0.09836724733993892, -0.04627791074510183, 0.42744738945076544, -0.29931399965238187, -0.19222496094880626, 0.15419897950449657, -0.3044171379879117, -0.13328026129954285, 0.14090920343334157, -0.1867546892815... |
710.1413 | Superconductivity in the New Platinum Germanides MPt4Ge12 (M =
Rare-earth and Alkaline-earth Metals) with Filled Skutterudite Structure | New germanium-platinum compounds with the filled-skutterudite crystal
structure were synthesized. The structure and composition were investigated by
X-ray diffraction and microprobe analysis. Magnetic susceptibility, specific
heat, and electrical resistivity measurements evidence superconductivity in
LaPt4Ge12 and Pr... | cond-mat.supr-con cond-mat.str-el | new germaniumplatinum compounds with the filledskutterudite crystal structure were synthesized the structure and composition were investigated by xray diffraction and microprobe analysis magnetic susceptibility specific heat and electrical resistivity measurements evidence superconductivity in lapt4ge12 and prpt4ge12 b... | [['new', 'germaniumplatinum', 'compounds', 'with', 'the', 'filledskutterudite', 'crystal', 'structure', 'were', 'synthesized', 'the', 'structure', 'and', 'composition', 'were', 'investigated', 'by', 'xray', 'diffraction', 'and', 'microprobe', 'analysis', 'magnetic', 'susceptibility', 'specific', 'heat', 'and', 'electri... | [-0.14502058225861264, 0.24233520719488816, -0.017748045796040623, 0.0412052200775915, -0.03985742192404965, -0.12996605894572677, 0.1346371460739257, 0.3969339698198296, -0.2199015384484526, -0.33994669192248866, 0.0020463836110485275, -0.37737399044757086, -0.07681821660316061, 0.17431416001913713, 0.1316929363667787... |
710.1414 | Twisted mass QCD in the charm sector | We present preliminary results for the charm quark mass $m_c$ and the $D$ and
$D_s$ mesons decay constants $f_D$ and $f_{D_s}$ from a lattice QCD calculation
with ${\rm N_f}$ = 2 dynamical fermions. We use the twisted mass fermionic
action defined at maximal twist so that physical quantities are automatically
${\cal ... | hep-lat | we present preliminary results for the charm quark mass m_c and the d and d_s mesons decay constants f_d and f_d_s from a lattice qcd calculation with rm n_f 2 dynamical fermions we use the twisted mass fermionic action defined at maximal twist so that physical quantities are automatically cal oa improved two lattice s... | [['we', 'present', 'preliminary', 'results', 'for', 'the', 'charm', 'quark', 'mass', 'm_c', 'and', 'the', 'd', 'and', 'd_s', 'mesons', 'decay', 'constants', 'f_d', 'and', 'f_d_s', 'from', 'a', 'lattice', 'qcd', 'calculation', 'with', 'rm', 'n_f', '2', 'dynamical', 'fermions', 'we', 'use', 'the', 'twisted', 'mass', 'fer... | [-0.10999491471565603, 0.26257138182240214, -0.07267570752443002, 0.06347627255753759, 0.029136727979633514, -0.12966815436951373, 0.14446599171810587, 0.3880195921489612, -0.14340423048628312, -0.3446023909331642, 0.0548987342919334, -0.34183776902922774, 0.08689342452324154, 0.15934857994395216, 0.02575927671357818, ... |
710.1415 | Quantum invariants and free Z_{p^2} -actions on 3-manifolds | We give a congruence for the quantum invariant of a Z_p-quotient of a
3$-manifold with a Z_{p^2} action. We show the congruence does not hold for
quotients of 3--manifolds with a Z_{5}xZ_{5} action.
| math.GT | we give a congruence for the quantum invariant of a z_pquotient of a 3manifold with a z_p2 action we show the congruence does not hold for quotients of 3manifolds with a z_5xz_5 action | [['we', 'give', 'a', 'congruence', 'for', 'the', 'quantum', 'invariant', 'of', 'a', 'z_pquotient', 'of', 'a', '3manifold', 'with', 'a', 'z_p2', 'action', 'we', 'show', 'the', 'congruence', 'does', 'not', 'hold', 'for', 'quotients', 'of', '3manifolds', 'with', 'a', 'z_5xz_5', 'action']] | [-0.2657493206281816, 0.12629803059802902, -0.18381946798293822, 0.06407053852754255, -0.11665424055630161, -0.15314706725879543, 0.0047626009496349484, 0.3382733086905172, -0.23620045191097644, -0.22555985947650287, 0.07767915350174712, -0.27106365546463956, -0.13078379913067986, 0.2202287409454584, -0.164611086519735... |
710.1416 | Universal pulse sequence to minimize spin dephasing in the central spin
decoherence problem | We present a remarkable finding that a recently discovered [G. S. Uhrig,
Phys. Rev. Lett. 98, 100504 (2007)] series of pulse sequences, designed to
optimally restore coherence to a qubit in the spin-boson model of decoherence,
is in fact completely model-independent and generically valid for arbitrary
dephasing Hamil... | quant-ph cond-mat.mes-hall | we present a remarkable finding that a recently discovered g s uhrig phys rev lett 98 100504 2007 series of pulse sequences designed to optimally restore coherence to a qubit in the spinboson model of decoherence is in fact completely modelindependent and generically valid for arbitrary dephasing hamiltonians given suf... | [['we', 'present', 'a', 'remarkable', 'finding', 'that', 'a', 'recently', 'discovered', 'g', 's', 'uhrig', 'phys', 'rev', 'lett', '98', '100504', '2007', 'series', 'of', 'pulse', 'sequences', 'designed', 'to', 'optimally', 'restore', 'coherence', 'to', 'a', 'qubit', 'in', 'the', 'spinboson', 'model', 'of', 'decoherence... | [-0.2067075295111401, 0.19338463116836796, -0.04906188502320133, 0.0006018007739580103, -0.016702976475085413, -0.18823918168773018, 0.06480621289284456, 0.37066675524011583, -0.2020510450626413, -0.2754992353138588, 0.01825613565816884, -0.24206178612075746, -0.10262831519283945, 0.21800869372340717, -0.07307061338649... |
710.1417 | Rotation of C60 in a single-molecule contact | The orientation of individual C60 molecules adsorbed on Cu(100) is reversibly
switched when the tip of a scanning tunneling microscope is approached to
contact the molecule. The probability of switching rises sharply upon
displacing the tip beyond a threshold. A mechanical mechanism is suggested to
induce the rotatio... | cond-mat.mtrl-sci | the orientation of individual c60 molecules adsorbed on cu100 is reversibly switched when the tip of a scanning tunneling microscope is approached to contact the molecule the probability of switching rises sharply upon displacing the tip beyond a threshold a mechanical mechanism is suggested to induce the rotation of t... | [['the', 'orientation', 'of', 'individual', 'c60', 'molecules', 'adsorbed', 'on', 'cu100', 'is', 'reversibly', 'switched', 'when', 'the', 'tip', 'of', 'a', 'scanning', 'tunneling', 'microscope', 'is', 'approached', 'to', 'contact', 'the', 'molecule', 'the', 'probability', 'of', 'switching', 'rises', 'sharply', 'upon', ... | [-0.1759298520126179, 0.18912379710259392, -0.09365264153765405, -0.036332203881066366, -0.01883264812732152, -0.23579007420031464, 0.1768228275810971, 0.4131050561280811, -0.3075664181116165, -0.2688943174138081, -0.04725755608695395, -0.2961322923428288, -0.09649180062115192, 0.1379733281210065, -0.025015286389080918... |
710.1418 | Non-Archimedean Ergodic Theory and Pseudorandom Generators | The paper develops techniques in order to construct computer programs,
pseudorandom number generators (PRNG), that produce uniformly distributed
sequences. The paper exploits an approach that treats standard processor
instructions (arithmetic and bitwise logical ones) as continuous functions on
the space of 2-adic in... | math.DS cs.IT math.IT | the paper develops techniques in order to construct computer programs pseudorandom number generators prng that produce uniformly distributed sequences the paper exploits an approach that treats standard processor instructions arithmetic and bitwise logical ones as continuous functions on the space of 2adic integers wit... | [['the', 'paper', 'develops', 'techniques', 'in', 'order', 'to', 'construct', 'computer', 'programs', 'pseudorandom', 'number', 'generators', 'prng', 'that', 'produce', 'uniformly', 'distributed', 'sequences', 'the', 'paper', 'exploits', 'an', 'approach', 'that', 'treats', 'standard', 'processor', 'instructions', 'arit... | [-0.19508142569111442, 0.09118432781019692, -0.1094327737155254, 0.09758654381766974, -0.025713271461427212, -0.12481989381376479, 0.03471283793078328, 0.3311367238347884, -0.32226017001084983, -0.2838043801020831, 0.07394475944420265, -0.2351896557083819, -0.18456326436717063, 0.25028059480246156, -0.15746462026800145... |
710.1419 | Gelfand-Kirillov conjecture for symplectic reflection algebras | We construct functorially a class of algebras using the formalism of double
derivations. These algebras extend to higher dimensions Crawley-Boevey and
Holland's construction of deformed preprojective algebras and encompass
symplectic reflection algebras associated to wreath products. We use this
construction to show ... | math.RA math.RT | we construct functorially a class of algebras using the formalism of double derivations these algebras extend to higher dimensions crawleyboevey and hollands construction of deformed preprojective algebras and encompass symplectic reflection algebras associated to wreath products we use this construction to show that t... | [['we', 'construct', 'functorially', 'a', 'class', 'of', 'algebras', 'using', 'the', 'formalism', 'of', 'double', 'derivations', 'these', 'algebras', 'extend', 'to', 'higher', 'dimensions', 'crawleyboevey', 'and', 'hollands', 'construction', 'of', 'deformed', 'preprojective', 'algebras', 'and', 'encompass', 'symplectic... | [-0.15324203868306452, 0.0339861192379988, -0.10461780754098247, 0.09262594565628998, -0.17182495374412787, -0.1485826653623653, -0.05394469818941528, 0.3508617072816818, -0.3577663529544107, -0.1855717046092914, 0.07212459004198711, -0.1780135458140003, -0.1784172635074825, 0.17435247876170662, -0.2094664876649697, -0... |
710.142 | ESO540-032: a Transition-Type Dwarf in the Sculptor Group | A color-magnitude diagram (CMD) based on HST/ACS data is presented for the
Sculptor group dwarf galaxy ESO540-032. The CMD is dominated by an old red
giant population but there is a small population of blue stars confined to the
central regions of the galaxy as orginally noted by Jerjen and Rejkuba from
ground-based ... | astro-ph | a colormagnitude diagram cmd based on hstacs data is presented for the sculptor group dwarf galaxy eso540032 the cmd is dominated by an old red giant population but there is a small population of blue stars confined to the central regions of the galaxy as orginally noted by jerjen and rejkuba from groundbased data from... | [['a', 'colormagnitude', 'diagram', 'cmd', 'based', 'on', 'hstacs', 'data', 'is', 'presented', 'for', 'the', 'sculptor', 'group', 'dwarf', 'galaxy', 'eso540032', 'the', 'cmd', 'is', 'dominated', 'by', 'an', 'old', 'red', 'giant', 'population', 'but', 'there', 'is', 'a', 'small', 'population', 'of', 'blue', 'stars', 'co... | [-0.01154099919112923, 0.08674360909917596, -0.10442113741301, 0.08862403624079888, -0.12678191856830381, -0.02268390244280454, 0.08916858081065585, 0.4522371365805157, -0.08561905877941171, -0.3753928503661882, 0.04902636686892947, -0.3191467736796767, -0.028715818244381807, 0.20989919849380384, -0.107293764926726, -0... |
710.1421 | Stochastic Simulations of the Repressilator Circuit | The genetic repressilator circuit consists of three transcription factors, or
repressors, which negatively regulate each other in a cyclic manner. This
circuit was synthetically constructed on plasmids in {\it Escherichia coli} and
was found to exhibit oscillations in the concentrations of the three
repressors. Since... | q-bio.MN | the genetic repressilator circuit consists of three transcription factors or repressors which negatively regulate each other in a cyclic manner this circuit was synthetically constructed on plasmids in it escherichia coli and was found to exhibit oscillations in the concentrations of the three repressors since the repr... | [['the', 'genetic', 'repressilator', 'circuit', 'consists', 'of', 'three', 'transcription', 'factors', 'or', 'repressors', 'which', 'negatively', 'regulate', 'each', 'other', 'in', 'a', 'cyclic', 'manner', 'this', 'circuit', 'was', 'synthetically', 'constructed', 'on', 'plasmids', 'in', 'it', 'escherichia', 'coli', 'an... | [-0.1234949100872173, 0.16848777733359704, -0.018633638637359527, 0.09519957880873015, 0.0003112488754970186, -0.1572767719215549, 0.05230623548028662, 0.35510682177675124, -0.2664140548885745, -0.3150438683655332, 0.07574030316489584, -0.2749870058094316, -0.2356905093170045, 0.20756195945774808, -0.04533671211341725,... |
710.1422 | Charm and bottom heavy baryon mass spectrum from lattice QCD with 2+1 | We present results for the mass spectrum of charm and bottom heavy baryons,
using MILC coarse lattice configurations with 2+1 flavors. Clover heavy quark
propagators with the Fermilab interpretation and improved staggered light quark
propagators are used to construct two point functions with local operators for
diffe... | hep-lat | we present results for the mass spectrum of charm and bottom heavy baryons using milc coarse lattice configurations with 21 flavors clover heavy quark propagators with the fermilab interpretation and improved staggered light quark propagators are used to construct two point functions with local operators for different ... | [['we', 'present', 'results', 'for', 'the', 'mass', 'spectrum', 'of', 'charm', 'and', 'bottom', 'heavy', 'baryons', 'using', 'milc', 'coarse', 'lattice', 'configurations', 'with', '21', 'flavors', 'clover', 'heavy', 'quark', 'propagators', 'with', 'the', 'fermilab', 'interpretation', 'and', 'improved', 'staggered', 'li... | [-0.036698116363921, 0.39910628264952525, -0.12529823269384602, 0.11762547743159767, -0.00865470384722393, -0.14734923839569092, 0.09995440192356267, 0.40655686322818785, -0.09425526841854055, -0.2621607549634634, 0.0008153533015181037, -0.3361465215098624, 0.06630892752140176, 0.04976259896933448, 0.09093410938101656,... |
710.1423 | Duffin-Kemmer-Petiau formalism reexamined: non-relativistic
approximation for spin 0 and spin 1 particles in a Riemannian space-time | It is shown that the generally covariant Duffin-Kemmer-Petiau equation,
formulated in the frame of the Tetrode-Weyl-Fock-Ivanenko tetrad formalism,
allows for a non-relativistic approximation if the metric tensor is of a
special form. The Pauli equation for a vector particle involves the Riemann
curvature tensor expl... | hep-th | it is shown that the generally covariant duffinkemmerpetiau equation formulated in the frame of the tetrodeweylfockivanenko tetrad formalism allows for a nonrelativistic approximation if the metric tensor is of a special form the pauli equation for a vector particle involves the riemann curvature tensor explicitly in a... | [['it', 'is', 'shown', 'that', 'the', 'generally', 'covariant', 'duffinkemmerpetiau', 'equation', 'formulated', 'in', 'the', 'frame', 'of', 'the', 'tetrodeweylfockivanenko', 'tetrad', 'formalism', 'allows', 'for', 'a', 'nonrelativistic', 'approximation', 'if', 'the', 'metric', 'tensor', 'is', 'of', 'a', 'special', 'for... | [-0.1402997976636116, 0.1791870150745864, -0.09614070062196094, 0.11687417215896102, -0.09053106648472589, -0.16161716200774476, -0.10044480391496897, 0.2864011596747727, -0.22697638692158573, -0.20756708247786235, -0.028438598504026403, -0.26797346436316455, -0.1380884323061192, 0.10747068667851693, 0.0537955125899247... |
710.1424 | The gluon propagator from large asymmetric lattices | The Landau-gauge gluon propagator is computed for the SU(3) gauge theory on
lattices up to a size of $32^3 \times 200$. We use the standard Wilson action
at $\beta = 6.0$ and compare our results with previous computations using large
asymmetric and symmetric lattices. In particular, we focus on the impact of the
latt... | hep-lat | the landaugauge gluon propagator is computed for the su3 gauge theory on lattices up to a size of 323 times 200 we use the standard wilson action at beta 60 and compare our results with previous computations using large asymmetric and symmetric lattices in particular we focus on the impact of the lattice geometry and m... | [['the', 'landaugauge', 'gluon', 'propagator', 'is', 'computed', 'for', 'the', 'su3', 'gauge', 'theory', 'on', 'lattices', 'up', 'to', 'a', 'size', 'of', '323', 'times', '200', 'we', 'use', 'the', 'standard', 'wilson', 'action', 'at', 'beta', '60', 'and', 'compare', 'our', 'results', 'with', 'previous', 'computations',... | [-0.07956841106411733, 0.17356776562838316, -0.07443434405076789, 0.048337728558554734, -0.04888471973779267, -0.07132624649787195, 0.06591479002893982, 0.4433186229012192, -0.16705865691071503, -0.27901816810800195, 0.10692715548355235, -0.27339515285183713, -0.055218741042564995, 0.17233436462813861, 0.03468261779706... |
710.1425 | Classification of 1st order symplectic spinor operators over contact
projective geometries | We give a classification of $1^{st}$ order invariant differential operators
acting between sections of certain bundles associated to Cartan geometries of
the so called metaplectic contact projective type. These bundles are associated
via representations, which are derived from the so called higher symplectic,
harmoni... | math.DG math.RT | we give a classification of 1st order invariant differential operators acting between sections of certain bundles associated to cartan geometries of the so called metaplectic contact projective type these bundles are associated via representations which are derived from the so called higher symplectic harmonic or gener... | [['we', 'give', 'a', 'classification', 'of', '1st', 'order', 'invariant', 'differential', 'operators', 'acting', 'between', 'sections', 'of', 'certain', 'bundles', 'associated', 'to', 'cartan', 'geometries', 'of', 'the', 'so', 'called', 'metaplectic', 'contact', 'projective', 'type', 'these', 'bundles', 'are', 'associa... | [-0.180159344793615, 0.11555622951845032, -0.021021103565833827, 0.09590395523845255, -0.1295217408766147, -0.15198457002091084, -0.0893421007479115, 0.3417821646372015, -0.30099860862955136, -0.2118141956251952, 0.10584894710224006, -0.257656562808078, -0.18683091568572865, 0.1957200487747124, -0.08816660592303605, 0.... |
710.1426 | Automorphisms of non-spherical buildings have unbounded displacement | If f is a nontrivial automorphism of a thick building Delta of purely
infinite type, we prove that there is no bound on the distance that f moves a
chamber. This has the following group-theoretic consequence: If G is a group of
automorphisms of Delta with bounded quotient, then the center of G is trivial.
| math.GR | if f is a nontrivial automorphism of a thick building delta of purely infinite type we prove that there is no bound on the distance that f moves a chamber this has the following grouptheoretic consequence if g is a group of automorphisms of delta with bounded quotient then the center of g is trivial | [['if', 'f', 'is', 'a', 'nontrivial', 'automorphism', 'of', 'a', 'thick', 'building', 'delta', 'of', 'purely', 'infinite', 'type', 'we', 'prove', 'that', 'there', 'is', 'no', 'bound', 'on', 'the', 'distance', 'that', 'f', 'moves', 'a', 'chamber', 'this', 'has', 'the', 'following', 'grouptheoretic', 'consequence', 'if',... | [-0.22345757999203422, 0.14186354748566044, -0.15041136524894022, -0.028965721298432487, -0.13031574555418707, -0.13750805245204406, 0.04869791629978202, 0.3450800340284001, -0.3318970505486835, -0.21449709068983794, 0.09175406621493908, -0.28051752332936636, -0.10411458981689066, 0.17839741564609787, -0.11293045285750... |
710.1427 | Testing the correctness of the Poynting vector \vec E\times\vec B as the
momentum density of gauge fields | Following our recent finding that the renowned formula $\vec x\times (\vec
E\times\vec B)$ is not the correct density for the electromagnetic angular
momentum, here we examine the validity of the Poynting vector $\vec E
\times\vec B$ as the electromagnetic momentum density (or energy flux). The
competitor is the gaug... | hep-ph | following our recent finding that the renowned formula vec xtimes vec etimesvec b is not the correct density for the electromagnetic angular momentum here we examine the validity of the poynting vector vec e timesvec b as the electromagnetic momentum density or energy flux the competitor is the gaugeinvariant canonical... | [['following', 'our', 'recent', 'finding', 'that', 'the', 'renowned', 'formula', 'vec', 'xtimes', 'vec', 'etimesvec', 'b', 'is', 'not', 'the', 'correct', 'density', 'for', 'the', 'electromagnetic', 'angular', 'momentum', 'here', 'we', 'examine', 'the', 'validity', 'of', 'the', 'poynting', 'vector', 'vec', 'e', 'timesve... | [-0.16635008894424091, 0.1682125965188093, -0.086606509052217, 0.09712502006903592, -0.1205251354874824, -0.09533336972954738, -0.018387016857399, 0.3252683192258701, -0.24998975447926888, -0.27316430086434323, -0.006553209791651598, -0.2714439070037128, -0.08668912844688534, 0.14826028981170727, 0.007289541943464428, ... |
710.1428 | Investigating rare diffusion events in silicon by
temperature-accelerated tight-binding molecular dynamics | withdrawn by author
| cond-mat.mtrl-sci | withdrawn by author | [['withdrawn', 'by', 'author']] | [-0.1931126763423284, -0.13287304838498434, -0.06387918690840404, -0.16779323915640512, -0.2956872383753459, -0.19406858459115028, -0.009246408939361572, 0.18121944864590964, -0.3720524919529756, -0.5650171637535095, -0.017427730063597362, -0.4845584146678448, -0.011748383442560831, -0.17437531054019928, -0.61779831101... |
710.1429 | The bound on viscosity and the generalized second law of thermodynamics | We describe a new paradox for ideal fluids. It arises in the accretion of an
\textit{ideal} fluid onto a black hole, where, under suitable boundary
conditions, the flow can violate the generalized second law of thermodynamics.
The paradox indicates that there is in fact a lower bound to the correlation
length of any ... | gr-qc hep-th physics.flu-dyn | we describe a new paradox for ideal fluids it arises in the accretion of an textitideal fluid onto a black hole where under suitable boundary conditions the flow can violate the generalized second law of thermodynamics the paradox indicates that there is in fact a lower bound to the correlation length of any textitreal... | [['we', 'describe', 'a', 'new', 'paradox', 'for', 'ideal', 'fluids', 'it', 'arises', 'in', 'the', 'accretion', 'of', 'an', 'textitideal', 'fluid', 'onto', 'a', 'black', 'hole', 'where', 'under', 'suitable', 'boundary', 'conditions', 'the', 'flow', 'can', 'violate', 'the', 'generalized', 'second', 'law', 'of', 'thermody... | [-0.13250743036343654, 0.16382380402102148, -0.15447081024644943, 0.07014901944714394, -0.05771706148374417, -0.13070704903817032, 0.07323629497805974, 0.22564439839547182, -0.2517932935947234, -0.2821186276709252, 0.08180240873338246, -0.2587771751043364, -0.12734879671472477, 0.2197264945929552, -0.07363112992039178,... |
710.143 | Analysis of Hamiltonian formulations of linearized General Relativity | The different forms of the Hamiltonian formulations of linearized General
Relativity/spin-two theories are discussed in order to show their similarities
and differences. It is demonstrated that in the linear model, non-covariant
modifications to the initial covariant Lagrangian (similar to those
modifications used in... | gr-qc hep-th | the different forms of the hamiltonian formulations of linearized general relativityspintwo theories are discussed in order to show their similarities and differences it is demonstrated that in the linear model noncovariant modifications to the initial covariant lagrangian similar to those modifications used in full gr... | [['the', 'different', 'forms', 'of', 'the', 'hamiltonian', 'formulations', 'of', 'linearized', 'general', 'relativityspintwo', 'theories', 'are', 'discussed', 'in', 'order', 'to', 'show', 'their', 'similarities', 'and', 'differences', 'it', 'is', 'demonstrated', 'that', 'in', 'the', 'linear', 'model', 'noncovariant', '... | [-0.11097982118475816, 0.11751816152744661, -0.09222092378019754, 0.13701782876575766, -0.08348585901382778, -0.12778840728320315, -0.08196840587957663, 0.3632562500216799, -0.28648673580859657, -0.29938624385561396, 0.08159876517415146, -0.2579872322177315, -0.1911284599918872, 0.15192157160449174, -0.0577021128680956... |
710.1431 | High-resolution polarimetry of Parsamian 21: revealing the structure of
an edge-on FU Ori disc | We present the first high spatial resolution near-infrared direct and
polarimetric observations of Parsamian 21, obtained with the VLT/NACO
instrument. We complemented these measurements with archival infrared
observations, such as HST/WFPC2 imaging, HST/NICMOS polarimetry, Spitzer IRAC
and MIPS photometry, Spitzer I... | astro-ph | we present the first high spatial resolution nearinfrared direct and polarimetric observations of parsamian 21 obtained with the vltnaco instrument we complemented these measurements with archival infrared observations such as hstwfpc2 imaging hstnicmos polarimetry spitzer irac and mips photometry spitzer irs spectrosc... | [['we', 'present', 'the', 'first', 'high', 'spatial', 'resolution', 'nearinfrared', 'direct', 'and', 'polarimetric', 'observations', 'of', 'parsamian', '21', 'obtained', 'with', 'the', 'vltnaco', 'instrument', 'we', 'complemented', 'these', 'measurements', 'with', 'archival', 'infrared', 'observations', 'such', 'as', '... | [-0.008000803733567832, 0.03975000684892916, -0.10042544612720324, 0.006236596326610655, -0.1273591624621812, -0.07542190047657224, 0.006975927307110303, 0.4671543597890313, -0.184833949097361, -0.3783569917383835, 0.13155589642293847, -0.2614860486233263, -0.10117525121517432, 0.1651363086213423, -0.1294814562024608, ... |
710.1432 | Pareto law of the expenditure of a person in convenience stores | We study the statistical laws of the expenditure of a person in convenience
stores by analysing around 100 million receipts. The density function of
expenditure exhibits a fat tail that follows a power law. We observe the Pareto
principle where both the top 25% and 2% of the customers account for 80% and
25% of the s... | physics.soc-ph | we study the statistical laws of the expenditure of a person in convenience stores by analysing around 100 million receipts the density function of expenditure exhibits a fat tail that follows a power law we observe the pareto principle where both the top 25 and 2 of the customers account for 80 and 25 of the stores sa... | [['we', 'study', 'the', 'statistical', 'laws', 'of', 'the', 'expenditure', 'of', 'a', 'person', 'in', 'convenience', 'stores', 'by', 'analysing', 'around', '100', 'million', 'receipts', 'the', 'density', 'function', 'of', 'expenditure', 'exhibits', 'a', 'fat', 'tail', 'that', 'follows', 'a', 'power', 'law', 'we', 'obse... | [-0.10856829557035651, 0.08083929206159982, -0.11838091698221186, 0.08372667270966551, -0.006119612380620334, -0.13058432431093284, 0.1206173035346407, 0.2870604598096439, -0.2597808517189092, -0.356453720770486, 0.08062520141066233, -0.3703577116422065, -0.06985806187542228, 0.18761392870264781, -0.08431424602696841, ... |
710.1433 | The Ly<alpha> and Ly<beta> profiles in solar prominences and prominence
fine structure | We present the first combined Ly<alpha> and Ly<beta> profiles in solar
prominences obtained by the SOHO/SUMER instrument and discuss their important
spatial variability with respect to predictions from 1D and multithread models.
| astro-ph | we present the first combined lyalpha and lybeta profiles in solar prominences obtained by the sohosumer instrument and discuss their important spatial variability with respect to predictions from 1d and multithread models | [['we', 'present', 'the', 'first', 'combined', 'lyalpha', 'and', 'lybeta', 'profiles', 'in', 'solar', 'prominences', 'obtained', 'by', 'the', 'sohosumer', 'instrument', 'and', 'discuss', 'their', 'important', 'spatial', 'variability', 'with', 'respect', 'to', 'predictions', 'from', '1d', 'and', 'multithread', 'models']... | [0.0097662411571946, 0.09430675063049421, 0.04158015933353454, 0.14078340074047446, -0.031311622937209904, -0.12678905291249976, 0.0037015799316577613, 0.4997611695434898, -0.14759011974092573, -0.35625522280497535, 0.08384256889621611, -0.29190878008375876, -0.14054472355928738, 0.21641228476073593, -0.032173750223591... |
710.1434 | Estimation Prospects of the Source Number Density of Ultra-high-energy
Cosmic Rays | We discuss the possibility of accurately estimating the source number density
of ultra-high-energy cosmic rays (UHECRs) using small-scale anisotropy in their
arrival distribution. The arrival distribution has information on their source
and source distribution. We calculate the propagation of UHE protons in a
structu... | astro-ph | we discuss the possibility of accurately estimating the source number density of ultrahighenergy cosmic rays uhecrs using smallscale anisotropy in their arrival distribution the arrival distribution has information on their source and source distribution we calculate the propagation of uhe protons in a structured extra... | [['we', 'discuss', 'the', 'possibility', 'of', 'accurately', 'estimating', 'the', 'source', 'number', 'density', 'of', 'ultrahighenergy', 'cosmic', 'rays', 'uhecrs', 'using', 'smallscale', 'anisotropy', 'in', 'their', 'arrival', 'distribution', 'the', 'arrival', 'distribution', 'has', 'information', 'on', 'their', 'sou... | [-0.10318311730201249, 0.21146334574018386, -0.011922715735606482, 0.14290340383959516, -0.04410359800839033, -0.0012052509389166297, 0.006337009470202436, 0.41230945378704803, -0.1883608907323758, -0.4500072258499151, 0.03374964537994702, -0.33629709751920295, 0.0015189701150463452, 0.2045197116625826, 0.0201081092872... |
710.1435 | Faster Least Squares Approximation | Least squares approximation is a technique to find an approximate solution to
a system of linear equations that has no exact solution. In a typical setting,
one lets $n$ be the number of constraints and $d$ be the number of variables,
with $n \gg d$. Then, existing exact methods find a solution vector in
$O(nd^2)$ ti... | cs.DS | least squares approximation is a technique to find an approximate solution to a system of linear equations that has no exact solution in a typical setting one lets n be the number of constraints and d be the number of variables with n gg d then existing exact methods find a solution vector in ond2 time we present two r... | [['least', 'squares', 'approximation', 'is', 'a', 'technique', 'to', 'find', 'an', 'approximate', 'solution', 'to', 'a', 'system', 'of', 'linear', 'equations', 'that', 'has', 'no', 'exact', 'solution', 'in', 'a', 'typical', 'setting', 'one', 'lets', 'n', 'be', 'the', 'number', 'of', 'constraints', 'and', 'd', 'be', 'th... | [-0.12109199813318164, 0.04141893266905582, -0.08695432950842118, 0.08344707127994383, -0.06862437557546222, -0.21519373244248657, 0.05157318486796938, 0.35314026411107313, -0.28186936779299154, -0.31780615855453526, 0.1465106403466853, -0.3117037857033359, -0.11159407320936099, 0.19293250007636892, -0.0001014914223045... |
710.1436 | Polish grid infrastructure for science and research | Structure, functionality, parameters and organization of the computing Grid
in Poland is described, mainly from the perspective of high-energy particle
physics community, currently its largest consumer and developer. It represents
distributed Tier-2 in the worldwide Grid infrastructure. It also provides
services and ... | cs.DC hep-ex | structure functionality parameters and organization of the computing grid in poland is described mainly from the perspective of highenergy particle physics community currently its largest consumer and developer it represents distributed tier2 in the worldwide grid infrastructure it also provides services and resources ... | [['structure', 'functionality', 'parameters', 'and', 'organization', 'of', 'the', 'computing', 'grid', 'in', 'poland', 'is', 'described', 'mainly', 'from', 'the', 'perspective', 'of', 'highenergy', 'particle', 'physics', 'community', 'currently', 'its', 'largest', 'consumer', 'and', 'developer', 'it', 'represents', 'di... | [-0.12289885238136108, 0.06953554684106185, -0.030893319761570618, 0.05657699739569988, -0.11523640039852079, -0.12957323003294213, 0.040713777574080956, 0.3587298845606191, -0.3060994192919865, -0.3830214274324933, 0.11570740090825651, -0.31536318156488086, -0.10729374748664167, 0.25105421114427856, -0.089358724064516... |
710.1437 | Perturbative matching of heavy-light currents at one-loop | We present results of a perturbative matching calculation performed at
one-loop for heavy-light currents. We use the Fermilab action for the heavy
quarks, the Asqtad action for the light quarks, and an improved gluon action.
We also present results for heavy-heavy currents with Fermilab heavy quarks and
improved glue... | hep-lat | we present results of a perturbative matching calculation performed at oneloop for heavylight currents we use the fermilab action for the heavy quarks the asqtad action for the light quarks and an improved gluon action we also present results for heavyheavy currents with fermilab heavy quarks and improved glue | [['we', 'present', 'results', 'of', 'a', 'perturbative', 'matching', 'calculation', 'performed', 'at', 'oneloop', 'for', 'heavylight', 'currents', 'we', 'use', 'the', 'fermilab', 'action', 'for', 'the', 'heavy', 'quarks', 'the', 'asqtad', 'action', 'for', 'the', 'light', 'quarks', 'and', 'an', 'improved', 'gluon', 'act... | [-0.030314642451323415, 0.3369867626167192, -0.13137365032785706, 0.13110210502292124, -0.01868921008949377, -0.08244392304795281, 0.10259003450675887, 0.4149084883380909, -0.073573216491816, -0.17462775457118238, -0.02359958467244798, -0.35616731617067543, 0.025116450685475553, 0.10772965074877958, 0.05793415350193272... |
710.1438 | The accuracy of merging approximation in generalized St. Petersburg
games | Merging asymptotic expansions of arbitrary length are established for the
distribution functions and for the probabilities of suitably centered and
normalized cumulative winnings in a full sequence of generalized St. Petersburg
games, extending the short expansions due to Cs\"org\H{o}, S., Merging
asymptotic expansio... | math.PR | merging asymptotic expansions of arbitrary length are established for the distribution functions and for the probabilities of suitably centered and normalized cumulative winnings in a full sequence of generalized st petersburg games extending the short expansions due to csorgho s merging asymptotic expansions in genera... | [['merging', 'asymptotic', 'expansions', 'of', 'arbitrary', 'length', 'are', 'established', 'for', 'the', 'distribution', 'functions', 'and', 'for', 'the', 'probabilities', 'of', 'suitably', 'centered', 'and', 'normalized', 'cumulative', 'winnings', 'in', 'a', 'full', 'sequence', 'of', 'generalized', 'st', 'petersburg'... | [-0.1502464891593788, 0.1499481068290386, -0.139745719783661, 0.09869277631844749, -0.03340538965595752, -0.05968631320565786, 0.06854283668643306, 0.31185657753772345, -0.23288313210605807, -0.25193580209527205, 0.10212941547452482, -0.28357159605576204, -0.09677381969546688, 0.15622221610806497, -0.07606798695813212,... |
710.1439 | Trading activity as driven Poisson process: comparison with empirical
data | We propose the point process model as the Poissonian-like stochastic sequence
with slowly diffusing mean rate and adjust the parameters of the model to the
empirical data of trading activity for 26 stocks traded on NYSE. The proposed
scaled stochastic differential equation provides the universal description of
the tr... | q-fin.TR physics.data-an physics.soc-ph | we propose the point process model as the poissonianlike stochastic sequence with slowly diffusing mean rate and adjust the parameters of the model to the empirical data of trading activity for 26 stocks traded on nyse the proposed scaled stochastic differential equation provides the universal description of the tradin... | [['we', 'propose', 'the', 'point', 'process', 'model', 'as', 'the', 'poissonianlike', 'stochastic', 'sequence', 'with', 'slowly', 'diffusing', 'mean', 'rate', 'and', 'adjust', 'the', 'parameters', 'of', 'the', 'model', 'to', 'the', 'empirical', 'data', 'of', 'trading', 'activity', 'for', '26', 'stocks', 'traded', 'on',... | [-0.06667419612921517, 0.09632731134328863, -0.09637404020458203, 0.1090047755490967, -0.042673210709773264, -0.14023556685524768, 0.1275809351776341, 0.3475729112738165, -0.28611109942872204, -0.30386030950166026, 0.09784856977358718, -0.3176596332983724, -0.10524192285434954, 0.18355985252379342, -0.06471754690824912... |
710.144 | The UV spectrum of the Galactic bulge | The UV excess shown by elliptical galaxies in their spectra is believed to be
caused by evolved low-mass stars, in particular sdB stars. The stellar system
most similar to the ellipticals for age and metallicity, in which it is
possible to resolve these stars, is the bulge of our Galaxy. sdB star
candidates were obse... | astro-ph | the uv excess shown by elliptical galaxies in their spectra is believed to be caused by evolved lowmass stars in particular sdb stars the stellar system most similar to the ellipticals for age and metallicity in which it is possible to resolve these stars is the bulge of our galaxy sdb star candidates were observed in ... | [['the', 'uv', 'excess', 'shown', 'by', 'elliptical', 'galaxies', 'in', 'their', 'spectra', 'is', 'believed', 'to', 'be', 'caused', 'by', 'evolved', 'lowmass', 'stars', 'in', 'particular', 'sdb', 'stars', 'the', 'stellar', 'system', 'most', 'similar', 'to', 'the', 'ellipticals', 'for', 'age', 'and', 'metallicity', 'in'... | [-0.026000062717450978, 0.08682835731608203, -0.10987132788686875, 0.11454817775503304, -0.11445486254770042, -0.043030559965546875, 0.08913573703653953, 0.4330118573801238, -0.13180837958617891, -0.3965689113976646, 0.032459024046174394, -0.30478461139259727, -0.010342028358448219, 0.20371093821538935, -0.089342078251... |
710.1441 | SUSY R parity violation and CP asymmetry in semi-leptonic tau-decays | We analyze the CP violation in the semileptonic | \Delta S|=1 tau-decays in
supersymmetric extensions of the standard model (SM) with R parity violating
term. We show that the CP asymmetry of tau-decay is enhanced significantly and
the current experimental limits obtained by CLEO collaborations can be easily
accommod... | hep-ph | we analyze the cp violation in the semileptonic delta s1 taudecays in supersymmetric extensions of the standard model sm with r parity violating term we show that the cp asymmetry of taudecay is enhanced significantly and the current experimental limits obtained by cleo collaborations can be easily accommodated we argu... | [['we', 'analyze', 'the', 'cp', 'violation', 'in', 'the', 'semileptonic', 'delta', 's1', 'taudecays', 'in', 'supersymmetric', 'extensions', 'of', 'the', 'standard', 'model', 'sm', 'with', 'r', 'parity', 'violating', 'term', 'we', 'show', 'that', 'the', 'cp', 'asymmetry', 'of', 'taudecay', 'is', 'enhanced', 'significant... | [-0.12051068371019169, 0.23453332372272098, -0.01728530443588298, 0.19166485488604965, -0.12087168838356582, -0.21867575068157954, 0.12435905876396057, 0.2606689574747858, -0.22163008086827687, -0.2715441252459103, 0.038580767092176935, -0.29879967656485, -0.01665689167894528, 0.09966591587880443, 0.04213907272869747, ... |
710.1442 | Coherence properties of photons emitted by single defect centers in
diamond | Photon interference among distant quantum emitters is a promising method to
generate large scale quantum networks. Interference is best achieved when
photons show long coherence times. For the nitrogen-vacancy defect center in
diamond we measure the coherence times of photons via optically induced Rabi
oscillations. ... | quant-ph | photon interference among distant quantum emitters is a promising method to generate large scale quantum networks interference is best achieved when photons show long coherence times for the nitrogenvacancy defect center in diamond we measure the coherence times of photons via optically induced rabi oscillations experi... | [['photon', 'interference', 'among', 'distant', 'quantum', 'emitters', 'is', 'a', 'promising', 'method', 'to', 'generate', 'large', 'scale', 'quantum', 'networks', 'interference', 'is', 'best', 'achieved', 'when', 'photons', 'show', 'long', 'coherence', 'times', 'for', 'the', 'nitrogenvacancy', 'defect', 'center', 'in'... | [-0.1342773987450684, 0.2257378567762748, -0.007972405273279156, 0.07629070260633733, 0.02754095731058506, -0.1666840771612984, 0.0802070929344292, 0.4459818106408071, -0.2436930567139026, -0.3208036526774216, 0.028480064460179873, -0.30818380840649506, -0.013423231745496242, 0.20810159302382458, 0.009269524159878868, ... |
710.1443 | Variations on themes of Kostant | Let g be a complex semisimple Lie algebra and let G' be the Langlands dual
group. We give a description of the cohomology algebra of an arbitrary
spherical Schubert variety in the loop Grassmannian for G' as a quotient of the
form Sym(g^e)/J. Here, J is an appropriate ideal in the symmetric algebra of
g^e, the centra... | math.RT math.AG | let g be a complex semisimple lie algebra and let g be the langlands dual group we give a description of the cohomology algebra of an arbitrary spherical schubert variety in the loop grassmannian for g as a quotient of the form symgej here j is an appropriate ideal in the symmetric algebra of ge the centralizer of a pr... | [['let', 'g', 'be', 'a', 'complex', 'semisimple', 'lie', 'algebra', 'and', 'let', 'g', 'be', 'the', 'langlands', 'dual', 'group', 'we', 'give', 'a', 'description', 'of', 'the', 'cohomology', 'algebra', 'of', 'an', 'arbitrary', 'spherical', 'schubert', 'variety', 'in', 'the', 'loop', 'grassmannian', 'for', 'g', 'as', 'a... | [-0.23417812468553031, 0.0348519151602774, -0.1312796287468554, -0.021455356683064666, -0.18342003994333891, -0.12187086732736156, -0.06718529926406012, 0.3033546333971583, -0.3585972244115431, -0.2043109837356081, 0.10957666602413986, -0.16578417173644275, -0.15008172059408675, 0.17699755059072264, -0.1552615981487224... |
710.1444 | Detecting Life-bearing Extra-solar Planets with Space Telescopes | One of the promising methods to search for life on extra-solar planets
(exoplanets) is to detect life's signatures in their atmospheres. Spectra of
exoplanet atmospheres at the modest resolution needed to search for oxygen,
carbon dioxide, water, and methane will demand large collecting areas and large
diameters to c... | astro-ph | one of the promising methods to search for life on extrasolar planets exoplanets is to detect lifes signatures in their atmospheres spectra of exoplanet atmospheres at the modest resolution needed to search for oxygen carbon dioxide water and methane will demand large collecting areas and large diameters to capture and... | [['one', 'of', 'the', 'promising', 'methods', 'to', 'search', 'for', 'life', 'on', 'extrasolar', 'planets', 'exoplanets', 'is', 'to', 'detect', 'lifes', 'signatures', 'in', 'their', 'atmospheres', 'spectra', 'of', 'exoplanet', 'atmospheres', 'at', 'the', 'modest', 'resolution', 'needed', 'to', 'search', 'for', 'oxygen'... | [-0.06838085636314183, 0.2003593700111075, -0.006740607663106195, 0.06105156225654313, -0.12964466690338847, -0.08027678563507176, 0.08949079719369402, 0.3562335718336994, -0.17199707238778816, -0.4128401610015143, 0.13608808497927888, -0.3337806152405939, -0.047912326669643464, 0.23791176773139378, -0.1017315377039845... |
710.1445 | String topology prospectra and Hochschild cohomology | We study string topology for classifying spaces of connected compact Lie
groups, drawing connections with Hochschild cohomology and equivariant homotopy
theory. First, for a compact Lie group $G$, we show that the string topology
prospectrum $LBG^{-TBG}$ is equivalent to the homotopy fixed-point prospectrum
for the c... | math.AT math.QA | we study string topology for classifying spaces of connected compact lie groups drawing connections with hochschild cohomology and equivariant homotopy theory first for a compact lie group g we show that the string topology prospectrum lbgtbg is equivalent to the homotopy fixedpoint prospectrum for the conjugation acti... | [['we', 'study', 'string', 'topology', 'for', 'classifying', 'spaces', 'of', 'connected', 'compact', 'lie', 'groups', 'drawing', 'connections', 'with', 'hochschild', 'cohomology', 'and', 'equivariant', 'homotopy', 'theory', 'first', 'for', 'a', 'compact', 'lie', 'group', 'g', 'we', 'show', 'that', 'the', 'string', 'top... | [-0.22807725225252531, 0.0585464732767553, -0.08759464104982591, 0.0847653858772811, -0.11013114946608496, -0.11220620818307052, -0.014949122984377243, 0.4424321436240236, -0.37990205823489936, -0.20268651325310957, 0.12408278637570283, -0.2043097962989555, -0.19339605440191998, 0.15733127033171973, -0.1844014395789086... |
710.1446 | The quadrupole mechanism of hole spin relaxation | For spin-3/2 holes the anisotropic part of the instantaneous Luttinger
Hamiltonian can be represented as an effective quadrupole coupling. We
investigate the hole spin relaxation process induced by nonadiabatic
fluctuations of this interaction. The obtained analytical solution of the
stochastic Liouville equation des... | cond-mat.mes-hall | for spin32 holes the anisotropic part of the instantaneous luttinger hamiltonian can be represented as an effective quadrupole coupling we investigate the hole spin relaxation process induced by nonadiabatic fluctuations of this interaction the obtained analytical solution of the stochastic liouville equation describes... | [['for', 'spin32', 'holes', 'the', 'anisotropic', 'part', 'of', 'the', 'instantaneous', 'luttinger', 'hamiltonian', 'can', 'be', 'represented', 'as', 'an', 'effective', 'quadrupole', 'coupling', 'we', 'investigate', 'the', 'hole', 'spin', 'relaxation', 'process', 'induced', 'by', 'nonadiabatic', 'fluctuations', 'of', '... | [-0.15809321500075219, 0.18826869917145153, -0.05084003074179319, 0.08015757919817836, -0.03034427458822558, -0.11492062600287185, -0.01671095195607367, 0.3222848039797761, -0.2662005262364718, -0.2667679707308046, -0.017212941565296867, -0.3234044927468693, -0.12398867940382016, 0.1831158390797844, 0.08476901091952724... |
710.1447 | Quantum information processing using nuclear and electron magnetic
resonance: review and prospects | This paper describes recent progress using nuclear magnetic resonance (NMR)
as a platform for implementing quantum information processing (QIP) tasks. The
basic ideas of NMR QIP are detailed, examining the successes and limitations of
liquid and solid state experiments. Finally, a future direction for
implementing qu... | quant-ph | this paper describes recent progress using nuclear magnetic resonance nmr as a platform for implementing quantum information processing qip tasks the basic ideas of nmr qip are detailed examining the successes and limitations of liquid and solid state experiments finally a future direction for implementing quantum proc... | [['this', 'paper', 'describes', 'recent', 'progress', 'using', 'nuclear', 'magnetic', 'resonance', 'nmr', 'as', 'a', 'platform', 'for', 'implementing', 'quantum', 'information', 'processing', 'qip', 'tasks', 'the', 'basic', 'ideas', 'of', 'nmr', 'qip', 'are', 'detailed', 'examining', 'the', 'successes', 'and', 'limitat... | [-0.12887551868334413, 0.1788963533804885, -0.05455312719901225, -0.02469320096341627, -0.07777463654721421, -0.19181567901146732, 0.0007303694209050653, 0.3785106493825359, -0.2396172416130347, -0.3067551831398824, 0.1134262868602361, -0.29620872072077226, -0.09805675755654063, 0.2737292465920161, 0.025308480532008355... |
710.1448 | Operational axioms for C*-algebra representation of transformations | It is shown how a C*-algebra representation of the transformations of a
physical system can be derived from two operational postulates: 1) the
existence of dynamically independent systems}; 2) the existence of symmetric
faithful states. Both notions are crucial for the possibility of performing
experiments on the sys... | quant-ph | it is shown how a calgebra representation of the transformations of a physical system can be derived from two operational postulates 1 the existence of dynamically independent systems 2 the existence of symmetric faithful states both notions are crucial for the possibility of performing experiments on the system in pre... | [['it', 'is', 'shown', 'how', 'a', 'calgebra', 'representation', 'of', 'the', 'transformations', 'of', 'a', 'physical', 'system', 'can', 'be', 'derived', 'from', 'two', 'operational', 'postulates', '1', 'the', 'existence', 'of', 'dynamically', 'independent', 'systems', '2', 'the', 'existence', 'of', 'symmetric', 'faith... | [-0.15061478307205428, 0.1595790078038279, -0.1295111237235273, 0.056691060796132474, -0.02792583548027692, -0.18320909117148082, 0.01516917665913418, 0.3310349643984927, -0.2743025151894817, -0.2709286763462462, 0.1034536291226226, -0.24990113856435953, -0.13577321854337485, 0.19422325910410926, -0.07079564567796792, ... |
710.1449 | Perturbing QCD with external fields | We present some up-to-date results on QCD phase transition in a
chromomagnetic constant background field and in an abelian monopole background
field. Our results indicate that the QCD critical temperature is not modified
by a monopole background field, whilst it is modified by a constant
chromomagnetic field. We impr... | hep-lat | we present some uptodate results on qcd phase transition in a chromomagnetic constant background field and in an abelian monopole background field our results indicate that the qcd critical temperature is not modified by a monopole background field whilst it is modified by a constant chromomagnetic field we improve our... | [['we', 'present', 'some', 'uptodate', 'results', 'on', 'qcd', 'phase', 'transition', 'in', 'a', 'chromomagnetic', 'constant', 'background', 'field', 'and', 'in', 'an', 'abelian', 'monopole', 'background', 'field', 'our', 'results', 'indicate', 'that', 'the', 'qcd', 'critical', 'temperature', 'is', 'not', 'modified', '... | [-0.14469717888404493, 0.23583047705608845, -0.07198660043270691, 0.06470171911844416, -0.08532617610973725, -0.047370347558804184, 0.028055568870183997, 0.37535789463183156, -0.10270226799774969, -0.26721984091336315, 0.06251332058699505, -0.2396644875407219, -0.1176175067742841, 0.14785479570644489, 0.032411236842365... |
710.145 | Prospects in the orbital and rotational dynamics of the Moon with the
advent of sub-centimeter lunar laser ranging | Lunar Laser Ranging (LLR) measurements are crucial for advanced exploration
of the laws of fundamental gravitational physics and geophysics. Current LLR
technology allows us to measure distances to the Moon with a precision
approaching 1 millimeter. As NASA pursues the vision of taking humans back to
the Moon, new, m... | gr-qc | lunar laser ranging llr measurements are crucial for advanced exploration of the laws of fundamental gravitational physics and geophysics current llr technology allows us to measure distances to the moon with a precision approaching 1 millimeter as nasa pursues the vision of taking humans back to the moon new more prec... | [['lunar', 'laser', 'ranging', 'llr', 'measurements', 'are', 'crucial', 'for', 'advanced', 'exploration', 'of', 'the', 'laws', 'of', 'fundamental', 'gravitational', 'physics', 'and', 'geophysics', 'current', 'llr', 'technology', 'allows', 'us', 'to', 'measure', 'distances', 'to', 'the', 'moon', 'with', 'a', 'precision'... | [-0.08460620171189519, 0.1321198035836301, -0.10027698860023289, 0.0456130533051374, -0.11956621250987703, -0.09529664853794707, 0.0493353028769701, 0.3007070390814324, -0.2618882149164121, -0.3550853576614625, 0.11264184571059775, -0.25709031581780956, -0.13685884669844417, 0.2570707233436036, -0.0817001098766923, 0.0... |
710.1451 | On some properties on bivariate Fibonacci and Lucas polynomials | In this paper we generalize to bivariate polynomials of Fibonacci and Lucas,
properties obtained for Chebyshev polynomials. We prove that the coordinates of
the bivariate polynomials over appropriate basis are families of integers
satisfying remarkable recurrence relations.
| math.NT | in this paper we generalize to bivariate polynomials of fibonacci and lucas properties obtained for chebyshev polynomials we prove that the coordinates of the bivariate polynomials over appropriate basis are families of integers satisfying remarkable recurrence relations | [['in', 'this', 'paper', 'we', 'generalize', 'to', 'bivariate', 'polynomials', 'of', 'fibonacci', 'and', 'lucas', 'properties', 'obtained', 'for', 'chebyshev', 'polynomials', 'we', 'prove', 'that', 'the', 'coordinates', 'of', 'the', 'bivariate', 'polynomials', 'over', 'appropriate', 'basis', 'are', 'families', 'of', 'i... | [-0.23722438823834463, 0.06256023006564057, -0.11352060866114255, 0.09516799114833309, -0.1000401907273241, -0.11196150011508851, -0.0020445242140291107, 0.3278630927356111, -0.359218335483928, -0.15182118273868755, 0.036541938457663195, -0.2614274990518351, -0.21883406454848275, 0.21781458947304133, -0.110699523341011... |
710.1452 | The metal-insulator transition and its relation to magnetic structure in
(LaMnO3)2n/(SrMnO3)n superlattices | Superlattices of (LaMnO3)2n/(SrMnO3)n (n=1 to 5), composed of the insulators
LaMnO3 and SrMnO3, undergo a metal-insulator transition as a function of n,
being metallic for n<=2 and insulating for n>=3. Measurements of transport,
magnetization and polarized neutron reflectivity reveal that the ferromagnetism
is relati... | cond-mat.str-el cond-mat.mtrl-sci | superlattices of lamno32nsrmno3n n1 to 5 composed of the insulators lamno3 and srmno3 undergo a metalinsulator transition as a function of n being metallic for n2 and insulating for n3 measurements of transport magnetization and polarized neutron reflectivity reveal that the ferromagnetism is relatively uniform in the ... | [['superlattices', 'of', 'lamno32nsrmno3n', 'n1', 'to', '5', 'composed', 'of', 'the', 'insulators', 'lamno3', 'and', 'srmno3', 'undergo', 'a', 'metalinsulator', 'transition', 'as', 'a', 'function', 'of', 'n', 'being', 'metallic', 'for', 'n2', 'and', 'insulating', 'for', 'n3', 'measurements', 'of', 'transport', 'magneti... | [-0.1953166380968122, 0.2935424693372278, -0.0024260083590412424, 0.022474901909230367, 0.03783833603152917, -0.1980523877244975, 0.09943837268011911, 0.4040900742014249, -0.23628144948965027, -0.27015194190621733, 0.03672746805740254, -0.38417067918039505, -0.12861228149517306, 0.12364125682839326, 0.04633077447346988... |
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