id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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708.0149 | Modeling the spectral energy distribution of ULIRGs I: the radio spectra | As a constraint for new starburst/AGN models of IRAS bright galaxies we
determine the radio spectra of 31 luminous and ultraluminous IRAS galaxies
(LIRGs/ULIRGs). We construct the radio spectra using both new and archival
data. From our sample of radio spectra we find that very few have a straight
power-law slope. Al... | astro-ph | as a constraint for new starburstagn models of iras bright galaxies we determine the radio spectra of 31 luminous and ultraluminous iras galaxies lirgsulirgs we construct the radio spectra using both new and archival data from our sample of radio spectra we find that very few have a straight powerlaw slope although som... | [['as', 'a', 'constraint', 'for', 'new', 'starburstagn', 'models', 'of', 'iras', 'bright', 'galaxies', 'we', 'determine', 'the', 'radio', 'spectra', 'of', '31', 'luminous', 'and', 'ultraluminous', 'iras', 'galaxies', 'lirgsulirgs', 'we', 'construct', 'the', 'radio', 'spectra', 'using', 'both', 'new', 'and', 'archival',... | [-0.05945422489519657, 0.11292002794630747, -0.03396778577875535, 0.09425021239509017, -0.07919771707364184, -0.08550513477964422, 0.05483903340063989, 0.5113691571405379, -0.12355092646656715, -0.32011984917532527, 0.06092723880626135, -0.32031046972941546, -0.011940435167023186, 0.1942065334682411, 0.0023798775776305... |
708.015 | Range-based attacks on links in random scale-free networks | $Range$ and $load$ play keys on the problem of attacking on links in random
scale-free (RSF) networks. In this Brief Report we obtain the relation between
$range$ and $load$ in RSF networks analytically by the generating function
theory, and then give an estimation about the impact of attacks on the
$efficiency$ of t... | cond-mat.stat-mech | range and load play keys on the problem of attacking on links in random scalefree rsf networks in this brief report we obtain the relation between range and load in rsf networks analytically by the generating function theory and then give an estimation about the impact of attacks on the efficiency of the network the an... | [['range', 'and', 'load', 'play', 'keys', 'on', 'the', 'problem', 'of', 'attacking', 'on', 'links', 'in', 'random', 'scalefree', 'rsf', 'networks', 'in', 'this', 'brief', 'report', 'we', 'obtain', 'the', 'relation', 'between', 'range', 'and', 'load', 'in', 'rsf', 'networks', 'analytically', 'by', 'the', 'generating', '... | [-0.1458189867120128, 0.05051849328328688, -0.04350085109255688, 0.07495662772237476, -0.016558337247007268, -0.11729392748282746, 0.1087862741632582, 0.4034597308504893, -0.1913239032024691, -0.320364756552979, 0.0782286167336996, -0.25961255775304337, -0.23573832231205563, 0.2465826777611361, -0.07375232982557527, 0.... |
708.0151 | Nonisomorphic Verdier octahedra on the same base | We show by an example that in a Verdier triangulated category, there may
exist two mutually nonisomorphic Verdier octahedra containing the same
commutative triangle.
| math.KT | we show by an example that in a verdier triangulated category there may exist two mutually nonisomorphic verdier octahedra containing the same commutative triangle | [['we', 'show', 'by', 'an', 'example', 'that', 'in', 'a', 'verdier', 'triangulated', 'category', 'there', 'may', 'exist', 'two', 'mutually', 'nonisomorphic', 'verdier', 'octahedra', 'containing', 'the', 'same', 'commutative', 'triangle']] | [-0.2453696057976534, 0.10973653774090053, -0.0053162606588254375, 0.09728079211587708, -0.04082387725550992, -0.2142675772580939, -0.09621853940188885, 0.4704752955585718, -0.4152338003429274, -0.14152264141011983, 0.02218022072823563, -0.2952741168749829, -0.17849609806823233, 0.14665153358752528, -0.2502720374225949... |
708.0152 | Non-standard neutrino interactions in reactor and superbeam experiments | The formalism of non-standard four-fermion interactions provides a
convenient, model-independent way of parameterizing a wide class of ``new
physics'' scenarios. In this article, we study the performance of reactor and
superbeam neutrino experiments in the presence of such non-standard
interactions (NSI). Due to inte... | hep-ph hep-ex | the formalism of nonstandard fourfermion interactions provides a convenient modelindependent way of parameterizing a wide class of new physics scenarios in this article we study the performance of reactor and superbeam neutrino experiments in the presence of such nonstandard interactions nsi due to interference between... | [['the', 'formalism', 'of', 'nonstandard', 'fourfermion', 'interactions', 'provides', 'a', 'convenient', 'modelindependent', 'way', 'of', 'parameterizing', 'a', 'wide', 'class', 'of', 'new', 'physics', 'scenarios', 'in', 'this', 'article', 'we', 'study', 'the', 'performance', 'of', 'reactor', 'and', 'superbeam', 'neutr... | [-0.09737374013236079, 0.16812840374365737, -0.04974182296002534, 0.1280665261764975, -0.10295247219753667, -0.12896645184821234, 0.08678210738401573, 0.3384909554241368, -0.25471486802875565, -0.31180171290269265, 0.09905174933597803, -0.28751340727142705, -0.14314380605355836, 0.24079861199066865, -0.0325035726827851... |
708.0153 | The entropy of randomized network ensembles | Randomized network ensembles are the null models of real networks and are
extensivelly used to compare a real system to a null hypothesis. In this paper
we study network ensembles with the same degree distribution, the same
degree-correlations or the same community structure of any given real network.
We characterize... | cond-mat.dis-nn cond-mat.stat-mech | randomized network ensembles are the null models of real networks and are extensivelly used to compare a real system to a null hypothesis in this paper we study network ensembles with the same degree distribution the same degreecorrelations or the same community structure of any given real network we characterize these... | [['randomized', 'network', 'ensembles', 'are', 'the', 'null', 'models', 'of', 'real', 'networks', 'and', 'are', 'extensivelly', 'used', 'to', 'compare', 'a', 'real', 'system', 'to', 'a', 'null', 'hypothesis', 'in', 'this', 'paper', 'we', 'study', 'network', 'ensembles', 'with', 'the', 'same', 'degree', 'distribution', ... | [-0.1384043270300557, 0.10411616139902893, -0.05677607560013659, 0.06668426982470428, 0.038136706774184195, -0.11160603235475719, 0.029738518989808095, 0.3956438983335112, -0.24270205004616593, -0.2947337895658982, 0.054943868741699, -0.283167505174549, -0.20132911232526135, 0.11682939371535976, -0.022233692166925726, ... |
708.0154 | Upper limit on the transition temperature for non-ideal Bose gases | In this paper we show that for a non-ideal Bose gas there exists an upper
limit on the transition temperature above which Bose-Einstein condensation
cannot occur regardless of the pressure applied. Such upper limits for some
realistic Bose gases are estimated. This result implies that there may also
exist an upper li... | cond-mat.stat-mech cond-mat.supr-con | in this paper we show that for a nonideal bose gas there exists an upper limit on the transition temperature above which boseeinstein condensation cannot occur regardless of the pressure applied such upper limits for some realistic bose gases are estimated this result implies that there may also exist an upper limit on... | [['in', 'this', 'paper', 'we', 'show', 'that', 'for', 'a', 'nonideal', 'bose', 'gas', 'there', 'exists', 'an', 'upper', 'limit', 'on', 'the', 'transition', 'temperature', 'above', 'which', 'boseeinstein', 'condensation', 'can', 'not', 'occur', 'regardless', 'of', 'the', 'pressure', 'applied', 'such', 'upper', 'limits',... | [-0.1637485730471642, 0.2416718744291032, -0.03879710366570596, 0.06645202281158734, 0.04110576935365039, -0.11831883431838477, 0.1159846890832187, 0.3443388736696314, -0.15307627552015296, -0.2433938639143766, 0.09186519935561376, -0.26440047775789843, -0.09699569518630535, 0.24538633480699637, -0.002749892306845572, ... |
708.0155 | Is D_s(2700) a charmed tetraquark state ? | In this article, we take the point of view that the $D_s(2700)$ be a
tetraquark state, which consists of a scalar diquark and a vector antidiquark,
and calculate its mass with the QCD sum rules. The numerical result indicates
that the mass of the vector charmed tetraquark state is about
$M_V=(3.75\pm0.18)\rm{GeV}$ or... | hep-ph | in this article we take the point of view that the d_s2700 be a tetraquark state which consists of a scalar diquark and a vector antidiquark and calculate its mass with the qcd sum rules the numerical result indicates that the mass of the vector charmed tetraquark state is about m_v375pm018rmgev or m_v371pm015rmgev fro... | [['in', 'this', 'article', 'we', 'take', 'the', 'point', 'of', 'view', 'that', 'the', 'd_s2700', 'be', 'a', 'tetraquark', 'state', 'which', 'consists', 'of', 'a', 'scalar', 'diquark', 'and', 'a', 'vector', 'antidiquark', 'and', 'calculate', 'its', 'mass', 'with', 'the', 'qcd', 'sum', 'rules', 'the', 'numerical', 'resul... | [-0.10129416121506235, 0.1937633309894914, -0.10630552293797438, 0.09565754520170028, -0.10759943674525453, -0.09544209910220364, 0.10586666925680926, 0.32409246935923064, -0.18604979058727622, -0.217460746909233, 0.0479852074802491, -0.28642839445253937, -0.05538267956904343, 0.07958987986138608, 0.0675216557445108, 0... |
708.0156 | Nucleosome Chiral Transition under Positive Torsional Stress in Single
Chromatin Fibers | Using magnetic tweezers to investigate the mechanical response of single
chromatin fibers, we show that fibers submitted to large positive torsion
transiently trap positive turns, at a rate of one turn per nucleosome. A
comparison with the response of fibers of tetrasomes (the (H3-H4)2 tetramer
bound with ~50 bp of D... | q-bio.BM | using magnetic tweezers to investigate the mechanical response of single chromatin fibers we show that fibers submitted to large positive torsion transiently trap positive turns at a rate of one turn per nucleosome a comparison with the response of fibers of tetrasomes the h3h42 tetramer bound with 50 bp of dna obtaine... | [['using', 'magnetic', 'tweezers', 'to', 'investigate', 'the', 'mechanical', 'response', 'of', 'single', 'chromatin', 'fibers', 'we', 'show', 'that', 'fibers', 'submitted', 'to', 'large', 'positive', 'torsion', 'transiently', 'trap', 'positive', 'turns', 'at', 'a', 'rate', 'of', 'one', 'turn', 'per', 'nucleosome', 'a',... | [-0.1643205137612919, 0.18052884717665924, -0.006660434196237475, 0.008638138106713692, 0.007576920053300758, -0.17302204711983601, 0.07092767322901636, 0.367746133202066, -0.23988526413061967, -0.2597249512776519, -0.01171188877779059, -0.26218529054070433, -0.14811469182216871, 0.15332252143416553, 0.0037976115786780... |
708.0157 | Matrix Factorizations, D-Branes and their Deformations | We review in elementary, non-technical terms the description of topological
B-type of D-branes in terms of boundary Landau-Ginzburg theory, as well as some
applications.
| hep-th | we review in elementary nontechnical terms the description of topological btype of dbranes in terms of boundary landauginzburg theory as well as some applications | [['we', 'review', 'in', 'elementary', 'nontechnical', 'terms', 'the', 'description', 'of', 'topological', 'btype', 'of', 'dbranes', 'in', 'terms', 'of', 'boundary', 'landauginzburg', 'theory', 'as', 'well', 'as', 'some', 'applications']] | [-0.1152871471325246, 0.1277385134017095, -0.03242309676716104, 0.13362025547151765, -0.09730737470090389, -0.07865170730898778, -0.02388494025702433, 0.2576174885810663, -0.18611991547125703, -0.3063449851082017, 0.0981131343190403, -0.21945935813710093, -0.2450552780671084, 0.15906246120963866, -0.2275640394849082, 0... |
708.0158 | A Compton Thick AGN Powering the Hyperluminous Infrared Galaxy IRAS
00182--7112 | We present X-ray observations of the Hyperluminous Infrared Galaxy (HLIRG)
IRAS 00182--7112 (F00183--7111) obtained using the XMM-Newton EPIC camera. A
luminous hard X-ray source co-incident with the nucleus is revealed, along with
weaker soft X-ray emission which may be extended or offset from the hard. The
EPIC spe... | astro-ph | we present xray observations of the hyperluminous infrared galaxy hlirg iras 001827112 f001837111 obtained using the xmmnewton epic camera a luminous hard xray source coincident with the nucleus is revealed along with weaker soft xray emission which may be extended or offset from the hard the epic spectrum is extremely... | [['we', 'present', 'xray', 'observations', 'of', 'the', 'hyperluminous', 'infrared', 'galaxy', 'hlirg', 'iras', '001827112', 'f001837111', 'obtained', 'using', 'the', 'xmmnewton', 'epic', 'camera', 'a', 'luminous', 'hard', 'xray', 'source', 'coincident', 'with', 'the', 'nucleus', 'is', 'revealed', 'along', 'with', 'wea... | [-0.022085506871492418, 0.1037932289279465, -0.04752490027625132, 0.125895398358894, -0.11810293300872922, -0.1224610130302608, -0.007439474017129996, 0.5328636079764546, -0.16604621215412235, -0.29678044613186344, 0.06464350388160715, -0.3387374780491818, 0.005970547217922519, 0.16786921993712237, -0.02185230593819489... |
708.0159 | Possible Way to Synthesize Superheavy Element Z=117 | Within the framework of the dinuclear system model, the production of
superheavy element Z=117 in possible projectile-target combinations is analyzed
systematically. The calculated results show that the production cross sections
are strongly dependent on the reaction systems. Optimal combinations,
corresponding excit... | nucl-th | within the framework of the dinuclear system model the production of superheavy element z117 in possible projectiletarget combinations is analyzed systematically the calculated results show that the production cross sections are strongly dependent on the reaction systems optimal combinations corresponding excitation en... | [['within', 'the', 'framework', 'of', 'the', 'dinuclear', 'system', 'model', 'the', 'production', 'of', 'superheavy', 'element', 'z117', 'in', 'possible', 'projectiletarget', 'combinations', 'is', 'analyzed', 'systematically', 'the', 'calculated', 'results', 'show', 'that', 'the', 'production', 'cross', 'sections', 'ar... | [-0.08333488891060513, 0.20542200036365293, -0.020103993326636937, 0.07899001059367468, 0.1406005388615947, -0.12136115418060829, 0.024972356353445274, 0.345361738147116, -0.229944888532995, -0.24345168353695618, -0.04806007871612612, -0.33856194615854246, -0.06528381220261126, 0.12074858099405997, 0.08879377754515429,... |
708.016 | Colliding neutrino beams | From several neutrino oscillation experiments, we understand now that
neutrinos have mass. However, we really don't know what mechanism is
responsible for producing this neutrino mass. Current or planned neutrino
experiments utilize neutrino beams and long-baseline detectors to explore
flavor mixing but do not addres... | hep-ex | from several neutrino oscillation experiments we understand now that neutrinos have mass however we really dont know what mechanism is responsible for producing this neutrino mass current or planned neutrino experiments utilize neutrino beams and longbaseline detectors to explore flavor mixing but do not address the qu... | [['from', 'several', 'neutrino', 'oscillation', 'experiments', 'we', 'understand', 'now', 'that', 'neutrinos', 'have', 'mass', 'however', 'we', 'really', 'dont', 'know', 'what', 'mechanism', 'is', 'responsible', 'for', 'producing', 'this', 'neutrino', 'mass', 'current', 'or', 'planned', 'neutrino', 'experiments', 'util... | [-0.06600102040987543, 0.28954444834760024, -0.0020576235952118977, 0.25373617320134223, -0.1119577901073448, -0.14663781398785827, 0.04760917456461238, 0.39077325317117834, -0.22658146930473816, -0.3472301755910334, 0.048647834525858656, -0.2965948286810485, -0.05679351884021383, 0.1924175281247185, 0.0488051668254901... |
708.0161 | Entanglement entropy in quantum spin chains with finite range
interaction | We study the entropy of entanglement of the ground state in a wide family of
one-dimensional quantum spin chains whose interaction is of finite range and
translation invariant. Such systems can be thought of as generalizations of the
XY model. The chain is divided in two parts: one containing the first
consecutive L ... | math-ph math.MP quant-ph | we study the entropy of entanglement of the ground state in a wide family of onedimensional quantum spin chains whose interaction is of finite range and translation invariant such systems can be thought of as generalizations of the xy model the chain is divided in two parts one containing the first consecutive l spins ... | [['we', 'study', 'the', 'entropy', 'of', 'entanglement', 'of', 'the', 'ground', 'state', 'in', 'a', 'wide', 'family', 'of', 'onedimensional', 'quantum', 'spin', 'chains', 'whose', 'interaction', 'is', 'of', 'finite', 'range', 'and', 'translation', 'invariant', 'such', 'systems', 'can', 'be', 'thought', 'of', 'as', 'gen... | [-0.16439919582387405, 0.12095044555846371, -0.047849533838493316, 0.05215480804804768, 0.0016737304971349513, -0.1540483250305872, 0.021939348048340548, 0.28569969533831435, -0.28572126217875676, -0.23236369390726386, 0.13022641590576323, -0.3266693391809379, -0.10882996057452106, 0.18222335097843326, -0.0379105731078... |
708.0162 | Implication of the proton electric FF space-like behavior puzzle in
various physical phenomena | By means of the 10-resonance unitary and analytic model of nucleon
electromagnetic structure it is demonstrated that the JLab proton polarization
data on the ratio $\mu_p G_{Ep}(Q^2)/G_{Mp}(Q^2)$ are consistent with all form
factor properties, however, they strongly require an existence of the zero in
G_{Ep}(Q^2) aro... | hep-ph | by means of the 10resonance unitary and analytic model of nucleon electromagnetic structure it is demonstrated that the jlab proton polarization data on the ratio mu_p g_epq2g_mpq2 are consistent with all form factor properties however they strongly require an existence of the zero in g_epq2 around q213 gev2 as a resul... | [['by', 'means', 'of', 'the', '10resonance', 'unitary', 'and', 'analytic', 'model', 'of', 'nucleon', 'electromagnetic', 'structure', 'it', 'is', 'demonstrated', 'that', 'the', 'jlab', 'proton', 'polarization', 'data', 'on', 'the', 'ratio', 'mu_p', 'g_epq2g_mpq2', 'are', 'consistent', 'with', 'all', 'form', 'factor', 'p... | [-0.11625684825801474, 0.18145411009891627, -0.09799038854630499, 0.09976390925798528, -0.033951994797012004, -0.027611617352767376, 0.05765006496653993, 0.35675544533325304, -0.1926649374758253, -0.22372582699587146, -0.005597987721701807, -0.3026302784570668, -0.09450147673948714, 0.16480790408694712, 0.0664654259594... |
708.0163 | Vacuum Energy Density in the Quantum Yang - Mills Theory | Using the effective potential approach for composite operators, we have
formulated a general method of calculation of the truly non-perturbative
Yang-Mills vacuum energy density (this is, by definition, the Bag constant
apart from the sign). It is the main dynamical characteristic of the QCD ground
state. Our method ... | hep-ph hep-th | using the effective potential approach for composite operators we have formulated a general method of calculation of the truly nonperturbative yangmills vacuum energy density this is by definition the bag constant apart from the sign it is the main dynamical characteristic of the qcd ground state our method allows one ... | [['using', 'the', 'effective', 'potential', 'approach', 'for', 'composite', 'operators', 'we', 'have', 'formulated', 'a', 'general', 'method', 'of', 'calculation', 'of', 'the', 'truly', 'nonperturbative', 'yangmills', 'vacuum', 'energy', 'density', 'this', 'is', 'by', 'definition', 'the', 'bag', 'constant', 'apart', 'f... | [-0.06768284931756054, 0.1493668858351313, -0.12037545066873938, 0.08786401834318906, -0.09541729327571219, -0.11889683349026607, 0.0491375887950031, 0.3345204336351595, -0.2390726416777431, -0.29198193883214807, 0.04941771332277385, -0.2556758086309387, -0.10562352171064886, 0.13553674829312445, 0.031279374982453194, ... |
708.0164 | Biologically Inspired Nanomaterials: A Conference Report | The understanding of the nanoscale physical properties of biomolecules and
biomaterials will ultimately promote the research in the biological sciences.
In this review, we focused on theory, simulation, and experiments involving
nanoscale materials inspired by biological systems. Specifically, self-assembly
in living... | physics.bio-ph physics.soc-ph | the understanding of the nanoscale physical properties of biomolecules and biomaterials will ultimately promote the research in the biological sciences in this review we focused on theory simulation and experiments involving nanoscale materials inspired by biological systems specifically selfassembly in living and synt... | [['the', 'understanding', 'of', 'the', 'nanoscale', 'physical', 'properties', 'of', 'biomolecules', 'and', 'biomaterials', 'will', 'ultimately', 'promote', 'the', 'research', 'in', 'the', 'biological', 'sciences', 'in', 'this', 'review', 'we', 'focused', 'on', 'theory', 'simulation', 'and', 'experiments', 'involving', ... | [-0.05354695872153604, 0.1905043079448795, -0.027355210734876217, 0.014104681492662403, -0.05586920745877756, -0.12452402621932344, -0.004080338207401197, 0.39892178025372604, -0.24804042372852564, -0.28527631010446286, 0.08250092981702269, -0.2729352438494701, -0.339530609479105, 0.2665473912601118, -0.037915958091616... |
708.0165 | Robust estimates in generalized partially linear models | In this paper, we introduce a family of robust estimates for the parametric
and nonparametric components under a generalized partially linear model, where
the data are modeled by $y_i|(\mathbf{x}_i,t_i)\sim F(\cdot,\mu_i)$ with
$\mu_i=H(\eta(t_i)+\mathbf{x}_i^{$\mathrm{T}$}\beta)$, for some known
distribution functio... | stat.ME | in this paper we introduce a family of robust estimates for the parametric and nonparametric components under a generalized partially linear model where the data are modeled by y_imathbfx_it_isim fcdotmu_i with mu_ihetat_imathbfx_imathrmtbeta for some known distribution function f and link function h it is shown that t... | [['in', 'this', 'paper', 'we', 'introduce', 'a', 'family', 'of', 'robust', 'estimates', 'for', 'the', 'parametric', 'and', 'nonparametric', 'components', 'under', 'a', 'generalized', 'partially', 'linear', 'model', 'where', 'the', 'data', 'are', 'modeled', 'by', 'y_imathbfx_it_isim', 'fcdotmu_i', 'with', 'mu_ihetat_ima... | [-0.05863996252620881, 0.0912024117088024, -0.08760865327810317, 0.08285853792224604, -0.018200729429249614, -0.14433323923157346, 0.03294922305356291, 0.40030603871588977, -0.2579243401701654, -0.26791477097119665, 0.14497644338153406, -0.27265398620142484, -0.170068300342266, 0.23207258521316862, -0.05873815260145446... |
708.0166 | Common origin of \theta_{13} and \Delta m^2_{12} in a model of neutrino
mass with quaternion symmetry | The smallness of the 1-3 lepton mixing angle $\theta_{13}$ and of the
neutrino mass-squared-difference ratio $\Delta m^2_{12}/\Delta m^2_{23}$ can be
understood as the departure from a common limit where they both vanish. We
discuss in general the conditions for realizing the mass degeneracy of a pair
of neutrinos an... | hep-ph hep-ex | the smallness of the 13 lepton mixing angle theta_13 and of the neutrino masssquareddifference ratio delta m2_12delta m2_23 can be understood as the departure from a common limit where they both vanish we discuss in general the conditions for realizing the mass degeneracy of a pair of neutrinos and show that the vanish... | [['the', 'smallness', 'of', 'the', '13', 'lepton', 'mixing', 'angle', 'theta_13', 'and', 'of', 'the', 'neutrino', 'masssquareddifference', 'ratio', 'delta', 'm2_12delta', 'm2_23', 'can', 'be', 'understood', 'as', 'the', 'departure', 'from', 'a', 'common', 'limit', 'where', 'they', 'both', 'vanish', 'we', 'discuss', 'in... | [-0.16028212305359743, 0.25806194051328274, -0.008102011371840228, 0.12155936712499808, -0.06565841888539023, -0.1280256491322238, 0.07422951614769462, 0.2935370877720751, -0.2630500968562456, -0.29768962056485115, 0.08842904813092638, -0.285865576631549, -0.08288541968139979, 0.13453359079813618, 0.002030243132229861,... |
708.0167 | On the limiting distributions of multivariate depth-based rank sum
statistics and related tests | A depth-based rank sum statistic for multivariate data introduced by Liu and
Singh [J. Amer. Statist. Assoc. 88 (1993) 252--260] as an extension of the
Wilcoxon rank sum statistic for univariate data has been used in multivariate
rank tests in quality control and in experimental studies. Those applications,
however, ... | math.ST stat.TH | a depthbased rank sum statistic for multivariate data introduced by liu and singh j amer statist assoc 88 1993 252260 as an extension of the wilcoxon rank sum statistic for univariate data has been used in multivariate rank tests in quality control and in experimental studies those applications however are based on a c... | [['a', 'depthbased', 'rank', 'sum', 'statistic', 'for', 'multivariate', 'data', 'introduced', 'by', 'liu', 'and', 'singh', 'j', 'amer', 'statist', 'assoc', '88', '1993', '252260', 'as', 'an', 'extension', 'of', 'the', 'wilcoxon', 'rank', 'sum', 'statistic', 'for', 'univariate', 'data', 'has', 'been', 'used', 'in', 'mul... | [-0.008520283042607168, -0.03125712880467869, -0.08706403364358116, 0.09757852692865143, -0.04444063294963711, -0.16489609846583575, 0.03868703762923698, 0.31916909253855874, -0.16211688807926888, -0.30879996000396565, 0.13356025675735014, -0.23092706310793695, -0.15877205175578532, 0.22048088363256335, -0.173339725185... |
708.0168 | Topological Free Entropy Dimension in Unital C^* algebras (II) :
Orthogonal Sum of Unital C^*-algebras | In the paper, we obtain a formula for topological free entropy dimension in
the orthogonal sum (or direct sum) of unital C^* algebras. As a corollary, we
compute the topological free entropy dimension of any family of self-adjoint
generators of a finite dimensional C^* algebra.
| math.OA | in the paper we obtain a formula for topological free entropy dimension in the orthogonal sum or direct sum of unital c algebras as a corollary we compute the topological free entropy dimension of any family of selfadjoint generators of a finite dimensional c algebra | [['in', 'the', 'paper', 'we', 'obtain', 'a', 'formula', 'for', 'topological', 'free', 'entropy', 'dimension', 'in', 'the', 'orthogonal', 'sum', 'or', 'direct', 'sum', 'of', 'unital', 'c', 'algebras', 'as', 'a', 'corollary', 'we', 'compute', 'the', 'topological', 'free', 'entropy', 'dimension', 'of', 'any', 'family', 'o... | [-0.18607067233986324, 0.14784098863601686, -0.04009564347151253, 0.010998225212097168, -0.072515168103079, -0.16390437099875677, 0.023579699134764574, 0.29268213394615383, -0.3286442653586467, -0.13557484969496728, 0.07829020738912125, -0.27864233400258753, -0.09347771650904582, 0.17002734210238687, -0.093862008986373... |
708.0169 | Data-driven goodness-of-fit tests | We propose and study a general method for construction of consistent
statistical tests on the basis of possibly indirect, corrupted, or partially
available observations. The class of tests devised in the paper contains
Neyman's smooth tests, data-driven score tests, and some types of multi-sample
tests as basic examp... | math.ST math.PR stat.ME stat.TH | we propose and study a general method for construction of consistent statistical tests on the basis of possibly indirect corrupted or partially available observations the class of tests devised in the paper contains neymans smooth tests datadriven score tests and some types of multisample tests as basic examples our te... | [['we', 'propose', 'and', 'study', 'a', 'general', 'method', 'for', 'construction', 'of', 'consistent', 'statistical', 'tests', 'on', 'the', 'basis', 'of', 'possibly', 'indirect', 'corrupted', 'or', 'partially', 'available', 'observations', 'the', 'class', 'of', 'tests', 'devised', 'in', 'the', 'paper', 'contains', 'ne... | [-0.040375853200197404, 0.0006007112758526967, -0.12100965739156411, 0.11340919879773644, -0.09533192804711728, -0.17012283566516417, 0.0988722768986449, 0.35922022726089675, -0.22517880132176166, -0.30419491563403717, 0.15641943667086836, -0.20316106371127676, -0.14478761833189685, 0.25253923331955846, -0.075265470846... |
708.017 | On the radar method in general-relativistic spacetimes | If a clock, mathematically modeled by a parametrized timelike curve in a
general-relativistic spacetime, is given, the radar method assigns a time and a
distance to every event which is sufficiently close to the clock. Several
geometric aspects of this method are reviewed and their physical interpretation
is discusse... | gr-qc | if a clock mathematically modeled by a parametrized timelike curve in a generalrelativistic spacetime is given the radar method assigns a time and a distance to every event which is sufficiently close to the clock several geometric aspects of this method are reviewed and their physical interpretation is discussed | [['if', 'a', 'clock', 'mathematically', 'modeled', 'by', 'a', 'parametrized', 'timelike', 'curve', 'in', 'a', 'generalrelativistic', 'spacetime', 'is', 'given', 'the', 'radar', 'method', 'assigns', 'a', 'time', 'and', 'a', 'distance', 'to', 'every', 'event', 'which', 'is', 'sufficiently', 'close', 'to', 'the', 'clock',... | [-0.15853532662197034, 0.11622610429720003, -0.13966957847967895, 0.07799204783419109, -0.0698443696054877, -0.18258217656604794, 0.03759436791154499, 0.3861245031715656, -0.2431726694411161, -0.24062737142096977, 0.09878540573860234, -0.21980929889773226, -0.15839740478110556, 0.22070520690509252, -0.12328660588863553... |
708.0171 | Virtual screening with support vector machines and structure kernels | Support vector machines and kernel methods have recently gained considerable
attention in chemoinformatics. They offer generally good performance for
problems of supervised classification or regression, and provide a flexible and
computationally efficient framework to include relevant information and prior
knowledge ... | q-bio.QM cs.LG | support vector machines and kernel methods have recently gained considerable attention in chemoinformatics they offer generally good performance for problems of supervised classification or regression and provide a flexible and computationally efficient framework to include relevant information and prior knowledge abou... | [['support', 'vector', 'machines', 'and', 'kernel', 'methods', 'have', 'recently', 'gained', 'considerable', 'attention', 'in', 'chemoinformatics', 'they', 'offer', 'generally', 'good', 'performance', 'for', 'problems', 'of', 'supervised', 'classification', 'or', 'regression', 'and', 'provide', 'a', 'flexible', 'and', ... | [0.0035053804656490686, 0.01761029474058887, -0.06431817988088975, 0.08996036073658616, -0.13293952562535802, -0.1837116288583881, 0.042579861510700236, 0.4751040125886599, -0.27938349477946756, -0.30059725224971773, 0.1444056581837746, -0.2565630829551568, -0.1474663902182753, 0.21745115145187205, -0.06101500034642716... |
708.0172 | Zero-Mode Contribution in Nucleon-Delta Transition | We investigate the transition form factors between nucleon and $\Delta$(1232)
particles by using a covariant quark-spectator-diquark field theory model in
(3+1) dimensions. Performing a light-front calculation in parallel with the
manifestly covariant calculation in light-front helicity basis, we examine the
light-fr... | hep-ph | we investigate the transition form factors between nucleon and delta1232 particles by using a covariant quarkspectatordiquark field theory model in 31 dimensions performing a lightfront calculation in parallel with the manifestly covariant calculation in lightfront helicity basis we examine the lightfront zeromode cont... | [['we', 'investigate', 'the', 'transition', 'form', 'factors', 'between', 'nucleon', 'and', 'delta1232', 'particles', 'by', 'using', 'a', 'covariant', 'quarkspectatordiquark', 'field', 'theory', 'model', 'in', '31', 'dimensions', 'performing', 'a', 'lightfront', 'calculation', 'in', 'parallel', 'with', 'the', 'manifest... | [-0.1428025504611137, 0.19460741759440492, -0.09538325547940091, 0.08070563790776457, -0.057888895605823824, -0.08342359711726506, 0.013655348344140552, 0.3291058454973002, -0.14630144178896906, -0.2236259006895125, -0.09563691427077477, -0.2547907119040333, -0.10512668638035566, 0.007451027681651924, 0.056227940570799... |
708.0173 | K-minus Estimator Approach to Large Scale Structure | Self similar 3D distributions of point-particles, with a given quasifractal
dimension D, were generated on a Menger sponge model and then compared with
\textit{2dfGRS} and \textit{Virgo project} data
\footnote{http://www.mso.anu.edu.au/2dFGRS/,
http://www.mpa-garching.mpg.de/Virgo/}. Using the principle of local know... | astro-ph | self similar 3d distributions of pointparticles with a given quasifractal dimension d were generated on a menger sponge model and then compared with textit2dfgrs and textitvirgo project data footnotehttpwwwmsoanueduau2dfgrs httpwwwmpagarchingmpgdevirgo using the principle of local knowledge it is argued that in a finit... | [['self', 'similar', '3d', 'distributions', 'of', 'pointparticles', 'with', 'a', 'given', 'quasifractal', 'dimension', 'd', 'were', 'generated', 'on', 'a', 'menger', 'sponge', 'model', 'and', 'then', 'compared', 'with', 'textit2dfgrs', 'and', 'textitvirgo', 'project', 'data', 'footnotehttpwwwmsoanueduau2dfgrs', 'httpww... | [-0.07066483619524627, 0.06297124879874734, -0.13847011830785885, 0.10825330795295143, -0.06464696684830881, -0.12137231816870904, 0.008184834714517544, 0.3714772453702508, -0.2354233818760979, -0.3260241586014355, 0.10035420523544158, -0.2801878428740273, -0.16525917955585584, 0.18550135780963192, -0.05333259920301257... |
708.0174 | HTL approach to the viscosity of quark plasma | The quark viscosity in the quark gluon plasma is evaluated in HTL
approximation. The different contributions to the viscosity arising from the
various components of the quark spectral function are discussed. The
calculation is extended to finite values of the chemical potential.
| hep-ph | the quark viscosity in the quark gluon plasma is evaluated in htl approximation the different contributions to the viscosity arising from the various components of the quark spectral function are discussed the calculation is extended to finite values of the chemical potential | [['the', 'quark', 'viscosity', 'in', 'the', 'quark', 'gluon', 'plasma', 'is', 'evaluated', 'in', 'htl', 'approximation', 'the', 'different', 'contributions', 'to', 'the', 'viscosity', 'arising', 'from', 'the', 'various', 'components', 'of', 'the', 'quark', 'spectral', 'function', 'are', 'discussed', 'the', 'calculation... | [-0.06068972768151157, 0.236173961710717, -0.15032082062125915, 0.08850801501622689, -0.028437603265047073, -0.013123969214835338, 0.019465475077075616, 0.30067296964781626, -0.24470182965021758, -0.20780100469433127, 0.01448468812408724, -0.2803866824002138, 0.020981491255086093, 0.0924266674999325, 0.0469123363672267... |
708.0175 | Convergence rates for Bayesian density estimation of
infinite-dimensional exponential families | We study the rate of convergence of posterior distributions in density
estimation problems for log-densities in periodic Sobolev classes characterized
by a smoothness parameter p. The posterior expected density provides a
nonparametric estimation procedure attaining the optimal minimax rate of
convergence under Helli... | math.ST stat.TH | we study the rate of convergence of posterior distributions in density estimation problems for logdensities in periodic sobolev classes characterized by a smoothness parameter p the posterior expected density provides a nonparametric estimation procedure attaining the optimal minimax rate of convergence under hellinger... | [['we', 'study', 'the', 'rate', 'of', 'convergence', 'of', 'posterior', 'distributions', 'in', 'density', 'estimation', 'problems', 'for', 'logdensities', 'in', 'periodic', 'sobolev', 'classes', 'characterized', 'by', 'a', 'smoothness', 'parameter', 'p', 'the', 'posterior', 'expected', 'density', 'provides', 'a', 'nonp... | [-0.09098744779019742, 0.09312579146833348, -0.12157258958480245, 0.07133676635692954, -0.048511312577269365, -0.09696779779183703, 0.10468479482066893, 0.38232577958622493, -0.3036843976962405, -0.24272016386023243, 0.11124399850849767, -0.22115346126862476, -0.0777049612958689, 0.16684922273900057, -0.106825831879836... |
708.0176 | Extreme statistics of complex random and quantum chaotic states | An exact analytical description of extreme intensity statistics in complex
random states is derived. These states have the statistical properties of the
Gaussian and Circular Unitary Ensemble eigenstates of random matrix theory.
Although the components are correlated by the normalization constraint, it is
still possi... | quant-ph cond-mat.stat-mech nlin.CD | an exact analytical description of extreme intensity statistics in complex random states is derived these states have the statistical properties of the gaussian and circular unitary ensemble eigenstates of random matrix theory although the components are correlated by the normalization constraint it is still possible t... | [['an', 'exact', 'analytical', 'description', 'of', 'extreme', 'intensity', 'statistics', 'in', 'complex', 'random', 'states', 'is', 'derived', 'these', 'states', 'have', 'the', 'statistical', 'properties', 'of', 'the', 'gaussian', 'and', 'circular', 'unitary', 'ensemble', 'eigenstates', 'of', 'random', 'matrix', 'theo... | [-0.08113954660702284, 0.1842136115999419, -0.10900976261638892, 0.11403385725447802, -0.004943725921789079, -0.16092477222086815, 0.019260787463754536, 0.3465139794454917, -0.26643995848688773, -0.26262156014156535, 0.09452736087340285, -0.2894740880928873, -0.13999553728371678, 0.17810619604486094, -0.044277872519219... |
708.0177 | Asymptotically minimax Bayes predictive densities | Given a random sample from a distribution with density function that depends
on an unknown parameter $\theta$, we are interested in accurately estimating
the true parametric density function at a future observation from the same
distribution. The asymptotic risk of Bayes predictive density estimates with
Kullback--Le... | math.ST stat.TH | given a random sample from a distribution with density function that depends on an unknown parameter theta we are interested in accurately estimating the true parametric density function at a future observation from the same distribution the asymptotic risk of bayes predictive density estimates with kullbackleibler los... | [['given', 'a', 'random', 'sample', 'from', 'a', 'distribution', 'with', 'density', 'function', 'that', 'depends', 'on', 'an', 'unknown', 'parameter', 'theta', 'we', 'are', 'interested', 'in', 'accurately', 'estimating', 'the', 'true', 'parametric', 'density', 'function', 'at', 'a', 'future', 'observation', 'from', 'th... | [-0.03598353672151481, 0.04915581495906005, -0.13082594236182252, 0.14115729293255747, -0.08154709899057057, -0.14094024545166398, 0.06724158690113874, 0.3767162273726324, -0.25602250028891066, -0.2763522893214177, 0.11558254364215986, -0.26733685174725785, -0.11635737366512092, 0.14655795406013128, -0.1258044080319304... |
708.0178 | Theoretical gravitational lensing. Beyond the weak-field small-angle
approximation | An overview is given on those theoretical gravitational lensing results that
can be formulated in a spacetime setting, without assuming that the
gravitational fields are weak and that the bending angles are small. The first
part is devoted to analytical methods considering spacetimes in which the
equations for light ... | gr-qc | an overview is given on those theoretical gravitational lensing results that can be formulated in a spacetime setting without assuming that the gravitational fields are weak and that the bending angles are small the first part is devoted to analytical methods considering spacetimes in which the equations for light rays... | [['an', 'overview', 'is', 'given', 'on', 'those', 'theoretical', 'gravitational', 'lensing', 'results', 'that', 'can', 'be', 'formulated', 'in', 'a', 'spacetime', 'setting', 'without', 'assuming', 'that', 'the', 'gravitational', 'fields', 'are', 'weak', 'and', 'that', 'the', 'bending', 'angles', 'are', 'small', 'the', ... | [-0.18606475676300333, 0.0713960830427252, -0.10032065874239539, 0.12737767295409724, -0.15752871810257726, -0.10688567004056976, -0.09083546572775744, 0.3394840958473437, -0.21041941611717144, -0.21245355035780983, 0.06775679351424105, -0.30821520533850966, -0.17132989896516151, 0.22559109472614877, -0.050968871656211... |
708.0179 | Crystal Structure and Physical Properties of Mg6Cu16Si7-type M6Ni16Si7,
for M = Mg, Sc, Ti, Nb, and Ta | Five compounds were investigated for magnetic character and
superconductivity, all with non-magnetic nickel and band structures containing
flat bands and steep bands. The syntheses and crystal structures, refined by
powder X-ray diffraction, are reported for M6Ni16Si7, where M = Mg, Sc, Ti, Nb,
and Ta. All compounds ... | cond-mat.supr-con cond-mat.mtrl-sci | five compounds were investigated for magnetic character and superconductivity all with nonmagnetic nickel and band structures containing flat bands and steep bands the syntheses and crystal structures refined by powder xray diffraction are reported for m6ni16si7 where m mg sc ti nb and ta all compounds form in the mg6c... | [['five', 'compounds', 'were', 'investigated', 'for', 'magnetic', 'character', 'and', 'superconductivity', 'all', 'with', 'nonmagnetic', 'nickel', 'and', 'band', 'structures', 'containing', 'flat', 'bands', 'and', 'steep', 'bands', 'the', 'syntheses', 'and', 'crystal', 'structures', 'refined', 'by', 'powder', 'xray', '... | [-0.1182017582503613, 0.22281601779395716, 0.07061707257293165, 0.010983068357454613, -0.021723804825451224, -0.21031666442286223, 0.13654825390782208, 0.4586762779019773, -0.18305786351207642, -0.3339411505160388, -0.013965566857950761, -0.4293134580552578, -0.05944629087112844, 0.1890933170588687, 0.08986596555449068... |
708.018 | A Factorization Law for Entanglement Decay | We present a simple and general factorization law for quantum systems shared
by two parties, which describes the time evolution of entanglement upon passage
of either component through an arbitrary noisy channel. The robustness of
entanglement-based quantum information processing protocols is thus easily and
fully ch... | quant-ph | we present a simple and general factorization law for quantum systems shared by two parties which describes the time evolution of entanglement upon passage of either component through an arbitrary noisy channel the robustness of entanglementbased quantum information processing protocols is thus easily and fully charact... | [['we', 'present', 'a', 'simple', 'and', 'general', 'factorization', 'law', 'for', 'quantum', 'systems', 'shared', 'by', 'two', 'parties', 'which', 'describes', 'the', 'time', 'evolution', 'of', 'entanglement', 'upon', 'passage', 'of', 'either', 'component', 'through', 'an', 'arbitrary', 'noisy', 'channel', 'the', 'rob... | [-0.1865129255503416, 0.16232338210364106, -0.11970487078651786, -0.0011153293563984335, 0.012619006959721447, -0.2572671211510897, 0.06027214678004384, 0.3605117575824261, -0.31278363917022944, -0.2653727010264993, 0.11082390679977834, -0.21870035097002982, -0.11433590571396053, 0.17996979597955942, -0.061166627239435... |
708.0181 | Post-ischaemic treatment with the cyclooxygenase-2 inhibitor nimesulide
reduces blood-brain barrier disruption and leukocyte infiltration following
transient focal cerebral ischaemia in rats | Several studies suggest that cyclooxygenase (COX)-2 plays a pivotal role in
the progression of ischaemic brain damage. In the present study, we
investigated the effects of selective inhibition of COX-2 with nimesulide (12
mg/kg) and selective inhibition of COX-1 with valeryl salicylate (VAS, 12-120
mg/kg) on prostagl... | q-bio.NC q-bio.TO | several studies suggest that cyclooxygenase cox2 plays a pivotal role in the progression of ischaemic brain damage in the present study we investigated the effects of selective inhibition of cox2 with nimesulide 12 mgkg and selective inhibition of cox1 with valeryl salicylate vas 12120 mgkg on prostaglandin e2 pge2 lev... | [['several', 'studies', 'suggest', 'that', 'cyclooxygenase', 'cox2', 'plays', 'a', 'pivotal', 'role', 'in', 'the', 'progression', 'of', 'ischaemic', 'brain', 'damage', 'in', 'the', 'present', 'study', 'we', 'investigated', 'the', 'effects', 'of', 'selective', 'inhibition', 'of', 'cox2', 'with', 'nimesulide', '12', 'mgk... | [-0.07626525720539937, 0.16128464663393705, 0.02021423904583431, 0.037601244322454125, 0.03244604712578625, -0.15837322687164612, 0.0831371380510148, 0.39471655678350914, -0.15727519919824323, -0.25096156843395917, 0.09782397678651684, -0.27558202041607155, -0.21393147057397405, 0.16351919720347155, -0.1415466203772357... |
708.0182 | Search for b--> u transitions in B- -> [K+pi-pi0]_D K- | We search for decays of a B meson into a neutral D meson and a kaon, with the
D meson decaying into K+pi-pi0. This final state can be reached through the b
--> c transition B- -> D0K- followed by the doubly Cabibbo-suppressed D0 -->
K+pi-pi0, or the b --> u transition B- --> D0bar K- followed by the
Cabibbo-favored D... | hep-ex | we search for decays of a b meson into a neutral d meson and a kaon with the d meson decaying into kpipi0 this final state can be reached through the b c transition b d0k followed by the doubly cabibbosuppressed d0 kpipi0 or the b u transition b d0bar k followed by the cabibbofavored d0bar k pipi 0 the interference of ... | [['we', 'search', 'for', 'decays', 'of', 'a', 'b', 'meson', 'into', 'a', 'neutral', 'd', 'meson', 'and', 'a', 'kaon', 'with', 'the', 'd', 'meson', 'decaying', 'into', 'kpipi0', 'this', 'final', 'state', 'can', 'be', 'reached', 'through', 'the', 'b', 'c', 'transition', 'b', 'd0k', 'followed', 'by', 'the', 'doubly', 'cab... | [-0.12972029250979955, 0.23968986758762703, -0.06306775367619204, 0.06307530890917405, -0.01641695259271988, -0.1940454622032121, 0.24956451493074253, 0.26216738948132845, -0.1790188629512808, -0.22694200442305634, -0.06804666618949601, -0.4225872837007046, 0.04613978594508288, 0.06987397025971274, 0.13814000845554153,... |
708.0183 | First-principles thermal equation of state and thermoelasticity for hcp
Fe under high pressures | We investigate the equation of state and elastic properties of nonmagnetic
hcp iron at high pressures and high temperatures using the first principles
linear response linear-muffin-tin-orbital method in the generalized-gradient
approximation. We calculate the Helmholtz free energy as a function of volume,
temperature... | cond-mat.other | we investigate the equation of state and elastic properties of nonmagnetic hcp iron at high pressures and high temperatures using the first principles linear response linearmuffintinorbital method in the generalizedgradient approximation we calculate the helmholtz free energy as a function of volume temperature and vol... | [['we', 'investigate', 'the', 'equation', 'of', 'state', 'and', 'elastic', 'properties', 'of', 'nonmagnetic', 'hcp', 'iron', 'at', 'high', 'pressures', 'and', 'high', 'temperatures', 'using', 'the', 'first', 'principles', 'linear', 'response', 'linearmuffintinorbital', 'method', 'in', 'the', 'generalizedgradient', 'app... | [-0.09392843169063844, 0.13058058298514064, -0.11040666584599891, -0.007974273252204574, -0.04718316696455766, -0.04540649366741679, 0.0902397411490052, 0.37548463342004806, -0.2877785724362937, -0.2669761400119851, 0.055529718093598135, -0.3567725811956515, -0.08890067591083012, 0.14929567428771406, 0.1178863131810493... |
708.0184 | Non-stationary quantum walks on the cycle | We consider quantum walks on the cycle in the non-stationary case where the
`coin' operation is allowed to change at each time step. We characterize, in
algebraic terms, the set of possible state transfers and prove that, as opposed
to the stationary case, it is possible to asymnptotically reach a uniform
distributio... | quant-ph | we consider quantum walks on the cycle in the nonstationary case where the coin operation is allowed to change at each time step we characterize in algebraic terms the set of possible state transfers and prove that as opposed to the stationary case it is possible to asymnptotically reach a uniform distribution among th... | [['we', 'consider', 'quantum', 'walks', 'on', 'the', 'cycle', 'in', 'the', 'nonstationary', 'case', 'where', 'the', 'coin', 'operation', 'is', 'allowed', 'to', 'change', 'at', 'each', 'time', 'step', 'we', 'characterize', 'in', 'algebraic', 'terms', 'the', 'set', 'of', 'possible', 'state', 'transfers', 'and', 'prove', ... | [-0.14054509406459742, 0.12640678327016788, -0.028390687737806605, 0.031974740426762606, -0.038517581034002116, -0.12423249461752331, 0.10993697209653028, 0.36367743982580203, -0.3097253440526025, -0.23910702238710405, 0.11197295915415703, -0.2626628476869443, -0.09626496536255782, 0.15650846873377933, -0.0730730068773... |
708.0185 | Semiparametric estimation of fractional cointegrating subspaces | We consider a common-components model for multivariate fractional
cointegration, in which the $s\geq1$ components have different memory
parameters. The cointegrating rank may exceed 1. We decompose the true
cointegrating vectors into orthogonal fractional cointegrating subspaces such
that vectors from distinct subspa... | math.ST stat.TH | we consider a commoncomponents model for multivariate fractional cointegration in which the sgeq1 components have different memory parameters the cointegrating rank may exceed 1 we decompose the true cointegrating vectors into orthogonal fractional cointegrating subspaces such that vectors from distinct subspaces yield... | [['we', 'consider', 'a', 'commoncomponents', 'model', 'for', 'multivariate', 'fractional', 'cointegration', 'in', 'which', 'the', 'sgeq1', 'components', 'have', 'different', 'memory', 'parameters', 'the', 'cointegrating', 'rank', 'may', 'exceed', '1', 'we', 'decompose', 'the', 'true', 'cointegrating', 'vectors', 'into'... | [-0.0787068419865545, 0.08811659313173459, -0.07121379713484105, 0.09639640380050236, -0.05890842608876226, -0.16598392125522254, 0.04653536418027826, 0.39125272284118123, -0.29128231401336474, -0.19933731737390362, 0.13381641999515237, -0.2608153427257234, -0.10386048645115514, 0.16599483445603963, -0.086046062181735,... |
708.0186 | Regional distribution of the prostaglandin E2 receptor EP1 in the rat
brain: accumulation in Purkinje cells of the cerebellum | Prostaglandin E2 (PGE2), is a major prostanoid produced by the activity of
cyclooxygenases (COX) in response to various physiological and pathological
stimuli. PGE2 exerts its effects by activating four specific E-type prostanoid
receptors (EP1, EP2, EP3, and EP4). In the present study, we analyzed the
expression of ... | q-bio.TO | prostaglandin e2 pge2 is a major prostanoid produced by the activity of cyclooxygenases cox in response to various physiological and pathological stimuli pge2 exerts its effects by activating four specific etype prostanoid receptors ep1 ep2 ep3 and ep4 in the present study we analyzed the expression of the pge2 recepto... | [['prostaglandin', 'e2', 'pge2', 'is', 'a', 'major', 'prostanoid', 'produced', 'by', 'the', 'activity', 'of', 'cyclooxygenases', 'cox', 'in', 'response', 'to', 'various', 'physiological', 'and', 'pathological', 'stimuli', 'pge2', 'exerts', 'its', 'effects', 'by', 'activating', 'four', 'specific', 'etype', 'prostanoid',... | [-0.07985621729474385, 0.12163663196325716, 0.021938233182138195, 0.06463549950664553, 0.01629053883241593, -0.1376273996869309, 0.03443803773649658, 0.38410255130794313, -0.19717879377098546, -0.20703303466062709, 0.03580334796828942, -0.26693982371749975, -0.3211052358047002, 0.1415629172070314, -0.09312044947097699,... |
708.0187 | Wide therapeutic time window for nimesulide neuroprotection in a model
of transient focal cerebral ischemia in the rat | Results from several studies indicate that cyclooxygenase-2 (COX-2) is
involved in ischemic brain injury. The purpose of this study was to evaluate
the neuroprotective effects of the selective COX-2 inhibitor nimesulide on
cerebral infarction and neurological deficits in a standardized model of
transient focal cerebr... | q-bio.NC q-bio.TO | results from several studies indicate that cyclooxygenase2 cox2 is involved in ischemic brain injury the purpose of this study was to evaluate the neuroprotective effects of the selective cox2 inhibitor nimesulide on cerebral infarction and neurological deficits in a standardized model of transient focal cerebral ische... | [['results', 'from', 'several', 'studies', 'indicate', 'that', 'cyclooxygenase2', 'cox2', 'is', 'involved', 'in', 'ischemic', 'brain', 'injury', 'the', 'purpose', 'of', 'this', 'study', 'was', 'to', 'evaluate', 'the', 'neuroprotective', 'effects', 'of', 'the', 'selective', 'cox2', 'inhibitor', 'nimesulide', 'on', 'cere... | [-0.04902460071410048, 0.15402513043339558, 0.013006136041864885, 0.048212660728627614, 0.03328357102341195, -0.16458349335027883, 0.10438570552372213, 0.39268203556439163, -0.13972562343540645, -0.3144454213222366, 0.13179300882748948, -0.30853366672106514, -0.21562631853798708, 0.1682786376934523, -0.1786135680750956... |
708.0188 | First principles investigations of the electronic, magnetic and chemical
bonding properties of CeTSn (T=Rh,Ru) | The electronic structures of CeRhSn and CeRuSn are self-consistently
calculated within density functional theory using the local spin density
approximation for exchange and correlation. In agreement with experimental
findings, the analyses of the electronic structures and of the chemical bonding
properties point to t... | cond-mat.str-el cond-mat.mtrl-sci | the electronic structures of cerhsn and cerusn are selfconsistently calculated within density functional theory using the local spin density approximation for exchange and correlation in agreement with experimental findings the analyses of the electronic structures and of the chemical bonding properties point to the ab... | [['the', 'electronic', 'structures', 'of', 'cerhsn', 'and', 'cerusn', 'are', 'selfconsistently', 'calculated', 'within', 'density', 'functional', 'theory', 'using', 'the', 'local', 'spin', 'density', 'approximation', 'for', 'exchange', 'and', 'correlation', 'in', 'agreement', 'with', 'experimental', 'findings', 'the', ... | [-0.1386535655413019, 0.1814664521792254, -0.0521175069979539, 0.055084562721037254, 0.058158132027050384, -0.06693981195138277, 0.0897819780167131, 0.3559374710741012, -0.25117340085929946, -0.31548160388085406, -0.014205246472939555, -0.3483097438798531, -0.0895894978955192, 0.09396753706019617, 0.13680441812673388, ... |
708.0189 | Pulsar model of the high energy phenomenology of LS 5039 | Under the assumption that LS 5039 is a system composed by a pulsar rotating
around an O6.5V star in a $\sim 3.9$ day orbit, we present the results of a
theoretical modeling of the high energy phenomenology observed by the High
Energy Stereoscopy Array (H.E.S.S.). This model (including detailed account of
the system g... | astro-ph | under the assumption that ls 5039 is a system composed by a pulsar rotating around an o65v star in a sim 39 day orbit we present the results of a theoretical modeling of the high energy phenomenology observed by the high energy stereoscopy array hess this model including detailed account of the system geometry kleinnis... | [['under', 'the', 'assumption', 'that', 'ls', '5039', 'is', 'a', 'system', 'composed', 'by', 'a', 'pulsar', 'rotating', 'around', 'an', 'o65v', 'star', 'in', 'a', 'sim', '39', 'day', 'orbit', 'we', 'present', 'the', 'results', 'of', 'a', 'theoretical', 'modeling', 'of', 'the', 'high', 'energy', 'phenomenology', 'observ... | [-0.11982845659949817, 0.11826282540732791, -0.05068969446583651, 0.12896743047313067, -0.048982762097148226, -0.11363947454374283, 0.0039708047261228785, 0.35958915956362036, -0.22292566930409521, -0.3557780442526564, 0.055581148833152835, -0.2856834164587781, -0.06401659809635021, 0.21372744948312175, 0.0037627569407... |
708.019 | GD 99 - an unusual, rarely observed DAV white dwarf | New observations of GD 99 are analysed. The unusual pulsation behaviour,
showing both long and short periods, has been confirmed. All the available
periods show a grouping of short and long period modes with roughly regular
spacing. If we interpret the groups separately, a binary nature can be a
possible explanation ... | astro-ph | new observations of gd 99 are analysed the unusual pulsation behaviour showing both long and short periods has been confirmed all the available periods show a grouping of short and long period modes with roughly regular spacing if we interpret the groups separately a binary nature can be a possible explanation as in th... | [['new', 'observations', 'of', 'gd', '99', 'are', 'analysed', 'the', 'unusual', 'pulsation', 'behaviour', 'showing', 'both', 'long', 'and', 'short', 'periods', 'has', 'been', 'confirmed', 'all', 'the', 'available', 'periods', 'show', 'a', 'grouping', 'of', 'short', 'and', 'long', 'period', 'modes', 'with', 'roughly', '... | [-0.1706551175409307, 0.1665826563257724, -0.10475973218368988, 0.13307343111373485, -0.09734072973175595, -0.14088519140301894, 0.06322036387088398, 0.43392668968687453, -0.23412227069493383, -0.31089020759488145, 0.13515107060666195, -0.24383224258684397, -0.11640354940512528, 0.22377379353468616, -0.0575874560357381... |
708.0191 | Engineering exotic phases for topologically-protected quantum
computation by emulating quantum dimer models | We use a nonperturbative extended contractor renormalization (ENCORE) method
for engineering quantum devices for the implementation of topologically
protected quantum bits described by an effective quantum dimer model on the
triangular lattice. By tuning the couplings of the device, topological
protection might be ac... | cond-mat.other cond-mat.str-el | we use a nonperturbative extended contractor renormalization encore method for engineering quantum devices for the implementation of topologically protected quantum bits described by an effective quantum dimer model on the triangular lattice by tuning the couplings of the device topological protection might be achieved... | [['we', 'use', 'a', 'nonperturbative', 'extended', 'contractor', 'renormalization', 'encore', 'method', 'for', 'engineering', 'quantum', 'devices', 'for', 'the', 'implementation', 'of', 'topologically', 'protected', 'quantum', 'bits', 'described', 'by', 'an', 'effective', 'quantum', 'dimer', 'model', 'on', 'the', 'tria... | [-0.1801846910774267, 0.2390641766018494, -0.03195938905212513, 0.04971512513059549, -0.017045376218447927, -0.1948411064076936, 0.06798422091690424, 0.35793989873906995, -0.22653333975488618, -0.317944400181919, 0.0549749034305153, -0.262974001063932, -0.13567610918211617, 0.18873181925300742, 0.008903949421827357, 0.... |
708.0192 | Motion by Stopping: Rectifying Brownian Motion of Non-spherical
Particles | We show that Brownian motion is spatially not symmetric for mesoscopic
particles embedded in a fluid if the particle is not in thermal equilibrium and
its shape is not spherical. In view of applications on molecular motors in
biological cells, we sustain non-equilibrium by stopping a non-spherical
particle at periodi... | cond-mat.soft | we show that brownian motion is spatially not symmetric for mesoscopic particles embedded in a fluid if the particle is not in thermal equilibrium and its shape is not spherical in view of applications on molecular motors in biological cells we sustain nonequilibrium by stopping a nonspherical particle at periodic site... | [['we', 'show', 'that', 'brownian', 'motion', 'is', 'spatially', 'not', 'symmetric', 'for', 'mesoscopic', 'particles', 'embedded', 'in', 'a', 'fluid', 'if', 'the', 'particle', 'is', 'not', 'in', 'thermal', 'equilibrium', 'and', 'its', 'shape', 'is', 'not', 'spherical', 'in', 'view', 'of', 'applications', 'on', 'molecul... | [-0.11209933652775363, 0.22301279416680336, -0.1094422219581902, 0.009585158655027045, -0.02572273188084364, -0.11855662321671843, -0.011844355560839176, 0.4165697598159313, -0.29420658788084986, -0.23202317387610674, 0.05124934069626033, -0.22321902050822973, -0.13827155192382634, 0.15260582587029786, -0.0372558902245... |
708.0193 | UV excess and AGB evolution in elliptical-galaxy stellar populations | The puzzling origin of the ``UV-upturn'' phenomenon, observed in some
elliptical galaxies, has recently been settled by identifying hot HB stars as
main contributors to galaxy ultraviolet luminosity excess. While a blue HB
morphology seems a natural characteristic of metal-poor stellar populations,
its appearence in ... | astro-ph | the puzzling origin of the uvupturn phenomenon observed in some elliptical galaxies has recently been settled by identifying hot hb stars as main contributors to galaxy ultraviolet luminosity excess while a blue hb morphology seems a natural characteristic of metalpoor stellar populations its appearence in metalrich sy... | [['the', 'puzzling', 'origin', 'of', 'the', 'uvupturn', 'phenomenon', 'observed', 'in', 'some', 'elliptical', 'galaxies', 'has', 'recently', 'been', 'settled', 'by', 'identifying', 'hot', 'hb', 'stars', 'as', 'main', 'contributors', 'to', 'galaxy', 'ultraviolet', 'luminosity', 'excess', 'while', 'a', 'blue', 'hb', 'mor... | [-0.028931214743964026, 0.09139848612458336, -0.11024710620105023, 0.1837528728745077, -0.1594625199735861, -0.052200084839399176, 0.04435380940786868, 0.480521667513683, -0.10001891955437366, -0.3472647262893826, -0.006020680723807592, -0.2928968094611349, -0.06881102483075495, 0.16056154785616863, -0.1265510512933692... |
708.0194 | Isomer triggering via nuclear excitation by electron capture | Triggering of long-lived nuclear isomeric states via coupling to the atomic
shells in the process of nuclear excitation by electron capture (NEEC) is
studied. NEEC occurring in highly-charged ions can excite the isomeric state to
a triggering level that subsequently decays to the ground state. We present
total cross ... | nucl-th physics.atom-ph | triggering of longlived nuclear isomeric states via coupling to the atomic shells in the process of nuclear excitation by electron capture neec is studied neec occurring in highlycharged ions can excite the isomeric state to a triggering level that subsequently decays to the ground state we present total cross sections... | [['triggering', 'of', 'longlived', 'nuclear', 'isomeric', 'states', 'via', 'coupling', 'to', 'the', 'atomic', 'shells', 'in', 'the', 'process', 'of', 'nuclear', 'excitation', 'by', 'electron', 'capture', 'neec', 'is', 'studied', 'neec', 'occurring', 'in', 'highlycharged', 'ions', 'can', 'excite', 'the', 'isomeric', 'st... | [-0.08788221862050705, 0.2325179123806513, -0.005005073043403999, 0.12159118699303856, 0.06059773852625354, -0.12661699114621364, 0.0702594086747426, 0.401100856421346, -0.1786959231368118, -0.2976396182467314, -0.014962388066289184, -0.27695224253164435, 0.01963498856110329, 0.16556463966315443, 0.09901668009644543, 0... |
708.0195 | Accurate seeing measurements with MASS and DIMM | Astronomical seeing is quantified by a single parameter, turbulence integral,
in the framework of the Kolmogorov turbulence model. This parameter can be
routinely measured by a Differential Image Motion Monitor, DIMM. A new
instrument, Multi-Aperture Scintillation Sensor (MASS), permits to measure the
seeing in the f... | astro-ph | astronomical seeing is quantified by a single parameter turbulence integral in the framework of the kolmogorov turbulence model this parameter can be routinely measured by a differential image motion monitor dimm a new instrument multiaperture scintillation sensor mass permits to measure the seeing in the free atmosphe... | [['astronomical', 'seeing', 'is', 'quantified', 'by', 'a', 'single', 'parameter', 'turbulence', 'integral', 'in', 'the', 'framework', 'of', 'the', 'kolmogorov', 'turbulence', 'model', 'this', 'parameter', 'can', 'be', 'routinely', 'measured', 'by', 'a', 'differential', 'image', 'motion', 'monitor', 'dimm', 'a', 'new', ... | [-0.06994138940677254, 0.16706240454125995, -0.0956354459922295, 0.07019787853850327, -0.06770073606458027, -0.13076700153437237, 0.01591566520235372, 0.4100087487216418, -0.2861969917398205, -0.3788987572770566, 0.1478316702899368, -0.24444587977874713, -0.050900923833978595, 0.2220603144491583, -0.145171324049847, 0.... |
708.0196 | More frequencies of KUV 02464+3239 | Preliminary results on KUV 02464+3239, a pulsating DA white dwarf are
presented. Located near the red edge of the DAV instability strip, KUV
02464+3239 shows large amplitude and long period pulsation modes. Up to now
only one mode was known from a 50-minute-long light curve. Our more extended
observations allowed the... | astro-ph | preliminary results on kuv 024643239 a pulsating da white dwarf are presented located near the red edge of the dav instability strip kuv 024643239 shows large amplitude and long period pulsation modes up to now only one mode was known from a 50minutelong light curve our more extended observations allowed the identifica... | [['preliminary', 'results', 'on', 'kuv', '024643239', 'a', 'pulsating', 'da', 'white', 'dwarf', 'are', 'presented', 'located', 'near', 'the', 'red', 'edge', 'of', 'the', 'dav', 'instability', 'strip', 'kuv', '024643239', 'shows', 'large', 'amplitude', 'and', 'long', 'period', 'pulsation', 'modes', 'up', 'to', 'now', 'o... | [-0.14445065685140435, 0.15488834560330195, -0.10986256384057924, 0.054674734876078386, -0.14079491051167928, -0.12688664270734246, 0.10148446386764673, 0.3517622815614397, -0.18966226966585964, -0.28193051866467367, 0.13033280259961347, -0.2911341865017841, -0.10499560224045788, 0.259145893685689, -0.04475926893858493... |
708.0197 | A frequency domain empirical likelihood for short- and long-range
dependence | This paper introduces a version of empirical likelihood based on the
periodogram and spectral estimating equations. This formulation handles
dependent data through a data transformation (i.e., a Fourier transform) and is
developed in terms of the spectral distribution rather than a time domain
probability distributio... | math.ST stat.TH | this paper introduces a version of empirical likelihood based on the periodogram and spectral estimating equations this formulation handles dependent data through a data transformation ie a fourier transform and is developed in terms of the spectral distribution rather than a time domain probability distribution the as... | [['this', 'paper', 'introduces', 'a', 'version', 'of', 'empirical', 'likelihood', 'based', 'on', 'the', 'periodogram', 'and', 'spectral', 'estimating', 'equations', 'this', 'formulation', 'handles', 'dependent', 'data', 'through', 'a', 'data', 'transformation', 'ie', 'a', 'fourier', 'transform', 'and', 'is', 'developed... | [-0.05215711286670067, 0.02049052699022298, -0.15911294466520592, 0.14278036363733312, -0.0989338247639286, -0.1243551770429604, 0.05025171204914937, 0.400316794440756, -0.23314989968534566, -0.3367911017674014, 0.1665577797476596, -0.22919528043215595, -0.11975415698176901, 0.20801355678217137, -0.06312202204802506, 0... |
708.0198 | The Chemical Composition of an Extrasolar Minor Planet | We report the relative abundances of 17 elements in the atmosphere of the
white dwarf star GD 362, material that, very probably, was contained previously
in a large asteroid or asteroids with composition similar to the Earth/Moon
system. The asteroid may have once been part of a larger parent body not unlike
one of t... | astro-ph | we report the relative abundances of 17 elements in the atmosphere of the white dwarf star gd 362 material that very probably was contained previously in a large asteroid or asteroids with composition similar to the earthmoon system the asteroid may have once been part of a larger parent body not unlike one of the terr... | [['we', 'report', 'the', 'relative', 'abundances', 'of', '17', 'elements', 'in', 'the', 'atmosphere', 'of', 'the', 'white', 'dwarf', 'star', 'gd', '362', 'material', 'that', 'very', 'probably', 'was', 'contained', 'previously', 'in', 'a', 'large', 'asteroid', 'or', 'asteroids', 'with', 'composition', 'similar', 'to', '... | [-0.07485468250500862, 0.18324330355590362, -0.08448189712266942, 0.006753681609254392, -0.0733158651006515, 0.00038351736901724926, 0.044063380537707295, 0.3033432694243603, -0.14961410561179528, -0.3816768138165601, 0.06271719968816662, -0.3375826636481969, -0.10225224796087161, 0.17912783747401517, -0.16959555381450... |
708.0199 | $\Lambda NN$ and $\Sigma NN$ systems at threshold: II. The effect of D
waves | Using the two-body interactions obtained from a chiral constituent quark
model we study all $\Lambda NN$ and $\Sigma NN$ states with I=0,1,2 and
J=1/2,3/2 at threshold, taking into account all three-body configurations with
S and D wave components. We constrain further the limits for the $\Lambda N$
spin-triplet scat... | hep-ph nucl-th | using the twobody interactions obtained from a chiral constituent quark model we study all lambda nn and sigma nn states with i012 and j1232 at threshold taking into account all threebody configurations with s and d wave components we constrain further the limits for the lambda n spintriplet scattering length a_121 usi... | [['using', 'the', 'twobody', 'interactions', 'obtained', 'from', 'a', 'chiral', 'constituent', 'quark', 'model', 'we', 'study', 'all', 'lambda', 'nn', 'and', 'sigma', 'nn', 'states', 'with', 'i012', 'and', 'j1232', 'at', 'threshold', 'taking', 'into', 'account', 'all', 'threebody', 'configurations', 'with', 's', 'and',... | [-0.16899317315750823, 0.20567669470304834, -0.049490814045018795, 0.0787475450329252, 0.026187423579142784, -0.17800401828069354, 0.08158759348641735, 0.3519567547692466, -0.19975345395505428, -0.2481643712608931, -0.05803027693014208, -0.34715283231944155, -0.015198237403084706, 0.08036597037073417, 0.193716881393464... |
708.02 | A Note on Shortest Developments | De Vrijer has presented a proof of the finite developments theorem which, in
addition to showing that all developments are finite, gives an effective
reduction strategy computing longest developments as well as a simple formula
computing their length.
We show that by applying a rather simple and intuitive principle... | cs.LO | de vrijer has presented a proof of the finite developments theorem which in addition to showing that all developments are finite gives an effective reduction strategy computing longest developments as well as a simple formula computing their length we show that by applying a rather simple and intuitive principle of dua... | [['de', 'vrijer', 'has', 'presented', 'a', 'proof', 'of', 'the', 'finite', 'developments', 'theorem', 'which', 'in', 'addition', 'to', 'showing', 'that', 'all', 'developments', 'are', 'finite', 'gives', 'an', 'effective', 'reduction', 'strategy', 'computing', 'longest', 'developments', 'as', 'well', 'as', 'a', 'simple'... | [-0.10378579878791545, 0.10626159023164898, -0.16003540793220358, 0.07444537041495398, -0.13626856090559158, -0.15266625012251703, 0.041358833293391704, 0.3255683418440943, -0.24246761652466375, -0.2826522617057587, 0.1073534861667819, -0.21604085861084363, -0.1987772945431061, 0.2712483585322237, -0.10093987734095815,... |
708.0201 | Four-wave mixing, quantum control and compensating losses in doped
negative-index photonic metamaterials | The possibility of compensating absorption in negative-index metatamterials
(NIMs) doped by resonant nonlinear-optical centers is shown. The role of
quantum interference and extraordinary properties of four-wave parametric
amplification of counter-propagating electromagnetic waves in NIMs are
discussed.
| quant-ph physics.optics | the possibility of compensating absorption in negativeindex metatamterials nims doped by resonant nonlinearoptical centers is shown the role of quantum interference and extraordinary properties of fourwave parametric amplification of counterpropagating electromagnetic waves in nims are discussed | [['the', 'possibility', 'of', 'compensating', 'absorption', 'in', 'negativeindex', 'metatamterials', 'nims', 'doped', 'by', 'resonant', 'nonlinearoptical', 'centers', 'is', 'shown', 'the', 'role', 'of', 'quantum', 'interference', 'and', 'extraordinary', 'properties', 'of', 'fourwave', 'parametric', 'amplification', 'of... | [-0.21257971133038933, 0.2611707919410297, 0.030553354682134732, -0.003677319053427449, -0.08116540951388222, -0.14558291326143913, -0.008349844899826816, 0.471570203772613, -0.20835322769624845, -0.23211914731987884, -0.05295185981917062, -0.3343780023444976, -0.20482086432831628, 0.22172488902828524, 0.03702874460390... |
708.0202 | Regular spanning subgraphs of bipartite graphs of high minimum degree | Let G be a simple balanced bipartite graph on $2n$ vertices, $\delta =
\delta(G)/n$, and $\rho={\delta + \sqrt{2 \delta -1} \over 2}$. If $\delta >
1/2$ then it has a $\lfloor \rho n \rfloor$-regular spanning subgraph. The
statement is nearly tight.
| math.CO | let g be a simple balanced bipartite graph on 2n vertices delta deltagn and rhodelta sqrt2 delta 1 over 2 if delta 12 then it has a lfloor rho n rfloorregular spanning subgraph the statement is nearly tight | [['let', 'g', 'be', 'a', 'simple', 'balanced', 'bipartite', 'graph', 'on', '2n', 'vertices', 'delta', 'deltagn', 'and', 'rhodelta', 'sqrt2', 'delta', '1', 'over', '2', 'if', 'delta', '12', 'then', 'it', 'has', 'a', 'lfloor', 'rho', 'n', 'rfloorregular', 'spanning', 'subgraph', 'the', 'statement', 'is', 'nearly', 'tight... | [-0.22954127671093577, 0.23461726031059194, -0.013039230863796547, 0.006057904531998146, -0.0453924899144719, -0.2959580124200632, 0.09729962661448452, 0.37378369458019733, -0.2514473359980103, -0.3270022934043987, 0.02325823163199756, -0.419563299872809, -0.10561043309927401, 0.0832113896548334, -0.035775860073044896,... |
708.0203 | The end of the Galactic spectrum | We use a diffusion galactic model to analyze the end of the Galactic cosmic
ray spectrum and its mixing with the extragalactic cosmic ray flux. We analyze
the transition between Galactic and extragalactic components using two
different extragalactic models. We compare the sum of the diffusive galactic
spectrum and ex... | astro-ph | we use a diffusion galactic model to analyze the end of the galactic cosmic ray spectrum and its mixing with the extragalactic cosmic ray flux we analyze the transition between galactic and extragalactic components using two different extragalactic models we compare the sum of the diffusive galactic spectrum and extrag... | [['we', 'use', 'a', 'diffusion', 'galactic', 'model', 'to', 'analyze', 'the', 'end', 'of', 'the', 'galactic', 'cosmic', 'ray', 'spectrum', 'and', 'its', 'mixing', 'with', 'the', 'extragalactic', 'cosmic', 'ray', 'flux', 'we', 'analyze', 'the', 'transition', 'between', 'galactic', 'and', 'extragalactic', 'components', '... | [-0.0555348551798878, 0.14650251937564462, -0.030496303291459168, 0.16106671151023225, -0.11830255083207573, 0.010109997420970882, 0.027978999157702283, 0.436187637171575, -0.24812223043824946, -0.32743673831490533, -0.023897439449293807, -0.38998760203165667, -0.005625598980779094, 0.20104936746065505, 0.0861039680395... |
708.0204 | Phase diagram and magnetocaloric effect of CoMnGe_{1-x}Sn_{x} alloys | We propose the phase diagram of a new pseudo-ternary compound,
CoMnGe_{1-x}Sn_{x}, in the range x less than or equal to 0.1. Our phase diagram
is a result of magnetic and calometric measurements. We demonstrate the
appearance of a hysteretic magnetostructural phase transition in the range
x=0.04 to x=0.055, similar t... | cond-mat.mtrl-sci cond-mat.str-el | we propose the phase diagram of a new pseudoternary compound comnge_1xsn_x in the range x less than or equal to 01 our phase diagram is a result of magnetic and calometric measurements we demonstrate the appearance of a hysteretic magnetostructural phase transition in the range x004 to x0055 similar to that observed in... | [['we', 'propose', 'the', 'phase', 'diagram', 'of', 'a', 'new', 'pseudoternary', 'compound', 'comnge_1xsn_x', 'in', 'the', 'range', 'x', 'less', 'than', 'or', 'equal', 'to', '01', 'our', 'phase', 'diagram', 'is', 'a', 'result', 'of', 'magnetic', 'and', 'calometric', 'measurements', 'we', 'demonstrate', 'the', 'appearan... | [-0.1499768356177775, 0.2197406722630546, -0.05370584711548325, -0.012772096348112648, -0.047257248936130584, -0.08392272574049466, 0.1322249396505214, 0.3853741642268537, -0.23861004168041122, -0.33382284011944985, 0.06952600555666225, -0.2930342972965784, -0.11098545494272365, 0.17459564885769935, -0.0130522006317900... |
708.0205 | Proximity DC squids in the long junction limit | We report the design and measurement of
Superconducting/normal/superconducting (SNS) proximity DC squids in the long
junction limit, i.e. superconducting loops interrupted by two normal metal
wires roughly a micrometer long. Thanks to the clean interface between the
metals, at low temperature a large supercurrent flo... | cond-mat.mes-hall cond-mat.supr-con | we report the design and measurement of superconductingnormalsuperconducting sns proximity dc squids in the long junction limit ie superconducting loops interrupted by two normal metal wires roughly a micrometer long thanks to the clean interface between the metals at low temperature a large supercurrent flows through ... | [['we', 'report', 'the', 'design', 'and', 'measurement', 'of', 'superconductingnormalsuperconducting', 'sns', 'proximity', 'dc', 'squids', 'in', 'the', 'long', 'junction', 'limit', 'ie', 'superconducting', 'loops', 'interrupted', 'by', 'two', 'normal', 'metal', 'wires', 'roughly', 'a', 'micrometer', 'long', 'thanks', '... | [-0.21175776044025932, 0.15321049943125026, -0.02093016666706738, 0.0400016701579917, -0.010845049876763031, -0.15071209046859727, 0.08565343101766112, 0.3676205803401941, -0.2449121618578427, -0.34145320360223913, 0.04501198972304633, -0.25823012942145035, -0.12046886199088984, 0.2150855247732685, -0.00665391848996541... |
708.0206 | Algebraic K-theory and abstract homotopy theory | We decompose the K-theory space of a Waldhausen category in terms of its
Dwyer-Kan simplicial localization. This leads to a criterion for functors to
induce equivalences of K-theory spectra that generalizes and explains many of
the criteria appearing in the literature. We show that under mild hypotheses, a
weakly exa... | math.KT math.AT | we decompose the ktheory space of a waldhausen category in terms of its dwyerkan simplicial localization this leads to a criterion for functors to induce equivalences of ktheory spectra that generalizes and explains many of the criteria appearing in the literature we show that under mild hypotheses a weakly exact funct... | [['we', 'decompose', 'the', 'ktheory', 'space', 'of', 'a', 'waldhausen', 'category', 'in', 'terms', 'of', 'its', 'dwyerkan', 'simplicial', 'localization', 'this', 'leads', 'to', 'a', 'criterion', 'for', 'functors', 'to', 'induce', 'equivalences', 'of', 'ktheory', 'spectra', 'that', 'generalizes', 'and', 'explains', 'ma... | [-0.18992066982900724, 0.018549936944054934, -0.14537018947885372, 0.12634306985091825, -0.055158892850158736, -0.10715991789766122, -0.02496301990140637, 0.3780019354016986, -0.4067868731144699, -0.20074493254651316, 0.009848172350757523, -0.1723909307147551, -0.1766850919375429, 0.17208206560462713, -0.26192082006309... |
708.0207 | Restless pions: orbifold boundary conditions and noise suppression in
lattice QCD | The study of one or more baryons in lattice QCD is severely hindered by the
exponential decay in time of the signal-to-noise ratio. The rate at which the
signal-to-noise decreases is a function of the the pion mass. More precisely,
it depends on the minimum allowed pion energy in the box, which, for periodic
boundary... | hep-lat hep-ph hep-th nucl-th | the study of one or more baryons in lattice qcd is severely hindered by the exponential decay in time of the signaltonoise ratio the rate at which the signaltonoise decreases is a function of the the pion mass more precisely it depends on the minimum allowed pion energy in the box which for periodic boundary conditions... | [['the', 'study', 'of', 'one', 'or', 'more', 'baryons', 'in', 'lattice', 'qcd', 'is', 'severely', 'hindered', 'by', 'the', 'exponential', 'decay', 'in', 'time', 'of', 'the', 'signaltonoise', 'ratio', 'the', 'rate', 'at', 'which', 'the', 'signaltonoise', 'decreases', 'is', 'a', 'function', 'of', 'the', 'the', 'pion', 'm... | [-0.15719553139171608, 0.20798392142982236, -0.0610188784554512, 0.10058131272856531, -0.03244277528331926, -0.10256705914313595, 0.09512139901348818, 0.3233643966497824, -0.18334591214264195, -0.25654723391025547, 0.0845904742831379, -0.2571041966004977, -0.014999844259508545, 0.12145125289772829, -0.00127194552416247... |
708.0208 | Collective oscillations in optical matter | Atom and nanoparticle arrays trapped in optical lattices are shown to be
capable of sustaining collective oscillations of frequency proportional to the
strength of the external light field. The spectrum of these oscillations
determines the mechanical stability of the arrays. This phenomenon is studied
for dimers, str... | cond-mat.soft cond-mat.other | atom and nanoparticle arrays trapped in optical lattices are shown to be capable of sustaining collective oscillations of frequency proportional to the strength of the external light field the spectrum of these oscillations determines the mechanical stability of the arrays this phenomenon is studied for dimers strings ... | [['atom', 'and', 'nanoparticle', 'arrays', 'trapped', 'in', 'optical', 'lattices', 'are', 'shown', 'to', 'be', 'capable', 'of', 'sustaining', 'collective', 'oscillations', 'of', 'frequency', 'proportional', 'to', 'the', 'strength', 'of', 'the', 'external', 'light', 'field', 'the', 'spectrum', 'of', 'these', 'oscillatio... | [-0.19033659774196657, 0.2293062241473168, -0.010327339821602576, 0.006314800479091131, -0.022151245525142606, -0.1414819391357014, -0.01094991516527863, 0.40256715967104983, -0.27684785508944726, -0.2764870513123102, 0.07390221481574162, -0.2788508856812349, -0.1652284050763298, 0.23067569127306342, -0.007970594242439... |
708.0209 | Models of Financial Markets with Extensive Participation Incentives | We consider models of financial markets in which all parties involved find
incentives to participate. Strategies are evaluated directly by their virtual
wealths. By tuning the price sensitivity and market impact, a phase diagram
with several attractor behaviors resembling those of real markets emerge,
reflecting the ... | q-fin.TR physics.soc-ph | we consider models of financial markets in which all parties involved find incentives to participate strategies are evaluated directly by their virtual wealths by tuning the price sensitivity and market impact a phase diagram with several attractor behaviors resembling those of real markets emerge reflecting the roles ... | [['we', 'consider', 'models', 'of', 'financial', 'markets', 'in', 'which', 'all', 'parties', 'involved', 'find', 'incentives', 'to', 'participate', 'strategies', 'are', 'evaluated', 'directly', 'by', 'their', 'virtual', 'wealths', 'by', 'tuning', 'the', 'price', 'sensitivity', 'and', 'market', 'impact', 'a', 'phase', '... | [-0.10484319428156177, 0.09540154425789127, -0.11014706049141267, 0.11460636496935844, -0.04447044018679466, -0.15096392441983167, 0.11451040762108114, 0.4112865301184088, -0.2383837711782925, -0.30081898883100694, 0.13371930878170557, -0.3198363115783218, -0.16475255076485357, 0.1825791957734568, -0.0690047369914786, ... |
708.021 | Triangulated categories of matrix factorizations for regular systems of
weights with $\epsilon=-1$ | We construct a full strongly exceptional collection in the triangulated
category of graded matrix factorizations of a polynomial associated to a
non-degenerate regular system of weights whose smallest exponents are equal to
-1. In the associated Grothendieck group, the strongly exceptional collection
defines a root b... | math.AG math.RT | we construct a full strongly exceptional collection in the triangulated category of graded matrix factorizations of a polynomial associated to a nondegenerate regular system of weights whose smallest exponents are equal to 1 in the associated grothendieck group the strongly exceptional collection defines a root basis o... | [['we', 'construct', 'a', 'full', 'strongly', 'exceptional', 'collection', 'in', 'the', 'triangulated', 'category', 'of', 'graded', 'matrix', 'factorizations', 'of', 'a', 'polynomial', 'associated', 'to', 'a', 'nondegenerate', 'regular', 'system', 'of', 'weights', 'whose', 'smallest', 'exponents', 'are', 'equal', 'to',... | [-0.20454960696898947, 0.09155458626450926, -0.0457642532816929, -0.007677252420008455, -0.11637118719972489, -0.15120523346718628, -0.00809512744805344, 0.31969490326605965, -0.37550598355691606, -0.15158006640949015, 0.1272433093002225, -0.27862829534427785, -0.13337825356823643, 0.12425379385808255, -0.0897966389794... |
708.0211 | The long-term evolution of the spin, pulse shape, and orbit of the
accretion-powered millisecond pulsar SAX J1808.4-3658 | We present a 7 yr timing study of the 2.5 ms X-ray pulsar SAX J1808.4-3658,
an X-ray transient with a recurrence time of ~2 yr, using data from the Rossi
X-ray Timing Explorer covering 4 transient outbursts (1998-2005). We verify
that the 401 Hz pulsation traces the spin frequency fundamental and not a
harmonic. Subs... | astro-ph | we present a 7 yr timing study of the 25 ms xray pulsar sax j180843658 an xray transient with a recurrence time of 2 yr using data from the rossi xray timing explorer covering 4 transient outbursts 19982005 we verify that the 401 hz pulsation traces the spin frequency fundamental and not a harmonic substantial pulse sh... | [['we', 'present', 'a', '7', 'yr', 'timing', 'study', 'of', 'the', '25', 'ms', 'xray', 'pulsar', 'sax', 'j180843658', 'an', 'xray', 'transient', 'with', 'a', 'recurrence', 'time', 'of', '2', 'yr', 'using', 'data', 'from', 'the', 'rossi', 'xray', 'timing', 'explorer', 'covering', '4', 'transient', 'outbursts', '19982005... | [-0.13925909815082813, 0.16653778268042463, -0.05650292378909332, 0.10323278102483871, -0.12901592433142164, -0.06080387203879924, 0.09773024887566124, 0.41101173731579405, -0.20266068224462788, -0.3307537561184659, 0.12458182531628299, -0.30510246989222756, -0.03781468982777079, 0.27519151814572135, -0.065824966897945... |
708.0212 | Bosonization of strongly interacting electrons | Strong repulsive interactions in a one-dimensional electron system suppress
the exchange coupling J of electron spins to a value much smaller than the
Fermi energy E_F. The conventional theoretical description of such systems
based on the bosonization approach and the concept of Tomonaga-Luttinger liquid
is applicabl... | cond-mat.mes-hall cond-mat.str-el | strong repulsive interactions in a onedimensional electron system suppress the exchange coupling j of electron spins to a value much smaller than the fermi energy e_f the conventional theoretical description of such systems based on the bosonization approach and the concept of tomonagaluttinger liquid is applicable onl... | [['strong', 'repulsive', 'interactions', 'in', 'a', 'onedimensional', 'electron', 'system', 'suppress', 'the', 'exchange', 'coupling', 'j', 'of', 'electron', 'spins', 'to', 'a', 'value', 'much', 'smaller', 'than', 'the', 'fermi', 'energy', 'e_f', 'the', 'conventional', 'theoretical', 'description', 'of', 'such', 'syste... | [-0.14287566936492355, 0.15609928285312555, -0.06676022296283642, 0.08360942119741341, -0.003012566777134809, -0.1505875374290715, 0.08101657919344032, 0.3466971724889465, -0.24356268931628217, -0.2892217599798607, -0.04179046011848163, -0.34711436493487297, -0.06753333319196643, 0.17733610028554272, 0.0712236755356617... |
708.0213 | Permutations of Strongly Self-Absorbing C*-algebras | Let G be a finite group acting on {1,...,n}. For any C*-algebra A, this
defines an action of \alpha of G on A^{\otimes n}. We show that if A
tensorially absorbs a UHF algebra of infinite type, the Jiang-Su algebra, or is
approximately divisible, then A \times_{\alpha} G has the corresponding
property as well.
| math.OA | let g be a finite group acting on 1n for any calgebra a this defines an action of alpha of g on aotimes n we show that if a tensorially absorbs a uhf algebra of infinite type the jiangsu algebra or is approximately divisible then a times_alpha g has the corresponding property as well | [['let', 'g', 'be', 'a', 'finite', 'group', 'acting', 'on', '1n', 'for', 'any', 'calgebra', 'a', 'this', 'defines', 'an', 'action', 'of', 'alpha', 'of', 'g', 'on', 'aotimes', 'n', 'we', 'show', 'that', 'if', 'a', 'tensorially', 'absorbs', 'a', 'uhf', 'algebra', 'of', 'infinite', 'type', 'the', 'jiangsu', 'algebra', 'or... | [-0.16926852611639467, 0.17965552519550934, -0.11424983531685064, -0.04785527273391684, -0.14027100300450843, -0.1523235594181137, -0.02665521573551275, 0.3974451935953564, -0.3428199444380071, -0.14175744332304155, 0.10994432403499053, -0.3022623149747098, -0.07614237189948282, 0.15486328769044053, -0.1118848171533533... |
708.0214 | Helioseismic Holography of Simulated Solar Convection and Prospects for
the Detection of Small-Scale Subsurface Flows | We perform helioseismic holography on realistic solar convection simulations
and compare the observed travel-time perturbations with the expected travel
times from the horizontal flows in the simulations computed from forward models
under the assumption of the Born approximation. We demonstrate reasonable
agreement b... | astro-ph | we perform helioseismic holography on realistic solar convection simulations and compare the observed traveltime perturbations with the expected travel times from the horizontal flows in the simulations computed from forward models under the assumption of the born approximation we demonstrate reasonable agreement betwe... | [['we', 'perform', 'helioseismic', 'holography', 'on', 'realistic', 'solar', 'convection', 'simulations', 'and', 'compare', 'the', 'observed', 'traveltime', 'perturbations', 'with', 'the', 'expected', 'travel', 'times', 'from', 'the', 'horizontal', 'flows', 'in', 'the', 'simulations', 'computed', 'from', 'forward', 'mo... | [-0.10829657691182326, 0.17465112960462378, -0.03410113764893726, 0.07545686437136676, -0.005837185947588209, -0.033432721576416455, 0.037037826914714994, 0.3638319574109108, -0.2504877011352301, -0.34157400805304744, 0.0941735138626185, -0.28699804152521863, -0.11586998965585682, 0.2189189505215029, -0.029433019989660... |
708.0215 | Comments on the Invariance of Physical Laws Under Particle
Re-Arrangement | Observationally and experimentally, physical laws express how particles
interact. Conversely, physical laws should be invariant under any
re-arrangement of those particles, e.g., the laws of gravity do not change if
one re-arranges the stars in the sky. To explore the physical meaning of these
assertions, arguments a... | gr-qc | observationally and experimentally physical laws express how particles interact conversely physical laws should be invariant under any rearrangement of those particles eg the laws of gravity do not change if one rearranges the stars in the sky to explore the physical meaning of these assertions arguments are presented ... | [['observationally', 'and', 'experimentally', 'physical', 'laws', 'express', 'how', 'particles', 'interact', 'conversely', 'physical', 'laws', 'should', 'be', 'invariant', 'under', 'any', 'rearrangement', 'of', 'those', 'particles', 'eg', 'the', 'laws', 'of', 'gravity', 'do', 'not', 'change', 'if', 'one', 'rearranges',... | [-0.11736617590422216, 0.22390799191400773, -0.10429382052110589, 0.09112537029280286, -0.08006670774649019, -0.13871152955714774, -0.0034905004315078257, 0.3512901035501905, -0.2705788639698016, -0.3450643594255266, 0.04116532907254346, -0.2879035455883359, -0.08260271738728751, 0.17078108471899253, -0.086520548402736... |
708.0216 | Modulation effects on Landau levels in a monolayer graphene | A monolayer graphene exists in an environment where a uniform magnetic field
interacts a spatially modulated magnetic field. The spatially modulated
magnetic field could affect Landau levels due to a uniform magnetic field. The
modulation effects on Landau levels are investigated through the Peierl's
tight-binding mo... | cond-mat.mes-hall | a monolayer graphene exists in an environment where a uniform magnetic field interacts a spatially modulated magnetic field the spatially modulated magnetic field could affect landau levels due to a uniform magnetic field the modulation effects on landau levels are investigated through the peierls tightbinding model th... | [['a', 'monolayer', 'graphene', 'exists', 'in', 'an', 'environment', 'where', 'a', 'uniform', 'magnetic', 'field', 'interacts', 'a', 'spatially', 'modulated', 'magnetic', 'field', 'the', 'spatially', 'modulated', 'magnetic', 'field', 'could', 'affect', 'landau', 'levels', 'due', 'to', 'a', 'uniform', 'magnetic', 'field... | [-0.22306558587775885, 0.23931624847606853, -0.034208940890939565, 0.06577032797535469, -0.009996308598217348, -0.10328387970342331, 0.054841732334395585, 0.38857890390197203, -0.28301602449180596, -0.30006307808857335, 0.008360632509305674, -0.22906957823633148, -0.09656515004950882, 0.1477245255998467, 0.045361963785... |
708.0217 | Impurity induced density of states and residual transport in nonunitary
superconductors | We obtain general expressions for the residual density of states, electrical
conductivity and thermal conductivity for non-unitary superconductors due to
impurity scattering. We apply the results to the so-called `B phase' of
PrOs4Sb12, which we describe using a non-unitary gap function derived from
symmetry consider... | cond-mat.supr-con cond-mat.str-el | we obtain general expressions for the residual density of states electrical conductivity and thermal conductivity for nonunitary superconductors due to impurity scattering we apply the results to the socalled b phase of pros4sb12 which we describe using a nonunitary gap function derived from symmetry considerations the... | [['we', 'obtain', 'general', 'expressions', 'for', 'the', 'residual', 'density', 'of', 'states', 'electrical', 'conductivity', 'and', 'thermal', 'conductivity', 'for', 'nonunitary', 'superconductors', 'due', 'to', 'impurity', 'scattering', 'we', 'apply', 'the', 'results', 'to', 'the', 'socalled', 'b', 'phase', 'of', 'p... | [-0.13517913566015305, 0.18999731398209752, -0.07387385833712798, 0.027011352354690196, -0.0738366935106497, -0.15749308272516208, 0.07257013806393223, 0.3632701182209458, -0.254265390853915, -0.21780306987819217, 0.06678299799317583, -0.30240338793881827, -0.14681671274500707, 0.150661600605836, -0.009424802802857898,... |
708.0218 | Spin measurements for 147Sm+n resonances: Further evidence for
non-statistical effects | We have determined the spins J of resonances in the 147Sm(n,gamma) reaction
by measuring multiplicities of gamma-ray cascades following neutron capture.
Using this technique, we were able to determine J values for all but 14 of the
140 known resonances below En = 1 keV, including 41 firm J assignments for
resonances ... | nucl-ex nucl-th | we have determined the spins j of resonances in the 147smngamma reaction by measuring multiplicities of gammaray cascades following neutron capture using this technique we were able to determine j values for all but 14 of the 140 known resonances below en 1 kev including 41 firm j assignments for resonances whose spins... | [['we', 'have', 'determined', 'the', 'spins', 'j', 'of', 'resonances', 'in', 'the', '147smngamma', 'reaction', 'by', 'measuring', 'multiplicities', 'of', 'gammaray', 'cascades', 'following', 'neutron', 'capture', 'using', 'this', 'technique', 'we', 'were', 'able', 'to', 'determine', 'j', 'values', 'for', 'all', 'but', ... | [-0.052234248238285846, 0.17401029712691524, -0.05819406325632978, 0.10792976792436093, -0.05031765468302183, -0.14691082054147653, 0.08929604406924531, 0.3723832940333523, -0.17985497970754902, -0.40300776559549073, 0.03600046300756124, -0.3520565317594446, -0.01005930242439111, 0.19516534067176206, 0.0222495661513676... |
708.0219 | Sharp bounds on the critical stability radius for relativistic charged
spheres: I | This paper has been withdrawn since its content is included in the more
general version arXiv:0804.1882
| gr-qc | this paper has been withdrawn since its content is included in the more general version arxiv08041882 | [['this', 'paper', 'has', 'been', 'withdrawn', 'since', 'its', 'content', 'is', 'included', 'in', 'the', 'more', 'general', 'version', 'arxiv08041882']] | [-0.07450536237253497, -0.022132130774358907, -0.14982220381498337, 0.035120735069115956, -0.13302757119139036, -0.0996809747380515, -0.0818760450851793, 0.3696073258916537, -0.22717497001091638, -0.28135504896442093, 0.14612262909455845, -0.2994191266596317, -0.14198137931525706, 0.09189498921235402, -0.26526059905687... |
708.022 | The Thermal Evolution of the Donors in AM CVn Binaries | (Abridged) We calculate the full stellar-structural evolution of donors in AM
CVn systems formed through the WD channel coupled to the binary's evolution.
Contrary to assumptions made in prior modelling, these donors are not fully
convective over much of the AM CVn phase and do not evolve adiabatically under
mass los... | astro-ph | abridged we calculate the full stellarstructural evolution of donors in am cvn systems formed through the wd channel coupled to the binarys evolution contrary to assumptions made in prior modelling these donors are not fully convective over much of the am cvn phase and do not evolve adiabatically under mass loss indefi... | [['abridged', 'we', 'calculate', 'the', 'full', 'stellarstructural', 'evolution', 'of', 'donors', 'in', 'am', 'cvn', 'systems', 'formed', 'through', 'the', 'wd', 'channel', 'coupled', 'to', 'the', 'binarys', 'evolution', 'contrary', 'to', 'assumptions', 'made', 'in', 'prior', 'modelling', 'these', 'donors', 'are', 'not... | [-0.12308431539572462, 0.22887212419647848, -0.07697761714729522, 0.06392276584068243, -0.03012430004852845, -0.10088291174711299, 0.10243382596118904, 0.40992864156350384, -0.23663061318585454, -0.34179433374040163, 0.09296173870749425, -0.2677539675072993, -0.03658207814789502, 0.1870980091973333, -0.0551769548623975... |
708.0221 | Neutral hydrogen in galactic fountains | Simulations of an isolated Milky Way-like galaxy, in which supernovae power a
galactic fountain, reproduce the observed velocity and 21cm brightness
statistics of galactic neutral hydrogen (HI). The simulated galaxy consists of
a thin HI disk, similar in extent and brightness to that observed in the Milky
Way, and ex... | astro-ph | simulations of an isolated milky waylike galaxy in which supernovae power a galactic fountain reproduce the observed velocity and 21cm brightness statistics of galactic neutral hydrogen hi the simulated galaxy consists of a thin hi disk similar in extent and brightness to that observed in the milky way and extraplanar ... | [['simulations', 'of', 'an', 'isolated', 'milky', 'waylike', 'galaxy', 'in', 'which', 'supernovae', 'power', 'a', 'galactic', 'fountain', 'reproduce', 'the', 'observed', 'velocity', 'and', '21cm', 'brightness', 'statistics', 'of', 'galactic', 'neutral', 'hydrogen', 'hi', 'the', 'simulated', 'galaxy', 'consists', 'of', ... | [-0.04303570989821868, 0.03443485954328165, -0.026749943573381344, 0.0722847602438066, -0.06244229878142585, 0.006128277153755627, 0.025771492242432425, 0.4097137156955517, -0.1841086246358761, -0.3142004077914205, -0.01916841436500396, -0.31253720254358586, 0.04222464450671343, 0.22364467165575627, 0.00731447937784259... |
708.0222 | Ignition and Propagation of Magnetic Avalanches in Mn$_{12}$-Acetate:
the effect of quantum tunneling | Using a wire heater to ignite magnetic avalanches in fixed magnetic field
applied along the easy axis of single crystals of the molecular magnet
Mn$_{12}$-acetate, we report fast local measurements of the temperature and
time-resolved measurements of the local magnetization as a function of magnetic
field. In additio... | cond-mat.mes-hall cond-mat.mtrl-sci | using a wire heater to ignite magnetic avalanches in fixed magnetic field applied along the easy axis of single crystals of the molecular magnet mn_12acetate we report fast local measurements of the temperature and timeresolved measurements of the local magnetization as a function of magnetic field in addition to confi... | [['using', 'a', 'wire', 'heater', 'to', 'ignite', 'magnetic', 'avalanches', 'in', 'fixed', 'magnetic', 'field', 'applied', 'along', 'the', 'easy', 'axis', 'of', 'single', 'crystals', 'of', 'the', 'molecular', 'magnet', 'mn_12acetate', 'we', 'report', 'fast', 'local', 'measurements', 'of', 'the', 'temperature', 'and', '... | [-0.1937390822802008, 0.2191387804445016, -0.04662867799670119, 0.008209991316819928, 0.0004367794062625425, -0.10217549649700906, 0.05316105667146441, 0.4041755360349552, -0.24833117882461891, -0.31875486230266464, 0.02008345613157684, -0.24314024433800854, -0.09523248165538631, 0.22694086748626582, 0.0753477155711002... |
708.0223 | Primordial non-Gaussianity from two curvaton decays | We study a model where two scalar fields, that are subdominant during
inflation, decay into radiation some time after inflation has ended but before
primordial nucleosynthesis. Perturbations of these two curvaton fields can be
responsible for the primordial curvature perturbation. We write down the full
non-linear eq... | hep-ph astro-ph | we study a model where two scalar fields that are subdominant during inflation decay into radiation some time after inflation has ended but before primordial nucleosynthesis perturbations of these two curvaton fields can be responsible for the primordial curvature perturbation we write down the full nonlinear equations... | [['we', 'study', 'a', 'model', 'where', 'two', 'scalar', 'fields', 'that', 'are', 'subdominant', 'during', 'inflation', 'decay', 'into', 'radiation', 'some', 'time', 'after', 'inflation', 'has', 'ended', 'but', 'before', 'primordial', 'nucleosynthesis', 'perturbations', 'of', 'these', 'two', 'curvaton', 'fields', 'can'... | [-0.1411569218424143, 0.2331776372305337, -0.06301890385699026, 0.14706347049006327, -0.051022935578611435, -0.113314158303936, -0.08312267463678008, 0.2645758007998596, -0.24946124685014698, -0.26396808674214944, 0.08699857653637719, -0.2701493692673316, -0.09473447260820562, 0.1509810608506179, 0.06019579577496999, -... |
708.0224 | Multisource Bayesian sequential change detection | Suppose that local characteristics of several independent compound Poisson
and Wiener processes change suddenly and simultaneously at some unobservable
disorder time. The problem is to detect the disorder time as quickly as
possible after it happens and minimize the rate of false alarms at the same
time. These proble... | math.ST cs.IT math.IT math.PR stat.TH | suppose that local characteristics of several independent compound poisson and wiener processes change suddenly and simultaneously at some unobservable disorder time the problem is to detect the disorder time as quickly as possible after it happens and minimize the rate of false alarms at the same time these problems a... | [['suppose', 'that', 'local', 'characteristics', 'of', 'several', 'independent', 'compound', 'poisson', 'and', 'wiener', 'processes', 'change', 'suddenly', 'and', 'simultaneously', 'at', 'some', 'unobservable', 'disorder', 'time', 'the', 'problem', 'is', 'to', 'detect', 'the', 'disorder', 'time', 'as', 'quickly', 'as',... | [-0.068754030762472, 0.12999497058725148, -0.06658186125771506, 0.08690053387272641, -0.08213536574838207, -0.16189654273372414, 0.10804907744244227, 0.3881214489004066, -0.3450039269375628, -0.282700854016171, 0.17109725221537125, -0.25682458041382306, -0.1458076796390944, 0.2139472134348347, -0.07991872628889798, 0.0... |
708.0225 | Symmetric groups and conjugacy classes | Let S_n be the symmetric group on n-letters. Fix n>5. Given any nontrivial
$\alpha,\beta\in S_n$, we prove that the product $\alpha^{S_n}\beta^{S_n}$ of
the conjugacy classes $\alpha^{S_n}$ and $\beta^{S_n}$ is never a conjugacy
class. Furthermore, if n is not even and $n$ is not a multiple of three, then
$\alpha^{S_... | math.GR | let s_n be the symmetric group on nletters fix n5 given any nontrivial alphabetain s_n we prove that the product alphas_nbetas_n of the conjugacy classes alphas_n and betas_n is never a conjugacy class furthermore if n is not even and n is not a multiple of three then alphas_nbetas_n is the union of at least three dist... | [['let', 's_n', 'be', 'the', 'symmetric', 'group', 'on', 'nletters', 'fix', 'n5', 'given', 'any', 'nontrivial', 'alphabetain', 's_n', 'we', 'prove', 'that', 'the', 'product', 'alphas_nbetas_n', 'of', 'the', 'conjugacy', 'classes', 'alphas_n', 'and', 'betas_n', 'is', 'never', 'a', 'conjugacy', 'class', 'furthermore', 'i... | [-0.1912697729981178, 0.16579750772904267, -0.0339107935607143, 0.021048100409702723, -0.039453389183557654, -0.166875954632732, -0.00282180378237715, 0.34225586888852055, -0.30781761269000446, -0.21963225750180035, 0.12074202486138501, -0.3189926404844631, -0.08645020851671889, 0.17620567616994504, -0.0741187408808376... |
708.0226 | GRB070610 : A Curious Galactic Transient | GRB 070610 is a typical high-energy event with a duration of 5s.Yet within
the burst localization we detect a highly unusual X-ray and optical transient,
SwiftJ195509.6+261406. We see high amplitude X-ray and optical variability on
very short time scales even at late times. Using near-infrared imaging assisted
by a l... | astro-ph | grb 070610 is a typical highenergy event with a duration of 5syet within the burst localization we detect a highly unusual xray and optical transient swiftj1955096261406 we see high amplitude xray and optical variability on very short time scales even at late times using nearinfrared imaging assisted by a laser guide s... | [['grb', '070610', 'is', 'a', 'typical', 'highenergy', 'event', 'with', 'a', 'duration', 'of', '5syet', 'within', 'the', 'burst', 'localization', 'we', 'detect', 'a', 'highly', 'unusual', 'xray', 'and', 'optical', 'transient', 'swiftj1955096261406', 'we', 'see', 'high', 'amplitude', 'xray', 'and', 'optical', 'variabili... | [-0.07217624275024005, 0.1259626511793575, -0.08010519413426326, 0.19536013734411717, -0.18068984984306224, -0.14251497964921994, 0.05251979034816481, 0.5025494000334388, -0.17868414890025885, -0.2850913923514584, 0.07912083810793005, -0.3384989955793759, -0.06732927320360628, 0.2890051296748912, -0.059375889950969554,... |
708.0227 | Lateral distribution and the energy determination of showers along the
ankle | The normalization constant of the lateral distribution function (LDF) of an
extensive air shower is a monotonous (almost linear) increasing function of the
energy of the primary. Therefore, the interpolated signal at some fixed
distance from the core can be calibrated to estimate the energy of the shower.
There is, s... | astro-ph | the normalization constant of the lateral distribution function ldf of an extensive air shower is a monotonous almost linear increasing function of the energy of the primary therefore the interpolated signal at some fixed distance from the core can be calibrated to estimate the energy of the shower there is somehow sur... | [['the', 'normalization', 'constant', 'of', 'the', 'lateral', 'distribution', 'function', 'ldf', 'of', 'an', 'extensive', 'air', 'shower', 'is', 'a', 'monotonous', 'almost', 'linear', 'increasing', 'function', 'of', 'the', 'energy', 'of', 'the', 'primary', 'therefore', 'the', 'interpolated', 'signal', 'at', 'some', 'fi... | [-0.11270451859696802, 0.1443805421548972, -0.11989223842515889, 0.0930849768027636, 0.001982174006487875, -0.04841346069949468, 0.009110421085063993, 0.39263105444120666, -0.28049458941975, -0.34859801136827384, 0.07907593303213889, -0.31174732022748813, -0.05658064331106474, 0.1577528479396889, -0.002534291040777725,... |
708.0228 | Optical Follow-up of New SMC Wing Be/X-ray Binaries | We investigate the optical counterparts of recently discovered Be/X-ray
binaries in the Small Magellanic Cloud. In total four sources, SXP101, SXP700,
SXP348 and SXP65.8 were detected during the Chandra Survey of the Wing of the
SMC. SXP700 and SXP65.8 were previously unknown. Many optical ground based
telescopes hav... | astro-ph | we investigate the optical counterparts of recently discovered bexray binaries in the small magellanic cloud in total four sources sxp101 sxp700 sxp348 and sxp658 were detected during the chandra survey of the wing of the smc sxp700 and sxp658 were previously unknown many optical ground based telescopes have been utili... | [['we', 'investigate', 'the', 'optical', 'counterparts', 'of', 'recently', 'discovered', 'bexray', 'binaries', 'in', 'the', 'small', 'magellanic', 'cloud', 'in', 'total', 'four', 'sources', 'sxp101', 'sxp700', 'sxp348', 'and', 'sxp658', 'were', 'detected', 'during', 'the', 'chandra', 'survey', 'of', 'the', 'wing', 'of'... | [-0.1127644793521012, 0.07159442499565381, -0.07733372271421456, 0.06502966777676897, -0.1034409155768733, -0.06717851100970179, 0.07709066332468102, 0.48148786180442377, -0.16055450986530032, -0.3234446724726548, 0.11189638810652879, -0.30058898090689085, -0.055808667105532464, 0.2198682612217512, -0.03127176877704539... |
708.0229 | Too small to form a galaxy: How the UV background determines the baryon
fraction | The cosmic ultraviolet background (UVB) heats the intergalactic medium (IGM),
as a result the gas in dark matter halos below a certain mass is too hot to
cool within a Hubble time. The UVB effectively suppresses the formation of
dwarf galaxies. Using high resolution cosmological hydrodynamical simulations
we show tha... | astro-ph | the cosmic ultraviolet background uvb heats the intergalactic medium igm as a result the gas in dark matter halos below a certain mass is too hot to cool within a hubble time the uvb effectively suppresses the formation of dwarf galaxies using high resolution cosmological hydrodynamical simulations we show that photo h... | [['the', 'cosmic', 'ultraviolet', 'background', 'uvb', 'heats', 'the', 'intergalactic', 'medium', 'igm', 'as', 'a', 'result', 'the', 'gas', 'in', 'dark', 'matter', 'halos', 'below', 'a', 'certain', 'mass', 'is', 'too', 'hot', 'to', 'cool', 'within', 'a', 'hubble', 'time', 'the', 'uvb', 'effectively', 'suppresses', 'the... | [-0.058139393713953096, 0.2077999702540825, -0.053468839862396644, 0.12612148945854595, -0.05139507015527629, -0.03217951112093209, 0.036689883792443916, 0.36580112506056306, -0.16615234546488455, -0.36348762532547857, 0.017318614303315088, -0.27872830979811, 0.0348018131482957, 0.17925883330108217, 0.00794532648038665... |
708.023 | Imaging spontaneous currents in superconducting arrays of pi-junctions | Superconductors separated by a thin tunneling barrier exhibit the Josephson
effect that allows charge transport at zero voltage, typically with no phase
shift between the superconductors in the lowest energy state. Recently,
Josephson junctions with ground state phase shifts of pi proposed by theory
three decades ago... | cond-mat.supr-con cond-mat.mes-hall | superconductors separated by a thin tunneling barrier exhibit the josephson effect that allows charge transport at zero voltage typically with no phase shift between the superconductors in the lowest energy state recently josephson junctions with ground state phase shifts of pi proposed by theory three decades ago have... | [['superconductors', 'separated', 'by', 'a', 'thin', 'tunneling', 'barrier', 'exhibit', 'the', 'josephson', 'effect', 'that', 'allows', 'charge', 'transport', 'at', 'zero', 'voltage', 'typically', 'with', 'no', 'phase', 'shift', 'between', 'the', 'superconductors', 'in', 'the', 'lowest', 'energy', 'state', 'recently', ... | [-0.27246486074069426, 0.2539638805870944, 0.005266933844481804, 0.017196172895068366, 0.015945830502781737, -0.21431675275192172, 0.0745779399619102, 0.39961147337493036, -0.21105172872213887, -0.27494736070757364, 0.0008151834263612016, -0.3096776097066753, -0.11325119061634692, 0.20953639773303503, 0.055998599666747... |
708.0231 | Forward inclusive dijet production and azimuthal correlations in pA
collisions | We derive forward inclusive dijet production in the scattering of a dilute
hadron off an arbitrary dense target, whose partons with small fraction of
momentum x are described by a Color Glass Condensate. Both multiple scattering
and non-linear QCD evolution at small-x are included. This is of relevance for
measuremen... | hep-ph nucl-th | we derive forward inclusive dijet production in the scattering of a dilute hadron off an arbitrary dense target whose partons with small fraction of momentum x are described by a color glass condensate both multiple scattering and nonlinear qcd evolution at smallx are included this is of relevance for measurements of t... | [['we', 'derive', 'forward', 'inclusive', 'dijet', 'production', 'in', 'the', 'scattering', 'of', 'a', 'dilute', 'hadron', 'off', 'an', 'arbitrary', 'dense', 'target', 'whose', 'partons', 'with', 'small', 'fraction', 'of', 'momentum', 'x', 'are', 'described', 'by', 'a', 'color', 'glass', 'condensate', 'both', 'multiple... | [-0.06408127270419192, 0.3048330818506002, -0.17345880164000926, 0.12908008106424357, -0.005641586796035257, -0.07880359080690744, -0.05497729749905385, 0.3689627941028121, -0.2272264595180122, -0.20993559001657192, -0.06400004962427813, -0.3649624955704373, 0.09771352372749635, 0.10648183349070003, 0.08478258225250612... |
708.0232 | Nucleon Spin Structure with hadronic collisions at COMPASS | In order to illustrate the capabilities of COMPASS using a hadronic beam, I
review some of the azimuthal asymmetries in hadronic collisions, that allow for
the extraction of transversity, Sivers and Boer-Mulders functions, necessary to
explore the partonic spin structure of the nucleon. I also report on some Monte
Ca... | hep-ph | in order to illustrate the capabilities of compass using a hadronic beam i review some of the azimuthal asymmetries in hadronic collisions that allow for the extraction of transversity sivers and boermulders functions necessary to explore the partonic spin structure of the nucleon i also report on some monte carlo simu... | [['in', 'order', 'to', 'illustrate', 'the', 'capabilities', 'of', 'compass', 'using', 'a', 'hadronic', 'beam', 'i', 'review', 'some', 'of', 'the', 'azimuthal', 'asymmetries', 'in', 'hadronic', 'collisions', 'that', 'allow', 'for', 'the', 'extraction', 'of', 'transversity', 'sivers', 'and', 'boermulders', 'functions', '... | [-0.04616708015187401, 0.24510841048641563, -0.15004658944624133, 0.16221037452198464, -0.042183366387266004, -0.02495472564613957, -0.025340974206513125, 0.39603152544531106, -0.1989270681770493, -0.16412519696742706, -0.08535743498702673, -0.3256473500434666, 0.05708859621049606, 0.12728123255839494, 0.14335717776892... |
708.0233 | EBIT Charge-Exchange Measurements and Astrophysical Applications | The past decade has seen a surge of interest in astrophysical charge exchange
(CX). The impetus was the discovery of X-ray emission from comets in 1996, soon
followed by the observation of CX emission in planetary atmospheres and
throughout the heliosphere. Geocoronal and heliospheric CX are now recognized
to contrib... | astro-ph | the past decade has seen a surge of interest in astrophysical charge exchange cx the impetus was the discovery of xray emission from comets in 1996 soon followed by the observation of cx emission in planetary atmospheres and throughout the heliosphere geocoronal and heliospheric cx are now recognized to contribute a co... | [['the', 'past', 'decade', 'has', 'seen', 'a', 'surge', 'of', 'interest', 'in', 'astrophysical', 'charge', 'exchange', 'cx', 'the', 'impetus', 'was', 'the', 'discovery', 'of', 'xray', 'emission', 'from', 'comets', 'in', '1996', 'soon', 'followed', 'by', 'the', 'observation', 'of', 'cx', 'emission', 'in', 'planetary', '... | [-0.043599398660233185, 0.1490043482532905, -0.013611315037950033, 0.09132917665485893, -0.08641103289330439, -0.04428904232073335, 0.03743936997958489, 0.4306054756405853, -0.25144294970819064, -0.2871324636432673, 0.053348280740113205, -0.356833245815529, -0.041684342386771836, 0.2343070110861933, -0.0367701754214302... |
708.0234 | Heat Kernel Asymptotics on Homogeneous Bundles | We consider Laplacians acting on sections of homogeneous vector bundles over
symmetric spaces. By using an integral representation of the heat semi-group we
find a formal solution for the heat kernel diagonal that gives a generating
function for the whole sequence of heat invariants. We argue that the obtained
formal... | math.DG hep-th math-ph math.AP math.MP | we consider laplacians acting on sections of homogeneous vector bundles over symmetric spaces by using an integral representation of the heat semigroup we find a formal solution for the heat kernel diagonal that gives a generating function for the whole sequence of heat invariants we argue that the obtained formal solu... | [['we', 'consider', 'laplacians', 'acting', 'on', 'sections', 'of', 'homogeneous', 'vector', 'bundles', 'over', 'symmetric', 'spaces', 'by', 'using', 'an', 'integral', 'representation', 'of', 'the', 'heat', 'semigroup', 'we', 'find', 'a', 'formal', 'solution', 'for', 'the', 'heat', 'kernel', 'diagonal', 'that', 'gives'... | [-0.1503634514251294, 0.01255992158571294, -0.07316030220558437, 0.09973759413338625, -0.11833368152953111, -0.07868284029313005, 0.03528144411348666, 0.3759094669841803, -0.28573578673486527, -0.1447970034697881, 0.11165519474933927, -0.2904276233166456, -0.1532337714273196, 0.2428226249722334, -0.0023521206556604457,... |
708.0235 | Indirect signals from braneworlds | It has been suggested that our universe could be a 3-dimensional brane where
the SM fields live embedded in a D-dimensional space-time. In flexible
raneworlds, in addition to the SM fields, new degrees of freedom appear on the
brane associated to brane fluctuations. These new fields, known as branons, are
standard WI... | astro-ph hep-ph | it has been suggested that our universe could be a 3dimensional brane where the sm fields live embedded in a ddimensional spacetime in flexible raneworlds in addition to the sm fields new degrees of freedom appear on the brane associated to brane fluctuations these new fields known as branons are standard wimps weakly ... | [['it', 'has', 'been', 'suggested', 'that', 'our', 'universe', 'could', 'be', 'a', '3dimensional', 'brane', 'where', 'the', 'sm', 'fields', 'live', 'embedded', 'in', 'a', 'ddimensional', 'spacetime', 'in', 'flexible', 'raneworlds', 'in', 'addition', 'to', 'the', 'sm', 'fields', 'new', 'degrees', 'of', 'freedom', 'appea... | [-0.13511529598962252, 0.24790197055996724, -0.0918563176602335, 0.12598163200850584, -0.13205476839121588, -0.13728305057320797, -0.05280158847314634, 0.28909386183925523, -0.18779111709970403, -0.30175393369888337, 0.03408956615595331, -0.26117102193160796, -0.09309811768790996, 0.12605810466035544, -0.02722538149797... |
708.0236 | The Chemical Evolution Of High Z Galaxies From The Relative Abundances
Of N, Si, S, And Fe In Damped Lyman Alpha Systems | Abundances of N, Si, S, and Fe for 45 damped Lyman alpha systems (DLAs) have
been compiled and detailed one-zone chemical evolution models have been
constructed for 30 of them. Assuming continuous star formation, we found that
final abundances in each object can be modelled by adjusting only two
parameters, i.e. its ... | astro-ph | abundances of n si s and fe for 45 damped lyman alpha systems dlas have been compiled and detailed onezone chemical evolution models have been constructed for 30 of them assuming continuous star formation we found that final abundances in each object can be modelled by adjusting only two parameters ie its timeaveraged ... | [['abundances', 'of', 'n', 'si', 's', 'and', 'fe', 'for', '45', 'damped', 'lyman', 'alpha', 'systems', 'dlas', 'have', 'been', 'compiled', 'and', 'detailed', 'onezone', 'chemical', 'evolution', 'models', 'have', 'been', 'constructed', 'for', '30', 'of', 'them', 'assuming', 'continuous', 'star', 'formation', 'we', 'foun... | [-0.026926600765706837, 0.17430131917487288, -0.024218585990045383, 0.09685206281444157, -0.06213343737462473, -0.09588837134314404, 0.049196472074296595, 0.46249668836449653, -0.1589429237978794, -0.3774876437199995, 0.018447912798672556, -0.2760455261753953, -0.008612379197769119, 0.17900627817573916, -0.047239115069... |
708.0237 | Fractal states in quantum information processing | The fractal character of some quantum properties has been shown for systems
described by continuous variables. Here, a definition of quantum fractal states
is given that suits the discrete systems used in quantum information
processing, including quantum coding and quantum computing. Several important
examples are pr... | quant-ph | the fractal character of some quantum properties has been shown for systems described by continuous variables here a definition of quantum fractal states is given that suits the discrete systems used in quantum information processing including quantum coding and quantum computing several important examples are provided | [['the', 'fractal', 'character', 'of', 'some', 'quantum', 'properties', 'has', 'been', 'shown', 'for', 'systems', 'described', 'by', 'continuous', 'variables', 'here', 'a', 'definition', 'of', 'quantum', 'fractal', 'states', 'is', 'given', 'that', 'suits', 'the', 'discrete', 'systems', 'used', 'in', 'quantum', 'informa... | [-0.128991892315832, 0.15949466320402597, -0.12035941017751137, 0.08972696952127002, 0.0016736770858583243, -0.1931082216678592, -0.026932938950662705, 0.33914309092189954, -0.2867854974920983, -0.22040538858298375, 0.12189440034917029, -0.2594802296295276, -0.2366924720370899, 0.29567707417046896, -0.08542698740189814... |
708.0238 | On the 2-point function of the O(N) model | The self-energy of the critical 3-dimensional O(N) model is calculated. The
analysis is performed in the context of the Non-Perturbative Renormalization
Group, by exploiting an approximation which takes into account contributions of
an infinite number of vertices. A very simple calculation yields the 2-point
function... | cond-mat.stat-mech hep-th | the selfenergy of the critical 3dimensional on model is calculated the analysis is performed in the context of the nonperturbative renormalization group by exploiting an approximation which takes into account contributions of an infinite number of vertices a very simple calculation yields the 2point function in the who... | [['the', 'selfenergy', 'of', 'the', 'critical', '3dimensional', 'on', 'model', 'is', 'calculated', 'the', 'analysis', 'is', 'performed', 'in', 'the', 'context', 'of', 'the', 'nonperturbative', 'renormalization', 'group', 'by', 'exploiting', 'an', 'approximation', 'which', 'takes', 'into', 'account', 'contributions', 'o... | [-0.10725563244894147, 0.09988622804899933, -0.12229029111331328, 0.07568915269337595, -0.028112254911102353, -0.06973168271128088, 0.0448356593772769, 0.3476736132055521, -0.2073464147374034, -0.27856541814282537, 0.00604944258229807, -0.29242056868039074, -0.08809807408833877, 0.2048232643562369, 0.0164709135517478, ... |
708.0239 | Minimal Universal Extra Dimensions | Highly degenerate spectra associated with universal extra dimensions (UED)
provide an interesting phenomenology not only from the point of view of
cosmology and astrophysics, but also for colliders. We study these exotic
signals for the simplest case, called minimal UED, where it is natural to find
slow charged parti... | hep-ph | highly degenerate spectra associated with universal extra dimensions ued provide an interesting phenomenology not only from the point of view of cosmology and astrophysics but also for colliders we study these exotic signals for the simplest case called minimal ued where it is natural to find slow charged particles dis... | [['highly', 'degenerate', 'spectra', 'associated', 'with', 'universal', 'extra', 'dimensions', 'ued', 'provide', 'an', 'interesting', 'phenomenology', 'not', 'only', 'from', 'the', 'point', 'of', 'view', 'of', 'cosmology', 'and', 'astrophysics', 'but', 'also', 'for', 'colliders', 'we', 'study', 'these', 'exotic', 'sign... | [-0.08842249064233214, 0.2493215883614972, -0.03863468449858446, 0.1583514226367697, -0.11558712425360841, -0.29086174894242534, -0.04686531810356038, 0.30444748756579226, -0.228428233326191, -0.30444405507296324, 0.0442845484995771, -0.32123475551368696, -0.08126213188682284, 0.17075133702111622, -0.01924148586297792,... |
708.024 | Double Horizon Limit, AdS Geometry and Entropy Function | We start from a generic metric which describes four dimensional stationary
black holes in an arbitrary theory of gravity and show that the AdS_2 part of
the near horizon geometry is a consequence of the double-horizon limit and
finiteness . We also show that the field configurations of the near horizon are
determined... | hep-th | we start from a generic metric which describes four dimensional stationary black holes in an arbitrary theory of gravity and show that the ads_2 part of the near horizon geometry is a consequence of the doublehorizon limit and finiteness we also show that the field configurations of the near horizon are determined if t... | [['we', 'start', 'from', 'a', 'generic', 'metric', 'which', 'describes', 'four', 'dimensional', 'stationary', 'black', 'holes', 'in', 'an', 'arbitrary', 'theory', 'of', 'gravity', 'and', 'show', 'that', 'the', 'ads_2', 'part', 'of', 'the', 'near', 'horizon', 'geometry', 'is', 'a', 'consequence', 'of', 'the', 'doublehor... | [-0.12961398395802826, 0.11228257618495263, -0.12310245802998543, 0.049723466956987976, -0.02542352285794914, -0.07394961550086737, -0.03390159427840263, 0.28746376898884773, -0.26434972853958605, -0.2659654242545366, 0.13685541486553848, -0.2792913987413049, -0.1444958624597639, 0.21225380028784274, -0.061940458111464... |
708.0241 | The impact of the fourth SM family on the Higgs observability at the LHC | It is shown that if the fourth SM fermion family exists then the Higgs boson
could be observed at the LHC with an integrated luminosity of few fb-1. The
Higgs discovery potential for different channels is discussed in the presence
of the fourth SM family.
| hep-ph | it is shown that if the fourth sm fermion family exists then the higgs boson could be observed at the lhc with an integrated luminosity of few fb1 the higgs discovery potential for different channels is discussed in the presence of the fourth sm family | [['it', 'is', 'shown', 'that', 'if', 'the', 'fourth', 'sm', 'fermion', 'family', 'exists', 'then', 'the', 'higgs', 'boson', 'could', 'be', 'observed', 'at', 'the', 'lhc', 'with', 'an', 'integrated', 'luminosity', 'of', 'few', 'fb1', 'the', 'higgs', 'discovery', 'potential', 'for', 'different', 'channels', 'is', 'discus... | [-0.07594693890617539, 0.22416181865749726, -0.0123270059728788, 0.13315861279455324, -0.0977196001344257, -0.18978668799002965, -0.05041379845804638, 0.3342308706707425, -0.25924022982103956, -0.2709306422414051, 0.037053819174050456, -0.3446268134439985, -0.022607106073862977, 0.15897084070990483, 0.05920036070876651... |
708.0242 | Distributing the Kalman Filter for Large-Scale Systems | This paper derives a \emph{distributed} Kalman filter to estimate a sparsely
connected, large-scale, $n-$dimensional, dynamical system monitored by a
network of $N$ sensors. Local Kalman filters are implemented on the
($n_l-$dimensional, where $n_l\ll n$) sub-systems that are obtained after
spatially decomposing the ... | cs.IT math.IT | this paper derives a emphdistributed kalman filter to estimate a sparsely connected largescale ndimensional dynamical system monitored by a network of n sensors local kalman filters are implemented on the n_ldimensional where n_lll n subsystems that are obtained after spatially decomposing the largescale system the res... | [['this', 'paper', 'derives', 'a', 'emphdistributed', 'kalman', 'filter', 'to', 'estimate', 'a', 'sparsely', 'connected', 'largescale', 'ndimensional', 'dynamical', 'system', 'monitored', 'by', 'a', 'network', 'of', 'n', 'sensors', 'local', 'kalman', 'filters', 'are', 'implemented', 'on', 'the', 'n_ldimensional', 'wher... | [-0.15535322608547691, 0.050732285237514274, -0.073522386426592, 0.017725203603850274, -0.029411627113333214, -0.1842030942308433, 0.026130973363457165, 0.3829031692129438, -0.31395605027108736, -0.28291949698620517, 0.14887883187140055, -0.2571437619236784, -0.15215919959870086, 0.1195196625918312, -0.0697537134620411... |
708.0243 | Effects of Orbital Eccentricity on Extrasolar Planet Transit Detection
and Lightcurves | It is shown herein that planets with eccentric orbits are more likely to
transit than circularly orbiting planets with the same semimajor axis by a
factor of (1-e^2)^{-1}. If the orbital parameters of discovered transiting
planets are known, as from follow-up radial velocity observations, then the
transit-detected pl... | astro-ph | it is shown herein that planets with eccentric orbits are more likely to transit than circularly orbiting planets with the same semimajor axis by a factor of 1e21 if the orbital parameters of discovered transiting planets are known as from followup radial velocity observations then the transitdetected planet population... | [['it', 'is', 'shown', 'herein', 'that', 'planets', 'with', 'eccentric', 'orbits', 'are', 'more', 'likely', 'to', 'transit', 'than', 'circularly', 'orbiting', 'planets', 'with', 'the', 'same', 'semimajor', 'axis', 'by', 'a', 'factor', 'of', '1e21', 'if', 'the', 'orbital', 'parameters', 'of', 'discovered', 'transiting',... | [-0.13943597299900526, 0.2057624593997612, -0.10597694484443453, 0.04624642647870228, -0.1622904225859154, -0.08984616114410751, 0.09242998484497596, 0.3583792469243666, -0.18348638228908704, -0.33650844370162014, 0.09186161667406723, -0.29194030551272526, -0.08007031597050004, 0.25317639267692965, -0.13378653497835458... |
708.0244 | Extracting current-induced spins: spin boundary conditions at narrow
Hall contacts | We consider the possibility to extract spins that are generated by an
electric current in a two-dimensional electron gas with Rashba-Dresselhaus
spin-orbit interaction (R2DEG) in the Hall geometry. To this end, we discuss
boundary conditions for the spin accumulations between a spin-orbit coupled
region and contact w... | cond-mat.mes-hall | we consider the possibility to extract spins that are generated by an electric current in a twodimensional electron gas with rashbadresselhaus spinorbit interaction r2deg in the hall geometry to this end we discuss boundary conditions for the spin accumulations between a spinorbit coupled region and contact without spi... | [['we', 'consider', 'the', 'possibility', 'to', 'extract', 'spins', 'that', 'are', 'generated', 'by', 'an', 'electric', 'current', 'in', 'a', 'twodimensional', 'electron', 'gas', 'with', 'rashbadresselhaus', 'spinorbit', 'interaction', 'r2deg', 'in', 'the', 'hall', 'geometry', 'to', 'this', 'end', 'we', 'discuss', 'bou... | [-0.1844642637226028, 0.18988931550171528, 0.018450094695333718, -0.003852028465061857, -0.02098442934118538, -0.13226189225781382, 0.03793012990469211, 0.3903831227911277, -0.2692747227633127, -0.2629612145634989, -0.007465534456474543, -0.3046048151231126, -0.08613553533551137, 0.1948971760933075, 0.03062860326680126... |
708.0245 | Simplicity of C*-algebras associated to row-finite locally convex
higher-rank graphs | In previous work, the authors showed that the C*-algebra C*(\Lambda) of a
row-finite higher-rank graph \Lambda with no sources is simple if and only if
\Lambda is both cofinal and aperiodic. In this paper, we generalise this result
to row-finite higher-rank graphs which are locally convex (but may contain
sources). O... | math.OA | in previous work the authors showed that the calgebra clambda of a rowfinite higherrank graph lambda with no sources is simple if and only if lambda is both cofinal and aperiodic in this paper we generalise this result to rowfinite higherrank graphs which are locally convex but may contain sources our main tool is fart... | [['in', 'previous', 'work', 'the', 'authors', 'showed', 'that', 'the', 'calgebra', 'clambda', 'of', 'a', 'rowfinite', 'higherrank', 'graph', 'lambda', 'with', 'no', 'sources', 'is', 'simple', 'if', 'and', 'only', 'if', 'lambda', 'is', 'both', 'cofinal', 'and', 'aperiodic', 'in', 'this', 'paper', 'we', 'generalise', 'th... | [-0.11437623829052816, 0.15116534105479895, -0.0586761408984395, 0.04699835991292881, -0.19927433898140276, -0.1544730997910457, -0.0437422648135994, 0.49591676030485404, -0.3215406407280603, -0.22204182603551695, 0.0900274925488269, -0.32426496314084424, -0.14654107108002618, 0.14811363571234756, -0.17061010899487883,... |
708.0246 | Severe right Ore sets and universal localisation | We introduce the notion of a severe right Ore set in the main as a tool to
study universal localisations of rings but also to provide a short proof of P.
M. Cohn's classification of homomorphisms from a ring to a division ring. We
prove that the category of finitely presented modules over a universal
localisation is ... | math.RA | we introduce the notion of a severe right ore set in the main as a tool to study universal localisations of rings but also to provide a short proof of p m cohns classification of homomorphisms from a ring to a division ring we prove that the category of finitely presented modules over a universal localisation is equiva... | [['we', 'introduce', 'the', 'notion', 'of', 'a', 'severe', 'right', 'ore', 'set', 'in', 'the', 'main', 'as', 'a', 'tool', 'to', 'study', 'universal', 'localisations', 'of', 'rings', 'but', 'also', 'to', 'provide', 'a', 'short', 'proof', 'of', 'p', 'm', 'cohns', 'classification', 'of', 'homomorphisms', 'from', 'a', 'rin... | [-0.17767906466244973, -0.01716814971895832, -0.1180936539348102, 0.045625130598894274, -0.04404233918158394, -0.15255138582803987, -0.03777796375292419, 0.32629372815441604, -0.4121091900148777, -0.1619745611137889, 0.1110310189254262, -0.16996862587646577, -0.10104618001390588, 0.23945321320236257, -0.161953892445925... |
708.0247 | Dark Matter Decaying Now | The instability of dark matter may produce visible signals in the spectrum of
cosmic gamma-rays. We consider this possibility in frameworks with additional
spatial dimensions and supersymmetry. Examples of particles include
superweakly-interacting massive particles such as gravitinos in supersymmetry
models, the ligh... | astro-ph hep-ph | the instability of dark matter may produce visible signals in the spectrum of cosmic gammarays we consider this possibility in frameworks with additional spatial dimensions and supersymmetry examples of particles include superweaklyinteracting massive particles such as gravitinos in supersymmetry models the lightest ka... | [['the', 'instability', 'of', 'dark', 'matter', 'may', 'produce', 'visible', 'signals', 'in', 'the', 'spectrum', 'of', 'cosmic', 'gammarays', 'we', 'consider', 'this', 'possibility', 'in', 'frameworks', 'with', 'additional', 'spatial', 'dimensions', 'and', 'supersymmetry', 'examples', 'of', 'particles', 'include', 'sup... | [-0.11840399913489819, 0.3223068244289607, -0.029790912258128324, 0.19680661551925974, -0.05323196823398272, -0.17647212535763782, -0.07361175348050893, 0.2979219723997327, -0.1589490698184818, -0.3501919482524196, 0.022058364677165324, -0.2824669486416193, -0.04937361621608337, 0.0656338486665239, -0.00202194362257917... |
708.0248 | Higgs decays in supersymmetric models with light neutralinos | In the Minimal Supersymmetric Standard Model, neutralinos lighter than 50 GeV
are compatible with all accelerator, precision, and cosmological bounds. Such
neutralinos might constitute a relevant decay channel for the Higgs boson,
modifying its expected signatures at hadron colliders. We study the branching
ratio h -... | hep-ph | in the minimal supersymmetric standard model neutralinos lighter than 50 gev are compatible with all accelerator precision and cosmological bounds such neutralinos might constitute a relevant decay channel for the higgs boson modifying its expected signatures at hadron colliders we study the branching ratio h chichi an... | [['in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'neutralinos', 'lighter', 'than', '50', 'gev', 'are', 'compatible', 'with', 'all', 'accelerator', 'precision', 'and', 'cosmological', 'bounds', 'such', 'neutralinos', 'might', 'constitute', 'a', 'relevant', 'decay', 'channel', 'for', 'the', 'higgs', 'boso... | [-0.07546300010039642, 0.30677779918156, -0.018721979577094316, 0.17709830948351932, -0.06465383024225312, -0.22031235625286416, 0.0195413321276666, 0.31005992933166443, -0.23127769181124305, -0.2702415736932908, 0.024751439872097665, -0.2946113121185091, 0.03166163933553522, 0.17870375409256667, 0.06415550953236669, 0... |
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