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 |
|---|---|---|---|---|---|---|
706.2014 | Fourier analysis of active-region plage | We study the dynamical interaction of the solar chromosphere with the
transition region in mossy and non-mossy active-region plage. We carefully
align image sequences taken with the Transition Region And Coronal Explorer
(TRACE) in the ultraviolet passbands around 1550, 1600, and 1700 A and the
extreme ultraviolet pa... | astro-ph | we study the dynamical interaction of the solar chromosphere with the transition region in mossy and nonmossy activeregion plage we carefully align image sequences taken with the transition region and coronal explorer trace in the ultraviolet passbands around 1550 1600 and 1700 a and the extreme ultraviolet passbands a... | [['we', 'study', 'the', 'dynamical', 'interaction', 'of', 'the', 'solar', 'chromosphere', 'with', 'the', 'transition', 'region', 'in', 'mossy', 'and', 'nonmossy', 'activeregion', 'plage', 'we', 'carefully', 'align', 'image', 'sequences', 'taken', 'with', 'the', 'transition', 'region', 'and', 'coronal', 'explorer', 'tra... | [-0.08926161291441859, 0.2170159327324928, -0.0025265402114850338, 0.11897491984886881, -0.02889124679211107, -0.08914850529544126, 0.09096071286620643, 0.476112402411864, -0.21579401368009193, -0.3294117494234185, 0.0783767025284049, -0.3368173331596461, -0.13016990554708063, 0.16593965228657498, -0.01708189460142127,... |
706.2015 | Infrared Limit of Gluon Amplitudes at Strong Coupling | In this note, we propose that the infrared structure of gluon amplitudes at
strong coupling can be fully extracted from a local consideration near cusps.
This is consistent with field theory and correctly reproduces the infrared
divergences of the four-gluon amplitude at strong coupling calculated recently
by Alday a... | hep-th | in this note we propose that the infrared structure of gluon amplitudes at strong coupling can be fully extracted from a local consideration near cusps this is consistent with field theory and correctly reproduces the infrared divergences of the fourgluon amplitude at strong coupling calculated recently by alday and ma... | [['in', 'this', 'note', 'we', 'propose', 'that', 'the', 'infrared', 'structure', 'of', 'gluon', 'amplitudes', 'at', 'strong', 'coupling', 'can', 'be', 'fully', 'extracted', 'from', 'a', 'local', 'consideration', 'near', 'cusps', 'this', 'is', 'consistent', 'with', 'field', 'theory', 'and', 'correctly', 'reproduces', 't... | [-0.11319926614873112, 0.14967199021950364, -0.16335539933294058, 0.11430057677207514, -0.023654261622577905, -0.07034963528625666, 0.005616230412852019, 0.36210604760795834, -0.20333498097956182, -0.2554868195950985, 0.0046388721815310415, -0.2903074631973868, -0.18922274187207222, 0.09640684711746872, -0.014316606316... |
706.2016 | Observations of Water Masers in the NGC 1333 IRAS 4 Region | The NGC 1333 IRAS 4 region was observed in the 22 GHz H2O maser line with an
angular resolution of about 0.08 arcseconds. Two groups of masers were
detected, one near IRAS 4A and the other near BI. Among the eight maser spots
detected near IRAS 4A, six spots are located close to A2, within 100 AU, and
the maser veloc... | astro-ph | the ngc 1333 iras 4 region was observed in the 22 ghz h2o maser line with an angular resolution of about 008 arcseconds two groups of masers were detected one near iras 4a and the other near bi among the eight maser spots detected near iras 4a six spots are located close to a2 within 100 au and the maser velocities are... | [['the', 'ngc', '1333', 'iras', '4', 'region', 'was', 'observed', 'in', 'the', '22', 'ghz', 'h2o', 'maser', 'line', 'with', 'an', 'angular', 'resolution', 'of', 'about', '008', 'arcseconds', 'two', 'groups', 'of', 'masers', 'were', 'detected', 'one', 'near', 'iras', '4a', 'and', 'the', 'other', 'near', 'bi', 'among', '... | [-0.11103858561359513, 0.08634081838485705, 0.054253291741658285, 0.003938646916618055, -0.07534667268658105, -0.15723846352790508, -0.022011708706999436, 0.5088923979932681, -0.1264005677150682, -0.2715461340565712, 0.08348959053341204, -0.31732671420710784, 0.0400978407318083, 0.15085552578481534, 0.00231377199237706... |
706.2017 | Twisted Alexander polynomial of links in the projective space | We use Reidemeister torsion to study a twisted Alexander polynomial, as
defined by Turaev, for links in the projective space. Using sign-refined
torsion we derive a skein relation for a normalized form of this polynomial.
| math.GT | we use reidemeister torsion to study a twisted alexander polynomial as defined by turaev for links in the projective space using signrefined torsion we derive a skein relation for a normalized form of this polynomial | [['we', 'use', 'reidemeister', 'torsion', 'to', 'study', 'a', 'twisted', 'alexander', 'polynomial', 'as', 'defined', 'by', 'turaev', 'for', 'links', 'in', 'the', 'projective', 'space', 'using', 'signrefined', 'torsion', 'we', 'derive', 'a', 'skein', 'relation', 'for', 'a', 'normalized', 'form', 'of', 'this', 'polynomia... | [-0.2873535770922899, 0.06384864635765553, -0.11208483810935702, 0.11884466360123562, -0.1744513918778726, -0.13426485595160298, -0.01136853609766279, 0.3170712911656925, -0.348353723217068, -0.26105123021240745, 0.003759223099664918, -0.15137702664027788, -0.21045626167740142, 0.20068675812466868, -0.15338144475328072... |
706.2018 | Space-like and time-like pion-rho transition form factors in the
light-cone formalism | Having calculated the light-cone wave function of the pseudoscalar meson by
using two equivalent and fully covariant methods, we generalize such methods to
the valence Fock states of the vector meson in the light-cone formalism. We
investigate the decay constant of the $\rho$ meson $f_{\rho}$, the
$\gamma^{\ast} \pi ... | hep-ph | having calculated the lightcone wave function of the pseudoscalar meson by using two equivalent and fully covariant methods we generalize such methods to the valence fock states of the vector meson in the lightcone formalism we investigate the decay constant of the rho meson f_rho the gammaast pi to rho and gamma rho t... | [['having', 'calculated', 'the', 'lightcone', 'wave', 'function', 'of', 'the', 'pseudoscalar', 'meson', 'by', 'using', 'two', 'equivalent', 'and', 'fully', 'covariant', 'methods', 'we', 'generalize', 'such', 'methods', 'to', 'the', 'valence', 'fock', 'states', 'of', 'the', 'vector', 'meson', 'in', 'the', 'lightcone', '... | [-0.1234990471197913, 0.2378022249167164, -0.08360380129306577, 0.10188939375414824, -0.05932453585167726, -0.07763330814001772, 0.10446774238437986, 0.3588384606565038, -0.21499947014575202, -0.19867457340781888, -0.039687767958578965, -0.3058013104988883, -0.07575175099967359, 0.09023290101419358, 0.10875216356556242... |
706.2019 | An operational interpretation for multipartite entanglement | We introduce an operational interpretation for pure-state global multipartite
entanglement based on quantum estimation. We show that the estimation of the
strength of low-noise locally depolarizing channels, as quantified by the
regularized quantum Fisher information, is directly related to the
Meyer-Wallach multipar... | quant-ph | we introduce an operational interpretation for purestate global multipartite entanglement based on quantum estimation we show that the estimation of the strength of lownoise locally depolarizing channels as quantified by the regularized quantum fisher information is directly related to the meyerwallach multipartite ent... | [['we', 'introduce', 'an', 'operational', 'interpretation', 'for', 'purestate', 'global', 'multipartite', 'entanglement', 'based', 'on', 'quantum', 'estimation', 'we', 'show', 'that', 'the', 'estimation', 'of', 'the', 'strength', 'of', 'lownoise', 'locally', 'depolarizing', 'channels', 'as', 'quantified', 'by', 'the', ... | [-0.1414296163560508, 0.16934369511274144, -0.0957826281317159, 0.06897930512295479, 0.04767272577850849, -0.1641654453978136, 0.03931388747878373, 0.3492857202821012, -0.2555963357248307, -0.22124241536797642, 0.07008151803165674, -0.26787624458552567, -0.12400853740317481, 0.1760891421226325, -0.09498899062345555, 0.... |
706.202 | Eigenvalue statistics of the real Ginibre ensemble | The real Ginibre ensemble consists of random $N \times N$ matrices formed
from i.i.d. standard Gaussian entries. By using the method of skew orthogonal
polynomials, the general $n$-point correlations for the real eigenvalues, and
for the complex eigenvalues, are given as $n \times n$ Pfaffians with explicit
entries. ... | cond-mat.stat-mech | the real ginibre ensemble consists of random n times n matrices formed from iid standard gaussian entries by using the method of skew orthogonal polynomials the general npoint correlations for the real eigenvalues and for the complex eigenvalues are given as n times n pfaffians with explicit entries a computationally t... | [['the', 'real', 'ginibre', 'ensemble', 'consists', 'of', 'random', 'n', 'times', 'n', 'matrices', 'formed', 'from', 'iid', 'standard', 'gaussian', 'entries', 'by', 'using', 'the', 'method', 'of', 'skew', 'orthogonal', 'polynomials', 'the', 'general', 'npoint', 'correlations', 'for', 'the', 'real', 'eigenvalues', 'and'... | [-0.14239612453289935, 0.1253258564644745, -0.0005515020189655794, 0.0740701283746701, 0.014244224901336271, -0.11061660879341936, -0.003663590328918921, 0.33431274203482914, -0.1925430955189104, -0.20664728346683486, 0.08833382668829448, -0.3154928675991156, -0.22038034271178264, 0.14670275496570645, -0.00060082064639... |
706.2021 | Structural fingerprinting in the transmission electron microscope:
Overview and opportunities to implement enhanced strategies for nanocrystal
identification | This paper illustrates the prospective need for structural fingerprinting
methods for nanocrystals. A review of the existing fingerprinting methods for
crystal structures by means of transmission electron microscopy which work for
a single setting of the specimen goniometer is given. Suggestions are made on
how some ... | cond-mat.mtrl-sci | this paper illustrates the prospective need for structural fingerprinting methods for nanocrystals a review of the existing fingerprinting methods for crystal structures by means of transmission electron microscopy which work for a single setting of the specimen goniometer is given suggestions are made on how some of t... | [['this', 'paper', 'illustrates', 'the', 'prospective', 'need', 'for', 'structural', 'fingerprinting', 'methods', 'for', 'nanocrystals', 'a', 'review', 'of', 'the', 'existing', 'fingerprinting', 'methods', 'for', 'crystal', 'structures', 'by', 'means', 'of', 'transmission', 'electron', 'microscopy', 'which', 'work', 'f... | [-0.0870493162650879, 0.08338507998916789, -0.07319387834144347, 0.032463179056521324, -0.07402665692341809, -0.15762735556572585, 0.04781008618259121, 0.4304800109281886, -0.26286133249267574, -0.28702570467324157, 0.10896764043931531, -0.2851854870393986, -0.15743933941334168, 0.22803456730794208, -0.0812690911705253... |
706.2022 | The Unusual Spectrum of Comet 96P/Machholz | We report spectra from 3000-5900 A for comet 96P/Machholz, obtained on 2007
Apr 27 UT with the 3-m Shane telescope at Lick Observatory. The spectra are
extremely carbon poor, and show a prominent NH_2 series, but no CN emission.
NH, NH_2, and C_2 gas production rates are (8.36 +/- 2.18)x10^25, (29.88 +/-
3.66)x10^25,... | astro-ph | we report spectra from 30005900 a for comet 96pmachholz obtained on 2007 apr 27 ut with the 3m shane telescope at lick observatory the spectra are extremely carbon poor and show a prominent nh_2 series but no cn emission nh nh_2 and c_2 gas production rates are 836 218x1025 2988 366x1025 and 452 061x1023 molecules sec1... | [['we', 'report', 'spectra', 'from', '30005900', 'a', 'for', 'comet', '96pmachholz', 'obtained', 'on', '2007', 'apr', '27', 'ut', 'with', 'the', '3m', 'shane', 'telescope', 'at', 'lick', 'observatory', 'the', 'spectra', 'are', 'extremely', 'carbon', 'poor', 'and', 'show', 'a', 'prominent', 'nh_2', 'series', 'but', 'no'... | [-0.041000053815712985, 0.14048979206262344, 0.009676323817911172, 0.04300474775531753, 0.05014066498507887, -0.1663439136017302, 0.06590582444003285, 0.47490046482834253, -0.1260400116725853, -0.31354914447574905, 0.11487807620627184, -0.37075566474084903, 0.0012332897614499535, 0.19677040811435254, -0.026859449260313... |
706.2023 | Electric fields in plasmas under pulsed currents | Electric fields in a plasma that conducts a high-current pulse are measured
as a function of time and space. The experiment is performed using a coaxial
configuration, in which a current rising to 160 kA in 100 ns is conducted
through a plasma that prefills the region between two coaxial electrodes. The
electric fiel... | physics.plasm-ph | electric fields in a plasma that conducts a highcurrent pulse are measured as a function of time and space the experiment is performed using a coaxial configuration in which a current rising to 160 ka in 100 ns is conducted through a plasma that prefills the region between two coaxial electrodes the electric field is d... | [['electric', 'fields', 'in', 'a', 'plasma', 'that', 'conducts', 'a', 'highcurrent', 'pulse', 'are', 'measured', 'as', 'a', 'function', 'of', 'time', 'and', 'space', 'the', 'experiment', 'is', 'performed', 'using', 'a', 'coaxial', 'configuration', 'in', 'which', 'a', 'current', 'rising', 'to', '160', 'ka', 'in', '100',... | [-0.1405452475194078, 0.17793861215836748, -0.055632799293617814, 0.001049970267150475, -0.021328479636042397, -0.12397259313195032, 0.014314604858981863, 0.45249223338478073, -0.21580716640194308, -0.3645009147193359, 0.020374755081673135, -0.26003742050299333, -0.007696090893325757, 0.2465918085386986, 0.069793047694... |
706.2024 | Generation interval contraction and epidemic data analysis | The generation interval is the time between the infection time of an infected
person and the infection time of his or her infector. Probability density
functions for generation intervals have been an important input for epidemic
models and epidemic data analysis. In this paper, we specify a general
stochastic SIR epi... | q-bio.QM math.PR stat.AP | the generation interval is the time between the infection time of an infected person and the infection time of his or her infector probability density functions for generation intervals have been an important input for epidemic models and epidemic data analysis in this paper we specify a general stochastic sir epidemic... | [['the', 'generation', 'interval', 'is', 'the', 'time', 'between', 'the', 'infection', 'time', 'of', 'an', 'infected', 'person', 'and', 'the', 'infection', 'time', 'of', 'his', 'or', 'her', 'infector', 'probability', 'density', 'functions', 'for', 'generation', 'intervals', 'have', 'been', 'an', 'important', 'input', '... | [-0.11835539680082705, 0.11484134929673144, -0.06213674722399948, 0.11986168671789747, -0.059214286064600635, -0.1898410624868622, 0.11063290631211893, 0.3611892378569886, -0.25461445579803066, -0.26453816382102024, 0.12852272583906346, -0.31892190546054267, -0.19862455347726515, 0.14411049475567214, -0.117744454064261... |
706.2025 | On the Performance Evaluation of Encounter-based Worm Interactions Based
on Node Characteristics | An encounter-based network is a frequently disconnected wireless ad-hoc
network requiring nearby neighbors to store and forward data utilizing mobility
and encounters over time. Using traditional approaches such as gateways or
firewalls for deterring worm propagation in encounter-based networks is
inappropriate. Beca... | cs.CR cs.NI | an encounterbased network is a frequently disconnected wireless adhoc network requiring nearby neighbors to store and forward data utilizing mobility and encounters over time using traditional approaches such as gateways or firewalls for deterring worm propagation in encounterbased networks is inappropriate because thi... | [['an', 'encounterbased', 'network', 'is', 'a', 'frequently', 'disconnected', 'wireless', 'adhoc', 'network', 'requiring', 'nearby', 'neighbors', 'to', 'store', 'and', 'forward', 'data', 'utilizing', 'mobility', 'and', 'encounters', 'over', 'time', 'using', 'traditional', 'approaches', 'such', 'as', 'gateways', 'or', '... | [-0.18174651141319675, 0.08121823446701269, -0.03875937598596255, 0.07469648900023924, -0.1056747552795479, -0.20168370585888623, 0.09792067722047273, 0.4266180025365872, -0.23402158086940358, -0.28062152868280044, 0.11290583207588405, -0.2811652866789164, -0.24644016953638923, 0.1671804802886282, -0.08042070409760643,... |
706.2026 | Quantum Teichm\"uller spaces and Kashaev's 6j-symbols | The Kashaev invariants of 3-manifolds are based on $6j$-symbols from the
representation theory of the Weyl algebra, a Hopf algebra corresponding to the
Borel subalgebra of $U_q(sl(2,\C))$. In this paper, we show that Kashaev's
$6j$-symbols are intertwining operators of local representations of quantum
Teichm\"uller s... | math.GT math.QA | the kashaev invariants of 3manifolds are based on 6jsymbols from the representation theory of the weyl algebra a hopf algebra corresponding to the borel subalgebra of u_qsl2c in this paper we show that kashaevs 6jsymbols are intertwining operators of local representations of quantum teichmuller spaces this relates kash... | [['the', 'kashaev', 'invariants', 'of', '3manifolds', 'are', 'based', 'on', '6jsymbols', 'from', 'the', 'representation', 'theory', 'of', 'the', 'weyl', 'algebra', 'a', 'hopf', 'algebra', 'corresponding', 'to', 'the', 'borel', 'subalgebra', 'of', 'u_qsl2c', 'in', 'this', 'paper', 'we', 'show', 'that', 'kashaevs', '6jsy... | [-0.17646446700382512, 0.12363322088458517, -0.15749521955149248, 0.06120666848073597, -0.11495293688130914, -0.07434841288340976, -0.03534924232553749, 0.27198520116508007, -0.3423661357592209, -0.19995961934910156, 0.09563303607683338, -0.2553256110259099, -0.265596631432345, 0.20670823207183275, -0.1872927276272094,... |
706.2027 | Collective behavior in a granular jet: Emergence of a liquid with zero
surface-tension | We perform the analog to the "water bell" experiment using non-cohesive
granular material. When a jet of granular material, many particles wide,
rebounds from a fixed cylindrical target, it deforms into a sharply-defined
sheet or cone with a shape that mimics a liquid with zero surface tension. The
particulate nature... | cond-mat.soft | we perform the analog to the water bell experiment using noncohesive granular material when a jet of granular material many particles wide rebounds from a fixed cylindrical target it deforms into a sharplydefined sheet or cone with a shape that mimics a liquid with zero surface tension the particulate nature of granula... | [['we', 'perform', 'the', 'analog', 'to', 'the', 'water', 'bell', 'experiment', 'using', 'noncohesive', 'granular', 'material', 'when', 'a', 'jet', 'of', 'granular', 'material', 'many', 'particles', 'wide', 'rebounds', 'from', 'a', 'fixed', 'cylindrical', 'target', 'it', 'deforms', 'into', 'a', 'sharplydefined', 'sheet... | [-0.0927905564876421, 0.2587306670223673, -0.15262394684130356, 0.019771739846051094, -0.0333306845729841, -0.1370143567263666, -0.009970130494958351, 0.349037720886473, -0.2543197936017047, -0.2845616654330303, 0.02816384716425091, -0.3327428750945107, -0.052445527825814985, 0.15305025127368965, 0.015961230281622163, ... |
706.2028 | Eigenvalues and lambda constants on Riemannian submersions | Given a Riemannian submersion, we study the relation between lambda constants
introduced by G.Perelman on the base manifold and the total space of a
Riemannian submersion. We also discuss the relationship between the first
eigenvalues of Laplacians on the base manifold and that of the total space. The
quantities on w... | math.DG math.AP | given a riemannian submersion we study the relation between lambda constants introduced by gperelman on the base manifold and the total space of a riemannian submersion we also discuss the relationship between the first eigenvalues of laplacians on the base manifold and that of the total space the quantities on warped ... | [['given', 'a', 'riemannian', 'submersion', 'we', 'study', 'the', 'relation', 'between', 'lambda', 'constants', 'introduced', 'by', 'gperelman', 'on', 'the', 'base', 'manifold', 'and', 'the', 'total', 'space', 'of', 'a', 'riemannian', 'submersion', 'we', 'also', 'discuss', 'the', 'relationship', 'between', 'the', 'firs... | [-0.18902852931725128, 0.07092615760380536, -0.014582039962988347, 0.10414917966617006, -0.09771906547913593, -0.030579029881794537, 0.029602494656241367, 0.38323196955025196, -0.24745143723807164, -0.24809678038582206, 0.1035933519077454, -0.29042618555415955, -0.188188564585289, 0.1616228779811146, -0.086645481259828... |
706.2029 | The Chemical Compositions of the Type II Cepheids -- The BL Her and W
Vir Variables | Abundance analyses from high-resolution optical spectra are presented for 19
Type II Cepheids in the Galactic field. The sample includes both short-period
(BL Her) and long-period (W Vir) stars. This is the first extensive abundance
analysis of these variables. The C, N, and O abundances with similar spreads
for the ... | astro-ph | abundance analyses from highresolution optical spectra are presented for 19 type ii cepheids in the galactic field the sample includes both shortperiod bl her and longperiod w vir stars this is the first extensive abundance analysis of these variables the c n and o abundances with similar spreads for the bl her and w v... | [['abundance', 'analyses', 'from', 'highresolution', 'optical', 'spectra', 'are', 'presented', 'for', '19', 'type', 'ii', 'cepheids', 'in', 'the', 'galactic', 'field', 'the', 'sample', 'includes', 'both', 'shortperiod', 'bl', 'her', 'and', 'longperiod', 'w', 'vir', 'stars', 'this', 'is', 'the', 'first', 'extensive', 'a... | [-0.06369090986646107, 0.14740276012088344, -0.037565896216352104, 0.06101500669903202, -0.1130112930021348, -0.14002690049654185, 0.1207237650101371, 0.37997689012078767, -0.19384900888110165, -0.3648981480873403, 0.008488334971834635, -0.31367633871847606, -0.020780600834316407, 0.1562320727637501, -0.124827133386447... |
706.203 | Hot Topics from the BABAR Experiment | With a sample of about 384 million BBbar pairs recorded with the BABAR
detector, we search for the flavor-changing charged current transition B+ ->
\tau\nu and perform an amplitude analysis of the effective flavor-changing
neutral current transition B+ -> \phi(1020)K*(892)+. We also extend our search
for other K* fin... | hep-ex | with a sample of about 384 million bbbar pairs recorded with the babar detector we search for the flavorchanging charged current transition b taunu and perform an amplitude analysis of the effective flavorchanging neutral current transition b phi1020k892 we also extend our search for other k final states in the decay b... | [['with', 'a', 'sample', 'of', 'about', '384', 'million', 'bbbar', 'pairs', 'recorded', 'with', 'the', 'babar', 'detector', 'we', 'search', 'for', 'the', 'flavorchanging', 'charged', 'current', 'transition', 'b', 'taunu', 'and', 'perform', 'an', 'amplitude', 'analysis', 'of', 'the', 'effective', 'flavorchanging', 'neut... | [-0.08996794718306675, 0.2100852211329471, -0.0202109129891756, 0.061354662849397924, -0.035617042266814086, -0.1513617788850506, 0.13079238600550672, 0.28302657860645875, -0.20394583979961337, -0.3381897566991078, 0.042773914212719664, -0.3887546551036271, 0.039048602544966886, 0.12723311831753045, 0.09922762282862882... |
706.2031 | Relativity tests by complementary rotating Michelson-Morley experiments | We report Relativity tests based on data from two simultaneous
Michelson-Morley experiments, spanning a period of more than one year. Both
were actively rotated on turntables. One (in Berlin, Germany) uses optical
Fabry-Perot resonators made of fused silica; the other (in Perth, Australia)
uses microwave whispering-g... | physics.class-ph gr-qc hep-ph physics.hist-ph | we report relativity tests based on data from two simultaneous michelsonmorley experiments spanning a period of more than one year both were actively rotated on turntables one in berlin germany uses optical fabryperot resonators made of fused silica the other in perth australia uses microwave whisperinggallery sapphire... | [['we', 'report', 'relativity', 'tests', 'based', 'on', 'data', 'from', 'two', 'simultaneous', 'michelsonmorley', 'experiments', 'spanning', 'a', 'period', 'of', 'more', 'than', 'one', 'year', 'both', 'were', 'actively', 'rotated', 'on', 'turntables', 'one', 'in', 'berlin', 'germany', 'uses', 'optical', 'fabryperot', '... | [-0.06694338631574963, 0.13934700331841426, -0.010212927321757537, -0.0379487892882113, -0.05522489091605846, -0.17283737450187286, 0.07097292316696012, 0.4202024469387729, -0.11666815715045276, -0.3581820869908096, 0.09390558952925704, -0.34997853937457846, -0.03157802550570972, 0.29470881508629637, -0.026145233761474... |
706.2032 | Heegaard Floer homology and fibred 3--manifolds | Given a closed 3--manifold $Y$, we show that the Heegaard Floer homology
determines whether $Y$ fibres over the circle with a fibre of negative Euler
characteristic. This is an analogue of an earlier result about knots proved by
Ghiggini and the author.
| math.GT | given a closed 3manifold y we show that the heegaard floer homology determines whether y fibres over the circle with a fibre of negative euler characteristic this is an analogue of an earlier result about knots proved by ghiggini and the author | [['given', 'a', 'closed', '3manifold', 'y', 'we', 'show', 'that', 'the', 'heegaard', 'floer', 'homology', 'determines', 'whether', 'y', 'fibres', 'over', 'the', 'circle', 'with', 'a', 'fibre', 'of', 'negative', 'euler', 'characteristic', 'this', 'is', 'an', 'analogue', 'of', 'an', 'earlier', 'result', 'about', 'knots',... | [-0.2814721728763765, 0.04676131412478363, -0.16372275081950993, 0.06679704284206742, -0.06339677139407113, -0.17088527944205062, -0.034052087437538875, 0.34909175114617463, -0.30884684719854877, -0.2492131261775891, 0.028687225632546914, -0.21251429129014945, -0.17276098757671812, 0.19758968813610928, -0.2317161180212... |
706.2033 | Power Allocation for Discrete-Input Delay-Limited Fading Channels | We consider power allocation algorithms for fixed-rate transmission over
Nakagami-m non-ergodic block-fading channels with perfect transmitter and
receiver channel state information and discrete input signal constellations,
under both short- and long-term power constraints. Optimal power allocation
schemes are shown ... | cs.IT math.IT | we consider power allocation algorithms for fixedrate transmission over nakagamim nonergodic blockfading channels with perfect transmitter and receiver channel state information and discrete input signal constellations under both short and longterm power constraints optimal power allocation schemes are shown to be dire... | [['we', 'consider', 'power', 'allocation', 'algorithms', 'for', 'fixedrate', 'transmission', 'over', 'nakagamim', 'nonergodic', 'blockfading', 'channels', 'with', 'perfect', 'transmitter', 'and', 'receiver', 'channel', 'state', 'information', 'and', 'discrete', 'input', 'signal', 'constellations', 'under', 'both', 'sho... | [-0.2218358826948384, 0.03434735174731752, -0.06868017078399802, 0.06558037021901494, -0.04677064938061299, -0.24140679478816293, 0.13460618107082492, 0.41648626721977, -0.26652212576729195, -0.23314767756503849, 0.11607268656961674, -0.20053544956380906, -0.17120984475272324, 0.22527788736259088, -0.13106950530827333,... |
706.2034 | Properties of positive solutions of an Elliptic Equation with negative
exponents | In this paper, we study the existence and non-existence result of positive
solutions to a singular elliptic equation with negative power on the bounded
smooth domain or in the whole Euclidean space. Our model arises in the study of
the steady states of thin films and other applied physics. We can get some
useful loca... | math.AP math.DG | in this paper we study the existence and nonexistence result of positive solutions to a singular elliptic equation with negative power on the bounded smooth domain or in the whole euclidean space our model arises in the study of the steady states of thin films and other applied physics we can get some useful local grad... | [['in', 'this', 'paper', 'we', 'study', 'the', 'existence', 'and', 'nonexistence', 'result', 'of', 'positive', 'solutions', 'to', 'a', 'singular', 'elliptic', 'equation', 'with', 'negative', 'power', 'on', 'the', 'bounded', 'smooth', 'domain', 'or', 'in', 'the', 'whole', 'euclidean', 'space', 'our', 'model', 'arises', ... | [-0.15413698731433778, 0.10450061592125585, -0.0891544211873903, 0.08062735766298064, -0.07848690733653567, -0.13970312017149158, -0.002897694565555347, 0.32170585494133686, -0.26511983376824194, -0.22998934594123432, 0.1345272368016017, -0.29647272888068404, -0.14813575002277965, 0.212054310813694, -0.0615477302215165... |
706.2035 | Critique of Feinstein's Proof that P is not Equal to NP | We examine a proof by Craig Alan Feinstein that P is not equal to NP. We
present counterexamples to claims made in his paper and expose a flaw in the
methodology he uses to make his assertions. The fault in his argument is the
incorrect use of reduction. Feinstein makes incorrect assumptions about the
complexity of a... | cs.CC | we examine a proof by craig alan feinstein that p is not equal to np we present counterexamples to claims made in his paper and expose a flaw in the methodology he uses to make his assertions the fault in his argument is the incorrect use of reduction feinstein makes incorrect assumptions about the complexity of a prob... | [['we', 'examine', 'a', 'proof', 'by', 'craig', 'alan', 'feinstein', 'that', 'p', 'is', 'not', 'equal', 'to', 'np', 'we', 'present', 'counterexamples', 'to', 'claims', 'made', 'in', 'his', 'paper', 'and', 'expose', 'a', 'flaw', 'in', 'the', 'methodology', 'he', 'uses', 'to', 'make', 'his', 'assertions', 'the', 'fault',... | [-0.10870103232323841, 0.013175191075987174, -0.1512330104636044, 0.10048616487345025, -0.17533587809933834, -0.19234119012889242, 0.09358682854496286, 0.33707859288869785, -0.2564356459946442, -0.31184444285365714, 0.08956394654878673, -0.26173641078737603, -0.17751269600502834, 0.18404094634593285, -0.186069452861214... |
706.2036 | Observation of back-action cancellation in interferometric and weak
force measurements | We experimentally demonstrate a cancellation of back-action noise in optical
measurements. Back-action cancellation was first proposed within the framework
of gravitational-wave detection by dual resonators as a way to drastically
improve their sensitivity. We have developed an experiment based on a
high-finesse Fabr... | quant-ph gr-qc | we experimentally demonstrate a cancellation of backaction noise in optical measurements backaction cancellation was first proposed within the framework of gravitationalwave detection by dual resonators as a way to drastically improve their sensitivity we have developed an experiment based on a highfinesse fabryperot c... | [['we', 'experimentally', 'demonstrate', 'a', 'cancellation', 'of', 'backaction', 'noise', 'in', 'optical', 'measurements', 'backaction', 'cancellation', 'was', 'first', 'proposed', 'within', 'the', 'framework', 'of', 'gravitationalwave', 'detection', 'by', 'dual', 'resonators', 'as', 'a', 'way', 'to', 'drastically', '... | [-0.17078770458017692, 0.15605978537244553, -0.07070471360706367, -0.027474620701888434, -0.04394731684946097, -0.12682509671699685, 0.06824253693831941, 0.4086021192980787, -0.19752937112487137, -0.32637342944060665, 0.03023599480534008, -0.26387414959474254, -0.18124652437220973, 0.24128023432925916, -0.0769801473742... |
706.2037 | Phase structure of a spherical surface model on fixed connectivity
meshes | An elastic surface model is investigated by using the canonical Monte Carlo
simulation technique on triangulated spherical meshes. The model undergoes a
first-order collapsing transition and a continuous surface fluctuation
transition. The shape of surfaces is maintained by a one-dimensional bending
energy, which is ... | cond-mat.stat-mech cond-mat.soft | an elastic surface model is investigated by using the canonical monte carlo simulation technique on triangulated spherical meshes the model undergoes a firstorder collapsing transition and a continuous surface fluctuation transition the shape of surfaces is maintained by a onedimensional bending energy which is defined... | [['an', 'elastic', 'surface', 'model', 'is', 'investigated', 'by', 'using', 'the', 'canonical', 'monte', 'carlo', 'simulation', 'technique', 'on', 'triangulated', 'spherical', 'meshes', 'the', 'model', 'undergoes', 'a', 'firstorder', 'collapsing', 'transition', 'and', 'a', 'continuous', 'surface', 'fluctuation', 'trans... | [-0.14712637027019057, 0.17051130816855284, -0.11540757130092845, 0.05934438852047355, 0.0031465313172545925, -0.11552239952062995, -0.02052602580555811, 0.39697317978174523, -0.28224636362223277, -0.2706288280093978, 0.043337906941626994, -0.25248397120017685, -0.12129043800563648, 0.15690535363933905, 0.0013669007849... |
706.2038 | The first-passage area for drifted Brownian motion and the moments of
the Airy distribution | An exact expression for the distribution of the area swept out by a drifted
Brownian motion till its first-passage time is derived. A study of the
asymptotic behaviour confirms earlier conjectures and clarifies their range of
validity. The analysis also leads to a simple closed-form solution for the
moments of the Ai... | cond-mat.stat-mech math.CO math.PR | an exact expression for the distribution of the area swept out by a drifted brownian motion till its firstpassage time is derived a study of the asymptotic behaviour confirms earlier conjectures and clarifies their range of validity the analysis also leads to a simple closedform solution for the moments of the airy dis... | [['an', 'exact', 'expression', 'for', 'the', 'distribution', 'of', 'the', 'area', 'swept', 'out', 'by', 'a', 'drifted', 'brownian', 'motion', 'till', 'its', 'firstpassage', 'time', 'is', 'derived', 'a', 'study', 'of', 'the', 'asymptotic', 'behaviour', 'confirms', 'earlier', 'conjectures', 'and', 'clarifies', 'their', '... | [-0.13516296691674176, 0.01283274744972279, -0.1650301434521405, 0.04978301328000665, -0.050015204217074054, -0.035144328561453324, 0.08694726145466052, 0.3354838026406349, -0.22686739065596517, -0.26306806728990645, 0.1019945025338598, -0.2609522697111627, -0.1355569923894023, 0.20131344989574743, -0.02644928428783731... |
706.2039 | Oscillatory secular modes: The thermal micropulses | Stars in the narrow mass range of about 2.5 and 3.5 solar masses can develop
a thermally unstable He-burning shell during its ignition phase. We study, from
the point of view secular stability theory, these so called thermal micropulses
and we investigate their properties; the thermal pulses constitute a convenient
c... | astro-ph | stars in the narrow mass range of about 25 and 35 solar masses can develop a thermally unstable heburning shell during its ignition phase we study from the point of view secular stability theory these so called thermal micropulses and we investigate their properties the thermal pulses constitute a convenient conceptual... | [['stars', 'in', 'the', 'narrow', 'mass', 'range', 'of', 'about', '25', 'and', '35', 'solar', 'masses', 'can', 'develop', 'a', 'thermally', 'unstable', 'heburning', 'shell', 'during', 'its', 'ignition', 'phase', 'we', 'study', 'from', 'the', 'point', 'of', 'view', 'secular', 'stability', 'theory', 'these', 'so', 'calle... | [-0.1019547628339403, 0.2282748111434041, -0.1213553867728254, 0.06995250298612878, -0.06915685702057808, -0.05027987020389165, 0.07213656917533458, 0.3728428176132801, -0.25373345399620356, -0.29498752565583053, 0.127330550434568, -0.22240797977860052, -0.05125293473103716, 0.17818761056678564, -0.051172550247384256, ... |
706.204 | Getting started in probabilistic graphical models | Probabilistic graphical models (PGMs) have become a popular tool for
computational analysis of biological data in a variety of domains. But, what
exactly are they and how do they work? How can we use PGMs to discover patterns
that are biologically relevant? And to what extent can PGMs help us formulate
new hypotheses... | q-bio.QM cs.LG physics.soc-ph stat.ME stat.ML | probabilistic graphical models pgms have become a popular tool for computational analysis of biological data in a variety of domains but what exactly are they and how do they work how can we use pgms to discover patterns that are biologically relevant and to what extent can pgms help us formulate new hypotheses that ar... | [['probabilistic', 'graphical', 'models', 'pgms', 'have', 'become', 'a', 'popular', 'tool', 'for', 'computational', 'analysis', 'of', 'biological', 'data', 'in', 'a', 'variety', 'of', 'domains', 'but', 'what', 'exactly', 'are', 'they', 'and', 'how', 'do', 'they', 'work', 'how', 'can', 'we', 'use', 'pgms', 'to', 'discov... | [0.00548821080249185, 0.06700580421453103, -0.16330995470977938, 0.18396911544289488, -0.19366225796357656, -0.19636117570245495, 0.045402634817247205, 0.418823241089017, -0.3056224895438227, -0.3371414268532625, 0.12778582859587354, -0.25389083188910705, -0.24711280415813702, 0.23112155406479126, -0.11313225547424875,... |
706.2041 | Disappearing cosmological constant in f(R) gravity | For higher-derivative f(R) gravity where R is the Ricci scalar, a class of
models is proposed which produce viable cosmology different from the LambdaCDM
one at recent times and satisfy cosmological, Solar system and laboratory
tests. These models have both flat and de Sitter space-times as particular
solutions in th... | astro-ph gr-qc hep-th | for higherderivative fr gravity where r is the ricci scalar a class of models is proposed which produce viable cosmology different from the lambdacdm one at recent times and satisfy cosmological solar system and laboratory tests these models have both flat and de sitter spacetimes as particular solutions in the absence... | [['for', 'higherderivative', 'fr', 'gravity', 'where', 'r', 'is', 'the', 'ricci', 'scalar', 'a', 'class', 'of', 'models', 'is', 'proposed', 'which', 'produce', 'viable', 'cosmology', 'different', 'from', 'the', 'lambdacdm', 'one', 'at', 'recent', 'times', 'and', 'satisfy', 'cosmological', 'solar', 'system', 'and', 'lab... | [-0.1272703427335636, 0.1405888101313826, -0.11344956706458931, 0.12530034608308147, -0.10775283033617859, -0.20689808740448073, -0.09724634832940433, 0.2648698531841631, -0.17726318698992832, -0.3117390515185598, 0.08646372695982778, -0.2507972166531806, -0.0729968952912864, 0.19272324914554897, -0.028144117665859007,... |
706.2042 | 1/4-BPS M-theory bubbles with SO(3) x SO(4) symmetry | In this paper we generalize the work of Lin, Lunin and Maldacena on the
classification of 1/2-BPS M-theory solutions to a specific class of 1/4-BPS
configurations. We are interested in the solutions of 11 dimensional
supergravity with $SO(3)\times SO(4)$ symmetry, and it is shown that such
solutions are constructed o... | hep-th | in this paper we generalize the work of lin lunin and maldacena on the classification of 12bps mtheory solutions to a specific class of 14bps configurations we are interested in the solutions of 11 dimensional supergravity with so3times so4 symmetry and it is shown that such solutions are constructed over a oneparamete... | [['in', 'this', 'paper', 'we', 'generalize', 'the', 'work', 'of', 'lin', 'lunin', 'and', 'maldacena', 'on', 'the', 'classification', 'of', '12bps', 'mtheory', 'solutions', 'to', 'a', 'specific', 'class', 'of', '14bps', 'configurations', 'we', 'are', 'interested', 'in', 'the', 'solutions', 'of', '11', 'dimensional', 'su... | [-0.166010860344007, 0.06647721675690263, -0.024107160925632344, 0.1003368015110027, -0.08695729964335139, -0.16081475043514123, -0.046978771915504085, 0.33379229448037223, -0.11124018142775943, -0.2634233034409893, 0.1770483579709738, -0.3151164747076109, -0.19901165193126266, 0.12971313905048495, -0.1557371126759487,... |
706.2043 | Phase Spaces in Special Relativity: Towards Eliminating Gravitational
Singularities | This paper shows one way to construct phase spaces in special relativity by
expanding Minkowski Space. These spaces appear to indicate that we can dispense
with gravitational singularities. The key mathematical ideas in the present
approach are to include a complex phase factor, such as, e^{i\phi} in the
Lorentz tran... | astro-ph | this paper shows one way to construct phase spaces in special relativity by expanding minkowski space these spaces appear to indicate that we can dispense with gravitational singularities the key mathematical ideas in the present approach are to include a complex phase factor such as eiphi in the lorentz transformation... | [['this', 'paper', 'shows', 'one', 'way', 'to', 'construct', 'phase', 'spaces', 'in', 'special', 'relativity', 'by', 'expanding', 'minkowski', 'space', 'these', 'spaces', 'appear', 'to', 'indicate', 'that', 'we', 'can', 'dispense', 'with', 'gravitational', 'singularities', 'the', 'key', 'mathematical', 'ideas', 'in', '... | [-0.11552894834810784, 0.15132027388307023, -0.09461443196758754, 0.07903577883409017, -0.12616223354219785, -0.11349336079716145, 0.012613036699681165, 0.3539584479915468, -0.2587712301630401, -0.2754569372900569, 0.08193377290248267, -0.21588575632231696, -0.12171741563151381, 0.17225386514139637, -0.0884184071951208... |
706.2044 | Lines of minima are uniformly quasi-geodesic | We continue the comparison between lines of minima and Teichmueller geodesics
begun in [CRS1]. We show that in the Teichmueller space of a surface S, lines
of minima are quasi-geodesic with respect to the Teichmueller metric. The
quasi-geodesic constants depend only on the topological type of S.
| math.GT | we continue the comparison between lines of minima and teichmueller geodesics begun in crs1 we show that in the teichmueller space of a surface s lines of minima are quasigeodesic with respect to the teichmueller metric the quasigeodesic constants depend only on the topological type of s | [['we', 'continue', 'the', 'comparison', 'between', 'lines', 'of', 'minima', 'and', 'teichmueller', 'geodesics', 'begun', 'in', 'crs1', 'we', 'show', 'that', 'in', 'the', 'teichmueller', 'space', 'of', 'a', 'surface', 's', 'lines', 'of', 'minima', 'are', 'quasigeodesic', 'with', 'respect', 'to', 'the', 'teichmueller', ... | [-0.2031045240835975, 0.11462065710625409, -0.12253517923755167, 0.0630883825537951, -0.043790044465466686, -0.07363563221778073, 0.07050403274352783, 0.3789277228972186, -0.28032045649445575, -0.20405540258608476, 0.043133226653520505, -0.3400177228588449, -0.14969032156564618, 0.24322966824326178, -0.1293386362655007... |
706.2045 | Measurement of Branching Fraction and Time-Dependent CP Asymmetry
Parameters in B0 -> D*+ D*- Ks Decays | We present a measurement of the branching fraction and time-dependent CP
violation parameters for B0 -> D*+ D*- Ks decays. We also obtain an upper limit
on the product branching fraction for the possible two-body decay, B0 ->
Ds1+(2536) D*-. These results are obtained from a 414 fb-1 data sample that
contains 449e10^... | hep-ex | we present a measurement of the branching fraction and timedependent cp violation parameters for b0 d d ks decays we also obtain an upper limit on the product branching fraction for the possible twobody decay b0 ds12536 d these results are obtained from a 414 fb1 data sample that contains 449e106 bbbar pairs collected ... | [['we', 'present', 'a', 'measurement', 'of', 'the', 'branching', 'fraction', 'and', 'timedependent', 'cp', 'violation', 'parameters', 'for', 'b0', 'd', 'd', 'ks', 'decays', 'we', 'also', 'obtain', 'an', 'upper', 'limit', 'on', 'the', 'product', 'branching', 'fraction', 'for', 'the', 'possible', 'twobody', 'decay', 'b0'... | [-0.1178508946592155, 0.1640818452563766, -0.05920362013128044, 0.061042402989105946, -0.06486393279159691, -0.14852564031286025, 0.14063881895567443, 0.2571575588671796, -0.15754933513478556, -0.26045093582526074, -0.02445593456487491, -0.4652188053118315, 0.10244910862408023, 0.1684882054557162, 0.14384807488505744, ... |
706.2046 | Non-Supersymmetric Unattractors in Born-Infeld Black Holes | We investigate unattractor behavior in non-extremal black holes in
Einstein-Born-Infeld-Dilaton theory of gravity in four-dimensional
asymptotically flat spacetime. We obtain solutions which are non-singular near
the horizon and dependent on the value of the dilaton field at the infinity,
using perturbation method. I... | hep-th | we investigate unattractor behavior in nonextremal black holes in einsteinborninfelddilaton theory of gravity in fourdimensional asymptotically flat spacetime we obtain solutions which are nonsingular near the horizon and dependent on the value of the dilaton field at the infinity using perturbation method it is shown ... | [['we', 'investigate', 'unattractor', 'behavior', 'in', 'nonextremal', 'black', 'holes', 'in', 'einsteinborninfelddilaton', 'theory', 'of', 'gravity', 'in', 'fourdimensional', 'asymptotically', 'flat', 'spacetime', 'we', 'obtain', 'solutions', 'which', 'are', 'nonsingular', 'near', 'the', 'horizon', 'and', 'dependent',... | [-0.13939652524468063, 0.09460514079490044, -0.10558573157047328, 0.09182337630377377, -0.056909147921262435, -0.13839599219358806, -0.016565272508831063, 0.2999755670180888, -0.17469666731878392, -0.24832254802261128, 0.13645490441918914, -0.3428455613806699, -0.12912865943338686, 0.15572792742835376, -0.0401436175644... |
706.2047 | Dynamic ordering of driven vortex matter in the peak effect regime of
amorphous MoGe films and 2H-NbSe2 crystals | Dynamic ordering of driven vortex matter has been investigated in the peak
effect regime of both amorphous MoGe films and 2H-NbSe2 crystals by mode
locking (ML) and dc transport measurements. ML features allow us to trace how
the shear rigidity of driven vortices evolves with the average velocity.
Determining the ons... | cond-mat.supr-con cond-mat.dis-nn | dynamic ordering of driven vortex matter has been investigated in the peak effect regime of both amorphous moge films and 2hnbse2 crystals by mode locking ml and dc transport measurements ml features allow us to trace how the shear rigidity of driven vortices evolves with the average velocity determining the onset of m... | [['dynamic', 'ordering', 'of', 'driven', 'vortex', 'matter', 'has', 'been', 'investigated', 'in', 'the', 'peak', 'effect', 'regime', 'of', 'both', 'amorphous', 'moge', 'films', 'and', '2hnbse2', 'crystals', 'by', 'mode', 'locking', 'ml', 'and', 'dc', 'transport', 'measurements', 'ml', 'features', 'allow', 'us', 'to', '... | [-0.1999609065209548, 0.2154266420927654, -0.1113475550526193, 0.029663762019074464, -0.07524591010272294, -0.11956297415406346, 0.09058040211472165, 0.3794723595850743, -0.28194379241212264, -0.2953500553796237, 0.04527223351251959, -0.2663993341262107, -0.1443474650142024, 0.16623415249901322, 0.04739249805053631, 0.... |
706.2048 | Thouless-Anderson-Palmer equation for analog neural network with
temporally fluctuating white synaptic noise | Effects of synaptic noise on the retrieval process of associative memory
neural networks are studied from the viewpoint of neurobiological and
biophysical understanding of information processing in the brain. We
investigate the statistical mechanical properties of stochastic analog neural
networks with temporally flu... | cond-mat.dis-nn cond-mat.stat-mech | effects of synaptic noise on the retrieval process of associative memory neural networks are studied from the viewpoint of neurobiological and biophysical understanding of information processing in the brain we investigate the statistical mechanical properties of stochastic analog neural networks with temporally fluctu... | [['effects', 'of', 'synaptic', 'noise', 'on', 'the', 'retrieval', 'process', 'of', 'associative', 'memory', 'neural', 'networks', 'are', 'studied', 'from', 'the', 'viewpoint', 'of', 'neurobiological', 'and', 'biophysical', 'understanding', 'of', 'information', 'processing', 'in', 'the', 'brain', 'we', 'investigate', 't... | [-0.10665214147884398, 0.06410402985452376, -0.06130855075637392, 0.07164787264076809, -0.09301934702477108, -0.13048100860025255, 0.04667964594510312, 0.3534535976926772, -0.2830041194609247, -0.30566661704856996, 0.08821614998846482, -0.2346302901967787, -0.2124455518113115, 0.17234583649163446, -0.06786783867491744,... |
706.2049 | Geometry of curves with exceptional secant planes: linear series along
the general curve | We study linear series on a general curve of genus $g$, whose images are
exceptional with regard to their secant planes. Working in the framework of an
extension of Brill-Noether theory to pairs of linear series, we prove that a
general curve has no linear series with exceptional secant planes, in a very
precise sens... | math.AG math.CO | we study linear series on a general curve of genus g whose images are exceptional with regard to their secant planes working in the framework of an extension of brillnoether theory to pairs of linear series we prove that a general curve has no linear series with exceptional secant planes in a very precise sense wheneve... | [['we', 'study', 'linear', 'series', 'on', 'a', 'general', 'curve', 'of', 'genus', 'g', 'whose', 'images', 'are', 'exceptional', 'with', 'regard', 'to', 'their', 'secant', 'planes', 'working', 'in', 'the', 'framework', 'of', 'an', 'extension', 'of', 'brillnoether', 'theory', 'to', 'pairs', 'of', 'linear', 'series', 'we... | [-0.1715750103393987, 0.008282081955755027, -0.07244053312266867, 0.025643291589269628, -0.09807803083587784, -0.12440016474116777, 0.01515623108773935, 0.32549164072696957, -0.2793868200044285, -0.23816023024481014, 0.09765017953004097, -0.28634961969430667, -0.16058239384040318, 0.2627437520884181, -0.105453762214356... |
706.205 | Black Holes and Large N Species Solution to the Hierarchy Problem | We provide the perturbative and non-perturbative arguments showing that
theories with large number of species of the quantum fields, imply an
inevitable hierarchy between the masses of the species and the Planck scale,
shedding a different light on the hierarchy problem. In particular, using the
black hole physics, w... | hep-th | we provide the perturbative and nonperturbative arguments showing that theories with large number of species of the quantum fields imply an inevitable hierarchy between the masses of the species and the planck scale shedding a different light on the hierarchy problem in particular using the black hole physics we prove ... | [['we', 'provide', 'the', 'perturbative', 'and', 'nonperturbative', 'arguments', 'showing', 'that', 'theories', 'with', 'large', 'number', 'of', 'species', 'of', 'the', 'quantum', 'fields', 'imply', 'an', 'inevitable', 'hierarchy', 'between', 'the', 'masses', 'of', 'the', 'species', 'and', 'the', 'planck', 'scale', 'sh... | [-0.14965377105872377, 0.23713582372734354, -0.045307527939622526, 0.10825763421036429, -0.05737011288945082, -0.1401208471765535, 0.03214968880863437, 0.2643753465912912, -0.22373138162968814, -0.32685249734327987, 0.07755678862834953, -0.27787119210900174, -0.05762757487361126, 0.15888344427651685, -0.024063120697341... |
706.2051 | Collapse of unit horizontal bundles equipped with a metric of
Cheeger-Gromoll type | We study unit horizontal bundles associated with Riemannian submersions.
First we investigate metric properties of an arbitrary unit horizontal bundle
equipped with a Riemannian metric of the Cheeger-Gromoll type. Next we examine
it from the Gromov-Hausdorff convergence theory point of view, and we state a
collapse t... | math.DG math.MG | we study unit horizontal bundles associated with riemannian submersions first we investigate metric properties of an arbitrary unit horizontal bundle equipped with a riemannian metric of the cheegergromoll type next we examine it from the gromovhausdorff convergence theory point of view and we state a collapse theorem ... | [['we', 'study', 'unit', 'horizontal', 'bundles', 'associated', 'with', 'riemannian', 'submersions', 'first', 'we', 'investigate', 'metric', 'properties', 'of', 'an', 'arbitrary', 'unit', 'horizontal', 'bundle', 'equipped', 'with', 'a', 'riemannian', 'metric', 'of', 'the', 'cheegergromoll', 'type', 'next', 'we', 'exami... | [-0.22529461786498206, 0.03276670513446719, -0.03657349202213651, 0.09514448322924011, -0.12664813938219163, -0.12325278039769096, -0.006439379329587948, 0.466840100522011, -0.29668855831279595, -0.16310947838286727, 0.14645177441633353, -0.3032981484055014, -0.17655296114636426, 0.12439387698136901, -0.182409534151902... |
706.2052 | Multicritical Points of Potts Spin Glasses on the Triangular Lattice | We predict the locations of several multicritical points of the Potts spin
glass model on the triangular lattice. In particular, continuous multicritical
lines, which consist of multicritical points, are obtained for two types of
two-state Potts (i.e., Ising) spin glasses with two- and three-body
interactions on the ... | cond-mat.dis-nn cond-mat.stat-mech | we predict the locations of several multicritical points of the potts spin glass model on the triangular lattice in particular continuous multicritical lines which consist of multicritical points are obtained for two types of twostate potts ie ising spin glasses with two and threebody interactions on the triangular lat... | [['we', 'predict', 'the', 'locations', 'of', 'several', 'multicritical', 'points', 'of', 'the', 'potts', 'spin', 'glass', 'model', 'on', 'the', 'triangular', 'lattice', 'in', 'particular', 'continuous', 'multicritical', 'lines', 'which', 'consist', 'of', 'multicritical', 'points', 'are', 'obtained', 'for', 'two', 'type... | [-0.11964518511350351, 0.14151357988911598, -0.0587494140686679, 0.017306730498305774, -0.056096983260729094, -0.1873456214300611, 0.041611120375719936, 0.3824522263878448, -0.22017484692518008, -0.2107668617867272, 0.10782165871615607, -0.2922400878721171, -0.15079216261986983, 0.159748884271407, 0.06326001844559373, ... |
706.2053 | Simple Model of Complex Reflection Behaviour in Two-Species Community | The model of smart migration for two-species community is developed, where
the individuals implement reflexive strategy of spatial redistribution.
Simulations have been used to figure out the situations where reflexy gives an
advantage over a non-reflexive spatial behaviour, and vice versa.
| q-bio.PE | the model of smart migration for twospecies community is developed where the individuals implement reflexive strategy of spatial redistribution simulations have been used to figure out the situations where reflexy gives an advantage over a nonreflexive spatial behaviour and vice versa | [['the', 'model', 'of', 'smart', 'migration', 'for', 'twospecies', 'community', 'is', 'developed', 'where', 'the', 'individuals', 'implement', 'reflexive', 'strategy', 'of', 'spatial', 'redistribution', 'simulations', 'have', 'been', 'used', 'to', 'figure', 'out', 'the', 'situations', 'where', 'reflexy', 'gives', 'an',... | [-0.06781694022938609, 0.06343145977334644, -0.12271080779028125, 0.04982765791064594, -0.11057176787871867, -0.1956421503680758, 0.02869375851005316, 0.37821957590058447, -0.27076557714608496, -0.2503183773253113, 0.0730759917292744, -0.22773100840859115, -0.15115039846859873, 0.14504877691506407, -0.09341138952877373... |
706.2054 | Determining the Sign of the Z-Penguin Amplitude | We point out that the precision measurements of the pseudo observables R_b^0,
A_b, and A_FB^0,b performed at LEP and SLC suggest that in models with
minimal-flavor-violation the sign of the Z-penguin amplitude is identical to
the one present in the standard model. We determine the allowed range for the
non-standard c... | hep-ph hep-ex | we point out that the precision measurements of the pseudo observables r_b0 a_b and a_fb0b performed at lep and slc suggest that in models with minimalflavorviolation the sign of the zpenguin amplitude is identical to the one present in the standard model we determine the allowed range for the nonstandard contribution ... | [['we', 'point', 'out', 'that', 'the', 'precision', 'measurements', 'of', 'the', 'pseudo', 'observables', 'r_b0', 'a_b', 'and', 'a_fb0b', 'performed', 'at', 'lep', 'and', 'slc', 'suggest', 'that', 'in', 'models', 'with', 'minimalflavorviolation', 'the', 'sign', 'of', 'the', 'zpenguin', 'amplitude', 'is', 'identical', '... | [-0.09543167061376379, 0.18002258031809515, -0.01721141893820938, 0.08690922908474107, -0.03359061419646176, -0.183881792463651, 0.15381360871134356, 0.2701258776680559, -0.24046499212633443, -0.27939315855344254, 0.011159929281728731, -0.3369454089768751, -0.024672002340269873, 0.18734500529569423, 0.06663532749670305... |
706.2055 | The TACTIC atmospheric Cherenkov Imaging telescope | The TACTIC $\gamma$-ray telescope, equipped with a light collector of area
$\sim$9.5m$^2$ and a medium resolution imaging camera of 349-pixels, has been
in operation at Mt.Abu, India since 2001. This paper describes the main
features of its various subsystems and its overall performance with regard to
(a) tracking ac... | astro-ph | the tactic gammaray telescope equipped with a light collector of area sim95m2 and a medium resolution imaging camera of 349pixels has been in operation at mtabu india since 2001 this paper describes the main features of its various subsystems and its overall performance with regard to a tracking accuracy of its 2axes d... | [['the', 'tactic', 'gammaray', 'telescope', 'equipped', 'with', 'a', 'light', 'collector', 'of', 'area', 'sim95m2', 'and', 'a', 'medium', 'resolution', 'imaging', 'camera', 'of', '349pixels', 'has', 'been', 'in', 'operation', 'at', 'mtabu', 'india', 'since', '2001', 'this', 'paper', 'describes', 'the', 'main', 'feature... | [-0.09032528345021439, 0.09710956968630907, -0.06931418802613161, 0.05830241020323205, -0.06413308021816318, -0.12619340290913014, 0.05673953011240251, 0.4257202647714336, -0.20053247056847495, -0.41188076393111195, 0.10410967081272575, -0.30035872863557656, -0.04444758666583333, 0.2598416548334222, -0.0616294810120735... |
706.2056 | Recent Developments in Bbar -> X_s gamma | We present a concise review of the recent theoretical progress concerning the
standard model calculation of the inclusive radiative Bbar -> X_s gamma decay.
Particular attention is thereby devoted to the calculations of the
next-to-next-to-leading order fixed-order O(alpha_s^2) contributions, non-local
O(alpha_s Lamb... | hep-ph | we present a concise review of the recent theoretical progress concerning the standard model calculation of the inclusive radiative bbar x_s gamma decay particular attention is thereby devoted to the calculations of the nexttonexttoleading order fixedorder oalpha_s2 contributions nonlocal oalpha_s lambdam_b power corre... | [['we', 'present', 'a', 'concise', 'review', 'of', 'the', 'recent', 'theoretical', 'progress', 'concerning', 'the', 'standard', 'model', 'calculation', 'of', 'the', 'inclusive', 'radiative', 'bbar', 'x_s', 'gamma', 'decay', 'particular', 'attention', 'is', 'thereby', 'devoted', 'to', 'the', 'calculations', 'of', 'the',... | [-0.060376085292325535, 0.13595842966226054, -0.048397500707364795, 0.10060774601314829, -0.09148092289913946, -0.07342138502107405, 0.07315367414032234, 0.2665713513409024, -0.19592577109196738, -0.17605295340850283, -0.008051380014686442, -0.3767457677802043, -0.039416936281790486, 0.12454756241945077, 0.052543340487... |
706.2057 | Marcus-Lushnikov processes, Smoluchowski's and Flory's models | The Marcus-Lushnikov process is a finite stochastic particle system in which
each particle is entirely characterized by its mass. Each pair of particles
with masses $x$ and $y$ merges into a single particle at a given rate $K(x,y)$.
We consider a {\it strongly gelling} kernel behaving as $K(x,y)=x^\alpha y + x
y^\alp... | math.PR | the marcuslushnikov process is a finite stochastic particle system in which each particle is entirely characterized by its mass each pair of particles with masses x and y merges into a single particle at a given rate kxy we consider a it strongly gelling kernel behaving as kxyxalpha y x yalpha for some alphain 01 in su... | [['the', 'marcuslushnikov', 'process', 'is', 'a', 'finite', 'stochastic', 'particle', 'system', 'in', 'which', 'each', 'particle', 'is', 'entirely', 'characterized', 'by', 'its', 'mass', 'each', 'pair', 'of', 'particles', 'with', 'masses', 'x', 'and', 'y', 'merges', 'into', 'a', 'single', 'particle', 'at', 'a', 'given'... | [-0.10388576484784402, 0.19647238091231214, -0.10540042873420521, 0.05570384707882806, -0.044764183241699035, -0.16804192200025225, 0.03158149357180198, 0.31566595256158786, -0.2806627859891449, -0.25835482364016177, 0.057501383057605084, -0.31556269821314686, -0.0946157364424277, 0.13231070083951918, 0.008941155815888... |
706.2058 | Thermal stability of n-dodecane : experiments and kinetic modelling | The thermal decomposition of n-dodecane, a component of some jet fuels, has
been studied in a jet-stirred reactor at temperatures from 793 to 1093 K, for
residence times between 1 and 5 s and at atmospheric pressure. Thermal
decomposition of hydrocarbon fuel prior the entrance in the combustion chamber
is an envisage... | physics.chem-ph | the thermal decomposition of ndodecane a component of some jet fuels has been studied in a jetstirred reactor at temperatures from 793 to 1093 k for residence times between 1 and 5 s and at atmospheric pressure thermal decomposition of hydrocarbon fuel prior the entrance in the combustion chamber is an envisaged way to... | [['the', 'thermal', 'decomposition', 'of', 'ndodecane', 'a', 'component', 'of', 'some', 'jet', 'fuels', 'has', 'been', 'studied', 'in', 'a', 'jetstirred', 'reactor', 'at', 'temperatures', 'from', '793', 'to', '1093', 'k', 'for', 'residence', 'times', 'between', '1', 'and', '5', 's', 'and', 'at', 'atmospheric', 'pressur... | [-0.0339248578042485, 0.16149274461874252, -0.06891039123080937, -0.04366930987768944, 0.04154324609526368, -0.08544293521766284, 0.03877258600167165, 0.407662668027157, -0.21860059961503328, -0.2875751710800064, 0.08725416579269335, -0.29703673238454514, 0.015309247072757215, 0.17375073172359604, -0.001925686594503101... |
706.2059 | BRIDGE: A Direct-tree Hybrid N-body Algorithm for Fully Self-consistent
Simulations of Star Clusters and their Parent Galaxies | We developed a new direct-tree hybrid N-body algorithm for fully
self-consistent N-body simulations of star clusters in their parent galaxies.
In such simulations, star clusters need high accuracy, while galaxies need a
fast scheme because of the large number of the particles required to model it.
In our new algorith... | astro-ph | we developed a new directtree hybrid nbody algorithm for fully selfconsistent nbody simulations of star clusters in their parent galaxies in such simulations star clusters need high accuracy while galaxies need a fast scheme because of the large number of the particles required to model it in our new algorithm the inte... | [['we', 'developed', 'a', 'new', 'directtree', 'hybrid', 'nbody', 'algorithm', 'for', 'fully', 'selfconsistent', 'nbody', 'simulations', 'of', 'star', 'clusters', 'in', 'their', 'parent', 'galaxies', 'in', 'such', 'simulations', 'star', 'clusters', 'need', 'high', 'accuracy', 'while', 'galaxies', 'need', 'a', 'fast', '... | [-0.08728898764104846, 0.07752687369859566, -0.10880392420175361, 0.06406534937310611, -0.085604131262859, -0.06542591562365146, 0.03488148953815434, 0.42076990884332793, -0.22253044489472307, -0.3600484019414308, 0.04462809811276508, -0.22263770947920128, -0.06663148202261025, 0.19357393748864013, 0.026448691987188504... |
706.206 | The autoignition of cyclopentane and cyclohexane in a shock tube | Ignition delay times of cyclohexane-oxygen-argon and
cyclopentane-oxygen-argon mixtures have been measured in a shock tube, the
onset of ignition being detected by OH radical emission. Mixtures contained 0.5
or 1 % of hydrocarbon for equivalence ratios ranging from 0.5 to 2. Reflected
shock waves allowed temperatures... | physics.chem-ph | ignition delay times of cyclohexaneoxygenargon and cyclopentaneoxygenargon mixtures have been measured in a shock tube the onset of ignition being detected by oh radical emission mixtures contained 05 or 1 of hydrocarbon for equivalence ratios ranging from 05 to 2 reflected shock waves allowed temperatures from 1230 to... | [['ignition', 'delay', 'times', 'of', 'cyclohexaneoxygenargon', 'and', 'cyclopentaneoxygenargon', 'mixtures', 'have', 'been', 'measured', 'in', 'a', 'shock', 'tube', 'the', 'onset', 'of', 'ignition', 'being', 'detected', 'by', 'oh', 'radical', 'emission', 'mixtures', 'contained', '05', 'or', '1', 'of', 'hydrocarbon', '... | [-0.0316391205098519, 0.10791643329261107, -0.03769556783779259, 0.03262837553809876, 0.014312475895368841, -0.1377765163915645, 0.04012584972397958, 0.3805862388254054, -0.21881803603371347, -0.3200906822263072, 0.0907957027651658, -0.2767527207584124, -0.045873961489016596, 0.2096555082665203, 0.015265638235699245, 0... |
706.2061 | Extension of the composite CBS-QB3 method to singlet diradical
calculations | The composite CBS-QB3 method is widely used to obtain accurate energies of
molecules and radicals although its use in the case of singlet diradicals gives
rise to some difficulties. The problem is related to the parameterized
correction this method introduces to account for spin-contamination. We report
a new term sp... | physics.chem-ph | the composite cbsqb3 method is widely used to obtain accurate energies of molecules and radicals although its use in the case of singlet diradicals gives rise to some difficulties the problem is related to the parameterized correction this method introduces to account for spincontamination we report a new term specific... | [['the', 'composite', 'cbsqb3', 'method', 'is', 'widely', 'used', 'to', 'obtain', 'accurate', 'energies', 'of', 'molecules', 'and', 'radicals', 'although', 'its', 'use', 'in', 'the', 'case', 'of', 'singlet', 'diradicals', 'gives', 'rise', 'to', 'some', 'difficulties', 'the', 'problem', 'is', 'related', 'to', 'the', 'pa... | [-0.05441979924459398, 0.08193914595176466, -0.039692542549649566, 0.10824527711156406, -0.015206012743874453, -0.15660871499373266, 0.021067109094777454, 0.36952480817368877, -0.241385129513219, -0.3225200642676403, 0.061726218151306966, -0.2706453616071182, -0.09162662007535498, 0.18745492091208385, -0.02613460942908... |
706.2062 | Kinetic modelling of a surrogate diesel fuel applied to 3D auto-ignition
in HCCI engines | The prediction of auto-ignition delay times in HCCI engines has risen
interest on detailed chemical models. This paper described a validated kinetic
mechanism for the oxidation of a model Diesel fuel (n-decane and
α-methylnaphthalene). The 3D model for the description of low and high
temperature auto-ignition in... | physics.chem-ph | the prediction of autoignition delay times in hcci engines has risen interest on detailed chemical models this paper described a validated kinetic mechanism for the oxidation of a model diesel fuel ndecane and 945methylnaphthalene the 3d model for the description of low and high temperature autoignition in engines is p... | [['the', 'prediction', 'of', 'autoignition', 'delay', 'times', 'in', 'hcci', 'engines', 'has', 'risen', 'interest', 'on', 'detailed', 'chemical', 'models', 'this', 'paper', 'described', 'a', 'validated', 'kinetic', 'mechanism', 'for', 'the', 'oxidation', 'of', 'a', 'model', 'diesel', 'fuel', 'ndecane', 'and', '945methy... | [-0.037711302130531095, 0.1077452221760507, -0.02959301984165651, 0.018295648318148918, 0.02559896339614367, -0.13603158034960328, 0.033858916857855914, 0.3559062747553605, -0.2063632579856389, -0.3291117358069444, 0.10237084933527812, -0.27308075964815687, -0.06681301424103686, 0.28772735666752475, -0.0344349444995648... |
706.2063 | Berry's phase for coherent states of Landau levels | The Berry phases for coherent states and squeezed coherent states of Landau
levels are calculated. Coherent states of Landau levels are interpreted as a
result of a magnetic flux moved adiabatically from infinity to a finite place
on the plane. The Abelian Berry phase for coherent states of Landau levels is
an analog... | quant-ph | the berry phases for coherent states and squeezed coherent states of landau levels are calculated coherent states of landau levels are interpreted as a result of a magnetic flux moved adiabatically from infinity to a finite place on the plane the abelian berry phase for coherent states of landau levels is an analog of ... | [['the', 'berry', 'phases', 'for', 'coherent', 'states', 'and', 'squeezed', 'coherent', 'states', 'of', 'landau', 'levels', 'are', 'calculated', 'coherent', 'states', 'of', 'landau', 'levels', 'are', 'interpreted', 'as', 'a', 'result', 'of', 'a', 'magnetic', 'flux', 'moved', 'adiabatically', 'from', 'infinity', 'to', '... | [-0.23362710228743586, 0.3492421974458282, -0.12671893066097353, 0.11460652616743401, 0.011894646106599327, -0.08432802871951985, 0.10805138944320984, 0.30485190352664104, -0.2526941079444982, -0.2694853837475986, -0.0268815463358486, -0.21467069707609512, -0.09404362151650963, 0.1715517428552581, -0.009278730539655363... |
706.2064 | Modelling of the gas-phase oxidation of cyclohexane | This paper presents a modeling study of the oxidation of cyclohexane from low
to intermediate temperature (650-1050 K), including the negative temperature
coefficient (NTC) zone. A detailed kinetic mechanism has been developed using
computer-aided generation. This comprehensive low-temperature mechanism
involves 513 ... | physics.chem-ph | this paper presents a modeling study of the oxidation of cyclohexane from low to intermediate temperature 6501050 k including the negative temperature coefficient ntc zone a detailed kinetic mechanism has been developed using computeraided generation this comprehensive lowtemperature mechanism involves 513 species and ... | [['this', 'paper', 'presents', 'a', 'modeling', 'study', 'of', 'the', 'oxidation', 'of', 'cyclohexane', 'from', 'low', 'to', 'intermediate', 'temperature', '6501050', 'k', 'including', 'the', 'negative', 'temperature', 'coefficient', 'ntc', 'zone', 'a', 'detailed', 'kinetic', 'mechanism', 'has', 'been', 'developed', 'u... | [-0.06114620376439368, 0.1662417200096257, -0.04899885757734663, 0.005247337678752718, -0.008271873770205334, -0.12786938588241817, 0.09601346904232518, 0.3585317634145317, -0.22945507724681624, -0.3398364825845986, 0.06412362500445032, -0.2917715355784434, -0.0442653972821689, 0.19481319868479108, 0.030837713450681967... |
706.2065 | Weak collapsing and geometrisation of aspherical 3-manifolds | Let M be a closed, orientable, irreducible, non-simply connected 3-manifold.
We prove that if M admits a sequence of Riemannian metrics whose sectional
curvature is locally controlled and whose thick part becomes asymptotically
hyperbolic and has a sufficiently small volume, then M is Seifert fibred or
contains an in... | math.GT | let m be a closed orientable irreducible nonsimply connected 3manifold we prove that if m admits a sequence of riemannian metrics whose sectional curvature is locally controlled and whose thick part becomes asymptotically hyperbolic and has a sufficiently small volume then m is seifert fibred or contains an incompressi... | [['let', 'm', 'be', 'a', 'closed', 'orientable', 'irreducible', 'nonsimply', 'connected', '3manifold', 'we', 'prove', 'that', 'if', 'm', 'admits', 'a', 'sequence', 'of', 'riemannian', 'metrics', 'whose', 'sectional', 'curvature', 'is', 'locally', 'controlled', 'and', 'whose', 'thick', 'part', 'becomes', 'asymptotically... | [-0.277072366932407, 0.15527305865751778, -0.13545601232243434, 0.033614199384049116, -0.12629172771370836, -0.2325786908622831, -0.0815344535496219, 0.340207313267248, -0.2255884169143558, -0.2300391894233014, 0.10733868367803683, -0.2593175803344431, -0.12495675666224478, 0.19502084576524795, -0.21387140146855796, -0... |
706.2066 | Primary reactions of the thermal decomposition of tricyclodecane | In order to better understand the thermal decomposition of polycyclanes, the
pyrolysis of tricyclodecane has been studied in a jet-stirred reactor at
temperatures from 848 to 933 K, for residence times between 0.5 and 6 s and at
atmospheric pressure, in order to obtain a conversion between 0.01 and 25 %.
The main pro... | physics.chem-ph | in order to better understand the thermal decomposition of polycyclanes the pyrolysis of tricyclodecane has been studied in a jetstirred reactor at temperatures from 848 to 933 k for residence times between 05 and 6 s and at atmospheric pressure in order to obtain a conversion between 001 and 25 the main products of th... | [['in', 'order', 'to', 'better', 'understand', 'the', 'thermal', 'decomposition', 'of', 'polycyclanes', 'the', 'pyrolysis', 'of', 'tricyclodecane', 'has', 'been', 'studied', 'in', 'a', 'jetstirred', 'reactor', 'at', 'temperatures', 'from', '848', 'to', '933', 'k', 'for', 'residence', 'times', 'between', '05', 'and', '6... | [-0.030930487039611387, 0.14076336435090495, -0.03306318650570104, -0.0030467829442229763, 0.04340120816627389, -0.0829772316441261, 0.04745183546790564, 0.3792607566534445, -0.23090278776362538, -0.35028759480036536, 0.09397281294564139, -0.2961706050275474, -0.04666367331660224, 0.19248208173566722, 0.022523876165184... |
706.2067 | Use of detailed kinetic mechanisms for the prediction of autoignitions | This paper describes how automatically generated detailed kinetic mechanisms
are obtained for the oxidation of alkanes and how these models could lead to a
better understanding of autoignition and cool flame risks at elevated
conditions. Examples of prediction of the occurrence of different autoignition
phenomena, su... | physics.chem-ph | this paper describes how automatically generated detailed kinetic mechanisms are obtained for the oxidation of alkanes and how these models could lead to a better understanding of autoignition and cool flame risks at elevated conditions examples of prediction of the occurrence of different autoignition phenomena such a... | [['this', 'paper', 'describes', 'how', 'automatically', 'generated', 'detailed', 'kinetic', 'mechanisms', 'are', 'obtained', 'for', 'the', 'oxidation', 'of', 'alkanes', 'and', 'how', 'these', 'models', 'could', 'lead', 'to', 'a', 'better', 'understanding', 'of', 'autoignition', 'and', 'cool', 'flame', 'risks', 'at', 'e... | [-0.048161189696645436, 0.23521776509152936, -0.055420201186302906, 0.059736789373645585, -0.01288108645254581, -0.1629744215243602, 0.02771598153122807, 0.3802340099753081, -0.22195941381910933, -0.3054899210198723, 0.10538785411870177, -0.29330855485381957, -0.08029801394094867, 0.2166020333077287, -0.020468163380658... |
706.2068 | Experimental study of the structure of rich premixed
1,3-butadiene/CH4/O2/Ar flame | The structure of a laminar rich premixed 1,3-C4H6/CH4/O2/Ar flame have been
investigated. 1,3-Butadiene, methane, oxygen and argon mole fractions are
0.033; 0.2073; 0.3315, and 0.4280, respectively, for an equivalent ratio of
1.80. The flame has been stabilized on a burner at a pressure of 6.7 kPa (50
Torr). The conc... | physics.chem-ph | the structure of a laminar rich premixed 13c4h6ch4o2ar flame have been investigated 13butadiene methane oxygen and argon mole fractions are 0033 02073 03315 and 04280 respectively for an equivalent ratio of 180 the flame has been stabilized on a burner at a pressure of 67 kpa 50 torr the concentration profiles of stabl... | [['the', 'structure', 'of', 'a', 'laminar', 'rich', 'premixed', '13c4h6ch4o2ar', 'flame', 'have', 'been', 'investigated', '13butadiene', 'methane', 'oxygen', 'and', 'argon', 'mole', 'fractions', 'are', '0033', '02073', '03315', 'and', '04280', 'respectively', 'for', 'an', 'equivalent', 'ratio', 'of', '180', 'the', 'fla... | [-0.008050138506300715, 0.2352682944714036, 0.008732776961132753, -0.06047532844240777, 0.1241413498960798, -0.14099750910531236, 0.09677308679721112, 0.41979964982370016, -0.1836570033049458, -0.30093101412469964, 0.07869912345998764, -0.33516265432127806, 0.07639287547331995, 0.13272173893823397, 0.023011132916105927... |
706.2069 | Building Portable Thread Schedulers for Hierarchical Multiprocessors:
the BubbleSched Framework | Exploiting full computational power of current more and more hierarchical
multiprocessor machines requires a very careful distribution of threads and
data among the underlying non-uniform architecture. Unfortunately, most
operating systems only provide a poor scheduling API that does not allow
applications to transmi... | cs.DC | exploiting full computational power of current more and more hierarchical multiprocessor machines requires a very careful distribution of threads and data among the underlying nonuniform architecture unfortunately most operating systems only provide a poor scheduling api that does not allow applications to transmit val... | [['exploiting', 'full', 'computational', 'power', 'of', 'current', 'more', 'and', 'more', 'hierarchical', 'multiprocessor', 'machines', 'requires', 'a', 'very', 'careful', 'distribution', 'of', 'threads', 'and', 'data', 'among', 'the', 'underlying', 'nonuniform', 'architecture', 'unfortunately', 'most', 'operating', 's... | [-0.16270872994988475, 0.04233325106045887, -0.1335898751333933, 0.05258150428900836, -0.1931887238752097, -0.24802822861689286, 0.11459499863173131, 0.45584306273032243, -0.2476166800610577, -0.3615106748167793, 0.0920491097658925, -0.18624975303572056, -0.14159400496815502, 0.2590530011720929, -0.12239805614890557, 0... |
706.207 | Probing CP violation in neutrino oscillations with neutrino telescopes | Measurements of flavor ratios of astrophysical neutrino fluxes are sensitive
to the two yet unknown mixing parameters $\theta_{13}$ and $\delta$ through the
combination $\sin\theta_{13}\cos\delta$. We extend previous studies by
considering the possibility that neutrino fluxes from more than a single type
of sources w... | hep-ph astro-ph | measurements of flavor ratios of astrophysical neutrino fluxes are sensitive to the two yet unknown mixing parameters theta_13 and delta through the combination sintheta_13cosdelta we extend previous studies by considering the possibility that neutrino fluxes from more than a single type of sources will be measured we ... | [['measurements', 'of', 'flavor', 'ratios', 'of', 'astrophysical', 'neutrino', 'fluxes', 'are', 'sensitive', 'to', 'the', 'two', 'yet', 'unknown', 'mixing', 'parameters', 'theta_13', 'and', 'delta', 'through', 'the', 'combination', 'sintheta_13cosdelta', 'we', 'extend', 'previous', 'studies', 'by', 'considering', 'the'... | [-0.0937091030854667, 0.2640921863644629, 0.018527764060041484, 0.16643117925458473, -0.05182925360725525, -0.1562990389495371, 0.10740567762454484, 0.3393267051361621, -0.17270055864215456, -0.37175846943024166, 0.10554611411837134, -0.312646727792341, -0.012286646890498817, 0.25987000107381714, 0.010696371955010183, ... |
706.2071 | Three loop DIS and transversity operator anomalous dimensions in the RI'
scheme | We discuss the computation of the three loop anomalous dimensions for various
operators used in deep inelastic scattering in the MSbar and RI' schemes. In
particular the results for the n = 5 and 6 Wilson operators in arbitrary linear
covariant gauge in the RI' scheme are new.
| hep-ph | we discuss the computation of the three loop anomalous dimensions for various operators used in deep inelastic scattering in the msbar and ri schemes in particular the results for the n 5 and 6 wilson operators in arbitrary linear covariant gauge in the ri scheme are new | [['we', 'discuss', 'the', 'computation', 'of', 'the', 'three', 'loop', 'anomalous', 'dimensions', 'for', 'various', 'operators', 'used', 'in', 'deep', 'inelastic', 'scattering', 'in', 'the', 'msbar', 'and', 'ri', 'schemes', 'in', 'particular', 'the', 'results', 'for', 'the', 'n', '5', 'and', '6', 'wilson', 'operators',... | [-0.12149950908496976, 0.194603360030166, -0.03981413505971432, 0.13459365133275378, 0.04790971756100337, -0.1554644839402209, 0.0010981700442572856, 0.38440941432689096, -0.1892338882576912, -0.24893047288060188, 0.07755531813265716, -0.2562928206703447, -0.15243225487721887, 0.1825271578644343, -0.040525043947359625,... |
706.2072 | A FRW Dark Fluid with a Non-Linear Inhomogeneous Equation of State | A dark Friedman-Robertson-Walker fluid governed by a non-linear inhomogeneous
equation of state is considered which can be viewed as a conveniently simple
paradigm for a whole class of models which exhibit phase transitions from a
non-phantom towards a phantom era (superacceleration transition). From another
side, su... | gr-qc | a dark friedmanrobertsonwalker fluid governed by a nonlinear inhomogeneous equation of state is considered which can be viewed as a conveniently simple paradigm for a whole class of models which exhibit phase transitions from a nonphantom towards a phantom era superacceleration transition from another side such dark fl... | [['a', 'dark', 'friedmanrobertsonwalker', 'fluid', 'governed', 'by', 'a', 'nonlinear', 'inhomogeneous', 'equation', 'of', 'state', 'is', 'considered', 'which', 'can', 'be', 'viewed', 'as', 'a', 'conveniently', 'simple', 'paradigm', 'for', 'a', 'whole', 'class', 'of', 'models', 'which', 'exhibit', 'phase', 'transitions'... | [-0.12889962943570157, 0.16052168595251715, -0.15807679121124757, 0.07965485267569809, -0.10246131996973418, -0.132870633899334, -0.05674589325540832, 0.2795255738643131, -0.2573337569400402, -0.2941828345647082, 0.07788475077645021, -0.2344528702399527, -0.08814067114144564, 0.16246006504765578, 0.018993151815444826, ... |
706.2073 | An Efficient OpenMP Runtime System for Hierarchical Arch | Exploiting the full computational power of always deeper hierarchical
multiprocessor machines requires a very careful distribution of threads and
data among the underlying non-uniform architecture. The emergence of multi-core
chips and NUMA machines makes it important to minimize the number of remote
memory accesses,... | cs.PL | exploiting the full computational power of always deeper hierarchical multiprocessor machines requires a very careful distribution of threads and data among the underlying nonuniform architecture the emergence of multicore chips and numa machines makes it important to minimize the number of remote memory accesses to fa... | [['exploiting', 'the', 'full', 'computational', 'power', 'of', 'always', 'deeper', 'hierarchical', 'multiprocessor', 'machines', 'requires', 'a', 'very', 'careful', 'distribution', 'of', 'threads', 'and', 'data', 'among', 'the', 'underlying', 'nonuniform', 'architecture', 'the', 'emergence', 'of', 'multicore', 'chips',... | [-0.18591751058280853, 0.02928196178693505, -0.062280785920628315, 0.048549954056868266, -0.13928352127750887, -0.20879830976402194, 0.1180674859065691, 0.4364671888279504, -0.2818265238070282, -0.39503872770302256, 0.07784443520459122, -0.17189914724339955, -0.09417728550535434, 0.1870504235316887, -0.0797183763372294... |
706.2074 | Analysis on Heavy Quarkonia Transitions with Pion Emission in Terms of
the QCD Multipole Expansion and Determination of Mass Spectra of Hybrids | One of the most important tasks in high energy physics is search for the
exotic states, such as glueball, hybrid and multi-quark states. The transitions
$\psi(ns)\to \psi(ms)+\pi\pi$ and $\Upsilon(ns)\to \Upsilon(ms)+\pi\pi$ attract
great attentions because they may reveal characteristics of hybrids. In this
work, we... | hep-ph | one of the most important tasks in high energy physics is search for the exotic states such as glueball hybrid and multiquark states the transitions psinsto psimspipi and upsilonnsto upsilonmspipi attract great attentions because they may reveal characteristics of hybrids in this work we analyze those transition modes ... | [['one', 'of', 'the', 'most', 'important', 'tasks', 'in', 'high', 'energy', 'physics', 'is', 'search', 'for', 'the', 'exotic', 'states', 'such', 'as', 'glueball', 'hybrid', 'and', 'multiquark', 'states', 'the', 'transitions', 'psinsto', 'psimspipi', 'and', 'upsilonnsto', 'upsilonmspipi', 'attract', 'great', 'attentions... | [-0.0774258367183958, 0.1966805944433184, -0.09615081943558983, 0.12798457770377109, -0.02241995354258531, -0.16248766134014805, 0.050482883726127095, 0.39290916081517935, -0.16951568836324243, -0.34027081911728996, 0.051499970696199486, -0.3094135468095742, -0.08567111427593674, 0.17010563098419634, 0.0004908101943107... |
706.2075 | Bianchi Model CMB Polarization and its Implications for CMB Anomalies | We derive the CMB radiative transfer equation in the form of a multipole
hierarchy in the nearly-Friedmann-Robertson-Walker limit of homogeneous, but
anisotropic, universes classified via their Bianchi type. Compared with
previous calculations, this allows a more sophisticated treatment of
recombination, produces pre... | astro-ph | we derive the cmb radiative transfer equation in the form of a multipole hierarchy in the nearlyfriedmannrobertsonwalker limit of homogeneous but anisotropic universes classified via their bianchi type compared with previous calculations this allows a more sophisticated treatment of recombination produces predictions f... | [['we', 'derive', 'the', 'cmb', 'radiative', 'transfer', 'equation', 'in', 'the', 'form', 'of', 'a', 'multipole', 'hierarchy', 'in', 'the', 'nearlyfriedmannrobertsonwalker', 'limit', 'of', 'homogeneous', 'but', 'anisotropic', 'universes', 'classified', 'via', 'their', 'bianchi', 'type', 'compared', 'with', 'previous', ... | [-0.10170577511397698, 0.1228880768287378, -0.07861331189657009, 0.08486199015808268, -0.11355671797863896, -0.10835945916010022, -0.014233209869949283, 0.35164484453607137, -0.22095922227476616, -0.3142139910705145, 0.06214820025952503, -0.31854969431559566, -0.06576900841948402, 0.18354951422301885, 0.033080399061015... |
706.2076 | A Finite Semantics of Simply-Typed Lambda Terms for Infinite Runs of<br>
Automata | Model checking properties are often described by means of finite automata.
Any particular such automaton divides the set of infinite trees into finitely
many classes, according to which state has an infinite run. Building the full
type hierarchy upon this interpretation of the base type gives a finite
semantics for s... | cs.LO | model checking properties are often described by means of finite automata any particular such automaton divides the set of infinite trees into finitely many classes according to which state has an infinite run building the full type hierarchy upon this interpretation of the base type gives a finite semantics for simply... | [['model', 'checking', 'properties', 'are', 'often', 'described', 'by', 'means', 'of', 'finite', 'automata', 'any', 'particular', 'such', 'automaton', 'divides', 'the', 'set', 'of', 'infinite', 'trees', 'into', 'finitely', 'many', 'classes', 'according', 'to', 'which', 'state', 'has', 'an', 'infinite', 'run', 'building... | [-0.11941303402717786, 0.1320065392094531, -0.09043371448184824, 0.12988400859283555, -0.16160369747616712, -0.20570917077615714, 0.08280133358338504, 0.3208954886180683, -0.3048182292977004, -0.23044204686596556, 0.12028119176766355, -0.1960517511368521, -0.06987582701167942, 0.19098936580121517, -0.10017055684917615,... |
706.2077 | Codon Usage Bias Measured Through Entropy Approach | Codon usage bias measure is defined through the mutual entropy calculation of
real codon frequency distribution against the quasi-equilibrium one. This
latter is defined in three manners: (1) the frequency of synonymous codons is
supposed to be equal (i.e., the arithmetic mean of their frequencies); (2) it
coincides ... | q-bio.GN | codon usage bias measure is defined through the mutual entropy calculation of real codon frequency distribution against the quasiequilibrium one this latter is defined in three manners 1 the frequency of synonymous codons is supposed to be equal ie the arithmetic mean of their frequencies 2 it coincides to the frequenc... | [['codon', 'usage', 'bias', 'measure', 'is', 'defined', 'through', 'the', 'mutual', 'entropy', 'calculation', 'of', 'real', 'codon', 'frequency', 'distribution', 'against', 'the', 'quasiequilibrium', 'one', 'this', 'latter', 'is', 'defined', 'in', 'three', 'manners', '1', 'the', 'frequency', 'of', 'synonymous', 'codons... | [-0.15163813343943647, 0.18854154712012547, -0.05146913516165858, 0.12226125864650715, -0.018329038422300735, -0.11676854538646611, 0.09554422426026576, 0.363642210627652, -0.28673924650700594, -0.26396966101178393, 0.04388626286791722, -0.24308145997929387, -0.08286572448824617, 0.166081972589547, -0.06893607818876096... |
706.2078 | Nonclassical dynamics of Bose condensates in an optical lattice in the
superfluid regime | A condensate in an optical lattice, prepared in the ground state of the
superfluid regime, is stimulated first by suddenly increasing the optical
lattice amplitude and then, after a waiting time, by abruptly decreasing this
amplitude to its initial value. Thus the system is first taken to the Mott
regime and then bac... | cond-mat.mes-hall cond-mat.other | a condensate in an optical lattice prepared in the ground state of the superfluid regime is stimulated first by suddenly increasing the optical lattice amplitude and then after a waiting time by abruptly decreasing this amplitude to its initial value thus the system is first taken to the mott regime and then back to th... | [['a', 'condensate', 'in', 'an', 'optical', 'lattice', 'prepared', 'in', 'the', 'ground', 'state', 'of', 'the', 'superfluid', 'regime', 'is', 'stimulated', 'first', 'by', 'suddenly', 'increasing', 'the', 'optical', 'lattice', 'amplitude', 'and', 'then', 'after', 'a', 'waiting', 'time', 'by', 'abruptly', 'decreasing', '... | [-0.14807406140209958, 0.22681542293081922, -0.12032799274164835, 0.019142258551000327, 0.015679299709112415, -0.1120823648818534, 0.06874896612658213, 0.3373497980881295, -0.3112655483176195, -0.22595882785955457, 0.10027600350293914, -0.2586906417105481, -0.11626174375615853, 0.16270419667984137, 0.009481250938269303... |
706.2079 | Collective Charge Excitations below the Metal-to-Insulator Transition in
BaVS3 | The charge response in the barium vanadium sulfide (BaVS3) single crystals is
characterized by dc resistivity and low frequency dielectric spectroscopy. A
broad relaxation mode in MHz range with huge dielectric constant ~= 10^6
emerges at the metal-to-insulator phase transition TMI ~= 67 K, weakens with
lowering temp... | cond-mat.str-el | the charge response in the barium vanadium sulfide bavs3 single crystals is characterized by dc resistivity and low frequency dielectric spectroscopy a broad relaxation mode in mhz range with huge dielectric constant 106 emerges at the metaltoinsulator phase transition tmi 67 k weakens with lowering temperature and eve... | [['the', 'charge', 'response', 'in', 'the', 'barium', 'vanadium', 'sulfide', 'bavs3', 'single', 'crystals', 'is', 'characterized', 'by', 'dc', 'resistivity', 'and', 'low', 'frequency', 'dielectric', 'spectroscopy', 'a', 'broad', 'relaxation', 'mode', 'in', 'mhz', 'range', 'with', 'huge', 'dielectric', 'constant', '106'... | [-0.1868279838003218, 0.34432299515698106, 0.025389227205887436, -0.04417283059796318, -0.022483234816409094, -0.16424048851476983, 0.140065932336729, 0.37456320570083335, -0.2919822504371405, -0.32040895662386903, 0.009673449393594637, -0.35979987165890637, -0.04419467709492892, 0.1284381679445505, 0.08252026901580393... |
706.208 | Experiments on the twisted vortex state in superfluid 3He-B | We have performed measurements and numerical simulations on a bundle of
vortex lines which is expanding along a rotating column of initially
vortex-free 3He-B. Expanding vortices form a propagating front: Within the
front the superfluid is involved in rotation and behind the front the twisted
vortex state forms, whic... | cond-mat.soft | we have performed measurements and numerical simulations on a bundle of vortex lines which is expanding along a rotating column of initially vortexfree 3heb expanding vortices form a propagating front within the front the superfluid is involved in rotation and behind the front the twisted vortex state forms which event... | [['we', 'have', 'performed', 'measurements', 'and', 'numerical', 'simulations', 'on', 'a', 'bundle', 'of', 'vortex', 'lines', 'which', 'is', 'expanding', 'along', 'a', 'rotating', 'column', 'of', 'initially', 'vortexfree', '3heb', 'expanding', 'vortices', 'form', 'a', 'propagating', 'front', 'within', 'the', 'front', '... | [-0.19429153710683827, 0.22661582543264314, -0.09804797637206251, -0.029559224010294965, -0.04252581100069707, -0.05392993093338064, 0.04168430792408124, 0.36773715640408217, -0.26377404407067323, -0.2045495425593809, 0.10159654420505088, -0.24808395992443766, -0.053104334761218355, 0.1564523916571371, 0.06351274554774... |
706.2081 | Preserving zeros of a polynomial | We study non-linear surjective mappings on subsets of ${\cal M}_n(F)$, which
preserve the zeros of some fixed polynomials in noncommuting variables.
Keywords: Matrix algebra, Multilinear polynomials, Preservers.
| math.RA | we study nonlinear surjective mappings on subsets of cal m_nf which preserve the zeros of some fixed polynomials in noncommuting variables keywords matrix algebra multilinear polynomials preservers | [['we', 'study', 'nonlinear', 'surjective', 'mappings', 'on', 'subsets', 'of', 'cal', 'm_nf', 'which', 'preserve', 'the', 'zeros', 'of', 'some', 'fixed', 'polynomials', 'in', 'noncommuting', 'variables', 'keywords', 'matrix', 'algebra', 'multilinear', 'polynomials', 'preservers']] | [-0.22474677819344732, 0.050821350111315645, 0.007635904889967706, 0.03836353027468754, -0.12718351006818315, -0.164778682851681, -0.00818260710824419, 0.3083542774741848, -0.41015751466706946, -0.0737143601808283, 0.13350671075750142, -0.3495426807138655, -0.21737579235600102, 0.09987686326106389, -0.1540148458616049,... |
706.2082 | Elementary Excitations of a Bose-Einstein Condensate in an Effective
Magnetic Field | We calculate the low energy elementary excitations of a Bose-Einstein
Condensate in an effective magnetic field. The field is created by the
interplay between light beams carrying orbital angular momentum and the trapped
atoms. We examine the role of the homogeneous magnetic field, familiar from
studies of rotating c... | cond-mat.other | we calculate the low energy elementary excitations of a boseeinstein condensate in an effective magnetic field the field is created by the interplay between light beams carrying orbital angular momentum and the trapped atoms we examine the role of the homogeneous magnetic field familiar from studies of rotating condens... | [['we', 'calculate', 'the', 'low', 'energy', 'elementary', 'excitations', 'of', 'a', 'boseeinstein', 'condensate', 'in', 'an', 'effective', 'magnetic', 'field', 'the', 'field', 'is', 'created', 'by', 'the', 'interplay', 'between', 'light', 'beams', 'carrying', 'orbital', 'angular', 'momentum', 'and', 'the', 'trapped', ... | [-0.18912567108762576, 0.2721250735593384, -0.0802351290901267, 0.11844553957800255, -0.03986078431842396, -0.0802663274461756, -0.014344772953238036, 0.36026112810784094, -0.2401115618444778, -0.29039684715806635, 0.0028798462920570493, -0.25966430280508623, -0.08816148654158176, 0.16460678710702908, 0.046553015732521... |
706.2083 | Huge negative differential conductance in Au-H2 molecular nanojunctions | Experimental results showing huge negative differential conductance in
gold-hydrogen molecular nanojunctions are presented. The results are analyzed
in terms of two-level system (TLS) models: it is shown that a simple TLS model
cannot produce peaklike structures in the differential conductance curves,
whereas an asym... | cond-mat.mes-hall | experimental results showing huge negative differential conductance in goldhydrogen molecular nanojunctions are presented the results are analyzed in terms of twolevel system tls models it is shown that a simple tls model cannot produce peaklike structures in the differential conductance curves whereas an asymmetricall... | [['experimental', 'results', 'showing', 'huge', 'negative', 'differential', 'conductance', 'in', 'goldhydrogen', 'molecular', 'nanojunctions', 'are', 'presented', 'the', 'results', 'are', 'analyzed', 'in', 'terms', 'of', 'twolevel', 'system', 'tls', 'models', 'it', 'is', 'shown', 'that', 'a', 'simple', 'tls', 'model', ... | [-0.17160506569404876, 0.10009013296255807, -0.07635782566922968, 0.073080578240596, 0.0021813460976205846, -0.18997616935220937, 0.007668820249858082, 0.3554453828862758, -0.23354875987335558, -0.32209340464924613, 0.008237726777361365, -0.3188580108445979, -0.1806608803134652, 0.24259691316664458, -0.0391491343322340... |
706.2084 | Phase lapses in scattering through multi-electron quantum dots:
Mean-field and few-particle regimes | We show that the observed evolution of the transmission phase through
multi-electron quantum dots with more than approximately ten electrons, which
shows a universal (i.e., independent of N) as yet unexplained behavior, is
consistent with an electrostatic model, where electron-electron interaction is
described by a m... | cond-mat.mes-hall | we show that the observed evolution of the transmission phase through multielectron quantum dots with more than approximately ten electrons which shows a universal ie independent of n as yet unexplained behavior is consistent with an electrostatic model where electronelectron interaction is described by a meanfield app... | [['we', 'show', 'that', 'the', 'observed', 'evolution', 'of', 'the', 'transmission', 'phase', 'through', 'multielectron', 'quantum', 'dots', 'with', 'more', 'than', 'approximately', 'ten', 'electrons', 'which', 'shows', 'a', 'universal', 'ie', 'independent', 'of', 'n', 'as', 'yet', 'unexplained', 'behavior', 'is', 'con... | [-0.14712890584161506, 0.20032216822938062, -0.08045669695921243, 0.04030256792157889, 0.038742328606545924, -0.20264481635019183, 0.06419384252466262, 0.3415024979263544, -0.23085829474776984, -0.2945670551210642, -0.003030785458162427, -0.30526068641245363, -0.16095377814769746, 0.21606439924612642, 0.035291324203833... |
706.2085 | Quantum phase transitions in a resonant-level model with dissipation:
Renormalization-group studies | We study a spinless level that hybridizes with a fermionic band and is also
coupled via its charge to a dissipative bosonic bath. We consider the general
case of a power-law hybridization function $\Gamma(\w)\propto |\w|^r$ with
$r\ge 0$, and a bosonic bath spectral function $B(\w)\propto \w^s$ with $s\ge
-1$. For $r... | cond-mat.str-el cond-mat.mes-hall | we study a spinless level that hybridizes with a fermionic band and is also coupled via its charge to a dissipative bosonic bath we consider the general case of a powerlaw hybridization function gammawpropto wr with rge 0 and a bosonic bath spectral function bwpropto ws with sge 1 for r1 and mathrmmax02r1s1 this bosefe... | [['we', 'study', 'a', 'spinless', 'level', 'that', 'hybridizes', 'with', 'a', 'fermionic', 'band', 'and', 'is', 'also', 'coupled', 'via', 'its', 'charge', 'to', 'a', 'dissipative', 'bosonic', 'bath', 'we', 'consider', 'the', 'general', 'case', 'of', 'a', 'powerlaw', 'hybridization', 'function', 'gammawpropto', 'wr', 'w... | [-0.12917667583872874, 0.21208325342999565, -0.0775384847316201, 0.08038701000106004, 0.03319556768466201, -0.24443716926638176, 0.1067876496559216, 0.34650871875281963, -0.21721798538195866, -0.2281976403185615, -0.01153587264922896, -0.345053174443267, -0.14298631680301493, 0.1329633477350904, 0.07146934555429552, 0.... |
706.2086 | On the relation between the proton-air cross section and fluctuations of
the shower longitudinal profile | The current status and prospects of deducing the proton-air cross section
from fluorescence telescope measurements of extensive air showers are
discussed. As it is not possible to observe the point of first interaction, $X_
{\rm 1}$, directly, other observables closely linked to $X_{\rm 1}$ must be
inferred from the ... | astro-ph | the current status and prospects of deducing the protonair cross section from fluorescence telescope measurements of extensive air showers are discussed as it is not possible to observe the point of first interaction x_ rm 1 directly other observables closely linked to x_rm 1 must be inferred from the measured longitud... | [['the', 'current', 'status', 'and', 'prospects', 'of', 'deducing', 'the', 'protonair', 'cross', 'section', 'from', 'fluorescence', 'telescope', 'measurements', 'of', 'extensive', 'air', 'showers', 'are', 'discussed', 'as', 'it', 'is', 'not', 'possible', 'to', 'observe', 'the', 'point', 'of', 'first', 'interaction', 'x... | [-0.03379466823103388, 0.1447840544573042, -0.08709121991084297, 0.09493616379645727, -0.043391058817924405, -0.039065011295626, -0.005442711992942718, 0.3934026811732335, -0.28177480692608975, -0.362909331645691, 0.0832153901332215, -0.3430351667064294, -0.06816645661431751, 0.19552041448684138, 0.019042456773727127, ... |
706.2087 | Generalized rotating-wave approximation for arbitrarily large coupling | A generalized version of the rotating-wave approximation for the single-mode
spin-boson Hamiltonian is presented. It is shown that performing a simple
change of basis prior to eliminating the off-resonant terms results in a
significantly more accurate expression for the energy levels of the system. The
generalized ap... | quant-ph | a generalized version of the rotatingwave approximation for the singlemode spinboson hamiltonian is presented it is shown that performing a simple change of basis prior to eliminating the offresonant terms results in a significantly more accurate expression for the energy levels of the system the generalized approximat... | [['a', 'generalized', 'version', 'of', 'the', 'rotatingwave', 'approximation', 'for', 'the', 'singlemode', 'spinboson', 'hamiltonian', 'is', 'presented', 'it', 'is', 'shown', 'that', 'performing', 'a', 'simple', 'change', 'of', 'basis', 'prior', 'to', 'eliminating', 'the', 'offresonant', 'terms', 'results', 'in', 'a', ... | [-0.1300715643413631, 0.10183152199190643, -0.0482925838857357, 0.05892518140442137, -0.017276587224166307, -0.1386815398399319, 0.06583706039403166, 0.35276808930294856, -0.19277122262865304, -0.294686426914164, 0.017968631958189818, -0.2102191198750266, -0.14179231094728623, 0.29792937295777455, 0.006246418738737702,... |
706.2088 | Laplacian instability of planar streamer ionization fronts - an example
of pulled front analysis | Streamer ionization fronts are pulled fronts propagating into a linearly
unstable state; the spatial decay of the initial condition of a planar front
selects dynamically one specific long time attractor out of a continuous
family. A transverse stability analysis has to take these features into
account. In this paper ... | nlin.PS | streamer ionization fronts are pulled fronts propagating into a linearly unstable state the spatial decay of the initial condition of a planar front selects dynamically one specific long time attractor out of a continuous family a transverse stability analysis has to take these features into account in this paper we in... | [['streamer', 'ionization', 'fronts', 'are', 'pulled', 'fronts', 'propagating', 'into', 'a', 'linearly', 'unstable', 'state', 'the', 'spatial', 'decay', 'of', 'the', 'initial', 'condition', 'of', 'a', 'planar', 'front', 'selects', 'dynamically', 'one', 'specific', 'long', 'time', 'attractor', 'out', 'of', 'a', 'continu... | [-0.18389133406711405, 0.1357974095272105, -0.10625965304194333, 0.06616973980963535, -0.054157890867991526, -0.10685954392376187, 0.011879472803105626, 0.3215506347863238, -0.2702076354857962, -0.24907826955170662, 0.09077550602181912, -0.2649952659123867, -0.11571483685039595, 0.18290028964230393, 0.05079143337111493... |
706.2089 | Electron Correlation Driven Heavy-Fermion Formation in LiV2O4 | Optical reflectivity measurements were performed on a single crystal of the
d-electron heavy-fermion (HF) metal LiV2O4. The results evidence the highly
incoherent character of the charge dynamics for all temperatures above T^*
\approx 20 K. The spectral weight of the optical conductivity is redistributed
over extreme... | cond-mat.str-el | optical reflectivity measurements were performed on a single crystal of the delectron heavyfermion hf metal liv2o4 the results evidence the highly incoherent character of the charge dynamics for all temperatures above t approx 20 k the spectral weight of the optical conductivity is redistributed over extremely broad en... | [['optical', 'reflectivity', 'measurements', 'were', 'performed', 'on', 'a', 'single', 'crystal', 'of', 'the', 'delectron', 'heavyfermion', 'hf', 'metal', 'liv2o4', 'the', 'results', 'evidence', 'the', 'highly', 'incoherent', 'character', 'of', 'the', 'charge', 'dynamics', 'for', 'all', 'temperatures', 'above', 't', 'a... | [-0.17010319677419625, 0.22307784052636156, -0.03930483920555702, 0.05800455052815238, 0.01061239970070695, -0.13354002157772393, 0.09474780828397918, 0.34661551428559634, -0.2719135393451591, -0.2732900714228644, -0.015474632689624297, -0.34507333932626516, -0.0822772060667998, 0.15415972124967248, 0.0585349273388239,... |
706.209 | The flavour projection of staggered fermions and the quarter-root trick | It is shown that the flavour projection of staggered fermions can be written
as a projection between the fields on four separate, but parallel, lattices,
where the fields on each are modified forms of the standard staggered fermion
field. Because the staggered Dirac operator acts equally on each lattice, it
respects ... | hep-lat | it is shown that the flavour projection of staggered fermions can be written as a projection between the fields on four separate but parallel lattices where the fields on each are modified forms of the standard staggered fermion field because the staggered dirac operator acts equally on each lattice it respects this fl... | [['it', 'is', 'shown', 'that', 'the', 'flavour', 'projection', 'of', 'staggered', 'fermions', 'can', 'be', 'written', 'as', 'a', 'projection', 'between', 'the', 'fields', 'on', 'four', 'separate', 'but', 'parallel', 'lattices', 'where', 'the', 'fields', 'on', 'each', 'are', 'modified', 'forms', 'of', 'the', 'standard',... | [-0.11872840123420071, 0.2021072643748935, -0.0965387374162674, 0.049466275470143546, -0.10262195529761695, -0.14510120086807518, 0.02815009789511321, 0.40834117273709947, -0.2736622779667678, -0.20223049918610242, 0.08290636530258663, -0.25260930965023654, -0.1038230479114704, 0.12053416996833778, -0.02327013151314590... |
706.2091 | Pion freeze-out as seen through HBT correlations in heavy ion collisions
from FAIR/AGS to RHIC energies | We perform a systematic analysis of several HBT parameters in heavy ion
collisions from $E_{\rm beam}=2$ AGeV to $\sqrt {s_{\rm NN}}=200$ GeV within
the UrQMD transport approach and compare the results to experimental data where
available. We find that the 'lifetime' of the emission source as calculated
from $\tau \s... | nucl-th | we perform a systematic analysis of several hbt parameters in heavy ion collisions from e_rm beam2 agev to sqrt s_rm nn200 gev within the urqmd transport approach and compare the results to experimental data where available we find that the lifetime of the emission source as calculated from tau sim sqrtr_o2r_s2 is larg... | [['we', 'perform', 'a', 'systematic', 'analysis', 'of', 'several', 'hbt', 'parameters', 'in', 'heavy', 'ion', 'collisions', 'from', 'e_rm', 'beam2', 'agev', 'to', 'sqrt', 's_rm', 'nn200', 'gev', 'within', 'the', 'urqmd', 'transport', 'approach', 'and', 'compare', 'the', 'results', 'to', 'experimental', 'data', 'where',... | [-0.06096313283496508, 0.208627826502462, -0.10049249743337207, 0.13225451658857337, 0.033178477378731426, -0.11707556318618696, 0.01799829022352104, 0.37404650885781104, -0.22771263397722083, -0.3350882083547979, -0.06089046109330163, -0.35915674094223615, 0.07455907509464657, 0.20394242055375467, 0.08774627548458132,... |
706.2092 | The Monte Carlo and fractional kinetics approaches to the underground
anomalous subdiffusion of contaminants | This paper deals with a comparison of Fractional Derivative and Monte carlo
approaches to the modelling of anomalous diffusion in the field of particle
transport. The goal of this research is to provide a better insight on the
behavior of (radioactive) contaminant tracers when flowing through
heterogeneous media.
| cond-mat.stat-mech | this paper deals with a comparison of fractional derivative and monte carlo approaches to the modelling of anomalous diffusion in the field of particle transport the goal of this research is to provide a better insight on the behavior of radioactive contaminant tracers when flowing through heterogeneous media | [['this', 'paper', 'deals', 'with', 'a', 'comparison', 'of', 'fractional', 'derivative', 'and', 'monte', 'carlo', 'approaches', 'to', 'the', 'modelling', 'of', 'anomalous', 'diffusion', 'in', 'the', 'field', 'of', 'particle', 'transport', 'the', 'goal', 'of', 'this', 'research', 'is', 'to', 'provide', 'a', 'better', 'i... | [-0.0737556254316587, 0.08825108244006212, -0.105951850314644, 0.037972666694258805, -0.08206017618067563, -0.07475742148623492, 0.009862496262940113, 0.3616494926003118, -0.2800707685140272, -0.3064466254387905, 0.08214032706988898, -0.34518874483183026, -0.10409579317395885, 0.19542803604902778, -0.019974684866610914... |
706.2093 | Some Insights in Superdiffusive Transport | In this paper we deal with high-order corrections for the Fractional
Derivative approach to anomalous diffusion, in super-diffusive regime, which
become relevand whenever one attempts to describe the behavior of particles
close to normal diffusion.
| cond-mat.stat-mech | in this paper we deal with highorder corrections for the fractional derivative approach to anomalous diffusion in superdiffusive regime which become relevand whenever one attempts to describe the behavior of particles close to normal diffusion | [['in', 'this', 'paper', 'we', 'deal', 'with', 'highorder', 'corrections', 'for', 'the', 'fractional', 'derivative', 'approach', 'to', 'anomalous', 'diffusion', 'in', 'superdiffusive', 'regime', 'which', 'become', 'relevand', 'whenever', 'one', 'attempts', 'to', 'describe', 'the', 'behavior', 'of', 'particles', 'close'... | [-0.05184629186987877, 0.14734466480748618, -0.09697756966617067, 0.07449847188271473, -0.10756025676999022, -0.17508397826596217, -0.022227078754975295, 0.3314377651275957, -0.31474749437149835, -0.2328422916779185, 0.04682047539801501, -0.3438948627342196, -0.1758437395808013, 0.14783970036489122, -0.0724661893156521... |
706.2094 | Frustration, Area Law, and Interference in Quantum Spin Models | We study frustrated quantum systems from a quantum information perspective.
Within this approach, we find that highly frustrated systems do not follow any
general ''area law'' of block entanglement, while weakly frustrated ones have
area laws similar to those of nonfrustrated systems away from criticality. To
calcula... | quant-ph cond-mat.other | we study frustrated quantum systems from a quantum information perspective within this approach we find that highly frustrated systems do not follow any general area law of block entanglement while weakly frustrated ones have area laws similar to those of nonfrustrated systems away from criticality to calculate the blo... | [['we', 'study', 'frustrated', 'quantum', 'systems', 'from', 'a', 'quantum', 'information', 'perspective', 'within', 'this', 'approach', 'we', 'find', 'that', 'highly', 'frustrated', 'systems', 'do', 'not', 'follow', 'any', 'general', 'area', 'law', 'of', 'block', 'entanglement', 'while', 'weakly', 'frustrated', 'ones'... | [-0.1871785056247408, 0.16660105490564614, -0.08291791806843174, 0.098860909079801, -0.024722569980712115, -0.23570140243518625, 0.08731349444701925, 0.3202205795751906, -0.2549752576126792, -0.26002079458243543, 0.05950281650748575, -0.3240803071008674, -0.16390890131394067, 0.1569501894978464, -0.0421225056614213, 0.... |
706.2095 | Normal and Anomalous Transport across an Interface: Monte Carlo and
Analytical Approach | In this paper we investigate the behavior of particles crossing a neat
interface between two media. A Monte Carlo and analytical model, based on
fractional derivatives, are presented and discussed in detail, together with a
comparison. Anomalous and normal diffusion are consdered.
| cond-mat.stat-mech | in this paper we investigate the behavior of particles crossing a neat interface between two media a monte carlo and analytical model based on fractional derivatives are presented and discussed in detail together with a comparison anomalous and normal diffusion are consdered | [['in', 'this', 'paper', 'we', 'investigate', 'the', 'behavior', 'of', 'particles', 'crossing', 'a', 'neat', 'interface', 'between', 'two', 'media', 'a', 'monte', 'carlo', 'and', 'analytical', 'model', 'based', 'on', 'fractional', 'derivatives', 'are', 'presented', 'and', 'discussed', 'in', 'detail', 'together', 'with'... | [-0.11922481014370555, 0.1168035963186767, -0.09372709413263493, 0.1110887085683871, -0.06544515867603988, -0.1203680066051098, 0.027958488889697302, 0.43371706528634557, -0.2172820847708641, -0.2917037272098951, 0.11770773447891016, -0.3328859669088227, -0.18395016324229357, 0.1772430559063739, 0.022249696838737624, 0... |
706.2096 | Measurement of the UHECR energy spectrum using data from the Surface
Detector of the Pierre Auger Observatory | At the southern site of the Pierre Auger Observatory, which is close to
completion, an exposure that significantly exceeds the largest forerunner
experiments has already been accumulated. We report a measurement of the cosmic
ray energy spectrum based on the high statistics collected by the surface
detector. The meth... | astro-ph | at the southern site of the pierre auger observatory which is close to completion an exposure that significantly exceeds the largest forerunner experiments has already been accumulated we report a measurement of the cosmic ray energy spectrum based on the high statistics collected by the surface detector the methods de... | [['at', 'the', 'southern', 'site', 'of', 'the', 'pierre', 'auger', 'observatory', 'which', 'is', 'close', 'to', 'completion', 'an', 'exposure', 'that', 'significantly', 'exceeds', 'the', 'largest', 'forerunner', 'experiments', 'has', 'already', 'been', 'accumulated', 'we', 'report', 'a', 'measurement', 'of', 'the', 'co... | [-0.075059172298689, 0.09143972998248905, -0.09377078696094926, 0.08211050797295424, -0.030398622517370515, -0.06228392314358008, 0.010650804303290825, 0.3762103513119713, -0.21120466481125544, -0.3698476101345723, 0.08112763718236238, -0.3649208179586345, -0.07111493485706252, 0.22209740842467116, -0.01878444556634696... |
706.2097 | The Physics of 2 is not 1+1 | One of the most surprising consequences of quantum mechanics is the
entanglement of two or more distant particles. In an entangled EPR two-particle
system, the value of the momentum (position) for neither single subsystem is
determined. However, if one of the subsystems is measured to have a certain
momentum (positio... | quant-ph | one of the most surprising consequences of quantum mechanics is the entanglement of two or more distant particles in an entangled epr twoparticle system the value of the momentum position for neither single subsystem is determined however if one of the subsystems is measured to have a certain momentum position the othe... | [['one', 'of', 'the', 'most', 'surprising', 'consequences', 'of', 'quantum', 'mechanics', 'is', 'the', 'entanglement', 'of', 'two', 'or', 'more', 'distant', 'particles', 'in', 'an', 'entangled', 'epr', 'twoparticle', 'system', 'the', 'value', 'of', 'the', 'momentum', 'position', 'for', 'neither', 'single', 'subsystem',... | [-0.1405457926935089, 0.17438915068952587, -0.10329710958014074, 0.05775171725869515, -0.03277021811007843, -0.18445974262431264, -0.019562442607597492, 0.3584894424716591, -0.2818800091913321, -0.2936026453055808, 0.042035888202515144, -0.30297125262193014, -0.09148070727929199, 0.17018201970686128, -0.031318370558199... |
706.2098 | Integrability of anisotropic and homogeneous Universes in scalar-tensor
theory of gravitation | In this paper, we develop a method based on the analysis of the Kovalewski
exponents to study the integrability of anisotropic and homogeneous Universes.
The formalism is developed in scalar-tensor gravity, the general relativistic
case appearing as a special case of this larger framework. Then, depending on
the rati... | gr-qc | in this paper we develop a method based on the analysis of the kovalewski exponents to study the integrability of anisotropic and homogeneous universes the formalism is developed in scalartensor gravity the general relativistic case appearing as a special case of this larger framework then depending on the rationality ... | [['in', 'this', 'paper', 'we', 'develop', 'a', 'method', 'based', 'on', 'the', 'analysis', 'of', 'the', 'kovalewski', 'exponents', 'to', 'study', 'the', 'integrability', 'of', 'anisotropic', 'and', 'homogeneous', 'universes', 'the', 'formalism', 'is', 'developed', 'in', 'scalartensor', 'gravity', 'the', 'general', 'rel... | [-0.13957341673643622, 0.10148692948820248, -0.10665518733073179, 0.0867918218320159, -0.05648211246892197, -0.11764149567469546, -0.04345839267615739, 0.27651359673193976, -0.19589995067209415, -0.26315065864983894, 0.08906950235003223, -0.21381091263004873, -0.1549833648429852, 0.16985482523498469, -0.031741882521301... |
706.2099 | Monte Carlo evaluation of FADE approach to anomalous kinetics | In this paper we propose a comparison between the CTRW (Monte Carlo) and
Fractional Derivative approaches to the modelling of anomalous diffusion
phenomena in the presence of an advection field. Galilei variant and invariant
schemes are revised.
| cond-mat.stat-mech | in this paper we propose a comparison between the ctrw monte carlo and fractional derivative approaches to the modelling of anomalous diffusion phenomena in the presence of an advection field galilei variant and invariant schemes are revised | [['in', 'this', 'paper', 'we', 'propose', 'a', 'comparison', 'between', 'the', 'ctrw', 'monte', 'carlo', 'and', 'fractional', 'derivative', 'approaches', 'to', 'the', 'modelling', 'of', 'anomalous', 'diffusion', 'phenomena', 'in', 'the', 'presence', 'of', 'an', 'advection', 'field', 'galilei', 'variant', 'and', 'invari... | [-0.1243220111229331, 0.11015680262770164, -0.10779898883963658, 0.10051216948085238, -0.07964390969356976, -0.10032374299810948, -0.01666003925964941, 0.3943001656616862, -0.2974752471152995, -0.3116010885081581, 0.06659855462635893, -0.27714541567036427, -0.16229215065470418, 0.14891589392681379, -0.09047578111592983... |
706.21 | Molecular opacities for low-mass metal-poor AGB stars undergoing the
Third Dredge Up | The concomitant overabundances of C, N and s-process elements are commonly
ascribed to the complex interplay of nucleosynthesis, mixing and mass loss
taking place in Asymptotic Giant Branch stars. At low metallicity, the
enhancement of C and/or N may be up to 1000 times larger than the original iron
content and signi... | astro-ph | the concomitant overabundances of c n and sprocess elements are commonly ascribed to the complex interplay of nucleosynthesis mixing and mass loss taking place in asymptotic giant branch stars at low metallicity the enhancement of c andor n may be up to 1000 times larger than the original iron content and significantly... | [['the', 'concomitant', 'overabundances', 'of', 'c', 'n', 'and', 'sprocess', 'elements', 'are', 'commonly', 'ascribed', 'to', 'the', 'complex', 'interplay', 'of', 'nucleosynthesis', 'mixing', 'and', 'mass', 'loss', 'taking', 'place', 'in', 'asymptotic', 'giant', 'branch', 'stars', 'at', 'low', 'metallicity', 'the', 'en... | [-0.04990933375972274, 0.18109616935253142, -0.0200373052888991, 0.08965608388478262, -0.07625379261658773, -0.045449901619730025, 0.10751111764448548, 0.36048188048375057, -0.2084388546556798, -0.3860484418459237, 0.04492199983643858, -0.27358448364722887, -0.03200312639145474, 0.1711770223367861, -0.04833680271955305... |
706.2101 | Dark Matter Annihilation in Substructures Revised | Upcoming $\gamma$-ray satellites will search for Dark Matter annihilations in
Milky Way substructures (or 'clumps'). The prospects for detecting these
objects strongly depend on the assumptions made on the distribution of Dark
Matter in substructures, and on the distribution of substructures in the Milky
Way halo. By... | astro-ph hep-ph | upcoming gammaray satellites will search for dark matter annihilations in milky way substructures or clumps the prospects for detecting these objects strongly depend on the assumptions made on the distribution of dark matter in substructures and on the distribution of substructures in the milky way halo by adopting sim... | [['upcoming', 'gammaray', 'satellites', 'will', 'search', 'for', 'dark', 'matter', 'annihilations', 'in', 'milky', 'way', 'substructures', 'or', 'clumps', 'the', 'prospects', 'for', 'detecting', 'these', 'objects', 'strongly', 'depend', 'on', 'the', 'assumptions', 'made', 'on', 'the', 'distribution', 'of', 'dark', 'mat... | [-0.07717297108527939, 0.20150703613208384, -0.02760566951474175, 0.1400230575208774, -0.0754343467997387, -0.07173305673703519, 0.019786439716838123, 0.3837877625029207, -0.15147765049117706, -0.4453944198210679, 0.04080333260589257, -0.3182915985761654, 0.04686635962709607, 0.24565927210503669, 0.04104015187684646, -... |
706.2102 | The lower mass function of the young open cluster Blanco 1: from 30 Mjup
to 3 Mo | We performed a deep wide field optical survey of the young (~100-150 Myr)
open cluster Blanco1 to study its low mass population well down into the brown
dwarf regime and estimate its mass function over the whole cluster mass
range.The survey covers 2.3 square degrees in the I and z-bands down to I ~ z ~
24 with the C... | astro-ph | we performed a deep wide field optical survey of the young 100150 myr open cluster blanco1 to study its low mass population well down into the brown dwarf regime and estimate its mass function over the whole cluster mass rangethe survey covers 23 square degrees in the i and zbands down to i z 24 with the cfh12k camera ... | [['we', 'performed', 'a', 'deep', 'wide', 'field', 'optical', 'survey', 'of', 'the', 'young', '100150', 'myr', 'open', 'cluster', 'blanco1', 'to', 'study', 'its', 'low', 'mass', 'population', 'well', 'down', 'into', 'the', 'brown', 'dwarf', 'regime', 'and', 'estimate', 'its', 'mass', 'function', 'over', 'the', 'whole',... | [-0.03541296890062344, 0.10739650398112686, -0.09628275005886232, 0.1006344987993939, -0.09198820106027548, -0.04075862289377922, 0.1113150886905145, 0.416760605937652, -0.18881425047773184, -0.3934156995458628, 0.06241512690485946, -0.24964909053599563, -0.020201754296386886, 0.1896862088327602, -0.05283937862303769, ... |
706.2103 | Aharonov-Bohm effect and broken valley-degeneracy in graphene rings | We analyze theoretically the electronic properties of Aharonov-Bohm rings
made of graphene. We show that the combined effect of the ring confinement and
applied magnetic flux offers a controllable way to lift the orbital degeneracy
originating from the two valleys, even in the absence of intervalley
scattering. The p... | cond-mat.mes-hall | we analyze theoretically the electronic properties of aharonovbohm rings made of graphene we show that the combined effect of the ring confinement and applied magnetic flux offers a controllable way to lift the orbital degeneracy originating from the two valleys even in the absence of intervalley scattering the phenome... | [['we', 'analyze', 'theoretically', 'the', 'electronic', 'properties', 'of', 'aharonovbohm', 'rings', 'made', 'of', 'graphene', 'we', 'show', 'that', 'the', 'combined', 'effect', 'of', 'the', 'ring', 'confinement', 'and', 'applied', 'magnetic', 'flux', 'offers', 'a', 'controllable', 'way', 'to', 'lift', 'the', 'orbital... | [-0.22142718593917182, 0.13175508020496046, -0.05240824690302582, 0.05407072794183183, -0.03368076752663615, -0.1428889733563001, 0.033969368769258663, 0.3898531404298705, -0.3056877939483604, -0.26395447600532224, 0.020631764002295362, -0.2500290479543273, -0.1409635120449034, 0.15985207789879594, 0.009639173330789482... |
706.2104 | Homogenization of nonlinear scalar conservation laws | We study the limit as $\e\to 0$ of the entropy solutions of the equation
$\p_t \ue + \dv_x[A(\frac{x}{\e},\ue)] =0$. We prove that the sequence $\ue$
two-scale converges towards a function $u(t,x,y)$, and $u$ is the unique
solution of a limit evolution problem. The remarkable point is that the limit
problem is not a ... | math.AP | we study the limit as eto 0 of the entropy solutions of the equation p_t ue dv_xafracxeue 0 we prove that the sequence ue twoscale converges towards a function utxy and u is the unique solution of a limit evolution problem the remarkable point is that the limit problem is not a scalar conservation law but rather a kine... | [['we', 'study', 'the', 'limit', 'as', 'eto', '0', 'of', 'the', 'entropy', 'solutions', 'of', 'the', 'equation', 'p_t', 'ue', 'dv_xafracxeue', '0', 'we', 'prove', 'that', 'the', 'sequence', 'ue', 'twoscale', 'converges', 'towards', 'a', 'function', 'utxy', 'and', 'u', 'is', 'the', 'unique', 'solution', 'of', 'a', 'limi... | [-0.16688020448821286, 0.07389946257074674, -0.1639654290676117, 0.0825044314423576, -0.04843787079056104, -0.12517152009531857, 0.054265322096956274, 0.2818538662046194, -0.3304274285833041, -0.20769149909416834, 0.07930493233337378, -0.32775133172671, -0.11074709894756476, 0.10989619163175424, -0.020391907138521976, ... |
706.2105 | Equilibrium of stellar dynamical systems in the context of the
Vlasov-Poisson model | This short review is devoted to the problem of the equilibrium of stellar
dynamical systems in the context of the Vlasov-Poisson model. In a first part
we will review some classical problems posed by the application of the
Vlasov-Poisson model to the astrophysical systems like globular clusters or
galaxies. In a seco... | astro-ph | this short review is devoted to the problem of the equilibrium of stellar dynamical systems in the context of the vlasovpoisson model in a first part we will review some classical problems posed by the application of the vlasovpoisson model to the astrophysical systems like globular clusters or galaxies in a second par... | [['this', 'short', 'review', 'is', 'devoted', 'to', 'the', 'problem', 'of', 'the', 'equilibrium', 'of', 'stellar', 'dynamical', 'systems', 'in', 'the', 'context', 'of', 'the', 'vlasovpoisson', 'model', 'in', 'a', 'first', 'part', 'we', 'will', 'review', 'some', 'classical', 'problems', 'posed', 'by', 'the', 'applicatio... | [-0.13311230911456637, 0.04359980928098881, -0.09526626976501, 0.10542125204014346, -0.0919610147186751, -0.05839011127797054, 0.009549149177282265, 0.29904934409760725, -0.24924469219618722, -0.29187382012605667, 0.1430047016413147, -0.2931670106359218, -0.1371191205659048, 0.2161084583893075, -0.08693981527252809, 0.... |
706.2106 | The size of the largest component below phase transition in
inhomogeneous random graphs | We study the "rank 1 case" of the inhomogeneous random graph model. In the
subcritical case we derive an exact formula for the asymptotic size of the
largest connected component scaled to log n. This result is new, it completes
the corresponding known result in the supercritical case. We provide some
examples of appl... | math.PR | we study the rank 1 case of the inhomogeneous random graph model in the subcritical case we derive an exact formula for the asymptotic size of the largest connected component scaled to log n this result is new it completes the corresponding known result in the supercritical case we provide some examples of application ... | [['we', 'study', 'the', 'rank', '1', 'case', 'of', 'the', 'inhomogeneous', 'random', 'graph', 'model', 'in', 'the', 'subcritical', 'case', 'we', 'derive', 'an', 'exact', 'formula', 'for', 'the', 'asymptotic', 'size', 'of', 'the', 'largest', 'connected', 'component', 'scaled', 'to', 'log', 'n', 'this', 'result', 'is', '... | [-0.14543199057465997, 0.058889390688222944, -0.04028627960460967, 0.07744068132135375, -0.04824603096871027, -0.1069017116157017, 0.04229643651894454, 0.290362100534398, -0.22332234685068372, -0.26050843455796613, 0.11868837370200018, -0.2608486214042481, -0.18031216191593558, 0.2080926799921897, -0.05136382727530496,... |
706.2107 | Constrained Ramsey Numbers | For two graphs S and T, the constrained Ramsey number f(S, T) is the minimum
n such that every edge coloring of the complete graph on n vertices, with any
number of colors, has a monochromatic subgraph isomorphic to S or a rainbow
(all edges differently colored) subgraph isomorphic to T. The Erdos-Rado
Canonical Rams... | math.CO | for two graphs s and t the constrained ramsey number fs t is the minimum n such that every edge coloring of the complete graph on n vertices with any number of colors has a monochromatic subgraph isomorphic to s or a rainbow all edges differently colored subgraph isomorphic to t the erdosrado canonical ramsey theorem i... | [['for', 'two', 'graphs', 's', 'and', 't', 'the', 'constrained', 'ramsey', 'number', 'fs', 't', 'is', 'the', 'minimum', 'n', 'such', 'that', 'every', 'edge', 'coloring', 'of', 'the', 'complete', 'graph', 'on', 'n', 'vertices', 'with', 'any', 'number', 'of', 'colors', 'has', 'a', 'monochromatic', 'subgraph', 'isomorphic... | [-0.15540152411470867, 0.19273688145731083, -0.051837912497927525, 0.01778343445023095, -0.06740331641195456, -0.19419478782187294, 0.07345867238749552, 0.3792222755760808, -0.2620265440327277, -0.30974832004425246, 0.05713568624647532, -0.32001096012549446, -0.10003461198511861, 0.1597316404388354, -0.0746420674512485... |
706.2108 | Unified description of Bjorken and Landau 1+1 hydrodynamics | We propose a generalization of the Bjorken in-out Ansatz for fluid
trajectories which, when applied to the (1+1) hydrodynamic equations, generates
a one-parameter family of analytic solutions interpolating between the
boost-invariant Bjorken picture and the non boost-invariant one by Landau. This
parameter characteri... | nucl-th hep-ph | we propose a generalization of the bjorken inout ansatz for fluid trajectories which when applied to the 11 hydrodynamic equations generates a oneparameter family of analytic solutions interpolating between the boostinvariant bjorken picture and the non boostinvariant one by landau this parameter characterises the prop... | [['we', 'propose', 'a', 'generalization', 'of', 'the', 'bjorken', 'inout', 'ansatz', 'for', 'fluid', 'trajectories', 'which', 'when', 'applied', 'to', 'the', '11', 'hydrodynamic', 'equations', 'generates', 'a', 'oneparameter', 'family', 'of', 'analytic', 'solutions', 'interpolating', 'between', 'the', 'boostinvariant',... | [-0.11235459902519851, 0.18465669587021694, -0.1888790276011844, 0.10234589252075621, -0.04063763157893462, -0.1082216647949903, -0.01162006242788936, 0.26937308004371036, -0.20489777891749614, -0.18583489047657503, -0.03085672125024231, -0.23983178931092353, -0.037757392899182285, 0.11651879225514437, 0.00979743758522... |
706.2109 | Bremsstrahlung in alpha-Decay Reexamined | A high-statistics measurement of bremsstrahlung emitted in the alpha decay of
210Po has been performed, which allows to follow the photon spectra up to
energies of ~ 500 keV. The measured differential emission probability is in
good agreement with our theoretical results obtained within the quasi classical
approximat... | nucl-ex nucl-th | a highstatistics measurement of bremsstrahlung emitted in the alpha decay of 210po has been performed which allows to follow the photon spectra up to energies of 500 kev the measured differential emission probability is in good agreement with our theoretical results obtained within the quasi classical approximation as ... | [['a', 'highstatistics', 'measurement', 'of', 'bremsstrahlung', 'emitted', 'in', 'the', 'alpha', 'decay', 'of', '210po', 'has', 'been', 'performed', 'which', 'allows', 'to', 'follow', 'the', 'photon', 'spectra', 'up', 'to', 'energies', 'of', '500', 'kev', 'the', 'measured', 'differential', 'emission', 'probability', 'i... | [-0.06934324452743809, 0.1850239465450298, -0.07285417620168656, 0.08414257064102959, 0.0073484604208901225, -0.10996048338711262, 0.02488369210765754, 0.36707817595832204, -0.19691609750425784, -0.36716553107930383, -0.06463339985514592, -0.3444343584149242, -0.01922105115420204, 0.20174911683449065, 0.066269084932377... |
706.211 | On the strong chromatic number of random graphs | Let G be a graph with n vertices, and let k be an integer dividing n. G is
said to be strongly k-colorable if for every partition of V(G) into disjoint
sets V_1 \cup ... \cup V_r, all of size exactly k, there exists a proper vertex
k-coloring of G with each color appearing exactly once in each V_i. In the case
when k... | math.CO math.PR | let g be a graph with n vertices and let k be an integer dividing n g is said to be strongly kcolorable if for every partition of vg into disjoint sets v_1 cup cup v_r all of size exactly k there exists a proper vertex kcoloring of g with each color appearing exactly once in each v_i in the case when k does not divide ... | [['let', 'g', 'be', 'a', 'graph', 'with', 'n', 'vertices', 'and', 'let', 'k', 'be', 'an', 'integer', 'dividing', 'n', 'g', 'is', 'said', 'to', 'be', 'strongly', 'kcolorable', 'if', 'for', 'every', 'partition', 'of', 'vg', 'into', 'disjoint', 'sets', 'v_1', 'cup', 'cup', 'v_r', 'all', 'of', 'size', 'exactly', 'k', 'ther... | [-0.21465361673085961, 0.20907536259488146, -0.042756581556822326, -0.05120421142854877, -0.09468834247601068, -0.2179705955915981, 0.01581955705208842, 0.38017569840339555, -0.28385683254879196, -0.29028260909929227, 0.015904786841322977, -0.3540405554489957, -0.10715964569258907, 0.07909412075546973, -0.0702270836983... |
706.2111 | Influence of dissipation on the extraction of quantum states via
repeated measurements | A quantum system put in interaction with another one that is repeatedly
measured is subject to a non-unitary dynamics, through which it is possible to
extract subspaces. This key idea has been exploited to propose schemes aimed at
the generation of pure quantum states (purification). All such schemes have so
far been... | quant-ph | a quantum system put in interaction with another one that is repeatedly measured is subject to a nonunitary dynamics through which it is possible to extract subspaces this key idea has been exploited to propose schemes aimed at the generation of pure quantum states purification all such schemes have so far been conside... | [['a', 'quantum', 'system', 'put', 'in', 'interaction', 'with', 'another', 'one', 'that', 'is', 'repeatedly', 'measured', 'is', 'subject', 'to', 'a', 'nonunitary', 'dynamics', 'through', 'which', 'it', 'is', 'possible', 'to', 'extract', 'subspaces', 'this', 'key', 'idea', 'has', 'been', 'exploited', 'to', 'propose', 's... | [-0.1377191845353486, 0.15389895719838226, -0.0641539746158944, 0.010747029489380111, 0.02833173919740754, -0.15045426650774768, 0.028630583318267275, 0.3354711966304522, -0.2319539700143246, -0.2671707368701593, 0.07859208361818067, -0.2674708066624589, -0.1092460143877866, 0.18611588342011803, -0.02053218401205312, 0... |
706.2112 | Kloosterman sums, elliptic curves, and irreducible polynomials with
prescribed trace and norm | Let $\F_q$ ($q=p^r$) be a finite field. In this paper the number of
irreducible polynomials of degree $m$ in $\F_q[x]$ with prescribed trace and
norm coefficients is calculated in certain special cases and a general bound
for that number is obtained improving the bound by Wan if $m$ is small compared
to $q$. As a cor... | math.NT math.CO | let f_q qpr be a finite field in this paper the number of irreducible polynomials of degree m in f_qx with prescribed trace and norm coefficients is calculated in certain special cases and a general bound for that number is obtained improving the bound by wan if m is small compared to q as a corollary sharp bounds are ... | [['let', 'f_q', 'qpr', 'be', 'a', 'finite', 'field', 'in', 'this', 'paper', 'the', 'number', 'of', 'irreducible', 'polynomials', 'of', 'degree', 'm', 'in', 'f_qx', 'with', 'prescribed', 'trace', 'and', 'norm', 'coefficients', 'is', 'calculated', 'in', 'certain', 'special', 'cases', 'and', 'a', 'general', 'bound', 'for'... | [-0.17718648559393307, 0.10837788219899214, -0.0509765279271318, -0.005915346107726423, -0.023851117632790086, -0.13772697924800656, 0.0123754250448923, 0.27834498547428455, -0.24582194576984928, -0.2830380861277637, 0.07443451655597207, -0.24296056523727363, -0.11033864108407322, 0.2517209774985745, -0.112047908637631... |
706.2113 | A family of acyclic functors | We determine a family of functors from a poset to abelian groups such that
the higher direct limits vanish on them. This is done by first characterizing
the projective functors. Then a spectral sequence arising from the grading of
the poset is used. Also the dual version for injective functors and higher
inverse limi... | math.AT | we determine a family of functors from a poset to abelian groups such that the higher direct limits vanish on them this is done by first characterizing the projective functors then a spectral sequence arising from the grading of the poset is used also the dual version for injective functors and higher inverse limits is... | [['we', 'determine', 'a', 'family', 'of', 'functors', 'from', 'a', 'poset', 'to', 'abelian', 'groups', 'such', 'that', 'the', 'higher', 'direct', 'limits', 'vanish', 'on', 'them', 'this', 'is', 'done', 'by', 'first', 'characterizing', 'the', 'projective', 'functors', 'then', 'a', 'spectral', 'sequence', 'arising', 'fro... | [-0.09650391786161697, 0.05061080744207808, -0.03910958981423667, 0.15278465193907984, -0.14498819543443847, -0.09234753556577771, -0.0007199626680548218, 0.38080357156242384, -0.43919252502647316, -0.19293457240035589, 0.12628682888338738, -0.20339691721407385, -0.119547303138075, 0.1447220748205754, -0.18636268925514... |
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