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 |
|---|---|---|---|---|---|---|
707.243 | A study of logarithmic corrections and universal amplitude ratios in the
two-dimensional 4-state Potts model | Monte Carlo (MC) and series expansion (SE) data for the energy, specific
heat, magnetization and susceptibility of the two-dimensional 4-state Potts
model in the vicinity of the critical point are analysed. The role of
logarithmic corrections is discussed and an approach is proposed in order to
account numerically fo... | cond-mat.stat-mech hep-lat hep-th | monte carlo mc and series expansion se data for the energy specific heat magnetization and susceptibility of the twodimensional 4state potts model in the vicinity of the critical point are analysed the role of logarithmic corrections is discussed and an approach is proposed in order to account numerically for these cor... | [['monte', 'carlo', 'mc', 'and', 'series', 'expansion', 'se', 'data', 'for', 'the', 'energy', 'specific', 'heat', 'magnetization', 'and', 'susceptibility', 'of', 'the', 'twodimensional', '4state', 'potts', 'model', 'in', 'the', 'vicinity', 'of', 'the', 'critical', 'point', 'are', 'analysed', 'the', 'role', 'of', 'logar... | [-0.10573098920040618, 0.0931183594406512, -0.03823567069086589, 0.09176586363403323, -0.0227817780901923, -0.10349557920064974, 0.05228981641802851, 0.3441252659418081, -0.21005655268795395, -0.2957264393986215, 0.08289871019415411, -0.3345951735667002, -0.09454423002898693, 0.2354756808536446, 0.02079246553445333, 0.... |
707.2431 | Quarkonium and hydrogen spectra with spin dependent relativistic wave
equation | A non-linear non-perturbative relativistic atomic theory introduces spin in
the dynamics of particle motion. The resulting energy levels of Hydrogen atom
are exactly same as the Dirac theory. The theory accounts for the energy due to
spin-orbit interaction and for the additional potential energy due to spin and
spin-... | physics.gen-ph | a nonlinear nonperturbative relativistic atomic theory introduces spin in the dynamics of particle motion the resulting energy levels of hydrogen atom are exactly same as the dirac theory the theory accounts for the energy due to spinorbit interaction and for the additional potential energy due to spin and spinorbit co... | [['a', 'nonlinear', 'nonperturbative', 'relativistic', 'atomic', 'theory', 'introduces', 'spin', 'in', 'the', 'dynamics', 'of', 'particle', 'motion', 'the', 'resulting', 'energy', 'levels', 'of', 'hydrogen', 'atom', 'are', 'exactly', 'same', 'as', 'the', 'dirac', 'theory', 'the', 'theory', 'accounts', 'for', 'the', 'en... | [-0.12035595937104861, 0.18033265119049488, -0.08648452877708412, 0.10018320085660923, -0.04601919328802669, -0.12318474756562556, 0.013812616727762978, 0.3227883194801661, -0.28467655136856196, -0.3212151948279121, -0.013797051471796431, -0.28133141944176115, -0.0603627917271125, 0.12903764352744954, 0.029345089683906... |
707.2432 | Pricing Asian Options for Jump Diffusions | We construct a sequence of functions that uniformly converge (on compact
sets) to the price of Asian option, which is written on a stock whose dynamics
follows a jump diffusion, exponentially fast. Each of the element in this
sequence solves a parabolic partial differen- tial equation (not an
integro-differential equ... | cs.CE | we construct a sequence of functions that uniformly converge on compact sets to the price of asian option which is written on a stock whose dynamics follows a jump diffusion exponentially fast each of the element in this sequence solves a parabolic partial differen tial equation not an integrodifferential equation as a... | [['we', 'construct', 'a', 'sequence', 'of', 'functions', 'that', 'uniformly', 'converge', 'on', 'compact', 'sets', 'to', 'the', 'price', 'of', 'asian', 'option', 'which', 'is', 'written', 'on', 'a', 'stock', 'whose', 'dynamics', 'follows', 'a', 'jump', 'diffusion', 'exponentially', 'fast', 'each', 'of', 'the', 'element... | [-0.12064709754283481, 0.04035239089799815, -0.11725923813926646, 0.07061530309847167, -0.07136543538374236, -0.12229223354849257, 0.06632295475471058, 0.39945233089825777, -0.32401979265327835, -0.2173040627289705, 0.15645205723328068, -0.2690863810668263, -0.13687005766691004, 0.25710805348721866, -0.0759954233712787... |
707.2433 | Kilohertz laser ablation for doping helium nanodroplets | A new setup for doping helium nanodroplets by means of laser ablation at
kilohertz repetition rate is presented. The doping process is characterized and
two distinct regimes of laser ablation are identified. The setup is shown to be
efficient and stable enough to be used for spectroscopy, as demonstrated on
beam-depl... | physics.atm-clus | a new setup for doping helium nanodroplets by means of laser ablation at kilohertz repetition rate is presented the doping process is characterized and two distinct regimes of laser ablation are identified the setup is shown to be efficient and stable enough to be used for spectroscopy as demonstrated on beamdepletion ... | [['a', 'new', 'setup', 'for', 'doping', 'helium', 'nanodroplets', 'by', 'means', 'of', 'laser', 'ablation', 'at', 'kilohertz', 'repetition', 'rate', 'is', 'presented', 'the', 'doping', 'process', 'is', 'characterized', 'and', 'two', 'distinct', 'regimes', 'of', 'laser', 'ablation', 'are', 'identified', 'the', 'setup', ... | [-0.06339744343943159, 0.25612778269048586, -0.022107714399891464, -0.015395443868654088, 0.05072299773363691, -0.22340838916011546, 0.0739510842917585, 0.48065788051799724, -0.22697759022151953, -0.2881759240831199, 0.030742749414945904, -0.3074782253488114, -0.03684702680299157, 0.259515327372049, -0.0220992411976974... |
707.2434 | 3-point off-shell vertex in scalar QED in arbitrary gauge and dimension | We calculate the complete one-loop off-shell three-point scalar-photon vertex
in arbitrary gauge and dimension for Scalar Quantum Electrodynamics. Explicit
results are presented for the particular cases of dimensions 3 and 4 both for
massive and massless scalars. We then propose non-perturbative forms of this
vertex ... | hep-th | we calculate the complete oneloop offshell threepoint scalarphoton vertex in arbitrary gauge and dimension for scalar quantum electrodynamics explicit results are presented for the particular cases of dimensions 3 and 4 both for massive and massless scalars we then propose nonperturbative forms of this vertex that coin... | [['we', 'calculate', 'the', 'complete', 'oneloop', 'offshell', 'threepoint', 'scalarphoton', 'vertex', 'in', 'arbitrary', 'gauge', 'and', 'dimension', 'for', 'scalar', 'quantum', 'electrodynamics', 'explicit', 'results', 'are', 'presented', 'for', 'the', 'particular', 'cases', 'of', 'dimensions', '3', 'and', '4', 'both... | [-0.1236446968762687, 0.20045041728385346, 0.022176849598677276, 0.12823182393374197, -0.07654551915927893, -0.18309732681761184, -0.03187628365035548, 0.3387233952612237, -0.06702584927660171, -0.22680071232564472, 0.009204824737497364, -0.30915604646455636, -0.17329516162647418, 0.09747188895751067, 0.051795617435817... |
707.2435 | Effective mean-field equations for cigar-shaped and disk-shaped
Bose-Einstein condensates | By applying the standard adiabatic approximation and using the accurate
analytical expression for the corresponding local chemical potential obtained
in our previous work [Phys. Rev. A \textbf{75}, 063610 (2007)] we derive an
effective 1D equation that governs the axial dynamics of mean-field
cigar-shaped condensates... | cond-mat.other | by applying the standard adiabatic approximation and using the accurate analytical expression for the corresponding local chemical potential obtained in our previous work phys rev a textbf75 063610 2007 we derive an effective 1d equation that governs the axial dynamics of meanfield cigarshaped condensates with repulsiv... | [['by', 'applying', 'the', 'standard', 'adiabatic', 'approximation', 'and', 'using', 'the', 'accurate', 'analytical', 'expression', 'for', 'the', 'corresponding', 'local', 'chemical', 'potential', 'obtained', 'in', 'our', 'previous', 'work', 'phys', 'rev', 'a', 'textbf75', '063610', '2007', 'we', 'derive', 'an', 'effec... | [-0.09628538261190758, 0.09967022036606536, -0.10468745362710918, 0.07254920494662008, -0.04873168946930788, -0.1436245746675436, 0.02061388327966048, 0.3284311373625873, -0.17235612830419167, -0.2774717159301854, -0.0025133588489624535, -0.2570850539452997, -0.145005376564597, 0.1784048736346701, 0.05088130188045452, ... |
707.2436 | On the Polyphase Decomposition for Design of Generalized Comb Decimation
Filters | Generalized comb filters (GCFs) are efficient anti-aliasing decimation
filters with improved selectivity and quantization noise (QN) rejection
performance around the so called folding bands with respect to classical comb
filters.
In this paper, we address the design of GCF filters by proposing an efficient
partial ... | cs.OH | generalized comb filters gcfs are efficient antialiasing decimation filters with improved selectivity and quantization noise qn rejection performance around the so called folding bands with respect to classical comb filters in this paper we address the design of gcf filters by proposing an efficient partial polyphase a... | [['generalized', 'comb', 'filters', 'gcfs', 'are', 'efficient', 'antialiasing', 'decimation', 'filters', 'with', 'improved', 'selectivity', 'and', 'quantization', 'noise', 'qn', 'rejection', 'performance', 'around', 'the', 'so', 'called', 'folding', 'bands', 'with', 'respect', 'to', 'classical', 'comb', 'filters', 'in'... | [-0.09891720565035939, 0.025205064972979016, -0.07255222968012094, -0.003679672719910741, -0.08878596073389053, -0.13148186442628504, 0.07086383784003555, 0.4520276641026139, -0.2775697513502091, -0.2782251572594978, 0.11612716804631054, -0.20015817030146718, -0.21431270259432494, 0.1404296770785004, -0.113669356577098... |
707.2437 | Investigation of a lattice Boltzmann model with a variable speed of
sound | A lattice Boltzmann model is considered in which the speed of sound can be
varied independently of the other parameters. The range over which the speed of
sound can be varied is investigated and good agreement is found between
simulations and theory. The onset of nonlinear effects due to variations in the
speed of so... | physics.flu-dyn physics.comp-ph | a lattice boltzmann model is considered in which the speed of sound can be varied independently of the other parameters the range over which the speed of sound can be varied is investigated and good agreement is found between simulations and theory the onset of nonlinear effects due to variations in the speed of sound ... | [['a', 'lattice', 'boltzmann', 'model', 'is', 'considered', 'in', 'which', 'the', 'speed', 'of', 'sound', 'can', 'be', 'varied', 'independently', 'of', 'the', 'other', 'parameters', 'the', 'range', 'over', 'which', 'the', 'speed', 'of', 'sound', 'can', 'be', 'varied', 'is', 'investigated', 'and', 'good', 'agreement', '... | [-0.10886158547167812, 0.201070234852742, -0.09220433852309923, 0.028563460005525815, -0.057438686961330566, -0.11740155672340329, 0.005904471454019827, 0.37235246639115266, -0.3000152375863259, -0.3064652487568288, 0.08134952865552202, -0.24475323937339596, -0.12149008224347987, 0.2454688424687743, -0.0415286658982555... |
707.2438 | LibCPIXE: a PIXE simulation open-source library for multilayered samples | Most particle induced X-ray emission (PIXE) data analysis codes are not
focused on handling multilayered samples. We have developed an open-source
library called "LibCPIXE", for PIXE data analysis. It is written in standard C
and implements functions for simulating X-ray yields of PIXE spectra taken from
arbitrary sa... | cond-mat.mtrl-sci | most particle induced xray emission pixe data analysis codes are not focused on handling multilayered samples we have developed an opensource library called libcpixe for pixe data analysis it is written in standard c and implements functions for simulating xray yields of pixe spectra taken from arbitrary samples includ... | [['most', 'particle', 'induced', 'xray', 'emission', 'pixe', 'data', 'analysis', 'codes', 'are', 'not', 'focused', 'on', 'handling', 'multilayered', 'samples', 'we', 'have', 'developed', 'an', 'opensource', 'library', 'called', 'libcpixe', 'for', 'pixe', 'data', 'analysis', 'it', 'is', 'written', 'in', 'standard', 'c',... | [-0.044716789996489245, 0.03374940513045748, -0.07621606872648212, 0.06627051516746481, -0.08402575136588371, -0.17911628860293338, -0.00736435714957192, 0.4525050323271582, -0.260216282268636, -0.35496305976829207, 0.13638285480865694, -0.2874859749861326, -0.06625192490999145, 0.3083928394905813, -0.01654228631486284... |
707.2439 | A Presentation for the Dual Symmetric Inverse Monoid | The dual symmetric inverse monoid $\mathscr{I}_n^*$ is the inverse monoid of
all isomorphisms between quotients of an $n$-set. We give a monoid presentation
of $\mathscr{I}_n^*$ and, along the way, establish criteria for a monoid to be
inverse when it is generated by completely regular elements.
| math.GR | the dual symmetric inverse monoid mathscri_n is the inverse monoid of all isomorphisms between quotients of an nset we give a monoid presentation of mathscri_n and along the way establish criteria for a monoid to be inverse when it is generated by completely regular elements | [['the', 'dual', 'symmetric', 'inverse', 'monoid', 'mathscri_n', 'is', 'the', 'inverse', 'monoid', 'of', 'all', 'isomorphisms', 'between', 'quotients', 'of', 'an', 'nset', 'we', 'give', 'a', 'monoid', 'presentation', 'of', 'mathscri_n', 'and', 'along', 'the', 'way', 'establish', 'criteria', 'for', 'a', 'monoid', 'to', ... | [-0.09036714741743582, 0.13938052108989174, -0.054680274712831475, 0.08020784777892363, -0.14918553901749643, -0.09728679634890584, -0.021907652013523633, 0.4011990746786428, -0.4859477404591649, -0.16602258945187165, 0.15215750258459254, -0.3004790663199369, -0.1332243974212297, 0.1833075160203978, -0.0933189618206301... |
707.244 | Moduli spaces of quadratic complexes and their singular surfaces | We construct the coarse moduli space $\cM_{qc}(\sigma)$ of quadratic line
complexes with a fixed Segre symbol $\sigma$ as well as the moduli space
$\cM_{ss}(\sigma)$ of the corresponding singular surfaces. We show that the map
associating to a quadratic line complex its singular surface induces a morphism
$\pi: \cM_{... | math.AG | we construct the coarse moduli space cm_qcsigma of quadratic line complexes with a fixed segre symbol sigma as well as the moduli space cm_sssigma of the corresponding singular surfaces we show that the map associating to a quadratic line complex its singular surface induces a morphism pi cm_qcsigma ra cm_sssigma final... | [['we', 'construct', 'the', 'coarse', 'moduli', 'space', 'cm_qcsigma', 'of', 'quadratic', 'line', 'complexes', 'with', 'a', 'fixed', 'segre', 'symbol', 'sigma', 'as', 'well', 'as', 'the', 'moduli', 'space', 'cm_sssigma', 'of', 'the', 'corresponding', 'singular', 'surfaces', 'we', 'show', 'that', 'the', 'map', 'associat... | [-0.22979942232858938, 0.05076675262630413, -0.07765523777877698, 0.08678678194152527, -0.09597289925212132, -0.13860981711415482, 0.018357316291600954, 0.3862003785420637, -0.3632505764482451, -0.1493706131109693, 0.07256378670085649, -0.24103874038355272, -0.2106687252516629, 0.19176895678287648, -0.09829513423648648... |
707.2441 | A Galois-theoretic approach to Kanev's correspondence | Let $G$ be a finite group, $\Lambda$ an absolutely irreducible $\Z[G]$-module
and $w$ a weight of $\Lambda$.
To any Galois covering with group $G$ we associate two correspondences, the
Schur and the Kanev correspondence.
We work out their relation and compute their invariants.
Using this, we give some new examp... | math.AG | let g be a finite group lambda an absolutely irreducible zgmodule and w a weight of lambda to any galois covering with group g we associate two correspondences the schur and the kanev correspondence we work out their relation and compute their invariants using this we give some new examples of prymtyurin varieties | [['let', 'g', 'be', 'a', 'finite', 'group', 'lambda', 'an', 'absolutely', 'irreducible', 'zgmodule', 'and', 'w', 'a', 'weight', 'of', 'lambda', 'to', 'any', 'galois', 'covering', 'with', 'group', 'g', 'we', 'associate', 'two', 'correspondences', 'the', 'schur', 'and', 'the', 'kanev', 'correspondence', 'we', 'work', 'ou... | [-0.2007278441187908, 0.08840995321719125, -0.1797617045319024, 0.018857611068700143, -0.14920273921364602, -0.1535352446876888, 0.031139391491997917, 0.39497353930799467, -0.3494517313544902, -0.2203153847598137, 0.05397390987161758, -0.269049807258372, -0.11863574091749231, 0.15772270420039036, -0.12337565325411423, ... |
707.2442 | Desynchronization of pulse-coupled oscillators with delayed excitatory
coupling | Collective behavior of pulse-coupled oscillators has been investigated
widely. As an example of pulse-coupled networks, fireflies display many kinds
of flashing patterns. Mirollo and Strogatz (1990) proposed a pulse-coupled
oscillator model to explain the synchronization of South East Asian fireflies
({\itshape Ptero... | math.DS | collective behavior of pulsecoupled oscillators has been investigated widely as an example of pulsecoupled networks fireflies display many kinds of flashing patterns mirollo and strogatz 1990 proposed a pulsecoupled oscillator model to explain the synchronization of south east asian fireflies itshape pteroptyx malaccae... | [['collective', 'behavior', 'of', 'pulsecoupled', 'oscillators', 'has', 'been', 'investigated', 'widely', 'as', 'an', 'example', 'of', 'pulsecoupled', 'networks', 'fireflies', 'display', 'many', 'kinds', 'of', 'flashing', 'patterns', 'mirollo', 'and', 'strogatz', '1990', 'proposed', 'a', 'pulsecoupled', 'oscillator', '... | [-0.1854433970955273, 0.13717834554791442, -0.0438150023082327, 0.052260974607928216, -0.02659279754954184, -0.22252772262732604, 0.021299513486983578, 0.4394201908684419, -0.23150403639768713, -0.27334717058849906, 0.09208664303285789, -0.2325846387218394, -0.26761535834521055, 0.19055923095396804, -0.1138179414776818... |
707.2443 | Correlated Anisotropies in the Cosmic Far-Infrared Background Detected
by MIPS/Spitzer: Constraint on the Bias | We report the detection of correlated anisotropies in the Cosmic Far-Infrared
Background at 160 microns. We measure the power spectrum in the Spitzer/SWIRE
Lockman Hole field. It reveals unambiguously a strong excess above cirrus and
Poisson contributions, at spatial scales between 5 and 30 arcminutes,
interpreted as... | astro-ph | we report the detection of correlated anisotropies in the cosmic farinfrared background at 160 microns we measure the power spectrum in the spitzerswire lockman hole field it reveals unambiguously a strong excess above cirrus and poisson contributions at spatial scales between 5 and 30 arcminutes interpreted as the sig... | [['we', 'report', 'the', 'detection', 'of', 'correlated', 'anisotropies', 'in', 'the', 'cosmic', 'farinfrared', 'background', 'at', '160', 'microns', 'we', 'measure', 'the', 'power', 'spectrum', 'in', 'the', 'spitzerswire', 'lockman', 'hole', 'field', 'it', 'reveals', 'unambiguously', 'a', 'strong', 'excess', 'above', ... | [-0.07332725780852661, 0.08590751343913246, -0.0899661814409978, 0.13051195887097142, -0.032505895025423615, -0.03419974768174845, -0.001994386352108497, 0.4250639584895812, -0.16786328681311652, -0.3491886664067575, 0.002818003722687105, -0.3601079961252317, -0.011366145918145776, 0.15985649392793053, 0.03198261437896... |
707.2444 | The equilibrium states for semigroups of rational maps | We consider the dynamics of skew product maps associated with finitely
generated semigroups of rational maps on the Riemann sphere. We show that under
some conditions on the dynamics and the potential function \psi, there exists a
unique equilibrium state for \psi and a unique $\exp(\P(\psi)-\psi)$-conformal
measure,... | math.DS math.CV math.PR | we consider the dynamics of skew product maps associated with finitely generated semigroups of rational maps on the riemann sphere we show that under some conditions on the dynamics and the potential function psi there exists a unique equilibrium state for psi and a unique expppsipsiconformal measure where ppsi denotes... | [['we', 'consider', 'the', 'dynamics', 'of', 'skew', 'product', 'maps', 'associated', 'with', 'finitely', 'generated', 'semigroups', 'of', 'rational', 'maps', 'on', 'the', 'riemann', 'sphere', 'we', 'show', 'that', 'under', 'some', 'conditions', 'on', 'the', 'dynamics', 'and', 'the', 'potential', 'function', 'psi', 'th... | [-0.18113334877071557, 0.1244243574846122, -0.10819230125182205, 0.040552401578881674, 0.011840253796738883, -0.10919818973720626, -0.002497483527770749, 0.3479012465449395, -0.3556728694174025, -0.12092667845664201, 0.09545950655161438, -0.3252684809267521, -0.16124394205743792, 0.21331225463223677, -0.015721440177272... |
707.2445 | The Wigner-Fokker-Planck equation: Stationary states and large time
behavior | This paper has been withdrawn by the authors due to a crucial error in the
proof of the main result. In a new manuscript (with two new authors) available
at arXiv:1010.2791v1 this problem has been resolved.
| quant-ph cond-mat.stat-mech math-ph math.AP math.MP | this paper has been withdrawn by the authors due to a crucial error in the proof of the main result in a new manuscript with two new authors available at arxiv10102791v1 this problem has been resolved | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'authors', 'due', 'to', 'a', 'crucial', 'error', 'in', 'the', 'proof', 'of', 'the', 'main', 'result', 'in', 'a', 'new', 'manuscript', 'with', 'two', 'new', 'authors', 'available', 'at', 'arxiv10102791v1', 'this', 'problem', 'has', 'been', 'resolved']] | [-0.07552619342293058, -0.009484522709889072, -0.1255208356705095, -0.018616672585319197, -0.0778206966817379, -0.08917593639343976, 0.005865696954008724, 0.3251249607120241, -0.24519088725958552, -0.3425157314964703, 0.12717986784742347, -0.24118493417544024, -0.1469667195209435, 0.16681421398617594, -0.21270470768213... |
707.2446 | Control of poultry chicken malaria by surface functionalized amorphous
nanosilica | Surface modified amorphous nanoporous silica molecules with hydrophobic as
well as hydrophilic character can be effectively used as therapeutic drug for
combating chicken malaria in poultry industry. The amorphous nanosilica was
developed by top-down approach using volcanic soil derived silica as source
material. Amo... | q-bio.BM q-bio.MN | surface modified amorphous nanoporous silica molecules with hydrophobic as well as hydrophilic character can be effectively used as therapeutic drug for combating chicken malaria in poultry industry the amorphous nanosilica was developed by topdown approach using volcanic soil derived silica as source material amorphou... | [['surface', 'modified', 'amorphous', 'nanoporous', 'silica', 'molecules', 'with', 'hydrophobic', 'as', 'well', 'as', 'hydrophilic', 'character', 'can', 'be', 'effectively', 'used', 'as', 'therapeutic', 'drug', 'for', 'combating', 'chicken', 'malaria', 'in', 'poultry', 'industry', 'the', 'amorphous', 'nanosilica', 'was... | [0.009670563547968351, 0.19139715332682405, -0.014337383307002741, -0.0016485824759503633, -0.003941468019359584, -0.20397748015339262, 0.03931641904235785, 0.41046870343692216, -0.20999616527416068, -0.27800745535481336, 0.08993611988613527, -0.27596866201352455, -0.19911741848296388, 0.148323339951056, -0.12795379989... |
707.2447 | Real analyticity of Hausdorff dimension for expanding rational
semigroups | We consider the dynamics of expanding semigroups generated by finitely many
rational maps on the Riemann sphere. We show that for an analytic family of
such semigroups, the Bowen parameter function is real-analytic and
plurisubharmonic. Combining this with a result obtained by the first author, we
show that if for ea... | math.DS math.CV math.PR | we consider the dynamics of expanding semigroups generated by finitely many rational maps on the riemann sphere we show that for an analytic family of such semigroups the bowen parameter function is realanalytic and plurisubharmonic combining this with a result obtained by the first author we show that if for each semi... | [['we', 'consider', 'the', 'dynamics', 'of', 'expanding', 'semigroups', 'generated', 'by', 'finitely', 'many', 'rational', 'maps', 'on', 'the', 'riemann', 'sphere', 'we', 'show', 'that', 'for', 'an', 'analytic', 'family', 'of', 'such', 'semigroups', 'the', 'bowen', 'parameter', 'function', 'is', 'realanalytic', 'and', ... | [-0.13033783262743887, 0.06891901378426597, -0.047507598501654855, 0.08752131536788414, -0.0540900483574982, -0.05401230948375522, -0.0007324322823237266, 0.3435404503334775, -0.3065835036238474, -0.15768963738913294, 0.1194317112748915, -0.33604596291495636, -0.15987308464317987, 0.278511284603284, -0.0720646877204422... |
707.2448 | Towards truly simultaneous PIXE and RBS analysis of layered objects in
cultural heritage | For a long time, RBS and PIXE techniques have been used in the field of
cultural heritage. Although the complementarity of both techniques has long
been acknowledged, its full potential has not been yet developed due to the
lack of general purpose software tools for analysing the data from both
techniques in a cohere... | cond-mat.mtrl-sci | for a long time rbs and pixe techniques have been used in the field of cultural heritage although the complementarity of both techniques has long been acknowledged its full potential has not been yet developed due to the lack of general purpose software tools for analysing the data from both techniques in a coherent wa... | [['for', 'a', 'long', 'time', 'rbs', 'and', 'pixe', 'techniques', 'have', 'been', 'used', 'in', 'the', 'field', 'of', 'cultural', 'heritage', 'although', 'the', 'complementarity', 'of', 'both', 'techniques', 'has', 'long', 'been', 'acknowledged', 'its', 'full', 'potential', 'has', 'not', 'been', 'yet', 'developed', 'du... | [-0.040043474412259625, 0.03730815581691088, -0.1446799829766248, 0.052806009505523964, -0.06342882059701958, -0.11457619261371452, 0.057328483972803886, 0.41459785486167333, -0.24894000770547572, -0.3127038729751963, 0.1286772614756435, -0.23154691486390974, -0.11662782229037967, 0.25110556763075526, -0.04540829528591... |
707.2449 | Hawking Radiation and Covariant Anomalies | Generalising the method of Wilczek and collaborators we provide a derivation
of Hawking radiation from charged black holes using only covariant gauge and
gravitational anomalies. The reliability and universality of the anomaly
cancellation approach to Hawking radiation is also discussed.
| hep-th gr-qc | generalising the method of wilczek and collaborators we provide a derivation of hawking radiation from charged black holes using only covariant gauge and gravitational anomalies the reliability and universality of the anomaly cancellation approach to hawking radiation is also discussed | [['generalising', 'the', 'method', 'of', 'wilczek', 'and', 'collaborators', 'we', 'provide', 'a', 'derivation', 'of', 'hawking', 'radiation', 'from', 'charged', 'black', 'holes', 'using', 'only', 'covariant', 'gauge', 'and', 'gravitational', 'anomalies', 'the', 'reliability', 'and', 'universality', 'of', 'the', 'anomal... | [-0.1172635005263146, 0.12972208152059467, -0.11784910003334517, 0.14819103530899155, -0.1156799993943423, -0.15229796500643716, 0.03858243480499368, 0.2525532769039273, -0.07927407338283957, -0.3002237900160253, 0.011014010745566339, -0.34499625756870955, -0.16222928161732852, 0.15438199952477588, -0.05887514012865722... |
707.245 | "Black Star" or Astrophysical Black Hole? | Recently wide publicity has been given to a claim by T. Vachaspati that
"black holes do not exist", that the objects known as black holes in
astrophysics should rather be called "black stars" and they not only do not
have event horizons but actually can be the source of spectacular gamma ray
bursts. In this short ess... | astro-ph | recently wide publicity has been given to a claim by t vachaspati that black holes do not exist that the objects known as black holes in astrophysics should rather be called black stars and they not only do not have event horizons but actually can be the source of spectacular gamma ray bursts in this short essay no fli... | [['recently', 'wide', 'publicity', 'has', 'been', 'given', 'to', 'a', 'claim', 'by', 't', 'vachaspati', 'that', 'black', 'holes', 'do', 'not', 'exist', 'that', 'the', 'objects', 'known', 'as', 'black', 'holes', 'in', 'astrophysics', 'should', 'rather', 'be', 'called', 'black', 'stars', 'and', 'they', 'not', 'only', 'do... | [-0.06561546773403226, 0.12417228515251362, -0.09007655023871099, 0.19614360681803458, -0.16842818243301236, -0.15934401718607427, 0.008976827674618392, 0.39765224739105676, -0.1812235291672907, -0.3301747735114951, 0.12464704344564975, -0.285365511051507, -0.1446028089187309, 0.24260083544204997, -0.1742891217034091, ... |
707.2451 | SUSY Unparticle and Conformal Sequestering | We investigate unparticle physics with supersymmetry (SUSY). The SUSY
breaking effects due to the gravity mediation induce soft masses for the SUSY
unparticles and hence break the conformal invariance. The unparticle physics
observable in near future experiments is only consistent if the SUSY breaking
effects from th... | hep-ph hep-th | we investigate unparticle physics with supersymmetry susy the susy breaking effects due to the gravity mediation induce soft masses for the susy unparticles and hence break the conformal invariance the unparticle physics observable in near future experiments is only consistent if the susy breaking effects from the hidd... | [['we', 'investigate', 'unparticle', 'physics', 'with', 'supersymmetry', 'susy', 'the', 'susy', 'breaking', 'effects', 'due', 'to', 'the', 'gravity', 'mediation', 'induce', 'soft', 'masses', 'for', 'the', 'susy', 'unparticles', 'and', 'hence', 'break', 'the', 'conformal', 'invariance', 'the', 'unparticle', 'physics', '... | [-0.11964758217800409, 0.3234715349972248, -0.03940607447558167, 0.22750547606450378, -0.17257800685580482, -0.18483575332952154, -0.028788914512419564, 0.2822920671791177, -0.24433509186333555, -0.28761451500362123, 0.09500154656945431, -0.2571356266535903, -0.1328346160245763, 0.01798051178180189, 0.03241330733395774... |
707.2452 | A new prescription for soft gluon resummation | We present a new prescription for the resummation of the divergent series of
perturbative corrections, due to soft gluon emission, to hard processes near
threshold in perturbative QCD (threshold resummation). This prescription is
based on Borel resummation, and contrary to the commonly used minimal
prescription, it d... | hep-ph | we present a new prescription for the resummation of the divergent series of perturbative corrections due to soft gluon emission to hard processes near threshold in perturbative qcd threshold resummation this prescription is based on borel resummation and contrary to the commonly used minimal prescription it does not i... | [['we', 'present', 'a', 'new', 'prescription', 'for', 'the', 'resummation', 'of', 'the', 'divergent', 'series', 'of', 'perturbative', 'corrections', 'due', 'to', 'soft', 'gluon', 'emission', 'to', 'hard', 'processes', 'near', 'threshold', 'in', 'perturbative', 'qcd', 'threshold', 'resummation', 'this', 'prescription', ... | [-0.036660616606554036, 0.09944472867014106, -0.21249829146069704, 0.18334351453970196, -0.0930143308335094, -0.06513808030504933, 0.06731758340542275, 0.3665873493338304, -0.16035285673194355, -0.1999273275936483, 0.005268603727291588, -0.2943572698120949, -0.032083462443082564, 0.14482937992540418, -0.030534004885515... |
707.2453 | Unfolding of differential energy spectra in the MAGIC experiment | The paper describes the different methods, used in the MAGIC experiment, to
unfold experimental energy distributions of cosmic ray particles (gamma-rays).
Questions and problems related to the unfolding are discussed. Various
procedures are proposed which can help to make the unfolding robust and
reliable. The differ... | astro-ph | the paper describes the different methods used in the magic experiment to unfold experimental energy distributions of cosmic ray particles gammarays questions and problems related to the unfolding are discussed various procedures are proposed which can help to make the unfolding robust and reliable the different method... | [['the', 'paper', 'describes', 'the', 'different', 'methods', 'used', 'in', 'the', 'magic', 'experiment', 'to', 'unfold', 'experimental', 'energy', 'distributions', 'of', 'cosmic', 'ray', 'particles', 'gammarays', 'questions', 'and', 'problems', 'related', 'to', 'the', 'unfolding', 'are', 'discussed', 'various', 'proce... | [-0.02249405499813812, 0.12236140928571186, -0.0964350036108896, 0.19401486243106544, -0.05757951634448199, -0.12096864795164457, -0.02441929794648396, 0.435615984279485, -0.24873827922061856, -0.34890920999977326, 0.09748125638228856, -0.28812921164734734, -0.10673395828122184, 0.26261312585501445, -0.0590570482262779... |
707.2454 | A semiregularity map annihilating obstructions to deforming holomorphic
maps | We study deformations of holomorphic maps of compact, complex, K\"ahler
manifolds. In particular, we describe a generalization of Bloch's
semiregularity map that annihilates obstructions to deform holomorphic maps
with fixed codomain.
| math.AG math.QA | we study deformations of holomorphic maps of compact complex kahler manifolds in particular we describe a generalization of blochs semiregularity map that annihilates obstructions to deform holomorphic maps with fixed codomain | [['we', 'study', 'deformations', 'of', 'holomorphic', 'maps', 'of', 'compact', 'complex', 'kahler', 'manifolds', 'in', 'particular', 'we', 'describe', 'a', 'generalization', 'of', 'blochs', 'semiregularity', 'map', 'that', 'annihilates', 'obstructions', 'to', 'deform', 'holomorphic', 'maps', 'with', 'fixed', 'codomain'... | [-0.21464636119743508, 0.01284875065809296, -0.08058934911124167, 0.14097873433943717, -0.17994926185647567, -0.14817722909332764, -0.07967465065960441, 0.37075635382244665, -0.32491816484159036, -0.0828476295235657, 0.049071898454830294, -0.2559624913058454, -0.28633870544933504, 0.16636230676404892, -0.21660780092521... |
707.2455 | Chiral Asymmetry from a 5D Higgs Mechanism | An intriguing feature of the Standard Model is that the representations of
the unbroken gauge symmetries are vector-like whereas those of the
spontaneously broken gauge symmetries are chiral. Here we provide a toy model
which shows that a natural explanation of this property could emerge in higher
dimensional field t... | hep-th hep-ph | an intriguing feature of the standard model is that the representations of the unbroken gauge symmetries are vectorlike whereas those of the spontaneously broken gauge symmetries are chiral here we provide a toy model which shows that a natural explanation of this property could emerge in higher dimensional field theor... | [['an', 'intriguing', 'feature', 'of', 'the', 'standard', 'model', 'is', 'that', 'the', 'representations', 'of', 'the', 'unbroken', 'gauge', 'symmetries', 'are', 'vectorlike', 'whereas', 'those', 'of', 'the', 'spontaneously', 'broken', 'gauge', 'symmetries', 'are', 'chiral', 'here', 'we', 'provide', 'a', 'toy', 'model'... | [-0.14198627811856568, 0.23625823607951382, -0.09079548792038677, 0.14394726363367005, -0.07444282267136838, -0.13275036615827543, -0.029708446911888932, 0.31969606193403405, -0.22918662621470337, -0.30914887014042697, 0.07657995326338675, -0.2474119739173065, -0.15887944759963307, 0.08308965026376289, -0.0310420224682... |
707.2456 | Effects of the low frequencies of noise on On-Off intermittency | A bifurcating system subject to multiplicative noise can exhibit on-off
intermittency close to the instability threshold. For a canonical system, we
discuss the dependence of this intermittency on the Power Spectrum Density
(PSD) of the noise. Our study is based on the calculation of the Probability
Density Function ... | cond-mat.stat-mech nlin.CD | a bifurcating system subject to multiplicative noise can exhibit onoff intermittency close to the instability threshold for a canonical system we discuss the dependence of this intermittency on the power spectrum density psd of the noise our study is based on the calculation of the probability density function pdf of t... | [['a', 'bifurcating', 'system', 'subject', 'to', 'multiplicative', 'noise', 'can', 'exhibit', 'onoff', 'intermittency', 'close', 'to', 'the', 'instability', 'threshold', 'for', 'a', 'canonical', 'system', 'we', 'discuss', 'the', 'dependence', 'of', 'this', 'intermittency', 'on', 'the', 'power', 'spectrum', 'density', '... | [-0.16978568868060254, 0.1176606259025822, -0.1053515744448604, 0.07303167708053053, 0.01172680750819324, -0.11219690184556891, 0.05564154639745815, 0.33347311498054977, -0.2392716128069648, -0.2599562841844804, 0.09685169655941663, -0.26822913966224166, -0.1806891900369355, 0.20278128215459565, -0.02764329613080319, 0... |
707.2457 | Glow Discharge AES: Methodological Peculiarities of Pulse Element
Analysis and Flash Desorption | Different techniques of Glow Discharge AES are described in this paper. The
most important parameters at such investigations are: the power of VHF-field,
pressure of the inert gas and concentration of the easily ionizable additive,
e.g. NaCl. The influences of these parameters were studied It is proposed a
high sensi... | physics.bio-ph | different techniques of glow discharge aes are described in this paper the most important parameters at such investigations are the power of vhffield pressure of the inert gas and concentration of the easily ionizable additive eg nacl the influences of these parameters were studied it is proposed a high sensitive flash... | [['different', 'techniques', 'of', 'glow', 'discharge', 'aes', 'are', 'described', 'in', 'this', 'paper', 'the', 'most', 'important', 'parameters', 'at', 'such', 'investigations', 'are', 'the', 'power', 'of', 'vhffield', 'pressure', 'of', 'the', 'inert', 'gas', 'and', 'concentration', 'of', 'the', 'easily', 'ionizable'... | [-0.07804803336287425, 0.1572565028028989, -0.041856947759002006, 0.014823049461804605, 0.01742836137247436, -0.150504925113637, 0.029247787174159278, 0.3518798377994886, -0.21946523875949958, -0.31473918749457774, 0.08727488082556245, -0.32865596642060313, -0.07634606895803966, 0.2150293095585178, -0.01900033483980223... |
707.2458 | Thermal imaginary part of a real-time static potential from classical
lattice gauge theory simulations | Recently, a finite-temperature real-time static potential has been introduced
via a Schr\"odinger-type equation satisfied by a certain heavy quarkonium
Green's function. Furthermore, it has been pointed out that it possesses an
imaginary part, which induces a finite width for the tip of the quarkonium peak
in the the... | hep-lat hep-ph | recently a finitetemperature realtime static potential has been introduced via a schrodingertype equation satisfied by a certain heavy quarkonium greens function furthermore it has been pointed out that it possesses an imaginary part which induces a finite width for the tip of the quarkonium peak in the thermal dilepto... | [['recently', 'a', 'finitetemperature', 'realtime', 'static', 'potential', 'has', 'been', 'introduced', 'via', 'a', 'schrodingertype', 'equation', 'satisfied', 'by', 'a', 'certain', 'heavy', 'quarkonium', 'greens', 'function', 'furthermore', 'it', 'has', 'been', 'pointed', 'out', 'that', 'it', 'possesses', 'an', 'imagi... | [-0.13441239630032453, 0.1990427893142027, -0.17333977141219084, 0.08144723378182923, -0.06877816026099026, -0.11071028432438577, 0.011845080602769053, 0.35301834015084094, -0.222737382188989, -0.2154456077326761, 0.0318550307763603, -0.28312810079851114, -0.15416280405412688, 0.15083386320964295, 0.041342379494768676,... |
707.2459 | Using globular clusters to test gravity in the weak acceleration regime | We report on the results from an ongoing program aimed at testing Newton's
law of gravity in the low acceleration regime using globular clusters. It is
shown that all clusters studied so far do behave like galaxies, that is, their
velocity dispersion profile flattens out at large radii where the acceleration
of gravi... | astro-ph | we report on the results from an ongoing program aimed at testing newtons law of gravity in the low acceleration regime using globular clusters it is shown that all clusters studied so far do behave like galaxies that is their velocity dispersion profile flattens out at large radii where the acceleration of gravity goe... | [['we', 'report', 'on', 'the', 'results', 'from', 'an', 'ongoing', 'program', 'aimed', 'at', 'testing', 'newtons', 'law', 'of', 'gravity', 'in', 'the', 'low', 'acceleration', 'regime', 'using', 'globular', 'clusters', 'it', 'is', 'shown', 'that', 'all', 'clusters', 'studied', 'so', 'far', 'do', 'behave', 'like', 'galax... | [-0.11981365304982819, 0.15058606641418879, -0.16248907958832357, 0.12797728991093232, -0.10197889591661205, -0.09822406480516042, 0.014603323933301032, 0.3367898015971851, -0.19293608853097902, -0.34408152895475475, 0.021987623942016258, -0.2791384900076349, -0.05028452608871077, 0.19273147106794383, -0.04587843832175... |
707.246 | Magnetic Interference Patterns and Vortices in Diffusive SNS junctions | We study theoretically the electronic and transport properties of a diffusive
superconductor-normal metal-superconductor (SNS) junction in the presence of a
perpendicular magnetic field. We show that the field dependence of the critical
current crosses over from the well-known Fraunhofer pattern in wide junctions
to ... | cond-mat.supr-con cond-mat.mes-hall | we study theoretically the electronic and transport properties of a diffusive superconductornormal metalsuperconductor sns junction in the presence of a perpendicular magnetic field we show that the field dependence of the critical current crosses over from the wellknown fraunhofer pattern in wide junctions to a monoto... | [['we', 'study', 'theoretically', 'the', 'electronic', 'and', 'transport', 'properties', 'of', 'a', 'diffusive', 'superconductornormal', 'metalsuperconductor', 'sns', 'junction', 'in', 'the', 'presence', 'of', 'a', 'perpendicular', 'magnetic', 'field', 'we', 'show', 'that', 'the', 'field', 'dependence', 'of', 'the', 'c... | [-0.21551698663880905, 0.1717990999056313, -0.04777161797168306, 0.04822437589106043, -0.038006184331607074, -0.07267826451705052, 0.023222226745789297, 0.3543750734892316, -0.30090147721616983, -0.27461082879185245, -0.00230565397382284, -0.25451819036299217, -0.139558649657724, 0.2064699119207664, 0.05499903685071890... |
707.2461 | Bosons, Fermions and Branes | Starting from considerations of Bosons at the real life Compton scale we go
on to a description of Fermions, specifically the Dirac equation in terms of an
underlying noncommutative geometry described by the Dirac $\gamma$ matrices and
generalize this to branes in an underlying C-space (with Clifford Algebra).
| physics.gen-ph | starting from considerations of bosons at the real life compton scale we go on to a description of fermions specifically the dirac equation in terms of an underlying noncommutative geometry described by the dirac gamma matrices and generalize this to branes in an underlying cspace with clifford algebra | [['starting', 'from', 'considerations', 'of', 'bosons', 'at', 'the', 'real', 'life', 'compton', 'scale', 'we', 'go', 'on', 'to', 'a', 'description', 'of', 'fermions', 'specifically', 'the', 'dirac', 'equation', 'in', 'terms', 'of', 'an', 'underlying', 'noncommutative', 'geometry', 'described', 'by', 'the', 'dirac', 'ga... | [-0.08246766368392855, 0.18650396075645403, -0.06899619657391061, 0.09909326779840437, -0.08666979703896989, -0.11811077155774304, 0.010505118252088627, 0.28790459494727355, -0.2783506844522587, -0.25724554792395793, 0.03541143887074819, -0.28636134151990217, -0.14616020203296406, 0.15933201196215427, -0.07214454621619... |
707.2462 | Search for B Meson Decays to omega K*0 | We report a search for the charmless vector-vector decay B0->omega K*0 with
520x10^6 BBbar pairs collected with the Belle detector at the KEKB e+e-
collider. We measure the branching fraction in units of 10^-6: Br = 1.2
+0.9-0.8 +-0.2 (<2.7), where the first error is statistical, the second
systematic, and the upper ... | hep-ex | we report a search for the charmless vectorvector decay b0omega k0 with 520x106 bbbar pairs collected with the belle detector at the kekb ee collider we measure the branching fraction in units of 106 br 12 0908 02 27 where the first error is statistical the second systematic and the upper limit is at the 90 confidence ... | [['we', 'report', 'a', 'search', 'for', 'the', 'charmless', 'vectorvector', 'decay', 'b0omega', 'k0', 'with', '520x106', 'bbbar', 'pairs', 'collected', 'with', 'the', 'belle', 'detector', 'at', 'the', 'kekb', 'ee', 'collider', 'we', 'measure', 'the', 'branching', 'fraction', 'in', 'units', 'of', '106', 'br', '12', '090... | [-0.1007959170185911, 0.15702622972561844, -0.026554429304919074, 0.049473947525257245, -0.009026176321120667, -0.08884044639333817, 0.16888582954249745, 0.256008697665363, -0.13932834131576652, -0.30311449903196525, 0.0017058817174984142, -0.476577270110803, 0.06467009048875687, 0.13228768396324345, 0.0897293870220892... |
707.2463 | Composite Messenger Baryon as a Cold Dark Matter | Among various supersymmetric (SUSY) models, gauge-mediated SUSY breaking
models with an ultra-light gravitino of mass m_{3/2} \lesssim O(10) eV are very
attractive, since they are completely free from notorious gravitino problems. A
drawback of such a scenario is the absence of the supersymmetric cold dark
matter. In... | hep-ph | among various supersymmetric susy models gaugemediated susy breaking models with an ultralight gravitino of mass m_32 lesssim o10 ev are very attractive since they are completely free from notorious gravitino problems a drawback of such a scenario is the absence of the supersymmetric cold dark matter in this letter we ... | [['among', 'various', 'supersymmetric', 'susy', 'models', 'gaugemediated', 'susy', 'breaking', 'models', 'with', 'an', 'ultralight', 'gravitino', 'of', 'mass', 'm_32', 'lesssim', 'o10', 'ev', 'are', 'very', 'attractive', 'since', 'they', 'are', 'completely', 'free', 'from', 'notorious', 'gravitino', 'problems', 'a', 'd... | [-0.14845209854510835, 0.33210267443254926, -0.04272181180948835, 0.18936926128697537, -0.10071251102324043, -0.1845274711515577, -0.04334535532897072, 0.30847516482130494, -0.2146180971813876, -0.41692332211615785, 0.06439766447874717, -0.2421350053711129, -0.04418361423692355, 0.13362123207688065, -0.0211520917336678... |
707.2464 | Nanometer-Resolved Collective Micromeniscus Oscillations through Optical
Diffraction | We study the dynamics of periodic arrays of micrometer-sized liquid-gas
menisci formed at superhydrophobic surfaces immersed into water. By measuring
the intensity of optical diffraction peaks in real time we are able to resolve
nanometer scale oscillations of the menisci with sub-microsecond time
resolution. Upon dr... | cond-mat.soft | we study the dynamics of periodic arrays of micrometersized liquidgas menisci formed at superhydrophobic surfaces immersed into water by measuring the intensity of optical diffraction peaks in real time we are able to resolve nanometer scale oscillations of the menisci with submicrosecond time resolution upon driving t... | [['we', 'study', 'the', 'dynamics', 'of', 'periodic', 'arrays', 'of', 'micrometersized', 'liquidgas', 'menisci', 'formed', 'at', 'superhydrophobic', 'surfaces', 'immersed', 'into', 'water', 'by', 'measuring', 'the', 'intensity', 'of', 'optical', 'diffraction', 'peaks', 'in', 'real', 'time', 'we', 'are', 'able', 'to', '... | [-0.18456203094923618, 0.22066925557887723, -0.05800034205270835, -0.01576224492728403, -0.029100265212299435, -0.15119430010648655, 0.00949654070007586, 0.3876638248966066, -0.26687689576797263, -0.3027301820129463, 0.10554201488464725, -0.2940064509274419, -0.09962211664977301, 0.2048902424321193, 0.00830143741956076... |
707.2465 | The XMM-Newton view of IRAS 09104+4109: evidence for a changing-look
Type 2 quasar? | We analyzed the spectroscopic data from the PN and the MOS cameras in the
0.4-10 keV band. We also used an archival BeppoSAX 1-50 keV observation of IRAS
09104+4109 to investigate possible variations of the quasar emission. The X-ray
emission in the EPIC band is dominated by the intra-cluster medium thermal
emission.... | astro-ph | we analyzed the spectroscopic data from the pn and the mos cameras in the 0410 kev band we also used an archival bepposax 150 kev observation of iras 091044109 to investigate possible variations of the quasar emission the xray emission in the epic band is dominated by the intracluster medium thermal emission we found t... | [['we', 'analyzed', 'the', 'spectroscopic', 'data', 'from', 'the', 'pn', 'and', 'the', 'mos', 'cameras', 'in', 'the', '0410', 'kev', 'band', 'we', 'also', 'used', 'an', 'archival', 'bepposax', '150', 'kev', 'observation', 'of', 'iras', '091044109', 'to', 'investigate', 'possible', 'variations', 'of', 'the', 'quasar', '... | [-0.03424670666766663, 0.05070000997814835, -0.027936980698723347, 0.05988548748476508, -0.0685707879679588, -0.11012138136623738, 0.059606744243986515, 0.5022718587424606, -0.1428776771373426, -0.33848343626984084, 0.06526161125705889, -0.37149601109170666, 0.03914811536669731, 0.16092364244589893, -0.0118708134948974... |
707.2466 | Initiation of granular surface flows in a narrow channel | We experimentally investigate how a long granular pile confined in a narrow
channel destabilizes when it is inclined above the angle of repose. A uniform
flow then develops, which is localized at the free surface. It first
accelerates before reaching a steady uniform regime. During this process, an
apparent erosion i... | cond-mat.soft | we experimentally investigate how a long granular pile confined in a narrow channel destabilizes when it is inclined above the angle of repose a uniform flow then develops which is localized at the free surface it first accelerates before reaching a steady uniform regime during this process an apparent erosion is obser... | [['we', 'experimentally', 'investigate', 'how', 'a', 'long', 'granular', 'pile', 'confined', 'in', 'a', 'narrow', 'channel', 'destabilizes', 'when', 'it', 'is', 'inclined', 'above', 'the', 'angle', 'of', 'repose', 'a', 'uniform', 'flow', 'then', 'develops', 'which', 'is', 'localized', 'at', 'the', 'free', 'surface', 'i... | [-0.14441607936628556, 0.21344110196300073, -0.08613298170905756, 0.010679073405768385, -0.012328812375811762, -0.1239309254102409, 0.05566325237680422, 0.3724171531264897, -0.29798089527206395, -0.2903944254779306, 0.08606795122277139, -0.25782798506613624, -0.08759422296364057, 0.12592969552221658, -0.035824642590198... |
707.2467 | Cyclic coverings of the $p$-adic projective line by Mumford curves | Exact bounds for the positions of the branch points for cyclic coverings of
the $p$-adic projective line by Mumford curves are calculated in two ways.
Firstly, by using Fumiharu Kato's *-trees, and secondly by giving explicit
matrix representations of the Schottky groups corresponding to the Mumford
curves above the ... | math.AG | exact bounds for the positions of the branch points for cyclic coverings of the padic projective line by mumford curves are calculated in two ways firstly by using fumiharu katos trees and secondly by giving explicit matrix representations of the schottky groups corresponding to the mumford curves above the projective ... | [['exact', 'bounds', 'for', 'the', 'positions', 'of', 'the', 'branch', 'points', 'for', 'cyclic', 'coverings', 'of', 'the', 'padic', 'projective', 'line', 'by', 'mumford', 'curves', 'are', 'calculated', 'in', 'two', 'ways', 'firstly', 'by', 'using', 'fumiharu', 'katos', 'trees', 'and', 'secondly', 'by', 'giving', 'expl... | [-0.15682203201059666, 0.07110654965206911, -0.12763079695610535, 0.08425457002940001, -0.07842351409123728, -0.13167836104036756, 0.11770554825758424, 0.3419721502189835, -0.3116995531546073, -0.2723630616372382, 0.07806073634290239, -0.23430214912837577, -0.1549716118412713, 0.28082855600277307, -0.11414120517050226,... |
707.2468 | Radial Dependence of Extinction in Parent Galaxies of Supernovae | The problem of extinction is the most important issue to be dealt with in the
process of obtaining true absolute magnitudes of core-collapse supernovae
(SNe). The plane-parallel model which gives absorption dependent on galaxy
inclination, widely used in the past, was shown not to describe extinction
adequately. We t... | astro-ph | the problem of extinction is the most important issue to be dealt with in the process of obtaining true absolute magnitudes of corecollapse supernovae sne the planeparallel model which gives absorption dependent on galaxy inclination widely used in the past was shown not to describe extinction adequately we try to appl... | [['the', 'problem', 'of', 'extinction', 'is', 'the', 'most', 'important', 'issue', 'to', 'be', 'dealt', 'with', 'in', 'the', 'process', 'of', 'obtaining', 'true', 'absolute', 'magnitudes', 'of', 'corecollapse', 'supernovae', 'sne', 'the', 'planeparallel', 'model', 'which', 'gives', 'absorption', 'dependent', 'on', 'gal... | [0.004487210420431592, 0.03228551772838958, -0.0973184826189136, 0.12476369689288566, -0.11980793791183506, -0.13552718432844582, 0.031910732814885046, 0.44707100636449204, -0.19888775815474743, -0.28022767139419197, 0.031227923936704285, -0.2819030622289662, -0.04187309912529336, 0.2020358369708151, -0.120693344109588... |
707.2469 | Pseudospectral versus finite-differences schemes in the numerical
integration of stochastic models of surface growth | We present a comparison between finite differences schemes and a
pseudospectral method applied to the numerical integration of stochastic
partial differential equations that model surface growth. We have studied, in
1+1 dimensions, the Kardar, Parisi and Zhang model (KPZ) and the Lai, Das Sarma
and Villain model (LDV... | cond-mat.stat-mech | we present a comparison between finite differences schemes and a pseudospectral method applied to the numerical integration of stochastic partial differential equations that model surface growth we have studied in 11 dimensions the kardar parisi and zhang model kpz and the lai das sarma and villain model ldv the pseudo... | [['we', 'present', 'a', 'comparison', 'between', 'finite', 'differences', 'schemes', 'and', 'a', 'pseudospectral', 'method', 'applied', 'to', 'the', 'numerical', 'integration', 'of', 'stochastic', 'partial', 'differential', 'equations', 'that', 'model', 'surface', 'growth', 'we', 'have', 'studied', 'in', '11', 'dimensi... | [-0.08173410500401872, 0.06111889231063956, -0.13871011728454516, 0.07773163265980645, -0.04031558337071574, -0.1410383291722062, -0.004337534388381404, 0.3699742680869952, -0.2251497283837399, -0.2771517877321107, 0.08287933013606705, -0.26053487478070947, -0.12966494173153742, 0.23973512663421817, 0.00629855697435966... |
707.247 | Environmental Effects of Dark Matter Haloes: The Clustering-Substructure
relation of Group-size Haloes | We estimate the two-point correlation function of dark matter haloes, with
masses >10^{13} h^{-1} Mo, that have or not significant substructure. The
haloes are identified with a friends of friends algorithm in a large LCDM
simulation at two redshift snapshots (z=0 and 1), while halo substructure is
determined using a... | astro-ph | we estimate the twopoint correlation function of dark matter haloes with masses 1013 h1 mo that have or not significant substructure the haloes are identified with a friends of friends algorithm in a large lcdm simulation at two redshift snapshots z0 and 1 while halo substructure is determined using an observationally ... | [['we', 'estimate', 'the', 'twopoint', 'correlation', 'function', 'of', 'dark', 'matter', 'haloes', 'with', 'masses', '1013', 'h1', 'mo', 'that', 'have', 'or', 'not', 'significant', 'substructure', 'the', 'haloes', 'are', 'identified', 'with', 'a', 'friends', 'of', 'friends', 'algorithm', 'in', 'a', 'large', 'lcdm', 's... | [-0.10051448120507626, 0.16422426167571827, -0.10290138497675874, 0.14212080758361137, -0.07167708516417064, -0.049459530126837285, -0.018115785749332987, 0.41724407209948516, -0.13912976364238347, -0.3755341359846699, 0.052769051161380365, -0.27549883318460006, -0.04663011681889554, 0.16899731813269475, 0.034107847034... |
707.2471 | On the number of independent adiabatic invariants for gyrating particles | It is pointed out that the three established adiabatic invariants are
separating invariants in the sense of Liouville. It is widely claimed that no
more than three adiabatic invariants can exist for the motion of a point
charge. However, additional independent (not separating) adiabatic invariants
do exist. For a for... | physics.plasm-ph | it is pointed out that the three established adiabatic invariants are separating invariants in the sense of liouville it is widely claimed that no more than three adiabatic invariants can exist for the motion of a point charge however additional independent not separating adiabatic invariants do exist for a force free ... | [['it', 'is', 'pointed', 'out', 'that', 'the', 'three', 'established', 'adiabatic', 'invariants', 'are', 'separating', 'invariants', 'in', 'the', 'sense', 'of', 'liouville', 'it', 'is', 'widely', 'claimed', 'that', 'no', 'more', 'than', 'three', 'adiabatic', 'invariants', 'can', 'exist', 'for', 'the', 'motion', 'of', '... | [-0.18974455445313818, 0.1651568740162973, -0.11577658821322602, 0.043720192742665816, -0.07582082622790853, -0.127222569657226, -0.034290959291105885, 0.33671280760403094, -0.2872357970299242, -0.26847904622894986, 0.05988370425590914, -0.224141195876796, -0.05680131056392778, 0.18932475227294873, -0.02691093936018203... |
707.2472 | Applications of the q-Fourier Analysis to the Symmetric Moment Problem | Sufficient condition for the symmetric moment problem to be determinate is
given using standards methods of $q$-Fourier analysis. This condition it cannot
be a particular case of Carleman's criterion.
| math.CA | sufficient condition for the symmetric moment problem to be determinate is given using standards methods of qfourier analysis this condition it cannot be a particular case of carlemans criterion | [['sufficient', 'condition', 'for', 'the', 'symmetric', 'moment', 'problem', 'to', 'be', 'determinate', 'is', 'given', 'using', 'standards', 'methods', 'of', 'qfourier', 'analysis', 'this', 'condition', 'it', 'can', 'not', 'be', 'a', 'particular', 'case', 'of', 'carlemans', 'criterion']] | [-0.0915042298535506, 0.04650761721034845, -0.14099077756206194, 0.11779432818293571, -0.14003205032398303, -0.1840941208569954, 0.015485591777057077, 0.35660205204039813, -0.26746129294236504, -0.24781104487677416, 0.20750478922079008, -0.14827549035350482, -0.14614185194174448, 0.20854619437207778, -0.140934664787103... |
707.2473 | Coulomb analogy for nonhermitian degeneracies near quantum phase
transitions | Degeneracies near the real axis in a complex-extended parameter space of a
hermitian Hamiltonian are studied. We present a method to measure distributions
of such degeneracies on the Riemann sheet of a selected level and apply it in
classification of quantum phase transitions. The degeneracies are shown to
behave sim... | quant-ph math-ph math.MP nucl-th | degeneracies near the real axis in a complexextended parameter space of a hermitian hamiltonian are studied we present a method to measure distributions of such degeneracies on the riemann sheet of a selected level and apply it in classification of quantum phase transitions the degeneracies are shown to behave similarl... | [['degeneracies', 'near', 'the', 'real', 'axis', 'in', 'a', 'complexextended', 'parameter', 'space', 'of', 'a', 'hermitian', 'hamiltonian', 'are', 'studied', 'we', 'present', 'a', 'method', 'to', 'measure', 'distributions', 'of', 'such', 'degeneracies', 'on', 'the', 'riemann', 'sheet', 'of', 'a', 'selected', 'level', '... | [-0.17559869665644345, 0.10728490153703381, -0.08655611174017713, 0.12567713451490067, -0.036497868826253374, -0.0896766158433533, 0.04781058256661421, 0.36265764462255073, -0.23069761845430262, -0.30012113993922085, 0.08957800973745945, -0.2828909534503493, -0.19154060040518903, 0.16200138046814685, -0.007029360560536... |
707.2474 | Visualization, Exploration and Data Analysis of Complex Astrophysical
Data | In this paper we show how advanced visualization tools can help the
researcher in investigating and extracting information from data. The focus is
on VisIVO, a novel open source graphics application, which blends high
performance multidimensional visualization techniques and up-to-date
technologies to cooperate with ... | astro-ph | in this paper we show how advanced visualization tools can help the researcher in investigating and extracting information from data the focus is on visivo a novel open source graphics application which blends high performance multidimensional visualization techniques and uptodate technologies to cooperate with other a... | [['in', 'this', 'paper', 'we', 'show', 'how', 'advanced', 'visualization', 'tools', 'can', 'help', 'the', 'researcher', 'in', 'investigating', 'and', 'extracting', 'information', 'from', 'data', 'the', 'focus', 'is', 'on', 'visivo', 'a', 'novel', 'open', 'source', 'graphics', 'application', 'which', 'blends', 'high', '... | [-0.08682409932529464, 0.017456744309261585, -0.07722590197311732, 0.07800017288225947, -0.1399591545330234, -0.1597026313120472, 0.035584827522222785, 0.3958715629194257, -0.29896214767585244, -0.35563385020941496, 0.1394749556089417, -0.3087602559413797, -0.14368644080721565, 0.2524509021596422, -0.10098085490968621,... |
707.2475 | Effect of General Relativity and rotation on the energy deposition rate
for $\nu + \bar{\nu} \to e^+ + e^- $ inside a compact star | We have studied the $\nu + \bar{\nu} \to e^+ + e^- $ energy deposition rate
in a rotating compact star. This reaction is important for the study of gamma
ray bursts. The General Relativistic (GR) effects on the energy deposition rate
have been incorporated. We find that the efficiency of the process is larger
for a r... | astro-ph hep-ph | we have studied the nu barnu to e e energy deposition rate in a rotating compact star this reaction is important for the study of gamma ray bursts the general relativistic gr effects on the energy deposition rate have been incorporated we find that the efficiency of the process is larger for a rotating star the total e... | [['we', 'have', 'studied', 'the', 'nu', 'barnu', 'to', 'e', 'e', 'energy', 'deposition', 'rate', 'in', 'a', 'rotating', 'compact', 'star', 'this', 'reaction', 'is', 'important', 'for', 'the', 'study', 'of', 'gamma', 'ray', 'bursts', 'the', 'general', 'relativistic', 'gr', 'effects', 'on', 'the', 'energy', 'deposition',... | [-0.09707628294506393, 0.1731993778769955, -0.060358536292686324, 0.07798932163444824, -0.03958303475061829, -0.028308981757485464, 0.02602515932632966, 0.35518138194352056, -0.2083721530487698, -0.30007131598638687, 0.027501716486471338, -0.26665983615924466, -0.005415094629181235, 0.24011224110642176, -0.014418744722... |
707.2476 | Shock waves in tidally compressed stars by massive black holes | We interest in the case of a main-sequence star deeply penetrating within the
tidal radius of a massive black hole. We focus on the compression phase leading
to a so-called pancake configuration of the star at the instant of maximal
compression. The aim is to study the tidal compression process paying
particular atte... | astro-ph | we interest in the case of a mainsequence star deeply penetrating within the tidal radius of a massive black hole we focus on the compression phase leading to a socalled pancake configuration of the star at the instant of maximal compression the aim is to study the tidal compression process paying particular attention ... | [['we', 'interest', 'in', 'the', 'case', 'of', 'a', 'mainsequence', 'star', 'deeply', 'penetrating', 'within', 'the', 'tidal', 'radius', 'of', 'a', 'massive', 'black', 'hole', 'we', 'focus', 'on', 'the', 'compression', 'phase', 'leading', 'to', 'a', 'socalled', 'pancake', 'configuration', 'of', 'the', 'star', 'at', 'th... | [-0.10631291738563522, 0.13107067196199507, -0.07658905080413081, 0.10431394350956323, -0.11609225848524718, -0.0506277979691805, 0.06827276556862594, 0.38647664683386407, -0.2303596566194098, -0.29217166682306633, 0.09571094717014224, -0.27011488410787066, -0.06509139573109608, 0.20194137484742486, -0.0376904236532514... |
707.2477 | $L^p$-Spectral theory of locally symmetric spaces with $Q$-rank one | We study the $L^p$-spectrum of the Laplace-Beltrami operator on certain
complete locally symmetric spaces $M=\Gamma\backslash X$ with finite volume and
arithmetic fundamental group $\Gamma$ whose universal covering $X$ is a
symmetric space of non-compact type. We also show, how the obtained results for
locally symmet... | math.SP math.DG | we study the lpspectrum of the laplacebeltrami operator on certain complete locally symmetric spaces mgammabackslash x with finite volume and arithmetic fundamental group gamma whose universal covering x is a symmetric space of noncompact type we also show how the obtained results for locally symmetric spaces can be ge... | [['we', 'study', 'the', 'lpspectrum', 'of', 'the', 'laplacebeltrami', 'operator', 'on', 'certain', 'complete', 'locally', 'symmetric', 'spaces', 'mgammabackslash', 'x', 'with', 'finite', 'volume', 'and', 'arithmetic', 'fundamental', 'group', 'gamma', 'whose', 'universal', 'covering', 'x', 'is', 'a', 'symmetric', 'space... | [-0.13678800445050002, 0.14415227758105506, -0.08642309260639278, 0.08285979633007876, -0.11659813562238758, -0.11213762779635462, -0.0034184798153794626, 0.3926966365088116, -0.28609351922165266, -0.14479902989485047, 0.16632873197509485, -0.2397779321128672, -0.14753575437617572, 0.22527121954004872, -0.1210177634080... |
707.2478 | Zeeman ratchets: pure spin current generation in mesoscopic conductors
with non-uniform magnetic fields | We consider the possibility to employ a quantum wire realized in a
two-dimensional electron gas (2DEG) as a spin ratchet. We show that a net spin
current without accompanying net charge transport can be induced in the
nonlinear regime by an unbiased external driving via an ac voltage applied
between the contacts at t... | cond-mat.mes-hall | we consider the possibility to employ a quantum wire realized in a twodimensional electron gas 2deg as a spin ratchet we show that a net spin current without accompanying net charge transport can be induced in the nonlinear regime by an unbiased external driving via an ac voltage applied between the contacts at the end... | [['we', 'consider', 'the', 'possibility', 'to', 'employ', 'a', 'quantum', 'wire', 'realized', 'in', 'a', 'twodimensional', 'electron', 'gas', '2deg', 'as', 'a', 'spin', 'ratchet', 'we', 'show', 'that', 'a', 'net', 'spin', 'current', 'without', 'accompanying', 'net', 'charge', 'transport', 'can', 'be', 'induced', 'in', ... | [-0.21201397924893103, 0.18721806276314762, 0.0031721788518889633, 0.01469008415545061, -0.003275815412591867, -0.1641092732143416, 0.04784158847932876, 0.43253232821546217, -0.25560414706490486, -0.26149582021214346, 0.000354251929955488, -0.2677636162843555, -0.11296473538796245, 0.23626467257876088, 0.04602425529069... |
707.2479 | Detecting synchronization clusters in multivariate time series via
coarse-graining of Markov chains | Synchronization cluster analysis is an approach to the detection of
underlying structures in data sets of multivariate time series, starting from a
matrix R of bivariate synchronization indices. A previous method utilized the
eigenvectors of R for cluster identification, analogous to several recent
attempts at group ... | physics.data-an | synchronization cluster analysis is an approach to the detection of underlying structures in data sets of multivariate time series starting from a matrix r of bivariate synchronization indices a previous method utilized the eigenvectors of r for cluster identification analogous to several recent attempts at group ident... | [['synchronization', 'cluster', 'analysis', 'is', 'an', 'approach', 'to', 'the', 'detection', 'of', 'underlying', 'structures', 'in', 'data', 'sets', 'of', 'multivariate', 'time', 'series', 'starting', 'from', 'a', 'matrix', 'r', 'of', 'bivariate', 'synchronization', 'indices', 'a', 'previous', 'method', 'utilized', 't... | [-0.101310285232724, 0.010528527621233326, -0.10880622902005818, 0.03724601954042402, -0.027547288068529706, -0.10914279049354958, 0.05277639781038121, 0.37569019016202376, -0.2847253505635127, -0.2886210242651478, 0.112912642311085, -0.2526572322276253, -0.19183180470204686, 0.1981210012913693, -0.03457553502206939, 0... |
707.248 | Renormalization of Lorentz violating theories | We classify the unitary, renormalizable, Lorentz violating quantum field
theories of interacting scalars and fermions, obtained improving the behavior
of Feynman diagrams by means of higher space derivatives. Higher time
derivatives are not generated by renormalization. Renormalizability is ensured
by a "weighted pow... | hep-th | we classify the unitary renormalizable lorentz violating quantum field theories of interacting scalars and fermions obtained improving the behavior of feynman diagrams by means of higher space derivatives higher time derivatives are not generated by renormalization renormalizability is ensured by a weighted power count... | [['we', 'classify', 'the', 'unitary', 'renormalizable', 'lorentz', 'violating', 'quantum', 'field', 'theories', 'of', 'interacting', 'scalars', 'and', 'fermions', 'obtained', 'improving', 'the', 'behavior', 'of', 'feynman', 'diagrams', 'by', 'means', 'of', 'higher', 'space', 'derivatives', 'higher', 'time', 'derivative... | [-0.1831089293163608, 0.24793215505113558, -0.07796824533267811, 0.1431099517697779, -0.08936302601138041, -0.15832369765433082, 0.022625120434289176, 0.3202542127997038, -0.21078285394192098, -0.29108532935026143, 0.0715582078056676, -0.27777937918324913, -0.13773466448765248, 0.16432574802699187, 0.007542570388544672... |
707.2481 | The (3+2) Neutrino Mass Spectrum and Double Chooz | The implications of extra sterile neutrinos for the Double Chooz experiment
is expounded. The so-called ``3+2'' mass spectrum with 2 sterile neutrinos
mixed with the active ones, is still allowed by the global neutrino data
including MiniBooNE. We probe its impact on the resultant reactor antineutrino
signal at the n... | hep-ph astro-ph hep-ex | the implications of extra sterile neutrinos for the double chooz experiment is expounded the socalled 32 mass spectrum with 2 sterile neutrinos mixed with the active ones is still allowed by the global neutrino data including miniboone we probe its impact on the resultant reactor antineutrino signal at the near and far... | [['the', 'implications', 'of', 'extra', 'sterile', 'neutrinos', 'for', 'the', 'double', 'chooz', 'experiment', 'is', 'expounded', 'the', 'socalled', '32', 'mass', 'spectrum', 'with', '2', 'sterile', 'neutrinos', 'mixed', 'with', 'the', 'active', 'ones', 'is', 'still', 'allowed', 'by', 'the', 'global', 'neutrino', 'data... | [-0.090846844844424, 0.2808642714102577, -0.005903137250921674, 0.15287337272376236, -0.04751966354836311, -0.1560076355143258, 0.09298230954519814, 0.26327978351729964, -0.24399500777797092, -0.35678271588588517, 0.07856959020645017, -0.35563078411810456, -0.022963493216102793, 0.17020521599925048, 0.01192449879581256... |
707.2482 | Multiple-Description Lattice Vector Quantization | In this thesis, we construct and analyze multiple-description codes based on
lattice vector quantization.
| cs.IT math.IT | in this thesis we construct and analyze multipledescription codes based on lattice vector quantization | [['in', 'this', 'thesis', 'we', 'construct', 'and', 'analyze', 'multipledescription', 'codes', 'based', 'on', 'lattice', 'vector', 'quantization']] | [-0.15020822347807034, 0.06609804322943091, -0.08738187174978, 0.0706664024037309, -0.045983106297041686, -0.18635691702365875, 0.07156677730381489, 0.4027215290282454, -0.24891636786716326, -0.146551820316485, 0.13108584137600182, -0.19599135060395514, -0.26222617125936915, 0.08651948640389102, -0.1410290137199419, 0.... |
707.2483 | Lyman-alpha radiative transfer during the Epoch of Reionization:
contribution to 21-cm signal fluctuations | During the epoch of reionization, Ly-alpha photons emitted by the first stars
can couple the neutral hydrogen spin temperature to the kinetic gas
temperature, providing the opportunity to observe the gas in emission or
absorption in the 21-cm line. Given the bright foregrounds, it is of prime
importance to determine ... | astro-ph | during the epoch of reionization lyalpha photons emitted by the first stars can couple the neutral hydrogen spin temperature to the kinetic gas temperature providing the opportunity to observe the gas in emission or absorption in the 21cm line given the bright foregrounds it is of prime importance to determine precisel... | [['during', 'the', 'epoch', 'of', 'reionization', 'lyalpha', 'photons', 'emitted', 'by', 'the', 'first', 'stars', 'can', 'couple', 'the', 'neutral', 'hydrogen', 'spin', 'temperature', 'to', 'the', 'kinetic', 'gas', 'temperature', 'providing', 'the', 'opportunity', 'to', 'observe', 'the', 'gas', 'in', 'emission', 'or', ... | [-0.07126202711671016, 0.12267957425356868, -0.04621535402477084, 0.07942019441771432, -0.07727226468535205, -0.07598554349587813, -0.004189593664171239, 0.3972678948286457, -0.22290833555022949, -0.2921358656638594, 0.017842561480895018, -0.32785674736288317, -0.034303661680256774, 0.16299682972890173, 0.0648996695292... |
707.2484 | Quantum vortex tunneling in $YBa_2Cu_3O_{7-\delta}$ thin films | Cuprate films offer a unique opportunity to observe vortex tunneling effects,
due to their unusually low superfluid density and short coherence length. Here,
we measure the magnetoresistance (\textit{MR}) due to vortex motion of a long
meander line of a superconducting film made of underdoped
$YBa_2Cu_3O_{7-\delta}$.... | cond-mat.supr-con cond-mat.str-el | cuprate films offer a unique opportunity to observe vortex tunneling effects due to their unusually low superfluid density and short coherence length here we measure the magnetoresistance textitmr due to vortex motion of a long meander line of a superconducting film made of underdoped yba_2cu_3o_7delta at low temperatu... | [['cuprate', 'films', 'offer', 'a', 'unique', 'opportunity', 'to', 'observe', 'vortex', 'tunneling', 'effects', 'due', 'to', 'their', 'unusually', 'low', 'superfluid', 'density', 'and', 'short', 'coherence', 'length', 'here', 'we', 'measure', 'the', 'magnetoresistance', 'textitmr', 'due', 'to', 'vortex', 'motion', 'of'... | [-0.1807198076311386, 0.23945205972878017, -0.04630400710315867, 0.017631716081976063, -0.05800535992691011, -0.16897511214836303, 0.1359574875460392, 0.41203619370406325, -0.2695724602995647, -0.2730259693755693, 0.0012608997075762036, -0.30304545601547667, -0.018426745753697675, 0.20436063536438112, -0.00052617471829... |
707.2485 | Spectral analysis of boundary layers in Rayleigh-Benard convection | A combined experimental and numerical study of the boundary layer in a 4:1
aspect-ratio Rayleigh-B\'{e}nard cell over a four-decade range of Rayleigh
numbers has been undertaken aimed at gaining a better insight into the
character of the boundary layers. The experiments involved the simultaneous
Laser Doppler Anemome... | physics.flu-dyn | a combined experimental and numerical study of the boundary layer in a 41 aspectratio rayleighbenard cell over a fourdecade range of rayleigh numbers has been undertaken aimed at gaining a better insight into the character of the boundary layers the experiments involved the simultaneous laser doppler anemometry lda mea... | [['a', 'combined', 'experimental', 'and', 'numerical', 'study', 'of', 'the', 'boundary', 'layer', 'in', 'a', '41', 'aspectratio', 'rayleighbenard', 'cell', 'over', 'a', 'fourdecade', 'range', 'of', 'rayleigh', 'numbers', 'has', 'been', 'undertaken', 'aimed', 'at', 'gaining', 'a', 'better', 'insight', 'into', 'the', 'ch... | [-0.16327027179586637, 0.18573963690069642, -0.03608261478032068, 0.0006686039032681965, 0.011869939940861694, -0.08284394943736273, 0.047876523917144406, 0.3356427154549868, -0.2504441698824083, -0.33306339821584596, 0.10197868061224276, -0.26050317854537525, -0.04760545649160031, 0.2155793239500853, 0.015105526759617... |
707.2486 | Transverse Target-Spin Asymmetry of Exclusive $\rho^0$ Meson Production
on Proton at HERMES | Preliminary measurements are reported on the azimuthal single-spin asymmetry
of exclusive rho0 mesons for a transversely polarized hydrogen target at HERMES
using the 27.6 GeV HERA positron beam. Within the generalized parton
distribution (GPD) formalism, this asymmetry is sensitive to the total angular
momentum of q... | hep-ex | preliminary measurements are reported on the azimuthal singlespin asymmetry of exclusive rho0 mesons for a transversely polarized hydrogen target at hermes using the 276 gev hera positron beam within the generalized parton distribution gpd formalism this asymmetry is sensitive to the total angular momentum of quarks an... | [['preliminary', 'measurements', 'are', 'reported', 'on', 'the', 'azimuthal', 'singlespin', 'asymmetry', 'of', 'exclusive', 'rho0', 'mesons', 'for', 'a', 'transversely', 'polarized', 'hydrogen', 'target', 'at', 'hermes', 'using', 'the', '276', 'gev', 'hera', 'positron', 'beam', 'within', 'the', 'generalized', 'parton',... | [-0.045159646276249944, 0.3246290793934141, -0.16293413816468724, 0.20927566898347114, -0.052924380357186475, -0.07284222978464586, -0.01751135032994291, 0.39672818779945374, -0.14598880417600094, -0.19236402949654913, -0.19962750175120644, -0.37391874789967233, 0.1602071092901639, 0.0899275305641658, 0.141140361470787... |
707.2487 | Gate-induced insulating state in bilayer graphene devices | The potential of graphene-based materials consisting of one or a few layers
of graphite for integrated electronics originates from the large
room-temperature carrier mobility in these systems (approx. 10,000 cm2/Vs).
However, the realization of electronic devices such as field-effect transistors
will require controll... | cond-mat.mes-hall cond-mat.mtrl-sci | the potential of graphenebased materials consisting of one or a few layers of graphite for integrated electronics originates from the large roomtemperature carrier mobility in these systems approx 10000 cm2vs however the realization of electronic devices such as fieldeffect transistors will require controlling and even... | [['the', 'potential', 'of', 'graphenebased', 'materials', 'consisting', 'of', 'one', 'or', 'a', 'few', 'layers', 'of', 'graphite', 'for', 'integrated', 'electronics', 'originates', 'from', 'the', 'large', 'roomtemperature', 'carrier', 'mobility', 'in', 'these', 'systems', 'approx', '10000', 'cm2vs', 'however', 'the', '... | [-0.18290015226360695, 0.16361944217074087, 0.0031642873065077324, -0.08772176807844492, -0.015081645756148968, -0.15394277205107873, 0.12256653905453375, 0.40881303529932994, -0.271363697284009, -0.32516010800617284, 0.01574229635931805, -0.29489303361412633, -0.14337500337619005, 0.24248293853605635, -0.0019723394138... |
707.2488 | Primitive contractions of Calabi-Yau threefolds II | We construct 16 new examples of Calabi--Yau threefolds with Picard group of
rank 1. Each of these examples is obtained by smoothing the image of a
primitive contraction with exceptional divisor being a del Pezzo surface of
degree 6, 7 or $\mathbb{P}^1\times \mathbb{P}^1$.
| math.AG | we construct 16 new examples of calabiyau threefolds with picard group of rank 1 each of these examples is obtained by smoothing the image of a primitive contraction with exceptional divisor being a del pezzo surface of degree 6 7 or mathbbp1times mathbbp1 | [['we', 'construct', '16', 'new', 'examples', 'of', 'calabiyau', 'threefolds', 'with', 'picard', 'group', 'of', 'rank', '1', 'each', 'of', 'these', 'examples', 'is', 'obtained', 'by', 'smoothing', 'the', 'image', 'of', 'a', 'primitive', 'contraction', 'with', 'exceptional', 'divisor', 'being', 'a', 'del', 'pezzo', 'sur... | [-0.217067209787147, 0.002707295791181021, -0.06930215596113094, 0.07352450188130227, -0.048473947389094635, -0.2622500477402016, -0.01472661656403351, 0.31252463235584804, -0.26424700662840245, -0.3087525156348251, 0.15084116514988763, -0.3189658461961635, -0.15273347201887086, 0.18380296766909576, -0.1941506875418993... |
707.2489 | A Little About Folklore | Comment on paper by P.W. Anderson is presented. This Anderson's work is shown
to contain a number of inaccurate and ungrounded statements. We point out, in
particular, that the total static dielectric function not only can be negative,
but inevitably has a minus sign in many stable systems. We also demonstrate
that i... | cond-mat.supr-con | comment on paper by pw anderson is presented this andersons work is shown to contain a number of inaccurate and ungrounded statements we point out in particular that the total static dielectric function not only can be negative but inevitably has a minus sign in many stable systems we also demonstrate that in many meta... | [['comment', 'on', 'paper', 'by', 'pw', 'anderson', 'is', 'presented', 'this', 'andersons', 'work', 'is', 'shown', 'to', 'contain', 'a', 'number', 'of', 'inaccurate', 'and', 'ungrounded', 'statements', 'we', 'point', 'out', 'in', 'particular', 'that', 'the', 'total', 'static', 'dielectric', 'function', 'not', 'only', '... | [-0.14206585744639513, 0.15222689941482143, -0.0746462563984096, 0.11004811875403014, -0.07093631315889747, -0.16597121911729837, 0.05616960596823848, 0.3795004923568042, -0.2300409706645147, -0.26101398078161614, 0.029823209982105466, -0.3203398376692433, -0.1895173145106149, 0.17538700106304658, -0.05713608110496818,... |
707.249 | Influence of a carbon over-coat on the X-ray reflectance of XEUS mirrors | We describe measurements of the X-ray reflectance in the range 2 to 10 keV of
samples representative of coated silicon wafers that are proposed for the
fabrication of the XEUS (X-ray Evolving Universe Spectrometer) mission. We
compare the reflectance of silicon samples coated with bare Pt, with that for
samples with ... | astro-ph | we describe measurements of the xray reflectance in the range 2 to 10 kev of samples representative of coated silicon wafers that are proposed for the fabrication of the xeus xray evolving universe spectrometer mission we compare the reflectance of silicon samples coated with bare pt with that for samples with an addit... | [['we', 'describe', 'measurements', 'of', 'the', 'xray', 'reflectance', 'in', 'the', 'range', '2', 'to', '10', 'kev', 'of', 'samples', 'representative', 'of', 'coated', 'silicon', 'wafers', 'that', 'are', 'proposed', 'for', 'the', 'fabrication', 'of', 'the', 'xeus', 'xray', 'evolving', 'universe', 'spectrometer', 'miss... | [-0.046757166934214896, 0.15415791767879797, -0.021763375757994953, -0.024490311390674504, 0.013560127550888746, -0.10808370422694039, 0.040327387640527526, 0.4899461197926373, -0.1904856310928332, -0.42692308955383107, 0.07667580737396464, -0.35370748874838237, -0.01879914659915156, 0.2414673978069675, -0.073421852021... |
707.2491 | Instability of bound states of a nonlinear Schr\"odinger equation with a
Dirac potential | We study analytically and numerically the stability of the standing waves for
a nonlinear Schr\"odinger equation with a point defect and a power type
nonlinearity. A main difficulty is to compute the number of negative
eigenvalues of the linearized operator around the standing waves, and it is
overcome by a perturbat... | nlin.PS nlin.SI | we study analytically and numerically the stability of the standing waves for a nonlinear schrodinger equation with a point defect and a power type nonlinearity a main difficulty is to compute the number of negative eigenvalues of the linearized operator around the standing waves and it is overcome by a perturbation me... | [['we', 'study', 'analytically', 'and', 'numerically', 'the', 'stability', 'of', 'the', 'standing', 'waves', 'for', 'a', 'nonlinear', 'schrodinger', 'equation', 'with', 'a', 'point', 'defect', 'and', 'a', 'power', 'type', 'nonlinearity', 'a', 'main', 'difficulty', 'is', 'to', 'compute', 'the', 'number', 'of', 'negative... | [-0.18591439246301888, 0.1369670208289542, -0.08185612745000981, 0.09618262325635772, -0.04994867320585234, -0.15633231131307018, 0.04668244844916361, 0.29290401487907564, -0.27846596159294923, -0.20484210731228814, 0.13284784596511268, -0.27248983175840374, -0.16126022180436517, 0.16328345269589176, 0.0278455219866538... |
707.2492 | Structural transformations of double-walled carbon nanotube bundle under
hydrostatic pressure | Three kinds of the response mechanisms to the external pressure have been
found for double-walled carbon nanotube (DWNT) bundle, depending strongly on
their average radius and symmetry. The small-diameter DWNT bundle undergoes a
small discontinuous volume change, and then deform continuously. The
intermediate-diamete... | cond-mat.mtrl-sci | three kinds of the response mechanisms to the external pressure have been found for doublewalled carbon nanotube dwnt bundle depending strongly on their average radius and symmetry the smalldiameter dwnt bundle undergoes a small discontinuous volume change and then deform continuously the intermediatediameter dwnt bund... | [['three', 'kinds', 'of', 'the', 'response', 'mechanisms', 'to', 'the', 'external', 'pressure', 'have', 'been', 'found', 'for', 'doublewalled', 'carbon', 'nanotube', 'dwnt', 'bundle', 'depending', 'strongly', 'on', 'their', 'average', 'radius', 'and', 'symmetry', 'the', 'smalldiameter', 'dwnt', 'bundle', 'undergoes', '... | [-0.19834520513541065, 0.21394703259769207, -0.06199568137041448, -0.022200957871973515, -0.0680930399588154, -0.1855125602063102, 0.03163752277517536, 0.47385139868129045, -0.2591372105865351, -0.24557795722406203, 0.10319576354231685, -0.25146907278879854, -0.16176291501081627, 0.10438295379572082, 0.0260424199999154... |
707.2493 | Inclusive semileptonic B decays and the determination of |V_ub| | We study the triple differential distribution of B-> Xu l nu, consistently
including all perturbative and non-perturbative effects through O(alphas^2
beta_0) and O(1/mb^3). The Fermi motion is parameterized in terms of a single
light-cone function for each structure function and for any value of q^2,
accounting for a... | hep-ph | we study the triple differential distribution of b xu l nu consistently including all perturbative and nonperturbative effects through oalphas2 beta_0 and o1mb3 the fermi motion is parameterized in terms of a single lightcone function for each structure function and for any value of q2 accounting for all subleading eff... | [['we', 'study', 'the', 'triple', 'differential', 'distribution', 'of', 'b', 'xu', 'l', 'nu', 'consistently', 'including', 'all', 'perturbative', 'and', 'nonperturbative', 'effects', 'through', 'oalphas2', 'beta_0', 'and', 'o1mb3', 'the', 'fermi', 'motion', 'is', 'parameterized', 'in', 'terms', 'of', 'a', 'single', 'li... | [-0.10231606536587977, 0.10507120135999112, -0.095229977681474, 0.09143230214464927, -0.07382451537651596, -0.0907094693803056, 0.08340016451310711, 0.32899277026040685, -0.24008518653594096, -0.2927462639269867, 0.03366252339091497, -0.30151949756502827, -0.061138779850336035, 0.18947610993334954, 0.00629061219957226,... |
707.2494 | The Achromatic Interfero Coronagraph | We report on the Achromatic Interfero Coronagraph, a focal imaging device
which aims at rejecting the energy contribution of a point-like source set
on-axis, so as to make detectable its angularly-close environment (applicable
to stellar environment: circumstellar matter, faint companions, planetary
systems, but also... | astro-ph | we report on the achromatic interfero coronagraph a focal imaging device which aims at rejecting the energy contribution of a pointlike source set onaxis so as to make detectable its angularlyclose environment applicable to stellar environment circumstellar matter faint companions planetary systems but also conceivably... | [['we', 'report', 'on', 'the', 'achromatic', 'interfero', 'coronagraph', 'a', 'focal', 'imaging', 'device', 'which', 'aims', 'at', 'rejecting', 'the', 'energy', 'contribution', 'of', 'a', 'pointlike', 'source', 'set', 'onaxis', 'so', 'as', 'to', 'make', 'detectable', 'its', 'angularlyclose', 'environment', 'applicable'... | [-0.09825154655248834, 0.0839793438962004, -0.10619644252046083, 0.09260178182907672, -0.15211502439976754, -0.12236485056555232, 0.07118850387035845, 0.3912382116780067, -0.18060455918879223, -0.3749608403752343, 0.09617125800174947, -0.2749711962504266, -0.09179869825498034, 0.22324990581434506, -0.10050660955051008,... |
707.2495 | Geometrical and electronic structures of the (5, 3) single-walled gold
nanotube from first-principles calculations | The geometrical and electronic structures of the 4 {\AA} diameter perfect and
deformed (5, 3) single-walled gold nanotube (SWGT) have been studied based upon
the density-functional theory in the local-density approximation (LDA). The
calculated relaxed geometries show clearly significant deviations from those of
the ... | cond-mat.mtrl-sci | the geometrical and electronic structures of the 4 aa diameter perfect and deformed 5 3 singlewalled gold nanotube swgt have been studied based upon the densityfunctional theory in the localdensity approximation lda the calculated relaxed geometries show clearly significant deviations from those of the ideally rolled t... | [['the', 'geometrical', 'and', 'electronic', 'structures', 'of', 'the', '4', 'aa', 'diameter', 'perfect', 'and', 'deformed', '5', '3', 'singlewalled', 'gold', 'nanotube', 'swgt', 'have', 'been', 'studied', 'based', 'upon', 'the', 'densityfunctional', 'theory', 'in', 'the', 'localdensity', 'approximation', 'lda', 'the',... | [-0.08171501018195634, 0.15073190689131263, -0.06839385399417508, 0.062487814808264375, 0.04731938670433703, -0.11443575178938252, 0.03402946165518924, 0.4163636611153682, -0.2552825217268297, -0.3113871474129458, -0.008343229288723143, -0.3141327189902465, -0.13811077250145554, 0.13357899130676829, 0.0428623981308192,... |
707.2496 | Tau anomalous magnetic moment form factor at Super B/Flavor factories | The proposed high-luminosity B/Flavor factories offer new opportunities for
the improved determination of the fundamental physical parameters of standard
heavy leptons. Compared to the electron or the muon case, the magnetic
properties of the $\tau$ lepton are largely unexplored. We show that the
electromagnetic prop... | hep-ph | the proposed highluminosity bflavor factories offer new opportunities for the improved determination of the fundamental physical parameters of standard heavy leptons compared to the electron or the muon case the magnetic properties of the tau lepton are largely unexplored we show that the electromagnetic properties of ... | [['the', 'proposed', 'highluminosity', 'bflavor', 'factories', 'offer', 'new', 'opportunities', 'for', 'the', 'improved', 'determination', 'of', 'the', 'fundamental', 'physical', 'parameters', 'of', 'standard', 'heavy', 'leptons', 'compared', 'to', 'the', 'electron', 'or', 'the', 'muon', 'case', 'the', 'magnetic', 'pro... | [-0.09955582359718392, 0.21317135600431356, -0.02248794859740883, 0.09432942087238189, -0.04762883370160125, -0.0925934407953173, 0.02708183720766101, 0.3653601464629173, -0.24650191647931932, -0.3280456382699776, 0.024947110055945812, -0.29768354463507424, 0.012052888527978211, 0.22109920455608517, 0.06839333408745006... |
707.2497 | A study of the ferromagnetic transition of $SrRuO_3$ in nanometer thick
bilayers with $YBa_2Cu_3O_y$, $La_{1.88}Sr_{0.12}CuO_{4-y}$, Au and Cr:
Signature of injected carriers in the pseudogap regime | The hypothesis regarding the existence of uncorrelated pre-formed pairs in
the pseudogap regime of superconducting $YBa_2Cu_3O_y$ is tested experimentally
using bilayers of $YBa_2Cu_3O_y$ and the itinerant ferromagnet $SrRuO_3$. In
our study, we monitor the influence of $YBa_2Cu_3O_y$ on $T_p$, the
ferromagnetic orde... | cond-mat.supr-con cond-mat.str-el | the hypothesis regarding the existence of uncorrelated preformed pairs in the pseudogap regime of superconducting yba_2cu_3o_y is tested experimentally using bilayers of yba_2cu_3o_y and the itinerant ferromagnet srruo_3 in our study we monitor the influence of yba_2cu_3o_y on t_p the ferromagnetic ordering temperature... | [['the', 'hypothesis', 'regarding', 'the', 'existence', 'of', 'uncorrelated', 'preformed', 'pairs', 'in', 'the', 'pseudogap', 'regime', 'of', 'superconducting', 'yba_2cu_3o_y', 'is', 'tested', 'experimentally', 'using', 'bilayers', 'of', 'yba_2cu_3o_y', 'and', 'the', 'itinerant', 'ferromagnet', 'srruo_3', 'in', 'our', ... | [-0.15391414111766677, 0.24725551440332755, -0.005950138801470017, 0.004933954762199368, 0.0038216675957067846, -0.16214109302904361, 0.10556129798269234, 0.4002274364274807, -0.239975698870153, -0.2874147672492724, -0.001347762425071918, -0.3861079948787124, -0.03510415771713433, 0.20823724896002274, 0.055773136590440... |
707.2498 | Subcritical dynamo bifurcation in the Taylor Green flow | We report direct numerical simulations of dynamo generation for flow
generated using a Taylor-Green forcing. We find that the bifurcation is
subcritical, and show its bifurcation diagram. We connect the associated
hysteretic behavior with hydrodynamics changes induced by the action of the
Lorentz force. We show the g... | physics.flu-dyn astro-ph | we report direct numerical simulations of dynamo generation for flow generated using a taylorgreen forcing we find that the bifurcation is subcritical and show its bifurcation diagram we connect the associated hysteretic behavior with hydrodynamics changes induced by the action of the lorentz force we show the geometry... | [['we', 'report', 'direct', 'numerical', 'simulations', 'of', 'dynamo', 'generation', 'for', 'flow', 'generated', 'using', 'a', 'taylorgreen', 'forcing', 'we', 'find', 'that', 'the', 'bifurcation', 'is', 'subcritical', 'and', 'show', 'its', 'bifurcation', 'diagram', 'we', 'connect', 'the', 'associated', 'hysteretic', '... | [-0.22135900957903393, 0.19550366190276075, -0.08615483822379734, 0.05187016244466141, -0.09720335328872774, -0.027185840781410814, -0.0075104234143304575, 0.34537375288110383, -0.3193862209306427, -0.26804312817017795, 0.09254423291488013, -0.2081817148095915, -0.22440471894330752, 0.23160145779363286, -0.005064962733... |
707.2499 | Invariance of the relativistic one-particle distribution function | The one-particle distribution function is of importance both in
non-relativistic and relativistic statistical physics. In the relativistic
framework, Lorentz invariance is possibly its most fundamental property. The
present article on the subject is a contrastive one: we review, discuss
critically, and, when necessar... | astro-ph | the oneparticle distribution function is of importance both in nonrelativistic and relativistic statistical physics in the relativistic framework lorentz invariance is possibly its most fundamental property the present article on the subject is a contrastive one we review discuss critically and when necessary complete ... | [['the', 'oneparticle', 'distribution', 'function', 'is', 'of', 'importance', 'both', 'in', 'nonrelativistic', 'and', 'relativistic', 'statistical', 'physics', 'in', 'the', 'relativistic', 'framework', 'lorentz', 'invariance', 'is', 'possibly', 'its', 'most', 'fundamental', 'property', 'the', 'present', 'article', 'on'... | [-0.06679762850570328, 0.1064453753734044, -0.10551118138976687, 0.12579664469961369, -0.06436818396197815, -0.09471696805135876, -0.030719589925937207, 0.3501686374930775, -0.2257821668126602, -0.24363034101677875, 0.04258887045423263, -0.25404252898970653, -0.1347321879447383, 0.15693351264823885, -0.0547904985244659... |
707.25 | Landen survey | Landen transformations are maps on the coefficients of an integral that
preserve its value. We present a brief survey of their appearnce in the
literature.
| math.CA | landen transformations are maps on the coefficients of an integral that preserve its value we present a brief survey of their appearnce in the literature | [['landen', 'transformations', 'are', 'maps', 'on', 'the', 'coefficients', 'of', 'an', 'integral', 'that', 'preserve', 'its', 'value', 'we', 'present', 'a', 'brief', 'survey', 'of', 'their', 'appearnce', 'in', 'the', 'literature']] | [-0.16283927105056742, -0.000768987708700782, -0.10673409137719621, 0.012888885646437606, -0.11136710441981752, 0.016035430676614244, 0.00024533736480710405, 0.42500936302045983, -0.2885435912758112, -0.21629677379193404, 0.19103391436995784, -0.33593328219528, -0.1808692361228168, 0.22033830607930818, -0.1036783003170... |
707.2501 | Single-walled carbon nanotube bundle under hydrostatic pressure studied
by the first-principles calculations | The structural, electronic, optical and vibrational properties of the
collapsed (10,10) single-walled carbon nanotube bundle under hydrostatic
pressure have been studied by the first-principles calculations. Some features
are observed in the present study: First, a collapsed structure is found, which
is distinct from... | cond-mat.mtrl-sci | the structural electronic optical and vibrational properties of the collapsed 1010 singlewalled carbon nanotube bundle under hydrostatic pressure have been studied by the firstprinciples calculations some features are observed in the present study first a collapsed structure is found which is distinct from both of the ... | [['the', 'structural', 'electronic', 'optical', 'and', 'vibrational', 'properties', 'of', 'the', 'collapsed', '1010', 'singlewalled', 'carbon', 'nanotube', 'bundle', 'under', 'hydrostatic', 'pressure', 'have', 'been', 'studied', 'by', 'the', 'firstprinciples', 'calculations', 'some', 'features', 'are', 'observed', 'in'... | [-0.15131009505946458, 0.15487033325834343, -0.09291421784299243, 0.02800825280713436, -0.041012178938451806, -0.07500238258862081, 0.03846898061204126, 0.47552889908097457, -0.2788988878355198, -0.28359792834704683, 0.03874295521119475, -0.2508468547279073, -0.1412662381171873, 0.13449800914854348, 0.06621140310752023... |
707.2502 | Electronic and Transport Properties of Radially Deformed Double-walled
Carbon Nanotube Intramolecular Junction | The electronic and transport property of a radially deformed double-walled
carbon nanotube (DWNT) intramolecular junction (IMJ) has been studied by the
tight-binding (TB) model combined with the first-principle calculations. The
geometrical structures of the DWNT IMJ have been first optimized in energy by
the univers... | cond-mat.mtrl-sci | the electronic and transport property of a radially deformed doublewalled carbon nanotube dwnt intramolecular junction imj has been studied by the tightbinding tb model combined with the firstprinciple calculations the geometrical structures of the dwnt imj have been first optimized in energy by the universal force fie... | [['the', 'electronic', 'and', 'transport', 'property', 'of', 'a', 'radially', 'deformed', 'doublewalled', 'carbon', 'nanotube', 'dwnt', 'intramolecular', 'junction', 'imj', 'has', 'been', 'studied', 'by', 'the', 'tightbinding', 'tb', 'model', 'combined', 'with', 'the', 'firstprinciple', 'calculations', 'the', 'geometri... | [-0.15724222119828102, 0.13386176105811515, -0.0691023724285691, 0.00814151773602813, 0.014032010929033494, -0.18095160294463164, 0.029366715251704426, 0.43298105393717096, -0.21202567094978667, -0.25068578456090623, 0.01844984458137387, -0.28216832424444493, -0.13735690357775163, 0.17528536120332333, 0.009761590585321... |
707.2503 | Intergrowth and thermoelectric properties in the Bi-Ca-Co-O system | Single crystals of the Bi-Ca-Co-O system have been grown using the flux
method with cooling from 900$\celsius$ and 950$\celsius$, respectively. The
single crystals are characterized by transmission electron microscopy and X-ray
diffraction. The misfit cobaltite
[Ca$_2$Bi$_{1.4}$Co$_{0.6}$O$_4$]$^{RS}$[CoO$_2$]$_{1.69... | cond-mat.mtrl-sci cond-mat.str-el | single crystals of the bicacoo system have been grown using the flux method with cooling from 900celsius and 950celsius respectively the single crystals are characterized by transmission electron microscopy and xray diffraction the misfit cobaltite ca_2bi_14co_06o_4rscoo_2_169 single crystals with quadruple n4 rocksalt... | [['single', 'crystals', 'of', 'the', 'bicacoo', 'system', 'have', 'been', 'grown', 'using', 'the', 'flux', 'method', 'with', 'cooling', 'from', '900celsius', 'and', '950celsius', 'respectively', 'the', 'single', 'crystals', 'are', 'characterized', 'by', 'transmission', 'electron', 'microscopy', 'and', 'xray', 'diffract... | [-0.11243394292771407, 0.18914006344563916, 0.02447946941044284, -0.12020251925376782, 0.0010365605174879962, -0.2397323107611764, 0.07995518097822733, 0.4425001362458282, -0.26324206079706686, -0.33413525587033244, 0.03013989466686793, -0.362789467558128, -0.08112172662588092, 0.21599306510505054, 0.029257814361448954... |
707.2504 | $B\to K$ Transition Form Factor up to ${\cal O}(1/m^2_b)$ within the
$k_T$ Factorization Approach | In the paper, we apply the $k_T$ factorization approach to deal with the
$B\to K$ transition form factor $F^{B\to K}_{+,0}(q^2)$ in the large recoil
regions. The B-meson wave functions $\Psi_B$ and $\bar\Psi_B$ that include the
three-particle Fock states' contributions are adopted to give a consistent PQCD
analysis o... | hep-ph | in the paper we apply the k_t factorization approach to deal with the bto k transition form factor fbto k_0q2 in the large recoil regions the bmeson wave functions psi_b and barpsi_b that include the threeparticle fock states contributions are adopted to give a consistent pqcd analysis of the form factor up to cal o 1m... | [['in', 'the', 'paper', 'we', 'apply', 'the', 'k_t', 'factorization', 'approach', 'to', 'deal', 'with', 'the', 'bto', 'k', 'transition', 'form', 'factor', 'fbto', 'k_0q2', 'in', 'the', 'large', 'recoil', 'regions', 'the', 'bmeson', 'wave', 'functions', 'psi_b', 'and', 'barpsi_b', 'that', 'include', 'the', 'threeparticl... | [-0.080917220559822, 0.1852271484101858, -0.09697768086693997, 0.10670881517401057, -0.05839321995154023, -0.06107317363659357, 0.01882121979509032, 0.3420923027543374, -0.20674617196444744, -0.21792022209832973, 0.002024182359929438, -0.3110609602234844, -0.09598414416505414, 0.14664188995353739, 0.059963209703036466,... |
707.2505 | Primitive Divisors in Arithmetic Dynamics | Let F(z) be a rational function in Q(z) of degree at least 2 with F(0) = 0
and such that F does not vanish to order d at 0. Let b be a rational number
having infinite orbit under iteration of F, and write F^n(b) = A_n/B_n as a
fraction in lowest terms. We prove that for all but finitely many n > 0, the
numerator A_n ... | math.NT math.DS | let fz be a rational function in qz of degree at least 2 with f0 0 and such that f does not vanish to order d at 0 let b be a rational number having infinite orbit under iteration of f and write fnb a_nb_n as a fraction in lowest terms we prove that for all but finitely many n 0 the numerator a_n has a primitive diviso... | [['let', 'fz', 'be', 'a', 'rational', 'function', 'in', 'qz', 'of', 'degree', 'at', 'least', '2', 'with', 'f0', '0', 'and', 'such', 'that', 'f', 'does', 'not', 'vanish', 'to', 'order', 'd', 'at', '0', 'let', 'b', 'be', 'a', 'rational', 'number', 'having', 'infinite', 'orbit', 'under', 'iteration', 'of', 'f', 'and', 'wr... | [-0.23368184350900784, 0.14085161885213893, -0.07535568407287688, -0.0179170820390157, -0.04377068107506992, -0.23732233151011833, 0.012443456676140028, 0.3105185453678132, -0.30863793558507624, -0.20470306249002793, 0.03196902218665595, -0.29092575928994585, -0.09283903804524536, 0.17540651796818046, -0.04051883527738... |
707.2506 | Mixed Integer Linear Programming For Exact Finite-Horizon Planning In
Decentralized Pomdps | We consider the problem of finding an n-agent joint-policy for the optimal
finite-horizon control of a decentralized Pomdp (Dec-Pomdp). This is a problem
of very high complexity (NEXP-hard in n >= 2). In this paper, we propose a new
mathematical programming approach for the problem. Our approach is based on two
ideas... | cs.AI | we consider the problem of finding an nagent jointpolicy for the optimal finitehorizon control of a decentralized pomdp decpomdp this is a problem of very high complexity nexphard in n 2 in this paper we propose a new mathematical programming approach for the problem our approach is based on two ideas first we represen... | [['we', 'consider', 'the', 'problem', 'of', 'finding', 'an', 'nagent', 'jointpolicy', 'for', 'the', 'optimal', 'finitehorizon', 'control', 'of', 'a', 'decentralized', 'pomdp', 'decpomdp', 'this', 'is', 'a', 'problem', 'of', 'very', 'high', 'complexity', 'nexphard', 'in', 'n', '2', 'in', 'this', 'paper', 'we', 'propose'... | [-0.09702977784099462, -0.026949365681593354, -0.0797228764479413, 0.06921361896617234, -0.12464265097568956, -0.178914453935526, 0.06025875400338229, 0.3592660861112964, -0.3183531850008424, -0.34617498279867337, 0.15047450484172875, -0.20295864404092387, -0.15599772478280277, 0.20734540306130042, -0.10934687143781725... |
707.2507 | Surface oscillations in channeled snow flows | An experimental device has been built to measure velocity profiles and
friction laws in channeled snow flows. The measurements show that the velocity
depends linearly on the vertical position in the flow and that the friction
coefficient is a first-order polynomial in velocity (u) and thickness (h) of
the flow. In al... | physics.class-ph | an experimental device has been built to measure velocity profiles and friction laws in channeled snow flows the measurements show that the velocity depends linearly on the vertical position in the flow and that the friction coefficient is a firstorder polynomial in velocity u and thickness h of the flow in all flows o... | [['an', 'experimental', 'device', 'has', 'been', 'built', 'to', 'measure', 'velocity', 'profiles', 'and', 'friction', 'laws', 'in', 'channeled', 'snow', 'flows', 'the', 'measurements', 'show', 'that', 'the', 'velocity', 'depends', 'linearly', 'on', 'the', 'vertical', 'position', 'in', 'the', 'flow', 'and', 'that', 'the... | [-0.15427531765201707, 0.15188490556565562, -0.09289335884196452, -0.015850585008046158, -0.008495685008348398, -0.07879220269729986, -0.014254783129633793, 0.34789854823763855, -0.30742871796931415, -0.2816624065596318, 0.09457892013235882, -0.2908083469381714, -0.0715049433649755, 0.2247792717519831, -0.0104000835338... |
707.2508 | Analysis of the SN1987A two-stage explosion hypothesis with account for
the MSW neutrino flavour conversion | Detection of 5 events by the Liquid Scintillation Detector (LSD) on February,
23, 1987 was interpreted in the literature as the detection of neutrinos from
the first stage of the two-stage supernova collapse. We pose rigid constraints
on the properties of the first stage of the collapse, taking into account
neutrino ... | astro-ph | detection of 5 events by the liquid scintillation detector lsd on february 23 1987 was interpreted in the literature as the detection of neutrinos from the first stage of the twostage supernova collapse we pose rigid constraints on the properties of the first stage of the collapse taking into account neutrino flavour c... | [['detection', 'of', '5', 'events', 'by', 'the', 'liquid', 'scintillation', 'detector', 'lsd', 'on', 'february', '23', '1987', 'was', 'interpreted', 'in', 'the', 'literature', 'as', 'the', 'detection', 'of', 'neutrinos', 'from', 'the', 'first', 'stage', 'of', 'the', 'twostage', 'supernova', 'collapse', 'we', 'pose', 'r... | [-0.05670744497451539, 0.17591263992270748, -0.01601641181562292, 0.12640213927156047, -0.07765923941654987, -0.07217342609319051, 0.05406200341684254, 0.29040690065410574, -0.21087959942126058, -0.3565707855465773, 0.1185167326674625, -0.26675748806079164, -0.035467516220370796, 0.14721218574069148, 0.0080838206126109... |
707.2509 | Tomography for amplitudes of hard exclusive processes | We discuss which part of information about hadron structure encoded in the
Generalized Parton Distributions (GPDs) [part of total GPD image] can be
restored from the known amplitude of a hard exclusive process. The physics
content of this partial image is analyzed. Among other things, we show that
this partial image ... | hep-ph hep-ex nucl-ex | we discuss which part of information about hadron structure encoded in the generalized parton distributions gpds part of total gpd image can be restored from the known amplitude of a hard exclusive process the physics content of this partial image is analyzed among other things we show that this partial image contains ... | [['we', 'discuss', 'which', 'part', 'of', 'information', 'about', 'hadron', 'structure', 'encoded', 'in', 'the', 'generalized', 'parton', 'distributions', 'gpds', 'part', 'of', 'total', 'gpd', 'image', 'can', 'be', 'restored', 'from', 'the', 'known', 'amplitude', 'of', 'a', 'hard', 'exclusive', 'process', 'the', 'physi... | [-0.06765444774293539, 0.11961731724523365, -0.1369109550829638, 0.1461878695280382, -0.15079969220390224, -0.06454721521680253, 0.006299286699181216, 0.3450380274743745, -0.29512232884463635, -0.23413355087842605, 0.05847474668678273, -0.3083831401532422, -0.09668934005171512, 0.12246083296985939, -0.03169194268382559... |
707.251 | Radiative gravitino decays from R-parity violation | We study radiative gravitino decay within the framework of R-violating
supersymmetry. For trilinear R-violating couplings that involve the third
generation of fermions, or for light gravitinos, we find that the radiative
loop-decay $\tilde{G} \to \gamma \nu$ dominates over the tree-level ones for a
wide set of parame... | hep-ph | we study radiative gravitino decay within the framework of rviolating supersymmetry for trilinear rviolating couplings that involve the third generation of fermions or for light gravitinos we find that the radiative loopdecay tildeg to gamma nu dominates over the treelevel ones for a wide set of parameters we calculate... | [['we', 'study', 'radiative', 'gravitino', 'decay', 'within', 'the', 'framework', 'of', 'rviolating', 'supersymmetry', 'for', 'trilinear', 'rviolating', 'couplings', 'that', 'involve', 'the', 'third', 'generation', 'of', 'fermions', 'or', 'for', 'light', 'gravitinos', 'we', 'find', 'that', 'the', 'radiative', 'loopdeca... | [-0.10905888413869869, 0.25141966219588713, -0.03489397196854289, 0.20329934525563642, -0.10464150524228341, -0.13801688072900917, 0.028315660311957938, 0.32269278962400044, -0.23539540983803636, -0.2911217593764131, 0.0575192226076012, -0.2589160578979834, -0.02001320571756108, 0.20328851684147642, 0.08279770705639175... |
707.2511 | Symmetries of perturbed conformal field theories | The symmetries of perturbed conformal field theories are analysed. We explain
which generators of the chiral algebras of a bulk theory survive a perturbation
by an exactly marginal bulk field. We also study the behaviour of D-branes
under current-current bulk deformations. We find that the branes always
continue to p... | hep-th | the symmetries of perturbed conformal field theories are analysed we explain which generators of the chiral algebras of a bulk theory survive a perturbation by an exactly marginal bulk field we also study the behaviour of dbranes under currentcurrent bulk deformations we find that the branes always continue to preserve... | [['the', 'symmetries', 'of', 'perturbed', 'conformal', 'field', 'theories', 'are', 'analysed', 'we', 'explain', 'which', 'generators', 'of', 'the', 'chiral', 'algebras', 'of', 'a', 'bulk', 'theory', 'survive', 'a', 'perturbation', 'by', 'an', 'exactly', 'marginal', 'bulk', 'field', 'we', 'also', 'study', 'the', 'behavi... | [-0.13482637678766074, 0.19022483621494543, -0.06777488438631682, 0.11591343148474527, -0.05687658839366015, -0.13689528436345214, -0.04480515447417822, 0.36057461762033843, -0.22173789134796928, -0.25000100127037833, 0.11778392358820008, -0.2734823886277702, -0.18603431762689177, 0.10101123222095125, -0.10082338851027... |
707.2512 | Generalized Neighbor-Interaction Models Induced by Nonlinear Lattices | It is shown that the tight-binding approximation of the nonlinear
Schr\"odinger equation with a periodic linear potential and periodic in space
nonlinearity coefficient gives rise to a number of nonlinear lattices with
complex, both linear and nonlinear, neighbor interactions. The obtained
lattices present non-standa... | cond-mat.other nlin.PS | it is shown that the tightbinding approximation of the nonlinear schrodinger equation with a periodic linear potential and periodic in space nonlinearity coefficient gives rise to a number of nonlinear lattices with complex both linear and nonlinear neighbor interactions the obtained lattices present nonstandard possib... | [['it', 'is', 'shown', 'that', 'the', 'tightbinding', 'approximation', 'of', 'the', 'nonlinear', 'schrodinger', 'equation', 'with', 'a', 'periodic', 'linear', 'potential', 'and', 'periodic', 'in', 'space', 'nonlinearity', 'coefficient', 'gives', 'rise', 'to', 'a', 'number', 'of', 'nonlinear', 'lattices', 'with', 'compl... | [-0.16984008299060288, 0.09444874003225856, -0.0563223587542661, 0.06773574585373432, -0.11118464108617247, -0.151554060052149, -0.021252429262107318, 0.3347900558222571, -0.3184001576560347, -0.2142838640138507, 0.09564554882767286, -0.30218023307996034, -0.21937185653444866, 0.1862720169491418, 0.07384579087627809, 0... |
707.2513 | Time for pulse traversal through slabs of dispersive and negative
($\epsilon$, $\mu$) materials | The traversal times for an electromagnetic pulse traversing a slab of
dispersive and dissipative material with negative dielectric permittivity
($\epsilon$) and magnetic permeability ($\mu$) have been calculated by using
the average flow of electromagnetic energy in the medium. The effects of
bandwidth of the pulse a... | cond-mat.mtrl-sci cond-mat.other physics.optics | the traversal times for an electromagnetic pulse traversing a slab of dispersive and dissipative material with negative dielectric permittivity epsilon and magnetic permeability mu have been calculated by using the average flow of electromagnetic energy in the medium the effects of bandwidth of the pulse and dissipatio... | [['the', 'traversal', 'times', 'for', 'an', 'electromagnetic', 'pulse', 'traversing', 'a', 'slab', 'of', 'dispersive', 'and', 'dissipative', 'material', 'with', 'negative', 'dielectric', 'permittivity', 'epsilon', 'and', 'magnetic', 'permeability', 'mu', 'have', 'been', 'calculated', 'by', 'using', 'the', 'average', 'f... | [-0.18703427379509305, 0.2233187579022133, -0.032899196388135696, 0.007275298639901796, -0.04223585892107402, -0.12095096267909668, 0.02999788621205023, 0.4928543294041321, -0.2029236137556533, -0.30731979275561183, 0.050481479902666104, -0.272585465555379, -0.06452627925084498, 0.20007984692113068, 0.02306499168137623... |
707.2514 | Radiation-cooled Dew Water Condensers Studied by Computational Fluid
Dynamic (CFD) | Harvesting condensed atmospheric vapour as dew water can be an alternative or
complementary potable water resource in specific arid or insular areas. Such
radiation-cooled condensing devices use already existing flat surfaces (roofs)
or innovative structures with more complex shapes to enhance the dew yield. The
Comp... | physics.flu-dyn | harvesting condensed atmospheric vapour as dew water can be an alternative or complementary potable water resource in specific arid or insular areas such radiationcooled condensing devices use already existing flat surfaces roofs or innovative structures with more complex shapes to enhance the dew yield the computation... | [['harvesting', 'condensed', 'atmospheric', 'vapour', 'as', 'dew', 'water', 'can', 'be', 'an', 'alternative', 'or', 'complementary', 'potable', 'water', 'resource', 'in', 'specific', 'arid', 'or', 'insular', 'areas', 'such', 'radiationcooled', 'condensing', 'devices', 'use', 'already', 'existing', 'flat', 'surfaces', '... | [-0.0894478957433953, 0.12058547130865345, -0.02063536743925212, 0.054864527501119496, -0.04430698591991641, -0.18010661534383446, -0.017735476405610993, 0.3974895212969345, -0.21450936283599353, -0.3678313882275643, 0.13148719767935543, -0.28141818800747886, -0.06217099235420158, 0.23636013155037933, -0.08037297074447... |
707.2515 | Generic measures for hyperbolic flows on non compact spaces | We consider the geodesic flow on a complete connected negatively curved
manifold. We show that the set of invariant borel probability measures contains
a dense $G_\delta$-subset consisting of ergodic measures fully supported on the
non-wandering set. We also trat the case of non-positively curved manifolds and
provid... | math.DS | we consider the geodesic flow on a complete connected negatively curved manifold we show that the set of invariant borel probability measures contains a dense g_deltasubset consisting of ergodic measures fully supported on the nonwandering set we also trat the case of nonpositively curved manifolds and provide general ... | [['we', 'consider', 'the', 'geodesic', 'flow', 'on', 'a', 'complete', 'connected', 'negatively', 'curved', 'manifold', 'we', 'show', 'that', 'the', 'set', 'of', 'invariant', 'borel', 'probability', 'measures', 'contains', 'a', 'dense', 'g_deltasubset', 'consisting', 'of', 'ergodic', 'measures', 'fully', 'supported', 'o... | [-0.20552116588346267, 0.09972224986127562, -0.045252777309271325, 0.10952751083593619, -0.06758204750357229, -0.11040280847565125, -0.011578364248730634, 0.41374950019413964, -0.20150957946061043, -0.114072230856931, 0.09765743744445213, -0.3362117059398116, -0.14498242176252238, 0.21565849526801653, -0.20089778817144... |
707.2516 | Evolution of Massive Haloes in non-Gaussian Scenarios | We have performed high-resolution cosmological N-body simulations of a
concordance LCDM model to study the evolution of virialized, dark matter haloes
in the presence of primordial non-Gaussianity. Following a standard procedure,
departures from Gaussianity are modeled through a quadratic Gaussian term in
the primord... | astro-ph | we have performed highresolution cosmological nbody simulations of a concordance lcdm model to study the evolution of virialized dark matter haloes in the presence of primordial nongaussianity following a standard procedure departures from gaussianity are modeled through a quadratic gaussian term in the primordial grav... | [['we', 'have', 'performed', 'highresolution', 'cosmological', 'nbody', 'simulations', 'of', 'a', 'concordance', 'lcdm', 'model', 'to', 'study', 'the', 'evolution', 'of', 'virialized', 'dark', 'matter', 'haloes', 'in', 'the', 'presence', 'of', 'primordial', 'nongaussianity', 'following', 'a', 'standard', 'procedure', '... | [-0.1444673137494074, 0.0960397761353104, -0.12622059751999956, 0.156979663418261, -0.11485467897728086, -0.08471990397191365, -0.04831849182718778, 0.2803448289719031, -0.19193562440556922, -0.3387438950335814, -0.006793371137636887, -0.2544249161319048, -0.0891411729519152, 0.17153531271334807, 0.04848994500072742, 0... |
707.2517 | Sound velocity and absorption measurements under high pressure using
picosecond ultrasonics in diamond anvil cell. Application to the stability
study of AlPdMn | We report an innovative high pressure method combining the diamond anvil cell
device with the technique of picosecond ultrasonics. Such an approach allows to
accurately measure sound velocity and attenuation of solids and liquids under
pressure of tens of GPa, overcoming all the drawbacks of traditional
techniques. T... | cond-mat.mtrl-sci | we report an innovative high pressure method combining the diamond anvil cell device with the technique of picosecond ultrasonics such an approach allows to accurately measure sound velocity and attenuation of solids and liquids under pressure of tens of gpa overcoming all the drawbacks of traditional techniques the po... | [['we', 'report', 'an', 'innovative', 'high', 'pressure', 'method', 'combining', 'the', 'diamond', 'anvil', 'cell', 'device', 'with', 'the', 'technique', 'of', 'picosecond', 'ultrasonics', 'such', 'an', 'approach', 'allows', 'to', 'accurately', 'measure', 'sound', 'velocity', 'and', 'attenuation', 'of', 'solids', 'and'... | [-0.053086841099310035, 0.1519093206839256, -0.07733068880214192, -0.05457933237281556, -0.042975260602200735, -0.11142835903721039, 0.07978329881306682, 0.3949706103029551, -0.28963572365875523, -0.31670919580467266, 0.09603885092656128, -0.2740866049187068, -0.12762671875123702, 0.22825223240172765, -0.03124838228241... |
707.2518 | Positive and negative pressure effects on the magnetic ordering and the
Kondo effect in the compound Ce2RhSi3 | The competition between magnetic ordering and the Kondo effect in Ce2RhSi3,
ordering antiferromagnetically at 7 K, is investigated by the measurements of
magnetization, heat capacity and electrical resistivity on the solid solutions,
Ce(2-x)La(x)RhSi3, Ce(2-y)Y(y)RhSi3, and Ce2RhSi(3-z)Ge(z), as well as by high
press... | cond-mat.str-el cond-mat.mtrl-sci | the competition between magnetic ordering and the kondo effect in ce2rhsi3 ordering antiferromagnetically at 7 k is investigated by the measurements of magnetization heat capacity and electrical resistivity on the solid solutions ce2xlaxrhsi3 ce2yyyrhsi3 and ce2rhsi3zgez as well as by high pressure studies on this comp... | [['the', 'competition', 'between', 'magnetic', 'ordering', 'and', 'the', 'kondo', 'effect', 'in', 'ce2rhsi3', 'ordering', 'antiferromagnetically', 'at', '7', 'k', 'is', 'investigated', 'by', 'the', 'measurements', 'of', 'magnetization', 'heat', 'capacity', 'and', 'electrical', 'resistivity', 'on', 'the', 'solid', 'solu... | [-0.1474706062010296, 0.18411929252994563, -0.012958787214713838, -0.005422510756926506, -0.012474492210938753, -0.07506681183563932, 0.15139843104846495, 0.3601126454919928, -0.27399010969466475, -0.31533838321788693, 0.07044843074378013, -0.38080978882059735, -0.10572203020521281, 0.16263686407155376, 0.0575101731459... |
707.2519 | Gravitational Collapse to Toroidal and Higher Genus asymptotically AdS
Black Holes | We match collapsing inhomogeneous as well as spatially homogeneous but
anisotropic spacetimes to vacuum static exteriors with a negative cosmological
constant and planar or hyperbolic symmetry. The collapsing interiors include
the inhomogeneous solutions of Szekeres and of Barnes, which in turn include
the Lemaitre-T... | gr-qc astro-ph hep-th | we match collapsing inhomogeneous as well as spatially homogeneous but anisotropic spacetimes to vacuum static exteriors with a negative cosmological constant and planar or hyperbolic symmetry the collapsing interiors include the inhomogeneous solutions of szekeres and of barnes which in turn include the lemaitretolman... | [['we', 'match', 'collapsing', 'inhomogeneous', 'as', 'well', 'as', 'spatially', 'homogeneous', 'but', 'anisotropic', 'spacetimes', 'to', 'vacuum', 'static', 'exteriors', 'with', 'a', 'negative', 'cosmological', 'constant', 'and', 'planar', 'or', 'hyperbolic', 'symmetry', 'the', 'collapsing', 'interiors', 'include', 't... | [-0.1339760702217883, 0.14297336326209736, -0.04663285539775598, 0.1310886664651945, -0.14049913682287835, -0.14926563195701018, -0.07981184674579589, 0.30425942307490794, -0.12441380758632402, -0.2935786209695163, 0.13560168008839132, -0.26179991001797626, -0.07771026795027686, 0.11139291847796469, -0.0258800667542658... |
707.252 | Schwinger's Magnetic Model of Matter: Can It Help Us With Grand
Unification? | Many have argued that research on grand unification or local realistic
physics will not be truly relevant until it makes predictions verified by
experiment, different from the prediction of prior theory (the standard model).
This paper proposes a new strategy (and candidate Lagrangians) for such models;
that strategy... | physics.gen-ph physics.class-ph | many have argued that research on grand unification or local realistic physics will not be truly relevant until it makes predictions verified by experiment different from the prediction of prior theory the standard model this paper proposes a new strategy and candidate lagrangians for such models that strategy in turn ... | [['many', 'have', 'argued', 'that', 'research', 'on', 'grand', 'unification', 'or', 'local', 'realistic', 'physics', 'will', 'not', 'be', 'truly', 'relevant', 'until', 'it', 'makes', 'predictions', 'verified', 'by', 'experiment', 'different', 'from', 'the', 'prediction', 'of', 'prior', 'theory', 'the', 'standard', 'mod... | [-0.058836528886732756, 0.14721759556713926, -0.13028096324277988, 0.11140620777886771, -0.08841925141271478, -0.1857013522873304, 0.0641858101444086, 0.34431023539475386, -0.1900354283861816, -0.33236983911517787, 0.023052627140286323, -0.2671553618976545, -0.14524943554116523, 0.17052079722292118, -0.0058140407542369... |
707.2521 | Nonlinear viscoelastic dynamics of nano-confined water | The viscoelastic dynamics of nano-confined water is studied by means of
atomic force microscopy (AFM). We observe a nonlinear viscoelastic behavior
remarkably similar to that widely observed in metastable complex fluids. We
show that the origin of the measured nonlinear viscoelasticity in nano-confined
water is a str... | cond-mat.soft | the viscoelastic dynamics of nanoconfined water is studied by means of atomic force microscopy afm we observe a nonlinear viscoelastic behavior remarkably similar to that widely observed in metastable complex fluids we show that the origin of the measured nonlinear viscoelasticity in nanoconfined water is a strain rate... | [['the', 'viscoelastic', 'dynamics', 'of', 'nanoconfined', 'water', 'is', 'studied', 'by', 'means', 'of', 'atomic', 'force', 'microscopy', 'afm', 'we', 'observe', 'a', 'nonlinear', 'viscoelastic', 'behavior', 'remarkably', 'similar', 'to', 'that', 'widely', 'observed', 'in', 'metastable', 'complex', 'fluids', 'we', 'sh... | [-0.1455976265649159, 0.2328859077360813, -0.08062841989431936, 0.0018057049664733287, 0.0035868005384460536, -0.10468306779713914, -0.015878161736464332, 0.3782544712499153, -0.32692387773848997, -0.2627618532480285, 0.04441941624949917, -0.261489260144126, -0.15858589133275397, 0.1742753778252345, 0.07017071200258071... |
707.2522 | On embedding well-separable graphs | Call a simple graph $H$ of order $n$ well-separable, if by deleting a
separator set of size $o(n)$ the leftover will have components of size at most
$o(n)$. We prove, that bounded degree well-separable spanning subgraphs are
easy to embed: for every $\gamma >0$ and positive integer $\Delta$ there exists
an $n_0$ such... | math.CO | call a simple graph h of order n wellseparable if by deleting a separator set of size on the leftover will have components of size at most on we prove that bounded degree wellseparable spanning subgraphs are easy to embed for every gamma 0 and positive integer delta there exists an n_0 such that if nn_0 deltah le delta... | [['call', 'a', 'simple', 'graph', 'h', 'of', 'order', 'n', 'wellseparable', 'if', 'by', 'deleting', 'a', 'separator', 'set', 'of', 'size', 'on', 'the', 'leftover', 'will', 'have', 'components', 'of', 'size', 'at', 'most', 'on', 'we', 'prove', 'that', 'bounded', 'degree', 'wellseparable', 'spanning', 'subgraphs', 'are',... | [-0.17023513818061667, 0.1866779094355144, 0.0100031037104169, -0.02285598118446375, -0.07934566996991635, -0.16790240160924824, 0.07758550023856131, 0.4067434258366886, -0.2770938043494856, -0.296663222589383, 0.0695363059100744, -0.3485826712297766, -0.07522428681044595, 0.13530939952715448, -0.03869478568728817, -0.... |
707.2523 | Quarkonium production in coherent hadron-hadron interactions at the LHC | The photoproduction of quarkonium in coherent hadron-hadron (pp/pA/AA$)
interactions for LHC energies is an important tool to investigate the QCD
dynamics at high energies. In this paper we estimate the integrated cross
section and rapidity distribution for J/Psi and Upsilon production using the
Color Glass Condensat... | hep-ph | the photoproduction of quarkonium in coherent hadronhadron pppaaa interactions for lhc energies is an important tool to investigate the qcd dynamics at high energies in this paper we estimate the integrated cross section and rapidity distribution for jpsi and upsilon production using the color glass condensate cgc form... | [['the', 'photoproduction', 'of', 'quarkonium', 'in', 'coherent', 'hadronhadron', 'pppaaa', 'interactions', 'for', 'lhc', 'energies', 'is', 'an', 'important', 'tool', 'to', 'investigate', 'the', 'qcd', 'dynamics', 'at', 'high', 'energies', 'in', 'this', 'paper', 'we', 'estimate', 'the', 'integrated', 'cross', 'section'... | [-0.00971421145922726, 0.23448126029342392, -0.1968675924747783, 0.19179344165419776, 0.022831269022491243, -0.06580826416907329, -0.05983440922240594, 0.3999009107549985, -0.1802486067560191, -0.2014228512961713, -0.07116000461096447, -0.3224841470623182, 0.0652199056958558, 0.11311141561184611, 0.07694483404269531, 0... |
707.2524 | Search for New Physics in High Mass Electron-Positron Events in ppbar
Collisions at sqrt(s) = 1.96 TeV | We report the results of a search for a narrow resonance in electron-positron
events in the invariant mass range of 150-950 GeV/c^2 using 1.3 fb^-1 of ppbar
collision data at sqrt(s) = 1.96 TeV collected by the CDF II detector at
Fermilab. No significant evidence of such a resonance is observed and we
interpret the r... | hep-ex | we report the results of a search for a narrow resonance in electronpositron events in the invariant mass range of 150950 gevc2 using 13 fb1 of ppbar collision data at sqrts 196 tev collected by the cdf ii detector at fermilab no significant evidence of such a resonance is observed and we interpret the results to exclu... | [['we', 'report', 'the', 'results', 'of', 'a', 'search', 'for', 'a', 'narrow', 'resonance', 'in', 'electronpositron', 'events', 'in', 'the', 'invariant', 'mass', 'range', 'of', '150950', 'gevc2', 'using', '13', 'fb1', 'of', 'ppbar', 'collision', 'data', 'at', 'sqrts', '196', 'tev', 'collected', 'by', 'the', 'cdf', 'ii'... | [-0.05504117221712614, 0.21794934762698231, -0.011153213096537976, 0.17653647867252467, -0.04873094026639004, -0.10929075010929896, 0.08693949915844985, 0.31960971275288047, -0.05455139205988609, -0.40576569882757735, -0.0019430377534731772, -0.3742831524630839, 0.1370573793961243, 0.16471179207843362, 0.07635161162570... |
707.2525 | Tilings With Very Elastic Tiles | We consider tiles of some fixed size, with an associated weighting on the
shapes of tile, of total mass 1. We study the pressure, $p$, of tilings with
those tiles; the pressure, one over the volume times the logarithm of the
partition function. (The quantity we define as "pressure" could, perhaps
equally harmoniously... | math-ph math.MP | we consider tiles of some fixed size with an associated weighting on the shapes of tile of total mass 1 we study the pressure p of tilings with those tiles the pressure one over the volume times the logarithm of the partition function the quantity we define as pressure could perhaps equally harmoniously with physics no... | [['we', 'consider', 'tiles', 'of', 'some', 'fixed', 'size', 'with', 'an', 'associated', 'weighting', 'on', 'the', 'shapes', 'of', 'tile', 'of', 'total', 'mass', '1', 'we', 'study', 'the', 'pressure', 'p', 'of', 'tilings', 'with', 'those', 'tiles', 'the', 'pressure', 'one', 'over', 'the', 'volume', 'times', 'the', 'loga... | [-0.1135422929670404, 0.1291888020589469, -0.10477286958246955, 0.06152010271940732, -0.05810925495772734, -0.11422337674676387, 0.0471471349244539, 0.32837533013039977, -0.3094683505665019, -0.30166996655247685, 0.084250717150024, -0.28028981214236914, -0.08593176636748227, 0.15342887703464045, -0.118698466674618, 0.0... |
707.2526 | Heavy flavour production in ALICE | We review the most recent studies on the performance of ALICE in heavy
flavour production measurements in both hadronic and semileptonic decay
channels.
| hep-ex | we review the most recent studies on the performance of alice in heavy flavour production measurements in both hadronic and semileptonic decay channels | [['we', 'review', 'the', 'most', 'recent', 'studies', 'on', 'the', 'performance', 'of', 'alice', 'in', 'heavy', 'flavour', 'production', 'measurements', 'in', 'both', 'hadronic', 'and', 'semileptonic', 'decay', 'channels']] | [-0.08038930844960977, 0.23957731538330732, -0.032918243183066014, 0.05184636597076188, -0.005635244528884473, -0.16001080409826143, 0.03648129923512106, 0.3181747684012289, -0.1593429823456656, -0.17571582547996356, 0.0063047436389910136, -0.44460454421198886, 0.05882404060305461, 0.14705687955669736, 0.04379611178908... |
707.2527 | Rate and Power Allocation for Discrete-Rate Link Adaptation | Link adaptation, in particular adaptive coded modulation (ACM), is a
promising tool for bandwidth-efficient transmission in a fading environment.
The main motivation behind employing ACM schemes is to improve the spectral
efficiency of wireless communication systems. In this paper, using a finite
number of capacity a... | cs.IT math.IT | link adaptation in particular adaptive coded modulation acm is a promising tool for bandwidthefficient transmission in a fading environment the main motivation behind employing acm schemes is to improve the spectral efficiency of wireless communication systems in this paper using a finite number of capacity achieving c... | [['link', 'adaptation', 'in', 'particular', 'adaptive', 'coded', 'modulation', 'acm', 'is', 'a', 'promising', 'tool', 'for', 'bandwidthefficient', 'transmission', 'in', 'a', 'fading', 'environment', 'the', 'main', 'motivation', 'behind', 'employing', 'acm', 'schemes', 'is', 'to', 'improve', 'the', 'spectral', 'efficien... | [-0.20206464531440887, 0.03076611864680965, -0.03088056655420411, 0.002141726742153086, -0.0042649284020186435, -0.2534398244153107, 0.13717891383210137, 0.4034244041529394, -0.27264796429343763, -0.26723790553796495, 0.11257290591771203, -0.20154631677714566, -0.15395486624911428, 0.21250201779447736, -0.1491274245699... |
707.2528 | On the Feigel Effect: Extraction of Momentum from Vacuum? | The Green-function formalism for the electromagnetic field in a
magnetoelectric (ME) medium is constructed, as a generalization of conventional
Casimir theory. Zero temperature is assumed. It is shown how the formalism
predicts electromagnetic momentum to be extracted from the vacuum field, just
analogous to how ener... | quant-ph hep-th | the greenfunction formalism for the electromagnetic field in a magnetoelectric me medium is constructed as a generalization of conventional casimir theory zero temperature is assumed it is shown how the formalism predicts electromagnetic momentum to be extracted from the vacuum field just analogous to how energy is ext... | [['the', 'greenfunction', 'formalism', 'for', 'the', 'electromagnetic', 'field', 'in', 'a', 'magnetoelectric', 'me', 'medium', 'is', 'constructed', 'as', 'a', 'generalization', 'of', 'conventional', 'casimir', 'theory', 'zero', 'temperature', 'is', 'assumed', 'it', 'is', 'shown', 'how', 'the', 'formalism', 'predicts', ... | [-0.11130024664099633, 0.1896709297722745, -0.1006170411106791, 0.028995147189255978, -0.10190645597492144, -0.09981915489204715, 0.019229867803498616, 0.3389896244946519, -0.19988594351284136, -0.3158272665699021, -0.04668457024060538, -0.246153439168827, -0.19150266118312828, 0.19691588799251575, -0.02518924057622936... |
707.2529 | Decoherence of coupled electron spins via nuclear spin dynamics in
quantum dots | In double quantum dots, the exchange interaction between two electron spins
renormalizes the excitation energy of pair-flips in the nuclear spin bath,
which in turn modifies the non-Markovian bath dynamics. As the energy
renormalization varies with the Overhauser field mismatch between the quantum
dots, the electron ... | cond-mat.mes-hall | in double quantum dots the exchange interaction between two electron spins renormalizes the excitation energy of pairflips in the nuclear spin bath which in turn modifies the nonmarkovian bath dynamics as the energy renormalization varies with the overhauser field mismatch between the quantum dots the electron singlett... | [['in', 'double', 'quantum', 'dots', 'the', 'exchange', 'interaction', 'between', 'two', 'electron', 'spins', 'renormalizes', 'the', 'excitation', 'energy', 'of', 'pairflips', 'in', 'the', 'nuclear', 'spin', 'bath', 'which', 'in', 'turn', 'modifies', 'the', 'nonmarkovian', 'bath', 'dynamics', 'as', 'the', 'energy', 're... | [-0.11824304256222996, 0.30327502824951025, -0.07987029845917634, 0.06293163752279189, 0.08248379360199631, -0.1632334449848927, -0.0007867228602716589, 0.35796242698515746, -0.29056888271360565, -0.27289823070168495, -0.06025588432527786, -0.3130343226766141, -0.007241991878140206, 0.17858937074083323, 0.0629495884584... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.