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 |
|---|---|---|---|---|---|---|
707.193 | Improved Simulation of the Mass Charging for ASTROD I | The electrostatic charging of the test mass in ASTROD I (Astrodynamical Space
Test of Relativity using Optical Devices I) mission can affect the quality of
the science data as a result of spurious Coulomb and Lorentz forces. To
estimate the size of the resultant disturbances, credible predictions of
charging rates an... | astro-ph | the electrostatic charging of the test mass in astrod i astrodynamical space test of relativity using optical devices i mission can affect the quality of the science data as a result of spurious coulomb and lorentz forces to estimate the size of the resultant disturbances credible predictions of charging rates and the ... | [['the', 'electrostatic', 'charging', 'of', 'the', 'test', 'mass', 'in', 'astrod', 'i', 'astrodynamical', 'space', 'test', 'of', 'relativity', 'using', 'optical', 'devices', 'i', 'mission', 'can', 'affect', 'the', 'quality', 'of', 'the', 'science', 'data', 'as', 'a', 'result', 'of', 'spurious', 'coulomb', 'and', 'loren... | [-0.10567116226514646, 0.16232468511248604, -0.02418029251889202, 0.08056471894467662, -0.02301230100373476, -0.08980215858585508, 0.04685684920086759, 0.3640767769690768, -0.2420607413913082, -0.3930243692301177, 0.052207440363812106, -0.30026001694011206, -0.046309958392435346, 0.2062520577665189, -0.0719665424356906... |
707.1931 | Shear viscosity and Bose statistics: Capillary flow above lambda point | The gradual fall of the shear viscosity below 2.8K, observed in a liquid
helium 4 flowing through a capillary, is examined. The disappearance of the
shear viscosity in a capillary flow is a manifestation of superfluidity in
dissipative phenomena, the onset mechanism of which is a subtle problem
compared to that of su... | cond-mat.supr-con cond-mat.stat-mech | the gradual fall of the shear viscosity below 28k observed in a liquid helium 4 flowing through a capillary is examined the disappearance of the shear viscosity in a capillary flow is a manifestation of superfluidity in dissipative phenomena the onset mechanism of which is a subtle problem compared to that of superflui... | [['the', 'gradual', 'fall', 'of', 'the', 'shear', 'viscosity', 'below', '28k', 'observed', 'in', 'a', 'liquid', 'helium', '4', 'flowing', 'through', 'a', 'capillary', 'is', 'examined', 'the', 'disappearance', 'of', 'the', 'shear', 'viscosity', 'in', 'a', 'capillary', 'flow', 'is', 'a', 'manifestation', 'of', 'superflui... | [-0.16030598734288887, 0.23943834336830552, -0.1388403838587015, 0.038177668981167465, -0.038218299997403615, -0.0970434526782916, 0.04595141965072862, 0.26387701129627433, -0.29465216283881385, -0.23137196668797325, 0.049707801470013205, -0.3100055022814939, -0.10811256646763447, 0.14874343366340495, 0.037112576742981... |
707.1932 | Fokker-Planck type equations for a simple gas and for a
semi-relativistic Brownian motion from a relativistic kinetic theory | A covariant Fokker-Planck type equation for a simple gas and an equation for
the Brownian motion are derived from a relativistic kinetic theory based on the
Boltzmann equation. For the simple gas the dynamic friction four-vector and the
diffusion tensor are identified and written in terms of integrals which take
into... | cond-mat.stat-mech | a covariant fokkerplanck type equation for a simple gas and an equation for the brownian motion are derived from a relativistic kinetic theory based on the boltzmann equation for the simple gas the dynamic friction fourvector and the diffusion tensor are identified and written in terms of integrals which take into acco... | [['a', 'covariant', 'fokkerplanck', 'type', 'equation', 'for', 'a', 'simple', 'gas', 'and', 'an', 'equation', 'for', 'the', 'brownian', 'motion', 'are', 'derived', 'from', 'a', 'relativistic', 'kinetic', 'theory', 'based', 'on', 'the', 'boltzmann', 'equation', 'for', 'the', 'simple', 'gas', 'the', 'dynamic', 'friction'... | [-0.0996433898246924, 0.13698598653317853, -0.10139441360300834, 0.08622423385979112, -0.05402040380745306, -0.12239292306278687, -0.080483880693973, 0.29864649529303977, -0.25629002062193706, -0.22692056830733195, 0.019866023133637025, -0.27477816231506064, -0.06115598234971729, 0.19748799548988497, 0.0379109811806760... |
707.1933 | New attractor mechanism for spherically symmetric extremal black holes | We introduce a new attractor mechanism to find the entropy for spherically
symmetric extremal black holes. The key ingredient is to find a two-dimensional
(2D) dilaton gravity with the dilaton potential $V(\phi)$. The condition of an
attractor is given by $\nabla^2\phi=V(\phi_0)$ and
$\bar{R}_2=-V^{\prime}(\phi_0)$ a... | hep-th gr-qc | we introduce a new attractor mechanism to find the entropy for spherically symmetric extremal black holes the key ingredient is to find a twodimensional 2d dilaton gravity with the dilaton potential vphi the condition of an attractor is given by nabla2phivphi_0 and barr_2vprimephi_0 and for a constant dilaton phiphi_0 ... | [['we', 'introduce', 'a', 'new', 'attractor', 'mechanism', 'to', 'find', 'the', 'entropy', 'for', 'spherically', 'symmetric', 'extremal', 'black', 'holes', 'the', 'key', 'ingredient', 'is', 'to', 'find', 'a', 'twodimensional', '2d', 'dilaton', 'gravity', 'with', 'the', 'dilaton', 'potential', 'vphi', 'the', 'condition'... | [-0.12489371010476452, 0.0712449240101985, -0.07895478084444618, 0.10970809975336505, -0.07042456772496812, -0.2325996832173859, -0.02764465745825034, 0.23500568597203392, -0.19857684480281085, -0.2626629293951978, 0.06926226028157637, -0.32224387098422164, -0.13321584799032435, 0.1836556264748558, -0.0833781361579895,... |
707.1934 | On plate decompositions of cone multipliers | An important inequality due to Wolff on plate decompositions of cone
multipliers is known to have consequences for a variety of problems in harmonic
analysis. We observe that the range in Wolff's inequality, for the conic and
the spherical versions, can be improved by using bilinear restriction results.
We also use t... | math.CA | an important inequality due to wolff on plate decompositions of cone multipliers is known to have consequences for a variety of problems in harmonic analysis we observe that the range in wolffs inequality for the conic and the spherical versions can be improved by using bilinear restriction results we also use this ine... | [['an', 'important', 'inequality', 'due', 'to', 'wolff', 'on', 'plate', 'decompositions', 'of', 'cone', 'multipliers', 'is', 'known', 'to', 'have', 'consequences', 'for', 'a', 'variety', 'of', 'problems', 'in', 'harmonic', 'analysis', 'we', 'observe', 'that', 'the', 'range', 'in', 'wolffs', 'inequality', 'for', 'the', ... | [-0.08850295478034587, 0.0498192786709253, -0.0962214426780563, 0.08876462783415004, -0.08915144057911155, -0.1279621107969433, 0.0009468864910082803, 0.3437657049812731, -0.2910893512778871, -0.2472699566611222, 0.1889675784290635, -0.25489958352409303, -0.13500398316509313, 0.2693221657204309, -0.11621656789447159, 0... |
707.1935 | On the distillation and purification of phase-diffused squeezed states | Recently it was discovered that non-Gaussian decoherence processes, such as
phase-diffusion, can be counteracted by purification and distillation protocols
that are solely built on Gaussian operations. Here, we make use of this
experimentally highly accessible regime, and provide a detailed experimental
and theoretic... | quant-ph | recently it was discovered that nongaussian decoherence processes such as phasediffusion can be counteracted by purification and distillation protocols that are solely built on gaussian operations here we make use of this experimentally highly accessible regime and provide a detailed experimental and theoretical analys... | [['recently', 'it', 'was', 'discovered', 'that', 'nongaussian', 'decoherence', 'processes', 'such', 'as', 'phasediffusion', 'can', 'be', 'counteracted', 'by', 'purification', 'and', 'distillation', 'protocols', 'that', 'are', 'solely', 'built', 'on', 'gaussian', 'operations', 'here', 'we', 'make', 'use', 'of', 'this', ... | [-0.08151474924867644, 0.1709015262313187, -0.13542329511221718, 0.06628818514017279, 0.0012389490380883216, -0.18996406782637623, 0.11164660196313086, 0.3901672001708956, -0.23047521416755284, -0.2775023796575089, 0.1406602146816166, -0.23454033174716374, -0.12704829366548973, 0.26183781669858625, -0.03472348655957509... |
707.1936 | A reinterpretation of Emerton's $p$-adic Banach spaces | It is shown that the $p$-adic Banach spaces introduced by Emerton are
isomorphic to the cohomology groups of the sheaf of continuous $\Q_{p}$-valued
functions on a certain space. Some applications of this result are discussed.
| math.NT | it is shown that the padic banach spaces introduced by emerton are isomorphic to the cohomology groups of the sheaf of continuous q_pvalued functions on a certain space some applications of this result are discussed | [['it', 'is', 'shown', 'that', 'the', 'padic', 'banach', 'spaces', 'introduced', 'by', 'emerton', 'are', 'isomorphic', 'to', 'the', 'cohomology', 'groups', 'of', 'the', 'sheaf', 'of', 'continuous', 'q_pvalued', 'functions', 'on', 'a', 'certain', 'space', 'some', 'applications', 'of', 'this', 'result', 'are', 'discussed... | [-0.18567511063712813, 0.10089277322678004, -0.11187753096387229, 0.14020059306537458, -0.08623223943526254, -0.04778958883081727, -0.056339375017320406, 0.3757270743303439, -0.36372668044093776, -0.14750798736863277, 0.15053991025642438, -0.1831937694155118, -0.2078918925322154, 0.26209777127951384, -0.213995377505745... |
707.1937 | Figure rotation of dark halos in CDM simulations | We investigate the figure rotation of dark matter halos identified in Lambda
CDM simulations. We find that when strict criteria are used to select suitable
halos for study, 5 of the 222 halos identified in our z=0 simulation output
undergo coherent figure rotation over a 5h^{-1}Gyr period. We discuss the
effects of v... | astro-ph | we investigate the figure rotation of dark matter halos identified in lambda cdm simulations we find that when strict criteria are used to select suitable halos for study 5 of the 222 halos identified in our z0 simulation output undergo coherent figure rotation over a 5h1gyr period we discuss the effects of varying the... | [['we', 'investigate', 'the', 'figure', 'rotation', 'of', 'dark', 'matter', 'halos', 'identified', 'in', 'lambda', 'cdm', 'simulations', 'we', 'find', 'that', 'when', 'strict', 'criteria', 'are', 'used', 'to', 'select', 'suitable', 'halos', 'for', 'study', '5', 'of', 'the', '222', 'halos', 'identified', 'in', 'our', 'z... | [-0.15392335789233802, 0.15149164726691586, -0.1075789179830324, 0.11027638877775255, -0.08776354704002318, -0.05537682003341615, 0.030628005461767315, 0.4216897754796914, -0.2077892506118154, -0.36299016674027024, 0.05430946386020098, -0.23631887518692696, -0.0676420813659206, 0.23467783152258823, 0.007175994192117027... |
707.1938 | The Material Orientation Relationship for the BCC-HCP Transition | The dynamical model of forming of martensitic crystals for the bcc-hcp
transition is offered. It is shown that all macroscopic morphological
characters (the habit plane, the macroshear and the orientational relationship)
are expressed through elastic moduluses Cij of an initial bcc phase.
| cond-mat.mtrl-sci | the dynamical model of forming of martensitic crystals for the bcchcp transition is offered it is shown that all macroscopic morphological characters the habit plane the macroshear and the orientational relationship are expressed through elastic moduluses cij of an initial bcc phase | [['the', 'dynamical', 'model', 'of', 'forming', 'of', 'martensitic', 'crystals', 'for', 'the', 'bcchcp', 'transition', 'is', 'offered', 'it', 'is', 'shown', 'that', 'all', 'macroscopic', 'morphological', 'characters', 'the', 'habit', 'plane', 'the', 'macroshear', 'and', 'the', 'orientational', 'relationship', 'are', 'e... | [-0.17149476096674335, 0.2045741719120997, -0.08204415272921324, -0.017854167317273094, -0.055463527131360026, -0.054135026401490906, 0.02381905228830874, 0.40245431270450355, -0.31946453601121905, -0.22734354273416102, 0.03998058144934476, -0.3198142945766449, -0.19514509001164698, 0.10130790979019366, 0.0933122188318... |
707.1939 | The Schroedinger functional for Gross-Neveu models | Gross-Neveu type models with a finite number of fermion flavours are studied
on a two-dimensional Euclidean space-time lattice. The models are
asymptotically free and are invariant under a chiral symmetry. These
similarities to QCD make them perfect benchmark systems for fermion actions
used in large scale lattice QC... | hep-lat | grossneveu type models with a finite number of fermion flavours are studied on a twodimensional euclidean spacetime lattice the models are asymptotically free and are invariant under a chiral symmetry these similarities to qcd make them perfect benchmark systems for fermion actions used in large scale lattice qcd compu... | [['grossneveu', 'type', 'models', 'with', 'a', 'finite', 'number', 'of', 'fermion', 'flavours', 'are', 'studied', 'on', 'a', 'twodimensional', 'euclidean', 'spacetime', 'lattice', 'the', 'models', 'are', 'asymptotically', 'free', 'and', 'are', 'invariant', 'under', 'a', 'chiral', 'symmetry', 'these', 'similarities', 't... | [-0.1726718812819854, 0.22967576076916885, -0.047040414900266114, 0.11308717078964037, -0.05569393808400491, -0.14654117785994458, -0.00605457316146385, 0.34643674252947676, -0.18554366542957723, -0.2700886532475124, 0.07427974332813392, -0.30201987512919004, -0.12068581988660299, 0.08398906283764518, 0.050481576149422... |
707.194 | Hubble Space Telescope times-series photometry of the planetary transit
of HD189733: no moon, no rings, starspots | We monitored three transits of the giant gas planet around the nearby K dwarf
HD 189733 with the ACS camera on the Hubble Space Telescope. The resulting
very-high accuracy lightcurve (signal-to-noise ratio near 15000 on individual
measurements, 35000 on 10-minute averages) allows a direct geometric
measurement of the... | astro-ph | we monitored three transits of the giant gas planet around the nearby k dwarf hd 189733 with the acs camera on the hubble space telescope the resulting veryhigh accuracy lightcurve signaltonoise ratio near 15000 on individual measurements 35000 on 10minute averages allows a direct geometric measurement of the orbital i... | [['we', 'monitored', 'three', 'transits', 'of', 'the', 'giant', 'gas', 'planet', 'around', 'the', 'nearby', 'k', 'dwarf', 'hd', '189733', 'with', 'the', 'acs', 'camera', 'on', 'the', 'hubble', 'space', 'telescope', 'the', 'resulting', 'veryhigh', 'accuracy', 'lightcurve', 'signaltonoise', 'ratio', 'near', '15000', 'on'... | [-0.1503916018311149, 0.11171776756333808, -0.07990147666528057, 0.05087683601424289, -0.1010226406252537, -0.08927828289019182, 0.077965877045137, 0.36109688210850344, -0.1462457133407812, -0.38198439213805474, 0.10175271721867224, -0.3108419996974333, -0.04118256832783421, 0.19015793995334743, -0.09973358350973098, 0... |
707.1941 | Unifying inflation with LambdaCDM epoch in modified f(R) gravity
consistent with Solar System tests | We suggest two realistic f(R) and one F(G) modified gravities which are
consistent with local tests and cosmological bounds. The typical property of
such theories is the presence of the effective cosmological constant epochs in
such a way that early-time inflation and late-time cosmic acceleration are
naturally unifi... | hep-th astro-ph gr-qc | we suggest two realistic fr and one fg modified gravities which are consistent with local tests and cosmological bounds the typical property of such theories is the presence of the effective cosmological constant epochs in such a way that earlytime inflation and latetime cosmic acceleration are naturally unified within... | [['we', 'suggest', 'two', 'realistic', 'fr', 'and', 'one', 'fg', 'modified', 'gravities', 'which', 'are', 'consistent', 'with', 'local', 'tests', 'and', 'cosmological', 'bounds', 'the', 'typical', 'property', 'of', 'such', 'theories', 'is', 'the', 'presence', 'of', 'the', 'effective', 'cosmological', 'constant', 'epoch... | [-0.1365020229426546, 0.14747003959146915, -0.13345322942642932, 0.139845139094065, -0.12998234920985538, -0.20327711520992495, -0.05906075485953256, 0.32769442445391583, -0.23847893526616656, -0.30949582899978134, 0.05626731402137213, -0.22167830438249642, -0.15148282992757028, 0.18933268617781132, -0.0578358941740229... |
707.1942 | Inverse-Compton emission from the lobes of 3C353 | Analysis of the radio synchrotron and X-ray inverse-Compton emission from
radio-loud active galaxies allows us to determine their particle acceleration
processes and electron energy spectra. Previous studies have provided new
constraints on the total energy budget and particle content of powerful radio
galaxies and q... | astro-ph | analysis of the radio synchrotron and xray inversecompton emission from radioloud active galaxies allows us to determine their particle acceleration processes and electron energy spectra previous studies have provided new constraints on the total energy budget and particle content of powerful radio galaxies and quasars... | [['analysis', 'of', 'the', 'radio', 'synchrotron', 'and', 'xray', 'inversecompton', 'emission', 'from', 'radioloud', 'active', 'galaxies', 'allows', 'us', 'to', 'determine', 'their', 'particle', 'acceleration', 'processes', 'and', 'electron', 'energy', 'spectra', 'previous', 'studies', 'have', 'provided', 'new', 'const... | [-0.018929718830501468, 0.08592093274799278, -0.07922717034752066, 0.12561336629247913, -0.15319895919593465, -0.036346880715831906, 0.06413077722633413, 0.4793400599155575, -0.16170711472821292, -0.33224910726615536, 0.07219994073723986, -0.3383264513768154, 0.000871838083387249, 0.20617064531527124, 0.048459037457683... |
707.1943 | Analysis of the transverse effect of Einstein's gravitational waves | The investigation of the transverse effect of gravitational waves (GWs) could
constitute a further tool to discriminate among several relativistic theories
of gravity on the ground. After a review of the TT gauge, the transverse effect
of GWs arising by standard general relativity (called Einstein's GWs in this
paper... | gr-qc | the investigation of the transverse effect of gravitational waves gws could constitute a further tool to discriminate among several relativistic theories of gravity on the ground after a review of the tt gauge the transverse effect of gws arising by standard general relativity called einsteins gws in this paper is rean... | [['the', 'investigation', 'of', 'the', 'transverse', 'effect', 'of', 'gravitational', 'waves', 'gws', 'could', 'constitute', 'a', 'further', 'tool', 'to', 'discriminate', 'among', 'several', 'relativistic', 'theories', 'of', 'gravity', 'on', 'the', 'ground', 'after', 'a', 'review', 'of', 'the', 'tt', 'gauge', 'the', 't... | [-0.16507318187016942, 0.18201340374486205, -0.11661432175140962, 0.066552319546723, -0.1143507957586513, -0.05207967970366638, -0.04363485198080719, 0.33060363044040564, -0.24555829869538442, -0.267326418220792, 0.06639638525886699, -0.25078945908746664, -0.13051326119715406, 0.19195506431696827, 0.027472751016674173,... |
707.1944 | A comprehensive set of simulations studying the influence of gas
expulsion on star cluster evolution | We have carried out a large set of N-body simulations studying the effect of
residual-gas expulsion on the survival rate and final properties of star
clusters.
We have varied the star formation efficiency, gas expulsion timescale and
strength of the external tidal field, obtaining a three-dimensional grid of
models... | astro-ph | we have carried out a large set of nbody simulations studying the effect of residualgas expulsion on the survival rate and final properties of star clusters we have varied the star formation efficiency gas expulsion timescale and strength of the external tidal field obtaining a threedimensional grid of models which can... | [['we', 'have', 'carried', 'out', 'a', 'large', 'set', 'of', 'nbody', 'simulations', 'studying', 'the', 'effect', 'of', 'residualgas', 'expulsion', 'on', 'the', 'survival', 'rate', 'and', 'final', 'properties', 'of', 'star', 'clusters', 'we', 'have', 'varied', 'the', 'star', 'formation', 'efficiency', 'gas', 'expulsion... | [-0.10635385334842487, 0.16654919252783318, -0.07998636856904955, 0.07971307328293398, -0.053282468219880356, -0.02856218754197975, 0.05107300934176166, 0.3876483861147325, -0.20210832002869045, -0.373522358841678, 0.08794810195318403, -0.2578276755909125, -0.01703267669793041, 0.18518695458936105, 0.02511524535449488,... |
707.1945 | Effect of NUT parameter on the analytic extension of the Cauchy horizon
that develop in colliding wave spacetimes | The Cauchy horizon forming colliding wave solution due to Chandrasekhar and
Xanthopoulos (CX) has been generalized by inclusion of the NUT (Newman - Unti -
Tamburino) parameter. This is done by transforming the part of the inner
horizon region of a Kerr-Newman-NUT black hole into the space of colliding
waves. By taki... | gr-qc | the cauchy horizon forming colliding wave solution due to chandrasekhar and xanthopoulos cx has been generalized by inclusion of the nut newman unti tamburino parameter this is done by transforming the part of the inner horizon region of a kerrnewmannut black hole into the space of colliding waves by taking appropriate... | [['the', 'cauchy', 'horizon', 'forming', 'colliding', 'wave', 'solution', 'due', 'to', 'chandrasekhar', 'and', 'xanthopoulos', 'cx', 'has', 'been', 'generalized', 'by', 'inclusion', 'of', 'the', 'nut', 'newman', 'unti', 'tamburino', 'parameter', 'this', 'is', 'done', 'by', 'transforming', 'the', 'part', 'of', 'the', 'i... | [-0.17087803599936485, 0.0943272601339388, -0.07044588597160202, 0.08906770477288178, -0.12024494731830883, -0.10525086788703479, -0.008119806928303221, 0.27573129299482135, -0.19973666428443815, -0.241029813588629, 0.124087893345608, -0.2944660917103114, -0.10562860675894752, 0.18156700779870555, -0.017088589445408836... |
707.1946 | The uniqueness of the helicoid in the Lorentz-Minkowski space L3 | In this paper we deal with the uniqueness of the Lorentzian helicoid and
Enneper's surface among properly embedded maximal surfaces with lightlike
boundary of mirror symmetry in the Lorentz-Minkowski space L3.
| math.DG | in this paper we deal with the uniqueness of the lorentzian helicoid and ennepers surface among properly embedded maximal surfaces with lightlike boundary of mirror symmetry in the lorentzminkowski space l3 | [['in', 'this', 'paper', 'we', 'deal', 'with', 'the', 'uniqueness', 'of', 'the', 'lorentzian', 'helicoid', 'and', 'ennepers', 'surface', 'among', 'properly', 'embedded', 'maximal', 'surfaces', 'with', 'lightlike', 'boundary', 'of', 'mirror', 'symmetry', 'in', 'the', 'lorentzminkowski', 'space', 'l3']] | [-0.1806284133945742, 0.12870529735641134, -0.043865048837277196, 0.04554894168095122, -0.08168889690310724, -0.1480243008944296, -0.0707458859692598, 0.4191888519112141, -0.1871084939808615, -0.2351103005329928, 0.10445700646678527, -0.3205255272107259, -0.1570474934433737, 0.09265716084008736, -0.19711884990477213, 0... |
707.1947 | Conditions for entanglement transformation between a class of
multipartite pure states with generalized Schmidt decompositions | In this note we generalize Nielsen's marjoization criterion for the
convertibility of bipartite pure states [Phys. Rev. Lett \textbf{83},
436(1999)] to a special class of multipartite pure states which have
generalized Schmidt decompositions.
| quant-ph | in this note we generalize nielsens marjoization criterion for the convertibility of bipartite pure states phys rev lett textbf83 4361999 to a special class of multipartite pure states which have generalized schmidt decompositions | [['in', 'this', 'note', 'we', 'generalize', 'nielsens', 'marjoization', 'criterion', 'for', 'the', 'convertibility', 'of', 'bipartite', 'pure', 'states', 'phys', 'rev', 'lett', 'textbf83', '4361999', 'to', 'a', 'special', 'class', 'of', 'multipartite', 'pure', 'states', 'which', 'have', 'generalized', 'schmidt', 'decom... | [-0.07154660550276598, 0.1560804509527741, -0.08941091224551201, -0.07400688188405888, -0.03363040840673831, -0.16303284218414657, 0.10902906197213358, 0.2398080988937328, -0.10411853799896856, -0.26587207435119536, -0.05773237892501657, -0.2075977252510887, -0.1972136766078972, 0.1119483750794203, -0.22486052259562478... |
707.1948 | NO Curvatons or Hybrid Quintessential Inflation | We consider a curvaton scenario in which the late-time domination and the
generation of the curvature perturbation is achieved by a non-oscillatory (NO)
curvaton potential. Instead of considering the conventional curvaton
oscillation, we consider ``weak trapping'' after preheating, which modifies the
evolution of the... | hep-ph astro-ph hep-th | we consider a curvaton scenario in which the latetime domination and the generation of the curvature perturbation is achieved by a nonoscillatory no curvaton potential instead of considering the conventional curvaton oscillation we consider weak trapping after preheating which modifies the evolution of the curvaton den... | [['we', 'consider', 'a', 'curvaton', 'scenario', 'in', 'which', 'the', 'latetime', 'domination', 'and', 'the', 'generation', 'of', 'the', 'curvature', 'perturbation', 'is', 'achieved', 'by', 'a', 'nonoscillatory', 'no', 'curvaton', 'potential', 'instead', 'of', 'considering', 'the', 'conventional', 'curvaton', 'oscilla... | [-0.1738307141378045, 0.268206351279088, -0.09337505459410661, 0.126118174785494, -0.06843518481658, -0.11062108377199166, -0.0473349489940319, 0.26468644084454307, -0.2598429125813177, -0.26445766779162533, 0.07897826422590808, -0.2079184348939878, -0.08604712882817428, 0.1379716944449195, 0.01432188185749621, -0.0370... |
707.1949 | SUSY Search in Future Collider and Dark Matter Experiments | The lightest superparticle in the MSSM is expected to be a Bino, Higgsino or
Wino. We consider the dark matter abundance constraint on these LSP scenarios
in the minimal SUGRA and AMSB models. We discuss the resulting collider signals
for the Bino LSP at LHC and the Higgsino and Wino LSP at CLIC. The Bino,
Higgsino a... | hep-ph | the lightest superparticle in the mssm is expected to be a bino higgsino or wino we consider the dark matter abundance constraint on these lsp scenarios in the minimal sugra and amsb models we discuss the resulting collider signals for the bino lsp at lhc and the higgsino and wino lsp at clic the bino higgsino and wino... | [['the', 'lightest', 'superparticle', 'in', 'the', 'mssm', 'is', 'expected', 'to', 'be', 'a', 'bino', 'higgsino', 'or', 'wino', 'we', 'consider', 'the', 'dark', 'matter', 'abundance', 'constraint', 'on', 'these', 'lsp', 'scenarios', 'in', 'the', 'minimal', 'sugra', 'and', 'amsb', 'models', 'we', 'discuss', 'the', 'resu... | [-0.0818498122513389, 0.3368347532656274, -0.026283903817795676, 0.33488640376153966, -0.12801899156895363, -0.2791506340267298, -0.017976530827581882, 0.3406479030956779, -0.17618589967857173, -0.34533048083108886, 0.05956968984187201, -0.26534746890243743, 0.07180627716854675, 0.13086358462115405, -0.0133205173008235... |
707.195 | B\"acklund Transformation for the BC-Type Toda Lattice | We study an integrable case of n-particle Toda lattice: open chain with
boundary terms containing 4 parameters. For this model we construct a
B\"acklund transformation and prove its basic properties: canonicity,
commutativity and spectrality. The B\"acklund transformation can be also viewed
as a discretized time dyna... | nlin.SI math-ph math.MP | we study an integrable case of nparticle toda lattice open chain with boundary terms containing 4 parameters for this model we construct a backlund transformation and prove its basic properties canonicity commutativity and spectrality the backlund transformation can be also viewed as a discretized time dynamics two lax... | [['we', 'study', 'an', 'integrable', 'case', 'of', 'nparticle', 'toda', 'lattice', 'open', 'chain', 'with', 'boundary', 'terms', 'containing', '4', 'parameters', 'for', 'this', 'model', 'we', 'construct', 'a', 'backlund', 'transformation', 'and', 'prove', 'its', 'basic', 'properties', 'canonicity', 'commutativity', 'an... | [-0.16320246902864372, 0.10228781557295284, -0.04307423843376672, 0.10152599863784471, -0.0753262137000296, -0.2033778837214766, -0.0637090818039072, 0.3709561333074165, -0.3490174380339571, -0.2011285962662034, 0.15567124108158387, -0.28440551562651767, -0.17015124865765893, 0.11198855879535871, -0.04062871311082324, ... |
707.1951 | Binding energies and modelling of nuclei in semiclassical simulations | We study the binding energies of spin-isospin saturated nuclei with nucleon
number $8 \le A \le 100$ in semiclassical Monte Carlo many-body simulations.
The model Hamiltonian consists of, (i) nucleon kinetic energy, (ii) a
nucleon-nucleon interaction potential, and (iii) an effective Pauli potential
which depends on ... | nucl-th astro-ph | we study the binding energies of spinisospin saturated nuclei with nucleon number 8 le a le 100 in semiclassical monte carlo manybody simulations the model hamiltonian consists of i nucleon kinetic energy ii a nucleonnucleon interaction potential and iii an effective pauli potential which depends on density the basic i... | [['we', 'study', 'the', 'binding', 'energies', 'of', 'spinisospin', 'saturated', 'nuclei', 'with', 'nucleon', 'number', '8', 'le', 'a', 'le', '100', 'in', 'semiclassical', 'monte', 'carlo', 'manybody', 'simulations', 'the', 'model', 'hamiltonian', 'consists', 'of', 'i', 'nucleon', 'kinetic', 'energy', 'ii', 'a', 'nucle... | [-0.07955346756467693, 0.1736897846459126, -0.09780794635933257, 0.14273135576929366, 0.01584916518952109, -0.1181235826378198, 0.06112034302169835, 0.3470210177067639, -0.19386158528548658, -0.2890183550508735, -0.08032943747230434, -0.31969665776574074, -0.061569125063304225, 0.13954701263254465, 0.08854913038264652,... |
707.1952 | Existence of positive solutions for nonlinear systems | This paper deals with the existence of positive solutions for the nonlinear
system q(t)\phi(p(t)u'_{i}(t)))'+f^{i}(t,\textbf{u})=0,\quad 0<t<1,\quad
i=1,2,...,n. This system often arises in the study of positive radial solutions
of nonlinear elliptic system. Here $\textbf{u}=(u_{1},...,u_{n})$ and $f^{i},
i=1,2,...,n... | math.AP | this paper deals with the existence of positive solutions for the nonlinear system qtphiptu_itfittextbfu0quad 0t1quad i12n this system often arises in the study of positive radial solutions of nonlinear elliptic system here textbfuu_1u_n and fi i12n are continuous and nonnegative functions pt qthboxrm 01to 0oo are cont... | [['this', 'paper', 'deals', 'with', 'the', 'existence', 'of', 'positive', 'solutions', 'for', 'the', 'nonlinear', 'system', 'qtphiptu_itfittextbfu0quad', '0t1quad', 'i12n', 'this', 'system', 'often', 'arises', 'in', 'the', 'study', 'of', 'positive', 'radial', 'solutions', 'of', 'nonlinear', 'elliptic', 'system', 'here'... | [-0.20005898088789903, 0.04893110799244963, -0.04367678275761696, 0.03946690146560566, -0.04320477339295814, -0.15135261215126286, -0.038497122382530224, 0.3300519858701871, -0.28469386221124576, -0.1530086938578349, 0.16448766724206507, -0.3572029899805784, -0.16550231512922506, 0.1859445245614132, -0.0810945569967421... |
707.1953 | Effect of antiferromagnetic exchange interactions on the Glauber
dynamics of one-dimensional Ising models | We study the effect of antiferromagnetic interactions on the single spin-flip
Glauber dynamics of two different one-dimensional (1D) Ising models with spin
$\pm 1$. The first model is an Ising chain with antiferromagnetic exchange
interaction limited to nearest neighbors and subject to an oscillating magnetic
field. ... | cond-mat.mtrl-sci cond-mat.stat-mech | we study the effect of antiferromagnetic interactions on the single spinflip glauber dynamics of two different onedimensional 1d ising models with spin pm 1 the first model is an ising chain with antiferromagnetic exchange interaction limited to nearest neighbors and subject to an oscillating magnetic field the system ... | [['we', 'study', 'the', 'effect', 'of', 'antiferromagnetic', 'interactions', 'on', 'the', 'single', 'spinflip', 'glauber', 'dynamics', 'of', 'two', 'different', 'onedimensional', '1d', 'ising', 'models', 'with', 'spin', 'pm', '1', 'the', 'first', 'model', 'is', 'an', 'ising', 'chain', 'with', 'antiferromagnetic', 'exch... | [-0.21710181866552203, 0.2038269559787567, 0.0047876828109084234, 0.07343186369731915, -0.03912271482747288, -0.1873682075222622, 0.019345254418961857, 0.390887763926999, -0.2959203213236886, -0.2538689728729674, 0.023555079659570734, -0.3115328436377323, -0.05972205713406761, 0.11077268900546822, 0.1483525911300671, -... |
707.1954 | Bandlimited Field Reconstruction for Wireless Sensor Networks | Wireless sensor networks are often used for environmental monitoring
applications. In this context sampling and reconstruction of a physical field
is one of the most important problems to solve. We focus on a bandlimited field
and find under which conditions on the network topology the reconstruction of
the field is ... | cs.OH | wireless sensor networks are often used for environmental monitoring applications in this context sampling and reconstruction of a physical field is one of the most important problems to solve we focus on a bandlimited field and find under which conditions on the network topology the reconstruction of the field is succ... | [['wireless', 'sensor', 'networks', 'are', 'often', 'used', 'for', 'environmental', 'monitoring', 'applications', 'in', 'this', 'context', 'sampling', 'and', 'reconstruction', 'of', 'a', 'physical', 'field', 'is', 'one', 'of', 'the', 'most', 'important', 'problems', 'to', 'solve', 'we', 'focus', 'on', 'a', 'bandlimited... | [-0.14087149239113106, 0.06550719138688472, -0.0836938242668864, 0.06779228028207054, -0.04829436564087418, -0.11897710962461885, 0.012453477285754192, 0.3960180935482013, -0.24518173544141786, -0.3142031979860521, 0.15705657918869262, -0.20973350539911892, -0.1895715842697898, 0.18871936460571556, -0.11088763822496323... |
707.1955 | Strong convergence of modified Ishikawa iterations for nonlinear
mappings | In this paper, we prove a strong convergence theorem of modified Ishikawa
iterations for relatively asymptotically nonexpansive mappings in Banach space.
Our results extend and improve the recent results by Nakajo, Takahashi, Kim,
Xu, Matsushita and some others.
| math.FA | in this paper we prove a strong convergence theorem of modified ishikawa iterations for relatively asymptotically nonexpansive mappings in banach space our results extend and improve the recent results by nakajo takahashi kim xu matsushita and some others | [['in', 'this', 'paper', 'we', 'prove', 'a', 'strong', 'convergence', 'theorem', 'of', 'modified', 'ishikawa', 'iterations', 'for', 'relatively', 'asymptotically', 'nonexpansive', 'mappings', 'in', 'banach', 'space', 'our', 'results', 'extend', 'and', 'improve', 'the', 'recent', 'results', 'by', 'nakajo', 'takahashi', ... | [-0.09032366220914834, 0.038771682846787815, -0.07466542625145332, 0.08049482609006904, -0.052386827313819447, -0.13188823542834535, 0.13769704876530514, 0.3133561513009104, -0.23599596124817301, -0.19671544508152716, 0.09447518877710241, -0.26636481987362776, -0.2005751697799644, 0.2391067330813589, -0.254247783481873... |
707.1956 | Nonlinear coherent transport of waves in disordered media | We present a diagrammatic theory for coherent backscattering from disordered
dilute media in the nonlinear regime. The approach is non-perturbative in the
strength of the nonlinearity. We show that the coherent backscattering
enhancement factor is strongly affected by the nonlinearity, and corroborate
these results b... | cond-mat.mes-hall cond-mat.dis-nn | we present a diagrammatic theory for coherent backscattering from disordered dilute media in the nonlinear regime the approach is nonperturbative in the strength of the nonlinearity we show that the coherent backscattering enhancement factor is strongly affected by the nonlinearity and corroborate these results by nume... | [['we', 'present', 'a', 'diagrammatic', 'theory', 'for', 'coherent', 'backscattering', 'from', 'disordered', 'dilute', 'media', 'in', 'the', 'nonlinear', 'regime', 'the', 'approach', 'is', 'nonperturbative', 'in', 'the', 'strength', 'of', 'the', 'nonlinearity', 'we', 'show', 'that', 'the', 'coherent', 'backscattering',... | [-0.13820707083343425, 0.18972108640526938, -0.08450727710603839, 0.051298580672462575, -0.03862307903667291, -0.1107106134424814, -0.005132446873984817, 0.3812666261672146, -0.2876591058447957, -0.22104249159100517, 0.03370600506766803, -0.32341155575381386, -0.24296145801134925, 0.2459666721697431, 0.0350140537161173... |
707.1957 | Moveability and Collision Analysis for Fully-Parallel Manipulators | The aim of this paper is to characterize the moveability of fully-parallel
manipulators in the presence of obstacles. Fully parallel manipulators are used
in applications where accuracy, stiffness or high speeds and accelerations are
required \cite{Merlet:97}. However, one of its main drawbacks is a relatively
small ... | cs.RO | the aim of this paper is to characterize the moveability of fullyparallel manipulators in the presence of obstacles fully parallel manipulators are used in applications where accuracy stiffness or high speeds and accelerations are required citemerlet97 however one of its main drawbacks is a relatively small workspace c... | [['the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'characterize', 'the', 'moveability', 'of', 'fullyparallel', 'manipulators', 'in', 'the', 'presence', 'of', 'obstacles', 'fully', 'parallel', 'manipulators', 'are', 'used', 'in', 'applications', 'where', 'accuracy', 'stiffness', 'or', 'high', 'speeds', 'and', 'accelera... | [-0.17716397689420635, 0.0377477461050515, -0.057252663645517676, -0.016739497973755815, -0.09523716365073283, -0.09744286444038153, -0.02543479162111816, 0.34490015727131307, -0.26640153093999175, -0.3195210454844627, 0.13493017186978126, -0.22296149704699256, -0.12638468376141698, 0.1464807323371882, -0.1312253263098... |
707.1958 | Solutions for a class of iterated singular equations | Some fundamental solutions of radial type for a class of iterated elliptic
singular equations including the iterated Euler equation are given.
| math.AP | some fundamental solutions of radial type for a class of iterated elliptic singular equations including the iterated euler equation are given | [['some', 'fundamental', 'solutions', 'of', 'radial', 'type', 'for', 'a', 'class', 'of', 'iterated', 'elliptic', 'singular', 'equations', 'including', 'the', 'iterated', 'euler', 'equation', 'are', 'given']] | [-0.21928478378270352, 0.025554364458436056, -0.08606929952899615, 0.08497608590516306, -0.16781391549323285, -0.16417435090988874, -0.1364860473466771, 0.16066039264911697, -0.35337124055340174, -0.18172383397108033, 0.15439681774227038, -0.2865235175649148, -0.1533469068152564, 0.29809791470567387, -0.070305506033556... |
707.1959 | Logarithmic corrections in the aging of the fully-frustrated Ising model | We study the dynamics of the critical two-dimensional fully-frustrated Ising
model by means of Monte Carlo simulations. The dynamical exponent is estimated
at equilibrium and is shown to be compatible with the value $z_c=2$. In a
second step, the system is prepared in the paramagnetic phase and then quenched
at its c... | cond-mat.stat-mech | we study the dynamics of the critical twodimensional fullyfrustrated ising model by means of monte carlo simulations the dynamical exponent is estimated at equilibrium and is shown to be compatible with the value z_c2 in a second step the system is prepared in the paramagnetic phase and then quenched at its critical te... | [['we', 'study', 'the', 'dynamics', 'of', 'the', 'critical', 'twodimensional', 'fullyfrustrated', 'ising', 'model', 'by', 'means', 'of', 'monte', 'carlo', 'simulations', 'the', 'dynamical', 'exponent', 'is', 'estimated', 'at', 'equilibrium', 'and', 'is', 'shown', 'to', 'be', 'compatible', 'with', 'the', 'value', 'z_c2'... | [-0.11923986042342052, 0.20228483756888926, -0.09885772611926665, 0.07206176910741427, 0.060639432999881504, -0.1584197384720553, 0.03127542256345233, 0.3576304303174934, -0.26013820604949267, -0.24919627963075625, 0.1277693991510908, -0.3375752270605761, -0.09575829031089916, 0.18662971338093973, 0.05886647559356751, ... |
707.196 | A planar vacuum diode with electrons possessing velocity distribution
function | The current-voltage characteristic of a planar vacuum diode with electrons
possessing velocity distribution function during an emission from the cathode
(electron beam) is theoretically considered in this article. The electron beam
movement in the volume is examined. An integral-differential equation for the
electric... | physics.gen-ph physics.class-ph | the currentvoltage characteristic of a planar vacuum diode with electrons possessing velocity distribution function during an emission from the cathode electron beam is theoretically considered in this article the electron beam movement in the volume is examined an integraldifferential equation for the electric field p... | [['the', 'currentvoltage', 'characteristic', 'of', 'a', 'planar', 'vacuum', 'diode', 'with', 'electrons', 'possessing', 'velocity', 'distribution', 'function', 'during', 'an', 'emission', 'from', 'the', 'cathode', 'electron', 'beam', 'is', 'theoretically', 'considered', 'in', 'this', 'article', 'the', 'electron', 'beam... | [-0.13834617427274795, 0.1307140132580379, -0.11217294603546846, 0.018336155166124767, 0.009697397383795658, -0.13551488676121537, -0.02820589188748682, 0.38835846338893326, -0.24022701424612125, -0.2627754258123082, -0.06322672410743495, -0.2912397898313865, -0.03160559128917439, 0.22850267549412667, -0.00934619272888... |
707.1961 | Ergodic theory of amenable semigroup actions | In this paper, among other things, we state and prove the mean ergodic
theorem for amenable semigroup algebras.
| math.DS math.FA | in this paper among other things we state and prove the mean ergodic theorem for amenable semigroup algebras | [['in', 'this', 'paper', 'among', 'other', 'things', 'we', 'state', 'and', 'prove', 'the', 'mean', 'ergodic', 'theorem', 'for', 'amenable', 'semigroup', 'algebras']] | [-0.106770734820101, 0.11199823616900378, -0.09936824678960773, 0.13039610790373343, -0.06652252583040132, -0.15092802751395437, 0.07110656358741431, 0.3737170203692383, -0.39989393908116555, -0.11466129134512609, 0.1604042654378443, -0.3344731786702242, -0.15723865003221565, 0.2574769578253229, -0.20832844182021087, -... |
707.1962 | Some further remarks on good sets | We show that in n-fold cartesian product, n >= 4, a related component need
not be a full component. We also prove that when n >= 4, uniform boundedness of
lengths of geodesics is not a necessary condition for boundedness of solutions
of (1) for bounded function f.
| math.FA | we show that in nfold cartesian product n 4 a related component need not be a full component we also prove that when n 4 uniform boundedness of lengths of geodesics is not a necessary condition for boundedness of solutions of 1 for bounded function f | [['we', 'show', 'that', 'in', 'nfold', 'cartesian', 'product', 'n', '4', 'a', 'related', 'component', 'need', 'not', 'be', 'a', 'full', 'component', 'we', 'also', 'prove', 'that', 'when', 'n', '4', 'uniform', 'boundedness', 'of', 'lengths', 'of', 'geodesics', 'is', 'not', 'a', 'necessary', 'condition', 'for', 'boundedn... | [-0.18119818198940027, 0.14886064923611347, -0.05526118025021708, 0.06972712441600616, -0.05971483720223541, -0.11664103754067226, -0.023701329133473337, 0.3597890288447556, -0.2804183229075178, -0.20722547192227744, 0.15213485684438163, -0.2368270383702348, -0.12101696039873945, 0.17286690058308127, -0.040422801394015... |
707.1963 | Kauffman Boolean model in undirected scale free networks | We investigate analytically and numerically the critical line in undirected
random Boolean networks with arbitrary degree distributions, including
scale-free topology of connections $P(k)\sim k^{-\gamma}$. We show that in
infinite scale-free networks the transition between frozen and chaotic phase
occurs for $3<\gamm... | cond-mat.dis-nn cond-mat.stat-mech | we investigate analytically and numerically the critical line in undirected random boolean networks with arbitrary degree distributions including scalefree topology of connections pksim kgamma we show that in infinite scalefree networks the transition between frozen and chaotic phase occurs for 3gamma 35 the observatio... | [['we', 'investigate', 'analytically', 'and', 'numerically', 'the', 'critical', 'line', 'in', 'undirected', 'random', 'boolean', 'networks', 'with', 'arbitrary', 'degree', 'distributions', 'including', 'scalefree', 'topology', 'of', 'connections', 'pksim', 'kgamma', 'we', 'show', 'that', 'in', 'infinite', 'scalefree', ... | [-0.1781428834623916, 0.14975842013619614, -0.05097683115551869, 0.10379863763470591, -0.026714137600113947, -0.19476969173087533, 0.07339192157572445, 0.39291095006046817, -0.25157155397027964, -0.25135897943982854, 0.04238987619868971, -0.2796853930558427, -0.2688223029900756, 0.1698651124012637, 0.0079433412761192, ... |
707.1964 | Weighted composition operators on weighted Bergman spaces of bounded
symmetric domains | In this paper, we study the weighted compositon operators on weighted Bergman
spaces of bounded symmetric domains. The necessary and sufficient conditions
for a weighted composition operator $W_{\phi,\psi}$ to be bounded and compact
are studied by using the Carleson measure techniques. In the last section, we
study t... | math.FA math.OA | in this paper we study the weighted compositon operators on weighted bergman spaces of bounded symmetric domains the necessary and sufficient conditions for a weighted composition operator w_phipsi to be bounded and compact are studied by using the carleson measure techniques in the last section we study the schatten p... | [['in', 'this', 'paper', 'we', 'study', 'the', 'weighted', 'compositon', 'operators', 'on', 'weighted', 'bergman', 'spaces', 'of', 'bounded', 'symmetric', 'domains', 'the', 'necessary', 'and', 'sufficient', 'conditions', 'for', 'a', 'weighted', 'composition', 'operator', 'w_phipsi', 'to', 'be', 'bounded', 'and', 'compa... | [-0.0896015928729492, 0.12128400659718204, -0.015306397688155081, 0.15587224269641892, -0.05899275940222045, -0.017930498848870106, -0.002662633246669144, 0.41146622072247896, -0.3135157719108404, -0.16796966956234446, 0.17796035804420562, -0.24579661058298513, -0.14122383391448096, 0.17810881165239742, -0.154901288541... |
707.1965 | Network of inherent structures in spin glasses: scaling and scale-free
distributions | The local minima (inherent structures) of a system and their associated
transition links give rise to a network. Here we consider the topological and
distance properties of such a network in the context of spin glasses. We use
steepest descent dynamics, determining for each disorder sample the transition
links appear... | cond-mat.dis-nn cond-mat.stat-mech | the local minima inherent structures of a system and their associated transition links give rise to a network here we consider the topological and distance properties of such a network in the context of spin glasses we use steepest descent dynamics determining for each disorder sample the transition links appearing wit... | [['the', 'local', 'minima', 'inherent', 'structures', 'of', 'a', 'system', 'and', 'their', 'associated', 'transition', 'links', 'give', 'rise', 'to', 'a', 'network', 'here', 'we', 'consider', 'the', 'topological', 'and', 'distance', 'properties', 'of', 'such', 'a', 'network', 'in', 'the', 'context', 'of', 'spin', 'glas... | [-0.19477875857800245, 0.12792821349948644, -0.07208383102715016, 0.08565463315229863, -0.025033695137128234, -0.10110733272694052, 0.05513850162923336, 0.399844296887517, -0.31050567723438144, -0.2848603012561798, 0.05795074800401926, -0.2627226461023092, -0.21406375049054624, 0.11284205771237611, -0.00802754279598593... |
707.1966 | Infinite dimensional differential games with hybrid controls | A two-person zero-sum infinite dimensional differential game of infinite
duration with discounted payoff involving hybrid controls is studied. The
minimizing player is allowed to take continuous, switching and impulse controls
whereas the maximizing player is allowed to take continuous and switching
controls. By taki... | math.OC | a twoperson zerosum infinite dimensional differential game of infinite duration with discounted payoff involving hybrid controls is studied the minimizing player is allowed to take continuous switching and impulse controls whereas the maximizing player is allowed to take continuous and switching controls by taking stra... | [['a', 'twoperson', 'zerosum', 'infinite', 'dimensional', 'differential', 'game', 'of', 'infinite', 'duration', 'with', 'discounted', 'payoff', 'involving', 'hybrid', 'controls', 'is', 'studied', 'the', 'minimizing', 'player', 'is', 'allowed', 'to', 'take', 'continuous', 'switching', 'and', 'impulse', 'controls', 'wher... | [-0.15871183418535761, 0.07977719762628632, -0.0835663308522531, 0.05467281190254393, -0.07724169358345015, -0.21784088682782438, 0.11553220437324074, 0.3575734858800258, -0.3346316217045699, -0.2309993579717619, 0.15178625462327286, -0.2662695489225111, -0.1067526393703052, 0.09430764869653753, -0.13570144707337023, 0... |
707.1967 | Borel hierarchies in infinite products of Polish spaces | Let H be a product of countably infinite number of copies of an uncountable
Polish space X. Let $\Sigma_\xi$ $(\bar {\Sigma}_\xi)$ be the class of Borel
sets of additive class \xi for the product of copies of the discrete topology
on X (the Polish topology on X), and let ${\cal B} = \cup_{\xi < \omega_1}
\bar{\Sigma}... | math.LO | let h be a product of countably infinite number of copies of an uncountable polish space x let sigma_xi bar sigma_xi be the class of borel sets of additive class xi for the product of copies of the discrete topology on x the polish topology on x and let cal b cup_xi omega_1 barsigma_xi we prove in the levysolovay model... | [['let', 'h', 'be', 'a', 'product', 'of', 'countably', 'infinite', 'number', 'of', 'copies', 'of', 'an', 'uncountable', 'polish', 'space', 'x', 'let', 'sigma_xi', 'bar', 'sigma_xi', 'be', 'the', 'class', 'of', 'borel', 'sets', 'of', 'additive', 'class', 'xi', 'for', 'the', 'product', 'of', 'copies', 'of', 'the', 'discr... | [-0.20074797986218562, 0.22576558516347386, -0.01437871976254078, -0.02763718974131804, -0.019123992925653092, -0.12423950355643264, 0.05398349769843312, 0.32901576614150635, -0.29761381349884547, -0.15266820979662812, 0.05224414408171119, -0.30096867272200495, 0.020342862892609375, 0.16727825748161054, -0.098731950856... |
707.1968 | Law of iterated logarithm for NA sequences with non-identical
distributions | Based on a law of the iterated logarithm for independent random variables
sequences, an iterated logarithm theorem for NA sequences with non-identical
distributions is obtained. The proof is based on a Kolmogrov-type exponential
inequality.
| math.PR | based on a law of the iterated logarithm for independent random variables sequences an iterated logarithm theorem for na sequences with nonidentical distributions is obtained the proof is based on a kolmogrovtype exponential inequality | [['based', 'on', 'a', 'law', 'of', 'the', 'iterated', 'logarithm', 'for', 'independent', 'random', 'variables', 'sequences', 'an', 'iterated', 'logarithm', 'theorem', 'for', 'na', 'sequences', 'with', 'nonidentical', 'distributions', 'is', 'obtained', 'the', 'proof', 'is', 'based', 'on', 'a', 'kolmogrovtype', 'exponent... | [-0.1386344742142793, 0.11027160308466674, -0.19149240710292803, 0.08466664264966367, 0.0027188061538970833, -0.171622552372741, 0.06618593983126408, 0.26816103596127394, -0.25877690010450105, -0.2169458752667362, 0.089024158505102, -0.26498031125149946, -0.14254219784881128, 0.25818151077537826, -0.12497459814855547, ... |
707.1969 | Doppler cooling of calcium ions using a dipole-forbidden transition | Doppler cooling of calcium ions has been experimentally demonstrated using
the S1/2 to D5/2 dipole-forbidden transition. Scattering forces and
fluorescence levels a factor of 5 smaller than for usual Doppler cooling on the
dipole allowed S1/2 to P1/2 transition have been achieved. Since the light
scattered from the i... | quant-ph | doppler cooling of calcium ions has been experimentally demonstrated using the s12 to d52 dipoleforbidden transition scattering forces and fluorescence levels a factor of 5 smaller than for usual doppler cooling on the dipole allowed s12 to p12 transition have been achieved since the light scattered from the ions can b... | [['doppler', 'cooling', 'of', 'calcium', 'ions', 'has', 'been', 'experimentally', 'demonstrated', 'using', 'the', 's12', 'to', 'd52', 'dipoleforbidden', 'transition', 'scattering', 'forces', 'and', 'fluorescence', 'levels', 'a', 'factor', 'of', '5', 'smaller', 'than', 'for', 'usual', 'doppler', 'cooling', 'on', 'the', ... | [-0.03295368619361206, 0.2615152186727899, -0.05060375254160087, 0.038108613943730135, -0.00809873857192303, -0.212124041565939, 0.011814085274052463, 0.4497446042142416, -0.22512118814905224, -0.31005266418582517, 0.05844825877268848, -0.3087557721490923, 0.016187551887215754, 0.23740638045496062, 0.042751943937649854... |
707.197 | Non-commutative Geometry Modified Non-Gaussianities of Cosmological
Perturbation | We investigate the noncommutative effect on the non-Gaussianities of
primordial cosmological perturbation. In the lowest order of string length and
slow-roll parameter, we find that in the models with small speed of sound the
noncommutative modifications could be observable if assuming a relatively low
string scale. ... | astro-ph hep-th | we investigate the noncommutative effect on the nongaussianities of primordial cosmological perturbation in the lowest order of string length and slowroll parameter we find that in the models with small speed of sound the noncommutative modifications could be observable if assuming a relatively low string scale in part... | [['we', 'investigate', 'the', 'noncommutative', 'effect', 'on', 'the', 'nongaussianities', 'of', 'primordial', 'cosmological', 'perturbation', 'in', 'the', 'lowest', 'order', 'of', 'string', 'length', 'and', 'slowroll', 'parameter', 'we', 'find', 'that', 'in', 'the', 'models', 'with', 'small', 'speed', 'of', 'sound', '... | [-0.16674126403266062, 0.20810829058930438, -0.10496737661781491, 0.1667702860569441, -0.0878647852974433, -0.11941791408925607, -0.05602475246464613, 0.2805327083915472, -0.2513492360450728, -0.3068562645705477, 0.06616395358396794, -0.24243813086180918, -0.09823960123924158, 0.17155236767865317, -0.03707281767480796,... |
707.1971 | Observation of Electromagnetically Induced Transparency for a Squeezed
Vacuum with the Time Domain Method | A probe light in a squeezed vacuum state was injected into cold 87 $Rb atoms
with an intense control light in a coherent state. A sub-MHz window was created
due to electromagnetically induced transparency, and the incident squeezed
vacuum could pass through the cold atoms without optical loss, as was
successfully mon... | quant-ph | a probe light in a squeezed vacuum state was injected into cold 87 rb atoms with an intense control light in a coherent state a submhz window was created due to electromagnetically induced transparency and the incident squeezed vacuum could pass through the cold atoms without optical loss as was successfully monitored ... | [['a', 'probe', 'light', 'in', 'a', 'squeezed', 'vacuum', 'state', 'was', 'injected', 'into', 'cold', '87', 'rb', 'atoms', 'with', 'an', 'intense', 'control', 'light', 'in', 'a', 'coherent', 'state', 'a', 'submhz', 'window', 'was', 'created', 'due', 'to', 'electromagnetically', 'induced', 'transparency', 'and', 'the', ... | [-0.08191931085955155, 0.3096687583226747, -0.1158026870046007, 0.013454375403581938, -0.02071625051464428, -0.15310628752207808, 0.10957885576052624, 0.4634993211611321, -0.2259025341389995, -0.3176865095043914, 0.016536511231638622, -0.28323771075035137, 0.04327098710723875, 0.2217152902627723, -0.014743959588374485,... |
707.1972 | Boost invariant marginally trapped surfaces in Minkowski 4-space | The extremal and partly marginally trapped surfaces in Minkowski 4-space,
which are invariant under the group of boost isometries, are classified.
Moreover, it is shown that there do not exist extremal surfaces of this kind
with constant Gaussian curvature. A procedure is given in order to construct a
partly marginal... | gr-qc | the extremal and partly marginally trapped surfaces in minkowski 4space which are invariant under the group of boost isometries are classified moreover it is shown that there do not exist extremal surfaces of this kind with constant gaussian curvature a procedure is given in order to construct a partly marginally trapp... | [['the', 'extremal', 'and', 'partly', 'marginally', 'trapped', 'surfaces', 'in', 'minkowski', '4space', 'which', 'are', 'invariant', 'under', 'the', 'group', 'of', 'boost', 'isometries', 'are', 'classified', 'moreover', 'it', 'is', 'shown', 'that', 'there', 'do', 'not', 'exist', 'extremal', 'surfaces', 'of', 'this', 'k... | [-0.15753788533589072, 0.19003817301445697, -0.0750357684352108, 0.05224709531506272, -0.05148232520583111, -0.17618922031534887, -0.04168803757056594, 0.41436771202731776, -0.2334559144502556, -0.25247741337060126, 0.13542334516721502, -0.2572969461514338, -0.13440127173640035, 0.18738874021722507, -0.1581362687551567... |
707.1973 | Size-Dependence of the Wavefunction of Self-Assembled Quantum Dots | The radiative and non-radiative decay rates of InAs quantum dots are measured
by controlling the local density of optical states near an interface. From
time-resolved measurements we extract the oscillator strength and the quantum
efficiency and their dependence on emission energy. From our results and a
theoretical ... | cond-mat.other | the radiative and nonradiative decay rates of inas quantum dots are measured by controlling the local density of optical states near an interface from timeresolved measurements we extract the oscillator strength and the quantum efficiency and their dependence on emission energy from our results and a theoretical model ... | [['the', 'radiative', 'and', 'nonradiative', 'decay', 'rates', 'of', 'inas', 'quantum', 'dots', 'are', 'measured', 'by', 'controlling', 'the', 'local', 'density', 'of', 'optical', 'states', 'near', 'an', 'interface', 'from', 'timeresolved', 'measurements', 'we', 'extract', 'the', 'oscillator', 'strength', 'and', 'the',... | [-0.0655779653768006, 0.16064832904759035, -0.029672833507586465, 0.055298206143963496, 0.025841413124611502, -0.16701279917339745, 0.05951707100887832, 0.4071211228833387, -0.2309900729573871, -0.31412200819897024, 0.013860831842267591, -0.3487588635964417, -0.09062686777967764, 0.2594083800789361, 0.04797827635744684... |
707.1974 | Fractional extensions of some boundary value problems in oil strata | In the present paper, we solve three boundary value problems related to the
temperature field in oil strata -- the fractional extensions of the incomplete
lumped formulation and lumped formulation in the linear case and the fractional
generalization of the incomplete lumped formulation in the radial case. By
using th... | math.AP | in the present paper we solve three boundary value problems related to the temperature field in oil strata the fractional extensions of the incomplete lumped formulation and lumped formulation in the linear case and the fractional generalization of the incomplete lumped formulation in the radial case by using the caput... | [['in', 'the', 'present', 'paper', 'we', 'solve', 'three', 'boundary', 'value', 'problems', 'related', 'to', 'the', 'temperature', 'field', 'in', 'oil', 'strata', 'the', 'fractional', 'extensions', 'of', 'the', 'incomplete', 'lumped', 'formulation', 'and', 'lumped', 'formulation', 'in', 'the', 'linear', 'case', 'and', ... | [-0.0669707699950474, 0.019724660989595577, -0.06843916296687287, 0.08293148529628525, -0.10104913310594081, -0.0789180477586342, -0.03825492005004586, 0.28516115302530426, -0.30829073628410697, -0.2463802709923281, 0.1711777277790437, -0.24904695835236149, -0.1861126461881213, 0.20572471824319413, -0.11695607232589585... |
707.1975 | A variant of Davenport's constant | Let p be a prime number. Let G be a finite abelian p-group of exponent n
(written additively) and A be a non-empty subset of $]n[:= \{1,2,..., n\}$ such
that elements of A are incongruent modulo p and non-zero modulo p. Let $k \geq
D(G)/|A|$ be any integer where D(G) denotes the well-known Davenport's
constant. In th... | math.NT | let p be a prime number let g be a finite abelian pgroup of exponent n written additively and a be a nonempty subset of n 12 n such that elements of a are incongruent modulo p and nonzero modulo p let k geq dga be any integer where dg denotes the wellknown davenports constant in this article we prove that for any seque... | [['let', 'p', 'be', 'a', 'prime', 'number', 'let', 'g', 'be', 'a', 'finite', 'abelian', 'pgroup', 'of', 'exponent', 'n', 'written', 'additively', 'and', 'a', 'be', 'a', 'nonempty', 'subset', 'of', 'n', '12', 'n', 'such', 'that', 'elements', 'of', 'a', 'are', 'incongruent', 'modulo', 'p', 'and', 'nonzero', 'modulo', 'p'... | [-0.21147558636193237, 0.16646508618857928, -0.07732408198390682, 0.00021395618275094492, -0.06908083377437343, -0.2042596312597967, 0.012679430280024042, 0.3314852040523711, -0.3267009514921273, -0.25346280094116735, 0.048942583065348655, -0.29743793139902824, -0.09842841935124642, 0.17723918750506037, -0.085192986041... |
707.1976 | Analytical solution for 3-dimensional, incompressible Navier-Stokes
equations | This paper provides primarily an analytical ad hoc -solution for
3-dimensional, incompressible Navier-Stokes equations with a suitable external
force field. The solution turns out to be smooth and integrable on the whole
space. There is gaussian decay of amplitudes.
| physics.gen-ph | this paper provides primarily an analytical ad hoc solution for 3dimensional incompressible navierstokes equations with a suitable external force field the solution turns out to be smooth and integrable on the whole space there is gaussian decay of amplitudes | [['this', 'paper', 'provides', 'primarily', 'an', 'analytical', 'ad', 'hoc', 'solution', 'for', '3dimensional', 'incompressible', 'navierstokes', 'equations', 'with', 'a', 'suitable', 'external', 'force', 'field', 'the', 'solution', 'turns', 'out', 'to', 'be', 'smooth', 'and', 'integrable', 'on', 'the', 'whole', 'space... | [-0.20331146615820053, 0.06939841037092265, -0.09619830530256224, 0.038345114614527956, -0.1356963752888334, -0.15522757262134781, -0.029625987781820677, 0.3358563249691939, -0.24604927060695794, -0.19094304960125533, 0.11028960994922389, -0.20462681169215685, -0.13960310014394614, 0.1783335484468784, -0.03200620806847... |
707.1977 | Monte Carlo Simulation and Statistical Analysis of the Effect of Coding
Table Specificity on Genetic Information Coding | We present a computer simulation, which is inspired by Penna model, to help
understanding the effect of genetic coding tables on population dynamics. To
represent populations we used real and artificial gene sequences in this model.
We coded these sequences using different amino acid tables in Nature, the
standard ta... | q-bio.PE q-bio.GN | we present a computer simulation which is inspired by penna model to help understanding the effect of genetic coding tables on population dynamics to represent populations we used real and artificial gene sequences in this model we coded these sequences using different amino acid tables in nature the standard table as ... | [['we', 'present', 'a', 'computer', 'simulation', 'which', 'is', 'inspired', 'by', 'penna', 'model', 'to', 'help', 'understanding', 'the', 'effect', 'of', 'genetic', 'coding', 'tables', 'on', 'population', 'dynamics', 'to', 'represent', 'populations', 'we', 'used', 'real', 'and', 'artificial', 'gene', 'sequences', 'in'... | [-0.07711676227768044, 0.07249199752542344, -0.06124921593364779, 0.13470293197315186, -0.047300129545504575, -0.1549119777762546, 0.0908721600541497, 0.4022870675793716, -0.2784964662418793, -0.29508978584883633, 0.08842316859626917, -0.23321254912170244, -0.27247955682840974, 0.18792386733220665, -0.11964176624890539... |
707.1978 | Weak quantization of Poisson structures | In this paper we prove that any Poisson structure on a sheaf of Lie
algebroids admits a weak deformation quantization, and give a sufficient
condition for such a Poisson structure to admit an actual deformation
quantization. We also answer the corresponding classification problems. In the
complex symplectic case, we ... | math.QA | in this paper we prove that any poisson structure on a sheaf of lie algebroids admits a weak deformation quantization and give a sufficient condition for such a poisson structure to admit an actual deformation quantization we also answer the corresponding classification problems in the complex symplectic case we recove... | [['in', 'this', 'paper', 'we', 'prove', 'that', 'any', 'poisson', 'structure', 'on', 'a', 'sheaf', 'of', 'lie', 'algebroids', 'admits', 'a', 'weak', 'deformation', 'quantization', 'and', 'give', 'a', 'sufficient', 'condition', 'for', 'such', 'a', 'poisson', 'structure', 'to', 'admit', 'an', 'actual', 'deformation', 'qu... | [-0.16159253764276704, -0.00041508913641640296, -0.09438095857699712, 0.09554545774279784, -0.17203225875273348, -0.10854734718178709, -0.0266274648765102, 0.371031867886583, -0.3516650292525689, -0.21926538078735272, 0.09819211724059035, -0.18792241603136062, -0.271882178944846, 0.15955269750828543, -0.204188536709795... |
707.1979 | Interacting bosons in an optical lattice | Several models of a strongly interacting Bose gas in an optical lattice are
studied within the functional-integral approach. The one-dimensional Bose gas
is briefly discussed. Then the Bose-Einstein condensate and the Mott insulator
of a three-dimensional Bose gas are described in mean-field approximation, and
the co... | cond-mat.other | several models of a strongly interacting bose gas in an optical lattice are studied within the functionalintegral approach the onedimensional bose gas is briefly discussed then the boseeinstein condensate and the mott insulator of a threedimensional bose gas are described in meanfield approximation and the correspondin... | [['several', 'models', 'of', 'a', 'strongly', 'interacting', 'bose', 'gas', 'in', 'an', 'optical', 'lattice', 'are', 'studied', 'within', 'the', 'functionalintegral', 'approach', 'the', 'onedimensional', 'bose', 'gas', 'is', 'briefly', 'discussed', 'then', 'the', 'boseeinstein', 'condensate', 'and', 'the', 'mott', 'ins... | [-0.1391279114028649, 0.2000561445756488, -0.09626880233680227, 0.0748711472475215, 0.02474325381331426, -0.1059607720331646, 0.022001522297347736, 0.30100435924653274, -0.2297978718849109, -0.20801857629479295, 0.031033824221581165, -0.3213394286087583, -0.10863360877085786, 0.12350444585659114, 0.07052785002878566, 0... |
707.198 | Atomic Landau-Zener tunneling in Fourier-synthesized optical lattices | We report on an experimental study of quantum transport of atoms in variable
periodic optical potentials. The band structure of both ratchet-type asymmetric
and symmetric lattice potentials is explored. The variable atom potential is
realized by superimposing a conventional standing wave potential of \lambda/2
spatia... | cond-mat.other | we report on an experimental study of quantum transport of atoms in variable periodic optical potentials the band structure of both ratchettype asymmetric and symmetric lattice potentials is explored the variable atom potential is realized by superimposing a conventional standing wave potential of lambda2 spatial perio... | [['we', 'report', 'on', 'an', 'experimental', 'study', 'of', 'quantum', 'transport', 'of', 'atoms', 'in', 'variable', 'periodic', 'optical', 'potentials', 'the', 'band', 'structure', 'of', 'both', 'ratchettype', 'asymmetric', 'and', 'symmetric', 'lattice', 'potentials', 'is', 'explored', 'the', 'variable', 'atom', 'pot... | [-0.20498577756920783, 0.1728986192272093, -0.02891991744612957, 0.011487860803310646, -0.017052780518808017, -0.14765071834823706, 0.06727632970219796, 0.4462081547187664, -0.2537406374382355, -0.21016863510921235, 0.023030151310660763, -0.2553546626983983, -0.1487348475095975, 0.16203206659737612, 0.06037922773691939... |
707.1981 | A Normalizing Intuitionistic Set Theory with Inaccessible Sets | We propose a set theory strong enough to interpret powerful type theories
underlying proof assistants such as LEGO and also possibly Coq, which at the
same time enables program extraction from its constructive proofs. For this
purpose, we axiomatize an impredicative constructive version of
Zermelo-Fraenkel set theory... | cs.LO | we propose a set theory strong enough to interpret powerful type theories underlying proof assistants such as lego and also possibly coq which at the same time enables program extraction from its constructive proofs for this purpose we axiomatize an impredicative constructive version of zermelofraenkel set theory izf w... | [['we', 'propose', 'a', 'set', 'theory', 'strong', 'enough', 'to', 'interpret', 'powerful', 'type', 'theories', 'underlying', 'proof', 'assistants', 'such', 'as', 'lego', 'and', 'also', 'possibly', 'coq', 'which', 'at', 'the', 'same', 'time', 'enables', 'program', 'extraction', 'from', 'its', 'constructive', 'proofs', ... | [-0.06835686743808994, -0.003926499455963756, -0.165395259664201, 0.14566169071183246, -0.21540513004990178, -0.15857506310986774, 0.1042702345341142, 0.29798299748752566, -0.33264912724880885, -0.2963220741859897, 0.050918705936580023, -0.2094932814562108, -0.10782724980428512, 0.18012569005693402, -0.1321825330263121... |
707.1982 | Nflation: observable predictions from the random matrix mass spectrum | We carry out numerical investigations of the perturbations in Nflation models
where the mass spectrum is generated by random matrix theory. The
tensor-to-scalar ratio and non-gaussianity are already known to take the
single-field values, and so the density perturbation spectral index is the main
parameter of interest... | astro-ph | we carry out numerical investigations of the perturbations in nflation models where the mass spectrum is generated by random matrix theory the tensortoscalar ratio and nongaussianity are already known to take the singlefield values and so the density perturbation spectral index is the main parameter of interest we stud... | [['we', 'carry', 'out', 'numerical', 'investigations', 'of', 'the', 'perturbations', 'in', 'nflation', 'models', 'where', 'the', 'mass', 'spectrum', 'is', 'generated', 'by', 'random', 'matrix', 'theory', 'the', 'tensortoscalar', 'ratio', 'and', 'nongaussianity', 'are', 'already', 'known', 'to', 'take', 'the', 'singlefi... | [-0.13074546690369326, 0.14525047551480033, -0.07286075086543156, 0.06329713590438127, -0.06648260572554684, -0.07301309144985611, -0.02175672686413451, 0.33659594908597007, -0.21783188905727158, -0.33702041362963053, 0.10071441230504342, -0.26486876402400755, -0.10670006954641913, 0.2079611783321466, 0.011635342472663... |
707.1983 | Hidden Life of Riemann's Zeta Function 1. Arrow, Bow, and Targets | The Riemann Hypothesis is reformulated as statements about eigenvalues of
some matrices entries of which are defined via Taylor coefficient of the zeta
function. These eigenvalues demonstrate interesting visual patterns allowing
one to state a number of conjectures.
| math.NT | the riemann hypothesis is reformulated as statements about eigenvalues of some matrices entries of which are defined via taylor coefficient of the zeta function these eigenvalues demonstrate interesting visual patterns allowing one to state a number of conjectures | [['the', 'riemann', 'hypothesis', 'is', 'reformulated', 'as', 'statements', 'about', 'eigenvalues', 'of', 'some', 'matrices', 'entries', 'of', 'which', 'are', 'defined', 'via', 'taylor', 'coefficient', 'of', 'the', 'zeta', 'function', 'these', 'eigenvalues', 'demonstrate', 'interesting', 'visual', 'patterns', 'allowing... | [-0.20423757806910495, 0.07083206962009794, -0.10813473581679557, 0.09464293690459606, -0.1092257627138966, -0.12334409979858289, 0.029916311369130488, 0.26949851097244965, -0.3086152088485266, -0.2975243442618337, 0.12849564486379295, -0.2679927842201371, -0.20037753536905112, 0.1723078537340227, -0.03427754242071196,... |
707.1984 | Old open clusters in the inner Galaxy: FSR1744, FSR89 and FSR31 | We establish the nature and derive fundamental and structural parameters of
the recently catalogued objects FSR1744, FSR89 and FSR31. This work intends to
provide clues to constrain the Galactic tidal disruption efficiency, improve
statistics of the open cluster parameter space, and better define their
age-distributi... | astro-ph | we establish the nature and derive fundamental and structural parameters of the recently catalogued objects fsr1744 fsr89 and fsr31 this work intends to provide clues to constrain the galactic tidal disruption efficiency improve statistics of the open cluster parameter space and better define their agedistribution func... | [['we', 'establish', 'the', 'nature', 'and', 'derive', 'fundamental', 'and', 'structural', 'parameters', 'of', 'the', 'recently', 'catalogued', 'objects', 'fsr1744', 'fsr89', 'and', 'fsr31', 'this', 'work', 'intends', 'to', 'provide', 'clues', 'to', 'constrain', 'the', 'galactic', 'tidal', 'disruption', 'efficiency', '... | [-0.06770657659003454, 0.1428968504808349, -0.07401850684441105, 0.10734172444514736, -0.09549273781023779, -0.03389854269872985, 0.03446026923470376, 0.40445387986669606, -0.22665258695071308, -0.3819381896557035, 0.049687850967124636, -0.2652068556864609, -0.0666619938493693, 0.15781418548707113, -0.04679801599321207... |
707.1985 | Intensity correlations, entanglement properties and ghost imaging in
multimode thermal-seeded parametric downconversion: Theory | We address parametric-downconversion seeded by multimode pseudo-thermal
fields. We show that this process may be used to generate multimode pairwise
correlated states with entanglement properties that can be tuned by controlling
the seed intensities. Multimode pseudo-thermal fields seeded
parametric-downconversion re... | quant-ph | we address parametricdownconversion seeded by multimode pseudothermal fields we show that this process may be used to generate multimode pairwise correlated states with entanglement properties that can be tuned by controlling the seed intensities multimode pseudothermal fields seeded parametricdownconversion represents... | [['we', 'address', 'parametricdownconversion', 'seeded', 'by', 'multimode', 'pseudothermal', 'fields', 'we', 'show', 'that', 'this', 'process', 'may', 'be', 'used', 'to', 'generate', 'multimode', 'pairwise', 'correlated', 'states', 'with', 'entanglement', 'properties', 'that', 'can', 'be', 'tuned', 'by', 'controlling',... | [-0.10428246492908026, 0.2962368670915667, -0.10461779425127639, 0.08242037237437216, -0.017422277363948524, -0.20908072128077038, 0.014815632751884146, 0.4473317257749538, -0.28197042668600464, -0.2770802044413156, -0.007671874491885926, -0.22811046325841744, -0.1301199123263359, 0.20146426995698777, -0.03086013502130... |
707.1986 | Crystallization of the resonating valence bond liquid as vortex
condensation | We show that the liquid-to-crystal quantum phase transition in the
Rokhsar--Kivelson dimer model on the two-dimensional triangular lattice occurs
as a condensation of vortex-like excitations called ``visons''. This conclusion
is drawn from the numerical studies of the vison spectrum in the liquid phase
by using the G... | cond-mat.str-el | we show that the liquidtocrystal quantum phase transition in the rokhsarkivelson dimer model on the twodimensional triangular lattice occurs as a condensation of vortexlike excitations called visons this conclusion is drawn from the numerical studies of the vison spectrum in the liquid phase by using the greens functio... | [['we', 'show', 'that', 'the', 'liquidtocrystal', 'quantum', 'phase', 'transition', 'in', 'the', 'rokhsarkivelson', 'dimer', 'model', 'on', 'the', 'twodimensional', 'triangular', 'lattice', 'occurs', 'as', 'a', 'condensation', 'of', 'vortexlike', 'excitations', 'called', 'visons', 'this', 'conclusion', 'is', 'drawn', '... | [-0.12814421082702687, 0.23215519123422426, -0.07916594911034086, -0.026560057934728407, 0.025081778619261016, -0.07900541547597165, 0.11893466863825562, 0.3763878171820016, -0.2033388105176744, -0.2719896338081786, 0.04778189022382278, -0.3249798253089899, -0.16662205157890206, 0.10199884505543326, 0.04380367439949796... |
707.1987 | Imaginary chemical potentials and the phase of the fermionic determinant | A numerical technique is proposed for an efficient numerical determination of
the average phase factor of the fermionic determinant continued to imaginary
values of the chemical potential. The method is tested in QCD with eight
flavors of dynamical staggered fermions. A direct check of the validity of
analytic contin... | hep-lat | a numerical technique is proposed for an efficient numerical determination of the average phase factor of the fermionic determinant continued to imaginary values of the chemical potential the method is tested in qcd with eight flavors of dynamical staggered fermions a direct check of the validity of analytic continuati... | [['a', 'numerical', 'technique', 'is', 'proposed', 'for', 'an', 'efficient', 'numerical', 'determination', 'of', 'the', 'average', 'phase', 'factor', 'of', 'the', 'fermionic', 'determinant', 'continued', 'to', 'imaginary', 'values', 'of', 'the', 'chemical', 'potential', 'the', 'method', 'is', 'tested', 'in', 'qcd', 'wi... | [-0.1810343754989321, 0.11716120627512061, -0.12055414889685133, 0.004232390649673162, -0.039832110559059816, -0.06427138418163822, 0.11076127008930074, 0.3493391044974101, -0.14317730212386584, -0.2414730516347018, 0.10874815412733535, -0.2549223904356812, -0.10651062503033741, 0.19569069576082807, 0.073254910791575, ... |
707.1988 | LHCb detector status and commissioning | The LHCb detector status and commissioning is presented.
| physics.ins-det | the lhcb detector status and commissioning is presented | [['the', 'lhcb', 'detector', 'status', 'and', 'commissioning', 'is', 'presented']] | [-0.0656240344978869, 0.24295528465881944, -0.10123121808283031, -0.05308805491949897, -0.1299588829278946, -0.139669434633106, -0.16201932122930884, 0.2801117552444339, -0.026674960739910603, -0.332692788913846, 0.1713197878561914, -0.4579945048317313, -0.028744732961058617, 0.12161475248285569, -0.08966806915123016, ... |
707.1989 | Electron-electron interaction effects in quantum point contacts | We consider interaction effects in quantum point contacts on the first
quantization plateau, taking into account all non momentum-conserving
processes. We compute low-temperature linear and non-linear conductance, shot
noise, and thermopower by perturbation theory, and show that they are
consistent with experimental ... | cond-mat.mes-hall | we consider interaction effects in quantum point contacts on the first quantization plateau taking into account all non momentumconserving processes we compute lowtemperature linear and nonlinear conductance shot noise and thermopower by perturbation theory and show that they are consistent with experimental observatio... | [['we', 'consider', 'interaction', 'effects', 'in', 'quantum', 'point', 'contacts', 'on', 'the', 'first', 'quantization', 'plateau', 'taking', 'into', 'account', 'all', 'non', 'momentumconserving', 'processes', 'we', 'compute', 'lowtemperature', 'linear', 'and', 'nonlinear', 'conductance', 'shot', 'noise', 'and', 'ther... | [-0.13248954762821086, 0.17412614432072993, -0.0752221189702848, 0.07181429835650811, -0.015624276226541648, -0.18949292882138657, 0.06566041469341144, 0.33207046770904625, -0.2431748618837446, -0.26451636801680756, 0.017850324975572422, -0.3763019026308838, -0.15532305766828358, 0.19115954605189878, 0.0064037117796639... |
707.199 | Phase transition in a stochastic prime number generator | We introduce a stochastic algorithm that acts as a prime number generator.
The dynamics of such algorithm gives rise to a continuous phase transition
which separates a phase where the algorithm is able to reduce a whole set of
integers into primes and a phase where the system reaches a frozen state with
low prime den... | physics.comp-ph | we introduce a stochastic algorithm that acts as a prime number generator the dynamics of such algorithm gives rise to a continuous phase transition which separates a phase where the algorithm is able to reduce a whole set of integers into primes and a phase where the system reaches a frozen state with low prime densit... | [['we', 'introduce', 'a', 'stochastic', 'algorithm', 'that', 'acts', 'as', 'a', 'prime', 'number', 'generator', 'the', 'dynamics', 'of', 'such', 'algorithm', 'gives', 'rise', 'to', 'a', 'continuous', 'phase', 'transition', 'which', 'separates', 'a', 'phase', 'where', 'the', 'algorithm', 'is', 'able', 'to', 'reduce', 'a... | [-0.15010064451630098, 0.15479061517351972, -0.14271746533815802, 0.02700144571423445, -0.034169609500523446, -0.10906832791522317, 0.08690597772887297, 0.30851188443344213, -0.27835904480354196, -0.27864514492805403, 0.0895586395301674, -0.2551150594077919, -0.17594646333834563, 0.1864188040189188, -0.0087598182592840... |
707.1991 | Tracking granules on the Sun's surface and reconstructing horizontal
velocity fields: I. the CST algorithm | Determination of horizontal velocity fields on the solar surface is crucial
for understanding the dynamics of structures like mesogranulation or
supergranulation or simply the distribution of magnetic fields.
We pursue here the development of a method called CST for coherent structure
tracking, which determines the... | astro-ph | determination of horizontal velocity fields on the solar surface is crucial for understanding the dynamics of structures like mesogranulation or supergranulation or simply the distribution of magnetic fields we pursue here the development of a method called cst for coherent structure tracking which determines the horiz... | [['determination', 'of', 'horizontal', 'velocity', 'fields', 'on', 'the', 'solar', 'surface', 'is', 'crucial', 'for', 'understanding', 'the', 'dynamics', 'of', 'structures', 'like', 'mesogranulation', 'or', 'supergranulation', 'or', 'simply', 'the', 'distribution', 'of', 'magnetic', 'fields', 'we', 'pursue', 'here', 't... | [-0.0902015724054586, 0.13779923270009353, -0.09826679256895493, 0.07467344900526639, -0.08309198489001432, -0.03262909721317036, -0.0255676748370147, 0.36755735507573595, -0.2657817056245328, -0.31345382846238745, 0.1071222253686555, -0.2174929878160406, -0.16307454315080708, 0.21763576213240188, -0.06735375418491032,... |
707.1992 | Noise-guided evolution within cyclical interactions | We study a stochastic predator-prey model on a square lattice, where each of
the six species has two superior and two inferior partners. The invasion
probabilities between species depend on the predator-prey pair and are
supplemented by Gaussian noise. Conditions are identified that warrant the
largest impact of nois... | q-bio.PE cond-mat.stat-mech physics.bio-ph | we study a stochastic predatorprey model on a square lattice where each of the six species has two superior and two inferior partners the invasion probabilities between species depend on the predatorprey pair and are supplemented by gaussian noise conditions are identified that warrant the largest impact of noise on th... | [['we', 'study', 'a', 'stochastic', 'predatorprey', 'model', 'on', 'a', 'square', 'lattice', 'where', 'each', 'of', 'the', 'six', 'species', 'has', 'two', 'superior', 'and', 'two', 'inferior', 'partners', 'the', 'invasion', 'probabilities', 'between', 'species', 'depend', 'on', 'the', 'predatorprey', 'pair', 'and', 'ar... | [-0.11763179284293744, 0.15530608703480347, -0.09363030858749928, 0.12481889148719012, -0.03472980025444964, -0.14042113185553862, 0.047789880640553555, 0.3936181259402809, -0.2487047572105535, -0.27921089818463724, 0.08879065949019462, -0.26595241525578067, -0.21140915420102446, 0.1639611294759609, 0.00406962828588132... |
707.1993 | Decoherence of a particle in a ring | We consider a particle coupled to a dissipative environment and derive a
perturbative formula for the dephasing rate based on the purity of the reduced
probability matrix. We apply this formula to the problem of a particle on a
ring, that interacts with a dirty metal environment. At low but finite
temperatures we fin... | cond-mat.mes-hall | we consider a particle coupled to a dissipative environment and derive a perturbative formula for the dephasing rate based on the purity of the reduced probability matrix we apply this formula to the problem of a particle on a ring that interacts with a dirty metal environment at low but finite temperatures we find a d... | [['we', 'consider', 'a', 'particle', 'coupled', 'to', 'a', 'dissipative', 'environment', 'and', 'derive', 'a', 'perturbative', 'formula', 'for', 'the', 'dephasing', 'rate', 'based', 'on', 'the', 'purity', 'of', 'the', 'reduced', 'probability', 'matrix', 'we', 'apply', 'this', 'formula', 'to', 'the', 'problem', 'of', 'a... | [-0.13530586548194362, 0.19827661158230442, -0.1030188515656986, 0.08618264139938848, 0.009405578520202722, -0.16860186479663333, 0.08095533717334127, 0.3302043630616166, -0.23965900663349132, -0.2492500118051584, 0.06096435220724043, -0.30032816949264646, -0.04900029829542081, 0.20585630028262342, -0.00750764711007762... |
707.1994 | Tracking granules at the Sun's surface and reconstructing velocity
fields. II. Error analysis | The determination of horizontal velocity fields at the solar surface is
crucial to understanding the dynamics and magnetism of the convection zone of
the sun. These measurements can be done by tracking granules.
Tracking granules from ground-based observations, however, suffers from the
Earth's atmospheric turbulen... | astro-ph | the determination of horizontal velocity fields at the solar surface is crucial to understanding the dynamics and magnetism of the convection zone of the sun these measurements can be done by tracking granules tracking granules from groundbased observations however suffers from the earths atmospheric turbulence which i... | [['the', 'determination', 'of', 'horizontal', 'velocity', 'fields', 'at', 'the', 'solar', 'surface', 'is', 'crucial', 'to', 'understanding', 'the', 'dynamics', 'and', 'magnetism', 'of', 'the', 'convection', 'zone', 'of', 'the', 'sun', 'these', 'measurements', 'can', 'be', 'done', 'by', 'tracking', 'granules', 'tracking... | [-0.11609473910290918, 0.1589563852485223, -0.08403192679824055, 0.0717624162192866, -0.05782105316044724, -0.08064196896410829, 0.010987152199114043, 0.3974165819137052, -0.2646403674662299, -0.3304364716622561, 0.1332635508567149, -0.259858123515636, -0.11757717455478377, 0.22497679812725463, -0.07430629485771756, 0.... |
707.1995 | Correlation functions of the open XXZ chain I | We consider the XXZ spin chain with diagonal boundary conditions in the
framework of algebraic Bethe Ansatz. Using the explicit computation of the
scalar products of Bethe states and a revisited version of the bulk inverse
problem, we calculate the elementary building blocks for the correlation
functions. In the limi... | hep-th | we consider the xxz spin chain with diagonal boundary conditions in the framework of algebraic bethe ansatz using the explicit computation of the scalar products of bethe states and a revisited version of the bulk inverse problem we calculate the elementary building blocks for the correlation functions in the limit of ... | [['we', 'consider', 'the', 'xxz', 'spin', 'chain', 'with', 'diagonal', 'boundary', 'conditions', 'in', 'the', 'framework', 'of', 'algebraic', 'bethe', 'ansatz', 'using', 'the', 'explicit', 'computation', 'of', 'the', 'scalar', 'products', 'of', 'bethe', 'states', 'and', 'a', 'revisited', 'version', 'of', 'the', 'bulk',... | [-0.20313481645924705, 0.1281222756286817, -0.05027468263038567, 0.10843556229291218, -0.039402758137189915, -0.11063628212016607, 0.005143038000512336, 0.3298443288409284, -0.27226851215319975, -0.20168764569929667, 0.14994874833085176, -0.25910602316393383, -0.10162545186218007, 0.16213615210726856, 0.067000797577618... |
707.1996 | Ratio Asymptotic of Hermite-Pad\'e Orthogonal Polynomials for Nikishin
Systems. II | We prove ratio asymptotic for sequences of multiple orthogonal polynomials
with respect to a Nikishin system of measures
${\mathcal{N}}(\sigma_1,...,\sigma_m)$ such that for each $k$, the support of
$\sigma_k$ consists of an interval $\widetilde{\Delta}_k$, on which
$\sigma_k^{\prime} > 0$ almost everywhere, and a se... | math.CV | we prove ratio asymptotic for sequences of multiple orthogonal polynomials with respect to a nikishin system of measures mathcalnsigma_1sigma_m such that for each k the support of sigma_k consists of an interval widetildedelta_k on which sigma_kprime 0 almost everywhere and a set without accumulation points in mathbbr ... | [['we', 'prove', 'ratio', 'asymptotic', 'for', 'sequences', 'of', 'multiple', 'orthogonal', 'polynomials', 'with', 'respect', 'to', 'a', 'nikishin', 'system', 'of', 'measures', 'mathcalnsigma_1sigma_m', 'such', 'that', 'for', 'each', 'k', 'the', 'support', 'of', 'sigma_k', 'consists', 'of', 'an', 'interval', 'widetilde... | [-0.2469950019520648, 0.05090612631094236, -0.047580475681164164, -0.03827469814271527, 0.01384927863453297, -0.11643445694898354, 0.0664472389728465, 0.3521339264995557, -0.27333600236538874, -0.1377985643066882, 0.09892166904025176, -0.33419185458741923, -0.08414338536045336, 0.18981347815629016, -0.06562029169079789... |
707.1997 | Low energy constants of \chiPT from the instanton vacuum model | In the framework of the instanton vacuum model we make expansion over the
current mass m and number of colors N_c and evaluate ${\cal O}(1/N_c, m, m/N_c,
m \ln m/N_c)$-corrections to the dynamical quark mass M, the quark condensate
$<\bar qq>$, the pion mass M_\pi and decay constant F_\pi. There are several
sources o... | hep-ph | in the framework of the instanton vacuum model we make expansion over the current mass m and number of colors n_c and evaluate cal o1n_c m mn_c m ln mn_ccorrections to the dynamical quark mass m the quark condensate bar qq the pion mass m_pi and decay constant f_pi there are several sources of these corrections meson l... | [['in', 'the', 'framework', 'of', 'the', 'instanton', 'vacuum', 'model', 'we', 'make', 'expansion', 'over', 'the', 'current', 'mass', 'm', 'and', 'number', 'of', 'colors', 'n_c', 'and', 'evaluate', 'cal', 'o1n_c', 'm', 'mn_c', 'm', 'ln', 'mn_ccorrections', 'to', 'the', 'dynamical', 'quark', 'mass', 'm', 'the', 'quark',... | [-0.14978255027196777, 0.2181437033700796, -0.09215257317483636, 0.1017909091962895, -0.029729930339643443, -0.08196838038258622, 0.057490920818502635, 0.34634349728659003, -0.17185131815658936, -0.26207572040738353, -0.015014263078189967, -0.3171826063222449, -0.04639468090215199, 0.0930083981029768, 0.034217698189666... |
707.1998 | Collective neutrino flavor transitions in supernovae and the role of
trajectory averaging | Non-linear effects on supernova neutrino oscillations, associated with
neutrino self-interactions, are known to induce collective flavor transitions
near the supernova core for theta_13 \neq 0. In scenarios with very shallow
electron density profiles, these transformations have been shown to couple with
ordinary matt... | hep-ph astro-ph | nonlinear effects on supernova neutrino oscillations associated with neutrino selfinteractions are known to induce collective flavor transitions near the supernova core for theta_13 neq 0 in scenarios with very shallow electron density profiles these transformations have been shown to couple with ordinary matter effect... | [['nonlinear', 'effects', 'on', 'supernova', 'neutrino', 'oscillations', 'associated', 'with', 'neutrino', 'selfinteractions', 'are', 'known', 'to', 'induce', 'collective', 'flavor', 'transitions', 'near', 'the', 'supernova', 'core', 'for', 'theta_13', 'neq', '0', 'in', 'scenarios', 'with', 'very', 'shallow', 'electron... | [-0.1061483448508873, 0.2038881738891095, -0.0572777677419757, 0.17115727050589735, -0.04533471132644013, -0.13527082804829066, 0.026120051346172787, 0.35648707565582116, -0.24210300995614226, -0.31675480764882624, 0.051225163084878164, -0.2733674829841153, -0.12935420371875747, 0.17184411515414422, 0.02666239826716309... |
707.1999 | Coarse topology, enlargeability, and essentialness | Using methods from coarse topology we show that fundamental classes of closed
enlargeable manifolds map non-trivially both to the rational homology of their
fundamental groups and to the K-theory of the corresponding reduced
C*-algebras. Our proofs do not depend on the Baum--Connes conjecture and
provide independent ... | math.AT math.DG math.GT math.KT | using methods from coarse topology we show that fundamental classes of closed enlargeable manifolds map nontrivially both to the rational homology of their fundamental groups and to the ktheory of the corresponding reduced calgebras our proofs do not depend on the baumconnes conjecture and provide independent confirmat... | [['using', 'methods', 'from', 'coarse', 'topology', 'we', 'show', 'that', 'fundamental', 'classes', 'of', 'closed', 'enlargeable', 'manifolds', 'map', 'nontrivially', 'both', 'to', 'the', 'rational', 'homology', 'of', 'their', 'fundamental', 'groups', 'and', 'to', 'the', 'ktheory', 'of', 'the', 'corresponding', 'reduce... | [-0.11183554645847632, 0.0456713986544249, -0.13672333698788727, 0.08640456315845733, -0.09723126125108036, -0.15716164026202428, 0.035213795921730774, 0.34165123180934676, -0.3230749158947556, -0.26883424375275217, 0.11069285713515624, -0.18942504635843863, -0.16216982681200737, 0.25863943761430197, -0.160241258468616... |
707.2 | Setup for shot noise measurements in carbon nanotubes | We have constructed a noise measurement setup for high impedance carbon
nanotube samples. Our setup, working in the frequency range of 600 - 900 MHz,
takes advantage of the fact that the shot noise power is reasonably large for
high impedance sources so that relatively large, fixed non-matching conditions
can be tole... | cond-mat.mes-hall | we have constructed a noise measurement setup for high impedance carbon nanotube samples our setup working in the frequency range of 600 900 mhz takes advantage of the fact that the shot noise power is reasonably large for high impedance sources so that relatively large fixed nonmatching conditions can be tolerated | [['we', 'have', 'constructed', 'a', 'noise', 'measurement', 'setup', 'for', 'high', 'impedance', 'carbon', 'nanotube', 'samples', 'our', 'setup', 'working', 'in', 'the', 'frequency', 'range', 'of', '600', '900', 'mhz', 'takes', 'advantage', 'of', 'the', 'fact', 'that', 'the', 'shot', 'noise', 'power', 'is', 'reasonably... | [-0.1271873403559713, 0.16358619589614226, -0.03161636009520175, -0.011515383907666831, -0.04196735310788248, -0.17281720435758138, 0.07202992816546969, 0.4365028373750986, -0.20580161355581938, -0.3688054746199472, 0.09652842654602364, -0.24995189004431606, -0.0292448173916223, 0.24864975143881404, -0.0979654773448904... |
707.2001 | Master crossover behavior of parachor correlations for one-component
fluids | The master asymptotic behavior of the usual parachor correlations, expressing
surface tension $\sigma$ as a power law of the density difference
$\rho_{L}-\rho_{V}$ between coexisting liquid and vapor, is analyzed for a
series of pure compounds close to their liquid-vapor critical point, using only
four critical param... | cond-mat.stat-mech | the master asymptotic behavior of the usual parachor correlations expressing surface tension sigma as a power law of the density difference rho_lrho_v between coexisting liquid and vapor is analyzed for a series of pure compounds close to their liquidvapor critical point using only four critical parameters beta_c1 alph... | [['the', 'master', 'asymptotic', 'behavior', 'of', 'the', 'usual', 'parachor', 'correlations', 'expressing', 'surface', 'tension', 'sigma', 'as', 'a', 'power', 'law', 'of', 'the', 'density', 'difference', 'rho_lrho_v', 'between', 'coexisting', 'liquid', 'and', 'vapor', 'is', 'analyzed', 'for', 'a', 'series', 'of', 'pur... | [-0.12576392508540932, 0.1554226235308674, -0.10758078143816818, 0.0484673360754774, 0.0052221457721152754, -0.17000725071123812, 0.08981271279358378, 0.2747121237302094, -0.2339148758505105, -0.294500324477473, 0.06740807571704761, -0.33588004090268625, -0.1300360035318672, 0.21523574044865168, 0.03819542119719004, 0.... |
707.2002 | Effect of Intra-molecular Disorder and Inter-molecular Electronic
Interactions on the Electronic Structure of Poly-p-Phenylene Vinylene (PPV) | We investigate the role of intra-molecular conformational disorder and
inter-molecular electronic interactions on the electronic structure of disorder
clusters of poly-p-phenylene vinylene (PPV) oligomers. Classical molecular
dynamics is used to determine probable molecular geometries, and
first-principle density fun... | cond-mat.soft cond-mat.mtrl-sci | we investigate the role of intramolecular conformational disorder and intermolecular electronic interactions on the electronic structure of disorder clusters of polypphenylene vinylene ppv oligomers classical molecular dynamics is used to determine probable molecular geometries and firstprinciple density functional the... | [['we', 'investigate', 'the', 'role', 'of', 'intramolecular', 'conformational', 'disorder', 'and', 'intermolecular', 'electronic', 'interactions', 'on', 'the', 'electronic', 'structure', 'of', 'disorder', 'clusters', 'of', 'polypphenylene', 'vinylene', 'ppv', 'oligomers', 'classical', 'molecular', 'dynamics', 'is', 'us... | [-0.14300594997250152, 0.2204393718097055, -0.028212710384669125, 0.11070151508866562, 0.06164783988699165, -0.13415089952854478, 0.021703822281667774, 0.4715003380551934, -0.24757869495554086, -0.26515525723902544, -0.08653156150355745, -0.33584391456857626, -0.168084674087182, 0.07346455421897449, 0.12214174513153885... |
707.2003 | A geometric model for Hochschild homology of Soergel bimodules | An important step in the calculation of the triply graded link homology
theory of Khovanov and Rozansky is the determination of the Hochschild homology
of Soergel bimodules for SL(n). We present a geometric model for this
Hochschild homology for any simple group G, as equivariant intersection
homology of B x B-orbit ... | math.AG math.RT | an important step in the calculation of the triply graded link homology theory of khovanov and rozansky is the determination of the hochschild homology of soergel bimodules for sln we present a geometric model for this hochschild homology for any simple group g as equivariant intersection homology of b x borbit closure... | [['an', 'important', 'step', 'in', 'the', 'calculation', 'of', 'the', 'triply', 'graded', 'link', 'homology', 'theory', 'of', 'khovanov', 'and', 'rozansky', 'is', 'the', 'determination', 'of', 'the', 'hochschild', 'homology', 'of', 'soergel', 'bimodules', 'for', 'sln', 'we', 'present', 'a', 'geometric', 'model', 'for',... | [-0.2510662302261264, 0.018703515388921465, -0.12609592341340897, 0.05320152110463705, -0.07577681041708807, -0.1175342557868519, -0.03858583641325585, 0.3359794179053326, -0.39391990578392655, -0.19675186970384745, 0.08801631132004464, -0.18166388062252928, -0.18757339825331257, 0.1586566985323571, -0.1996534244967548... |
707.2004 | The environs of the HII region Gum31 | We analyze the distribution of the interstellar matter in the environs of the
\hii region Gum 31, excited by the open cluster NGC 3324, located in the
complex Carina region, with the aim of investigating the action of the massive
stars on the surrounding neutral material. We use 21cm-line data, radio
continuum images... | astro-ph | we analyze the distribution of the interstellar matter in the environs of the hii region gum 31 excited by the open cluster ngc 3324 located in the complex carina region with the aim of investigating the action of the massive stars on the surrounding neutral material we use 21cmline data radio continuum images at 0843 ... | [['we', 'analyze', 'the', 'distribution', 'of', 'the', 'interstellar', 'matter', 'in', 'the', 'environs', 'of', 'the', 'hii', 'region', 'gum', '31', 'excited', 'by', 'the', 'open', 'cluster', 'ngc', '3324', 'located', 'in', 'the', 'complex', 'carina', 'region', 'with', 'the', 'aim', 'of', 'investigating', 'the', 'actio... | [-0.0705980806631902, 0.07748767469928951, -0.022919437887245105, 0.043763134885464974, -0.02884918231345517, -0.009042392439094552, 0.05650992748049791, 0.4559461060976773, -0.14862100264024838, -0.30376920890912673, 0.05397445451541755, -0.2847714517428948, 0.029982935410940596, 0.12148723911061034, 0.019673120833753... |
707.2005 | INTEGRAL-ISGRI observations of the CygOB2 region: earching for hard
X-ray point sources in a region containing several non-thermal emitting
massive stars | Aims: We analyze INTEGRAL-ISGRI data in order to probe the hard X-ray
emission (above 20 keV) from point sources in the Cyg OB2 region and to
investigate the putative non-thermal high-energy emission from early-type stars
(Wolf-Rayet and O-type stars). Among the targets located in the field of view,
we focus on the s... | astro-ph | aims we analyze integralisgri data in order to probe the hard xray emission above 20 kev from point sources in the cyg ob2 region and to investigate the putative nonthermal highenergy emission from earlytype stars wolfrayet and otype stars among the targets located in the field of view we focus on the still unidentifie... | [['aims', 'we', 'analyze', 'integralisgri', 'data', 'in', 'order', 'to', 'probe', 'the', 'hard', 'xray', 'emission', 'above', '20', 'kev', 'from', 'point', 'sources', 'in', 'the', 'cyg', 'ob2', 'region', 'and', 'to', 'investigate', 'the', 'putative', 'nonthermal', 'highenergy', 'emission', 'from', 'earlytype', 'stars',... | [-0.06985983792560008, 0.09282550826377425, -0.0447812213085733, 0.14495171603671678, -0.1310329307488638, -0.09775502582950191, 0.08562169053649168, 0.4256985251619635, -0.16174323824057754, -0.37446060484072186, 0.07824002393859028, -0.3359380061495431, 0.014129517394696225, 0.25567195709889656, -0.02936679353593778,... |
707.2006 | Working Modes and Aspects in Fully-Parallel Manipulator | The aim of this paper is to characterize the notion of aspect in the
workspace and in the joint space for parallel manipulators. In opposite to the
serial manipulators, the parallel manipulators can admit not only multiple
inverse kinematic solutions, but also multiple direct kinematic solutions. The
notion of aspect... | cs.RO | the aim of this paper is to characterize the notion of aspect in the workspace and in the joint space for parallel manipulators in opposite to the serial manipulators the parallel manipulators can admit not only multiple inverse kinematic solutions but also multiple direct kinematic solutions the notion of aspect intro... | [['the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'characterize', 'the', 'notion', 'of', 'aspect', 'in', 'the', 'workspace', 'and', 'in', 'the', 'joint', 'space', 'for', 'parallel', 'manipulators', 'in', 'opposite', 'to', 'the', 'serial', 'manipulators', 'the', 'parallel', 'manipulators', 'can', 'admit', 'not', 'only'... | [-0.17172327854670585, 0.027430710936896502, -0.05881877735257149, 0.012006388622602181, -0.13304687560669012, -0.1249574541623172, -0.026087194945929305, 0.36926889519606315, -0.29175811270517965, -0.3060715724075479, 0.09727268716320396, -0.20665163593233696, -0.13770472857568944, 0.13920584084732193, -0.073787061258... |
707.2007 | Functions of q-positive type | In this paper we characterize the subspace of $\mathcal{L}_{q,1,v}$ of
function which are the q-Bessel Fourier transform of positive functions in
$\mathcal{L}_{q,1,v}$. As application we give a q-version of the Bochner's
theorem.
| math.CA | in this paper we characterize the subspace of mathcall_q1v of function which are the qbessel fourier transform of positive functions in mathcall_q1v as application we give a qversion of the bochners theorem | [['in', 'this', 'paper', 'we', 'characterize', 'the', 'subspace', 'of', 'mathcall_q1v', 'of', 'function', 'which', 'are', 'the', 'qbessel', 'fourier', 'transform', 'of', 'positive', 'functions', 'in', 'mathcall_q1v', 'as', 'application', 'we', 'give', 'a', 'qversion', 'of', 'the', 'bochners', 'theorem']] | [-0.12053299912561972, 0.01735533184061448, -0.16400227546691895, 0.10868869036979352, -0.040411650824050106, -0.026869269739836454, 0.008438640681561083, 0.3230368549625079, -0.3138398063679536, -0.17562017689148585, 0.14602033706226697, -0.24688188806176187, -0.24707961948588492, 0.23148601011683542, -0.1116111636782... |
707.2008 | Optimal Non-Linear Models for Sparsity and Sampling | Given a set of vectors (the data) in a Hilbert space H, we prove the
existence of an optimal collection of subspaces minimizing the sum of the
square of the distances between each vector and its closest subspace in the
collection. This collection of subspaces gives the best sparse representation
for the given data, i... | math.CA | given a set of vectors the data in a hilbert space h we prove the existence of an optimal collection of subspaces minimizing the sum of the square of the distances between each vector and its closest subspace in the collection this collection of subspaces gives the best sparse representation for the given data in a sen... | [['given', 'a', 'set', 'of', 'vectors', 'the', 'data', 'in', 'a', 'hilbert', 'space', 'h', 'we', 'prove', 'the', 'existence', 'of', 'an', 'optimal', 'collection', 'of', 'subspaces', 'minimizing', 'the', 'sum', 'of', 'the', 'square', 'of', 'the', 'distances', 'between', 'each', 'vector', 'and', 'its', 'closest', 'subspa... | [-0.1223833396617638, 0.07115751827858359, -0.025053648681471676, 0.02023456542191922, -0.03514717195451942, -0.08984640008535459, 0.04052897869907713, 0.3606127768518849, -0.3376170762250541, -0.20599320352497236, 0.13427530254096343, -0.272312598158671, -0.13979957806943377, 0.18482452899571772, -0.10790865073426509,... |
707.2009 | Exit problems associated with affine reflection groups | We obtain a formula for the distribution of the first exit time of Brownian
motion from the alcove of an affine Weyl group. In most cases the formula is
expressed compactly, in terms of Pfaffians. Expected exit times are derived in
the type \~A case. The results extend to other Markov processes. We also give
formulas... | math.PR math.GR | we obtain a formula for the distribution of the first exit time of brownian motion from the alcove of an affine weyl group in most cases the formula is expressed compactly in terms of pfaffians expected exit times are derived in the type a case the results extend to other markov processes we also give formulas for the ... | [['we', 'obtain', 'a', 'formula', 'for', 'the', 'distribution', 'of', 'the', 'first', 'exit', 'time', 'of', 'brownian', 'motion', 'from', 'the', 'alcove', 'of', 'an', 'affine', 'weyl', 'group', 'in', 'most', 'cases', 'the', 'formula', 'is', 'expressed', 'compactly', 'in', 'terms', 'of', 'pfaffians', 'expected', 'exit',... | [-0.12730790526364688, 0.09316414437148243, -0.0898474044551682, 0.06116936053724292, -0.08111233749415403, -0.08755789209663133, 0.009022195651023477, 0.3250999201612294, -0.2601588369694964, -0.20112855702546645, 0.13177969724796482, -0.271303543381186, -0.11748906919721191, 0.23350690258091983, -0.08771072033082025,... |
707.201 | Threshold Resummation in B --> X_c l nu_l Decays | We compute the QCD form factor resumming threshold logarithms in B --> X_c +
l + nu_l decays to next-to-leading logarithmic approximation. We present an
interpolation formula including soft as well as collinear effects softened by
the non-vanishing charm mass.
| hep-ph | we compute the qcd form factor resumming threshold logarithms in b x_c l nu_l decays to nexttoleading logarithmic approximation we present an interpolation formula including soft as well as collinear effects softened by the nonvanishing charm mass | [['we', 'compute', 'the', 'qcd', 'form', 'factor', 'resumming', 'threshold', 'logarithms', 'in', 'b', 'x_c', 'l', 'nu_l', 'decays', 'to', 'nexttoleading', 'logarithmic', 'approximation', 'we', 'present', 'an', 'interpolation', 'formula', 'including', 'soft', 'as', 'well', 'as', 'collinear', 'effects', 'softened', 'by',... | [-0.13006028538016048, 0.2150979611831497, -0.08298230659518693, 0.18841122727639772, -0.06123225194578235, -0.1056389502702734, 0.09880828501332577, 0.28244210235975886, -0.21823983226676244, -0.20490355001812852, -0.03769709869929765, -0.366178761362224, -0.02289269179911227, 0.05626432632876409, 0.10278319026268012,... |
707.2011 | The genetic code multiplet structure, in one number | The standard genetic code multiplet structure as well as the correct
degeneracies, class by class, are all extracted from the (unique) number 23,
the order of the permutation group of 23 objects.
| q-bio.OT | the standard genetic code multiplet structure as well as the correct degeneracies class by class are all extracted from the unique number 23 the order of the permutation group of 23 objects | [['the', 'standard', 'genetic', 'code', 'multiplet', 'structure', 'as', 'well', 'as', 'the', 'correct', 'degeneracies', 'class', 'by', 'class', 'are', 'all', 'extracted', 'from', 'the', 'unique', 'number', '23', 'the', 'order', 'of', 'the', 'permutation', 'group', 'of', '23', 'objects']] | [-0.07197594820172526, 0.10303736018249765, 0.05718680162681267, 0.11646102552185766, -0.07367001379316207, -0.07697401350014843, 0.014530292071867734, 0.3027124087093398, -0.3316028458211804, -0.45264904224313796, 0.1252123472349922, -0.26144280890002847, -0.12724147114204243, 0.1640779385343194, 0.022720529232174158,... |
707.2012 | Generalized motion of level sets by functions of their curvatures on
Riemannian manifolds | We consider the generalized evolution of compact level sets by functions of
their normal vectors and second fundamental forms on a Riemannian manifold M.
The level sets of a function $u:M\to\mathbb{R}$ evolve in such a way whenever u
solves an equation $u_{t}+F(Du, D^{2}u)=0$, for some real function F satisfying
a ge... | math.AP math.DG | we consider the generalized evolution of compact level sets by functions of their normal vectors and second fundamental forms on a riemannian manifold m the level sets of a function umtomathbbr evolve in such a way whenever u solves an equation u_tfdu d2u0 for some real function f satisfying a geometric condition we sh... | [['we', 'consider', 'the', 'generalized', 'evolution', 'of', 'compact', 'level', 'sets', 'by', 'functions', 'of', 'their', 'normal', 'vectors', 'and', 'second', 'fundamental', 'forms', 'on', 'a', 'riemannian', 'manifold', 'm', 'the', 'level', 'sets', 'of', 'a', 'function', 'umtomathbbr', 'evolve', 'in', 'such', 'a', 'w... | [-0.16211246310720323, 0.1300400168618378, -0.08530657794499011, 0.07843919597723505, -0.06692037758357064, -0.1524070936939097, -0.01650746838465609, 0.3648561442451965, -0.29220502263746717, -0.22205253342879047, 0.10969364771692737, -0.2658259335127729, -0.1543659301144847, 0.18643567441311595, -0.0734958462923748, ... |
707.2013 | Deconfinement Transition of AdS/QCD at ${\cal O}(\alpha'^3)$ | We study the confinement/deconfinement phase transition of holographic
AdS/QCD models by using Ricci flat $AdS_5$ black holes up to ${\cal
O}(\alpha'^3)$, which corresponds to the $\lambda$ expansion correction in the
dual field theory to $\lambda^{-3/2}$, where $\lambda$ is the 't Hooft coupling
constant. We conside... | hep-th gr-qc hep-ph | we study the confinementdeconfinement phase transition of holographic adsqcd models by using ricci flat ads_5 black holes up to cal oalpha3 which corresponds to the lambda expansion correction in the dual field theory to lambda32 where lambda is the t hooft coupling constant we consider two cases one is the hardwall ad... | [['we', 'study', 'the', 'confinementdeconfinement', 'phase', 'transition', 'of', 'holographic', 'adsqcd', 'models', 'by', 'using', 'ricci', 'flat', 'ads_5', 'black', 'holes', 'up', 'to', 'cal', 'oalpha3', 'which', 'corresponds', 'to', 'the', 'lambda', 'expansion', 'correction', 'in', 'the', 'dual', 'field', 'theory', '... | [-0.11057856521722287, 0.1990740421381205, -0.06208255212460581, 0.09066982399624428, -0.06688819888481641, -0.18289433165504407, -0.001827638660882893, 0.31873263274191893, -0.172476855762086, -0.19901745626623168, 0.06618864015494282, -0.318540713583974, -0.05293613577529482, 0.04365544395572315, 0.000286797786965545... |
707.2014 | On the error exponent of variable-length block-coding schemes over
finite-state Markov channels with feedback | The error exponent of Markov channels with feedback is studied in the
variable-length block-coding setting. Burnashev's classic result is extended
and a single letter characterization for the reliability function of
finite-state Markov channels is presented, under the assumption that the
channel state is causally obs... | cs.IT math.IT | the error exponent of markov channels with feedback is studied in the variablelength blockcoding setting burnashevs classic result is extended and a single letter characterization for the reliability function of finitestate markov channels is presented under the assumption that the channel state is causally observed bo... | [['the', 'error', 'exponent', 'of', 'markov', 'channels', 'with', 'feedback', 'is', 'studied', 'in', 'the', 'variablelength', 'blockcoding', 'setting', 'burnashevs', 'classic', 'result', 'is', 'extended', 'and', 'a', 'single', 'letter', 'characterization', 'for', 'the', 'reliability', 'function', 'of', 'finitestate', '... | [-0.13904686598357574, 0.07820212778945763, -0.07628699868256526, 0.0909499352640142, -0.05544318452850485, -0.25057890310743325, 0.0782663649366167, 0.4030250122029615, -0.33802487639089424, -0.2191417977734599, 0.14403611824281953, -0.242961748342921, -0.12018044628778733, 0.157193379636894, -0.10891991229828006, 0.1... |
707.2015 | Trapping of ultracold polar molecules with a Thin Wire Electrostatic
Trap | We describe the realization of a dc electric-field trap for ultracold polar
molecules, the thin-wire electrostatic trap (TWIST). The thin wires that form
the electrodes of the TWIST allow us to superimpose the trap onto a
magneto-optical trap (MOT). In our experiment, ultracold polar NaCs molecules
in their electroni... | physics.atom-ph | we describe the realization of a dc electricfield trap for ultracold polar molecules the thinwire electrostatic trap twist the thin wires that form the electrodes of the twist allow us to superimpose the trap onto a magnetooptical trap mot in our experiment ultracold polar nacs molecules in their electronic ground stat... | [['we', 'describe', 'the', 'realization', 'of', 'a', 'dc', 'electricfield', 'trap', 'for', 'ultracold', 'polar', 'molecules', 'the', 'thinwire', 'electrostatic', 'trap', 'twist', 'the', 'thin', 'wires', 'that', 'form', 'the', 'electrodes', 'of', 'the', 'twist', 'allow', 'us', 'to', 'superimpose', 'the', 'trap', 'onto',... | [-0.14352039461222926, 0.2230380095640888, -0.023051727319847833, -0.04966954453298927, 0.061922403512878366, -0.16224987510319674, 0.06832759529666117, 0.43548877788393686, -0.216653673365461, -0.23087384748492348, -0.018938807229082404, -0.22696197394993198, -0.0010752872762720236, 0.1840558511498018, 0.0112158219059... |
707.2016 | Spectropolarimetric observations of the transiting planetary system of
the K dwarf HD 189733 | With a Jupiter-mass planet orbiting at a distance of only 0.031 AU, the
active K2 dwarf HD 189733 is a potential candidate in which to study the
magnetospheric interactions of a cool star with its recently-discovered
close-orbiting giant planet. We decided to explore the strength and topology of
the large-scale magne... | astro-ph | with a jupitermass planet orbiting at a distance of only 0031 au the active k2 dwarf hd 189733 is a potential candidate in which to study the magnetospheric interactions of a cool star with its recentlydiscovered closeorbiting giant planet we decided to explore the strength and topology of the largescale magnetosphere ... | [['with', 'a', 'jupitermass', 'planet', 'orbiting', 'at', 'a', 'distance', 'of', 'only', '0031', 'au', 'the', 'active', 'k2', 'dwarf', 'hd', '189733', 'is', 'a', 'potential', 'candidate', 'in', 'which', 'to', 'study', 'the', 'magnetospheric', 'interactions', 'of', 'a', 'cool', 'star', 'with', 'its', 'recentlydiscovered... | [-0.17092314730011707, 0.1465440329601034, -0.032679379221500784, 0.041500750826570856, -0.11000291903802473, -0.10382601384423162, 0.039112010177238324, 0.37629859137352195, -0.1831394346142591, -0.36510540296521965, 0.06455958531900487, -0.27363987036330106, -0.09790732127795877, 0.21389826968823314, -0.0391368988366... |
707.2017 | The Isoconditioning Loci of A Class of Closed-Chain Manipulators | The subject of this paper is a special class of closed-chain manipulators.
First, we analyze a family of two-degree-of-freedom (dof) five-bar planar
linkages. Two Jacobian matrices appear in the kinematic relations between the
joint-rate and the Cartesian-velocity vectors, which are called the ``inverse
kinematics" a... | cs.RO | the subject of this paper is a special class of closedchain manipulators first we analyze a family of twodegreeoffreedom dof fivebar planar linkages two jacobian matrices appear in the kinematic relations between the jointrate and the cartesianvelocity vectors which are called the inverse kinematics and the direct kine... | [['the', 'subject', 'of', 'this', 'paper', 'is', 'a', 'special', 'class', 'of', 'closedchain', 'manipulators', 'first', 'we', 'analyze', 'a', 'family', 'of', 'twodegreeoffreedom', 'dof', 'fivebar', 'planar', 'linkages', 'two', 'jacobian', 'matrices', 'appear', 'in', 'the', 'kinematic', 'relations', 'between', 'the', 'j... | [-0.23780854246498825, 0.08447138923541482, -0.04164262062645164, -0.04420621906354991, -0.07237769266076644, -0.13866870707776077, 0.011018893973307749, 0.35185253491689417, -0.2732226297002414, -0.2518701371190877, 0.09645760070034784, -0.23774637499470905, -0.183726416374075, 0.1750508817458718, -0.07332409337596518... |
707.2018 | A signature of the donor star in the extra-galactic X-ray binary LMC X-2 | Two nights of phase-resolved medium resolution VLT spectroscopy of the
extra-galactic low mass X-ray binary LMC X-2 have revealed a 0.32+/-0.02 day
spectroscopic period in the radial velocity curve of the HeII lambda4686
emission line that we interpret as the orbital period. However, similar to
previous findings, thi... | astro-ph | two nights of phaseresolved medium resolution vlt spectroscopy of the extragalactic low mass xray binary lmc x2 have revealed a 032002 day spectroscopic period in the radial velocity curve of the heii lambda4686 emission line that we interpret as the orbital period however similar to previous findings this radial veloc... | [['two', 'nights', 'of', 'phaseresolved', 'medium', 'resolution', 'vlt', 'spectroscopy', 'of', 'the', 'extragalactic', 'low', 'mass', 'xray', 'binary', 'lmc', 'x2', 'have', 'revealed', 'a', '032002', 'day', 'spectroscopic', 'period', 'in', 'the', 'radial', 'velocity', 'curve', 'of', 'the', 'heii', 'lambda4686', 'emissi... | [-0.11423958908779615, 0.08105414364462261, -0.10642448568867754, 0.060413969970548785, -0.12478048935538738, -0.11623134219167841, 0.08423619250291249, 0.4556142898732858, -0.19764035298498286, -0.29860396181165383, 0.068010694244784, -0.2976003535128883, -0.02098739875591551, 0.23416588757964257, -0.0694243094302939,... |
707.2019 | From GHz to mHz: A Multiwavelength Study of the Acoustically Active 14
August 2004 M7.4 Solar Flare | We carried out an electromagnetic acoustic analysis of the solar flare of 14
August 2004 in active region AR10656 from the radio to the hard X-ray spectrum.
The flare was a GOES soft X-ray class M7.4 and produced a detectable sun quake,
confirming earlier inferences that relatively low-energy flares may be able to
ge... | astro-ph | we carried out an electromagnetic acoustic analysis of the solar flare of 14 august 2004 in active region ar10656 from the radio to the hard xray spectrum the flare was a goes soft xray class m74 and produced a detectable sun quake confirming earlier inferences that relatively lowenergy flares may be able to generate s... | [['we', 'carried', 'out', 'an', 'electromagnetic', 'acoustic', 'analysis', 'of', 'the', 'solar', 'flare', 'of', '14', 'august', '2004', 'in', 'active', 'region', 'ar10656', 'from', 'the', 'radio', 'to', 'the', 'hard', 'xray', 'spectrum', 'the', 'flare', 'was', 'a', 'goes', 'soft', 'xray', 'class', 'm74', 'and', 'produc... | [-0.07038431030858093, 0.2623069259564972, -0.01714874322846497, 0.16562566271393883, -0.0734031358844645, -0.04713672957047313, 0.04983746909162625, 0.4038603048847646, -0.2090037356061088, -0.3295122890889195, 0.06324125748748581, -0.290654854405494, -0.07408085288590796, 0.2165371777147663, -0.016255944984296628, -0... |
707.202 | Error exponents in hypothesis testing for correlated states on a spin
chain | We study various error exponents in a binary hypothesis testing problem and
extend recent results on the quantum Chernoff and Hoeffding bounds for product
states to a setting when both the null-hypothesis and the counter-hypothesis
can be correlated states on a spin chain. Our results apply to states
satisfying a cer... | quant-ph | we study various error exponents in a binary hypothesis testing problem and extend recent results on the quantum chernoff and hoeffding bounds for product states to a setting when both the nullhypothesis and the counterhypothesis can be correlated states on a spin chain our results apply to states satisfying a certain ... | [['we', 'study', 'various', 'error', 'exponents', 'in', 'a', 'binary', 'hypothesis', 'testing', 'problem', 'and', 'extend', 'recent', 'results', 'on', 'the', 'quantum', 'chernoff', 'and', 'hoeffding', 'bounds', 'for', 'product', 'states', 'to', 'a', 'setting', 'when', 'both', 'the', 'nullhypothesis', 'and', 'the', 'cou... | [-0.10767119841873121, 0.19165595592012707, -0.09977344884356798, 0.16081163018259784, 0.015995689916988493, -0.17922830657744912, 0.06426206883370982, 0.32720562014777976, -0.27338920730415367, -0.23038838889685945, 0.12116775256876743, -0.3033412999119347, -0.12378576445117803, 0.21797079459147553, -0.044611684059802... |
707.2021 | On-Shell Description of Unsteady Flames | The problem of non-perturbative description of unsteady premixed flames with
arbitrary gas expansion is solved in the two-dimensional case. Considering the
flame as a surface of discontinuity with arbitrary local burning rate and gas
velocity jumps given on it, we show that the front dynamics can be determined
withou... | physics.flu-dyn | the problem of nonperturbative description of unsteady premixed flames with arbitrary gas expansion is solved in the twodimensional case considering the flame as a surface of discontinuity with arbitrary local burning rate and gas velocity jumps given on it we show that the front dynamics can be determined without havi... | [['the', 'problem', 'of', 'nonperturbative', 'description', 'of', 'unsteady', 'premixed', 'flames', 'with', 'arbitrary', 'gas', 'expansion', 'is', 'solved', 'in', 'the', 'twodimensional', 'case', 'considering', 'the', 'flame', 'as', 'a', 'surface', 'of', 'discontinuity', 'with', 'arbitrary', 'local', 'burning', 'rate',... | [-0.1120680475872545, 0.11748797880461503, -0.0974549692609605, 0.023228658859226654, -0.07345929538999546, -0.09442534797795196, -0.02170097385533154, 0.32078207936137915, -0.3043975043457319, -0.22788660812805941, 0.11729335847454384, -0.24660900981410683, -0.08610860021175579, 0.21618742108880046, -0.002859903360157... |
707.2022 | W and Z Boson Production at sqrt(S)=1.96TeV with the D0 Detector | Preliminary measurements of the cross-section for the processes ppbar --> W
--> mu nu, e nu; ppbar --> Z --> mu mu, e e, tau tau from the D0 detector are
presented. Integrated luminosities for these data samples are 96 pb-1 for W -->
mu nu, 177.3 pb-1 for W --> e nu and Z --> e e, 148pb-1 for Z --> mu mu and 207
pb-1... | hep-ex | preliminary measurements of the crosssection for the processes ppbar w mu nu e nu ppbar z mu mu e e tau tau from the d0 detector are presented integrated luminosities for these data samples are 96 pb1 for w mu nu 1773 pb1 for w e nu and z e e 148pb1 for z mu mu and 207 pb1 for z tau tau a measurement of the muon charge... | [['preliminary', 'measurements', 'of', 'the', 'crosssection', 'for', 'the', 'processes', 'ppbar', 'w', 'mu', 'nu', 'e', 'nu', 'ppbar', 'z', 'mu', 'mu', 'e', 'e', 'tau', 'tau', 'from', 'the', 'd0', 'detector', 'are', 'presented', 'integrated', 'luminosities', 'for', 'these', 'data', 'samples', 'are', '96', 'pb1', 'for',... | [-0.02629487367705741, 0.21770638622634045, -0.023660886107832877, 0.1319003455050358, -0.005050464351704225, -0.17431204526796254, 0.06093098895320959, 0.35311008378043085, -0.17031187743563717, -0.3164507438078386, -0.09250069006000124, -0.42991661670011116, 0.2219188058569412, 0.1912542575513175, 0.15553729996990856... |
707.2023 | Quantum Dot Version of Berry's Phase: Half-Integer Orbital Angular
Momenta | We show that Berry's geometrical (topological) phase for circular quantum
dots with an odd number of electrons is equal to \pi and that eigenvalues of
the orbital angular momentum run over half-integer values. The non-zero value
of the Berry's phase is provided by axial symmetry and two-dimensionality of
the system. ... | cond-mat.mes-hall | we show that berrys geometrical topological phase for circular quantum dots with an odd number of electrons is equal to pi and that eigenvalues of the orbital angular momentum run over halfinteger values the nonzero value of the berrys phase is provided by axial symmetry and twodimensionality of the system its particul... | [['we', 'show', 'that', 'berrys', 'geometrical', 'topological', 'phase', 'for', 'circular', 'quantum', 'dots', 'with', 'an', 'odd', 'number', 'of', 'electrons', 'is', 'equal', 'to', 'pi', 'and', 'that', 'eigenvalues', 'of', 'the', 'orbital', 'angular', 'momentum', 'run', 'over', 'halfinteger', 'values', 'the', 'nonzero... | [-0.22047310925942534, 0.2506373148666171, -0.06965984166987861, -0.013934204604205054, -0.03634770762679788, -0.1420230224612169, 0.06191373820959901, 0.29655080793891103, -0.21075145432259887, -0.3051527358203506, 0.016585450303197528, -0.27913508204122384, -0.09046490527689457, 0.18507156665824975, -0.00269494065238... |
707.2024 | A muon-spin relaxation study of BiMnO3 | We present the results of muon-spin relaxation measurements on ferromagnetic
BiMnO3. Below T_C=98.0(1) K oscillations in the time-dependence of the muon
polarization are observed, characteristic of a quasistatic magnetic field at a
single muon site, allowing us to probe the critical behaviour associated with
the magn... | cond-mat.str-el | we present the results of muonspin relaxation measurements on ferromagnetic bimno3 below t_c9801 k oscillations in the timedependence of the muon polarization are observed characteristic of a quasistatic magnetic field at a single muon site allowing us to probe the critical behaviour associated with the magnetic phase ... | [['we', 'present', 'the', 'results', 'of', 'muonspin', 'relaxation', 'measurements', 'on', 'ferromagnetic', 'bimno3', 'below', 't_c9801', 'k', 'oscillations', 'in', 'the', 'timedependence', 'of', 'the', 'muon', 'polarization', 'are', 'observed', 'characteristic', 'of', 'a', 'quasistatic', 'magnetic', 'field', 'at', 'a'... | [-0.18388564336359256, 0.2500086913427727, -0.035758396748780875, 0.06823209088403158, -0.042861510753877216, -0.11309983010229828, 0.08409045385657349, 0.36338553913347016, -0.2367695630374518, -0.28868081658096106, 0.019999466123888372, -0.3313209915963503, -0.04132800676174216, 0.19669491679735154, 0.094252841958742... |
707.2025 | Toeplitz and Hankel operators and Dixmier traces on the unit ball of
\mathbb C^n | We compute the Dixmier trace of pseudo-Toeplitz operators on the Fock space.
As an application we find a formula for the Dixmier trace of the product of
commutators of Toeplitz operators on the Hardy and weighted Bergman spaces on
the unit ball of \mathbb C^d. This generalizes an earlier work of Helton-Howe
for the u... | math.CV math.FA | we compute the dixmier trace of pseudotoeplitz operators on the fock space as an application we find a formula for the dixmier trace of the product of commutators of toeplitz operators on the hardy and weighted bergman spaces on the unit ball of mathbb cd this generalizes an earlier work of heltonhowe for the usual tra... | [['we', 'compute', 'the', 'dixmier', 'trace', 'of', 'pseudotoeplitz', 'operators', 'on', 'the', 'fock', 'space', 'as', 'an', 'application', 'we', 'find', 'a', 'formula', 'for', 'the', 'dixmier', 'trace', 'of', 'the', 'product', 'of', 'commutators', 'of', 'toeplitz', 'operators', 'on', 'the', 'hardy', 'and', 'weighted',... | [-0.12085146408100597, 0.05799333638650915, -0.016786492506011587, 0.0927100729590404, -0.03989205991498149, 0.028038527022619716, 0.0034275223180407384, 0.3181995218161677, -0.28921710383757704, -0.11130913447771894, 0.1513300070416976, -0.2990471407252013, -0.12567079610756185, 0.18256578440243593, -0.139129846005654... |
707.2026 | Cotorsion pairs generated by modules of bounded projective dimension | We apply the theory of cotorsion pairs to study closure properties of classes
of modules with finite projective dimension with respect to direct limit
operations and to filtrations.
We also prove that if the ring is an order in an $\aleph_0$-noetherian ring Q
of small finitistic dimension 0, then the cotorsion pair... | math.RA math.RT | we apply the theory of cotorsion pairs to study closure properties of classes of modules with finite projective dimension with respect to direct limit operations and to filtrations we also prove that if the ring is an order in an aleph_0noetherian ring q of small finitistic dimension 0 then the cotorsion pair generated... | [['we', 'apply', 'the', 'theory', 'of', 'cotorsion', 'pairs', 'to', 'study', 'closure', 'properties', 'of', 'classes', 'of', 'modules', 'with', 'finite', 'projective', 'dimension', 'with', 'respect', 'to', 'direct', 'limit', 'operations', 'and', 'to', 'filtrations', 'we', 'also', 'prove', 'that', 'if', 'the', 'ring', '... | [-0.17036783784167486, 0.06048849351956572, -0.04602067522558101, 0.04693097335134706, -0.06006951203433734, -0.20864726387466606, -0.09257826772178367, 0.3304382506444046, -0.4092402756802759, -0.11715260754258298, 0.07375325676278745, -0.26035204194904715, -0.05332054607988743, 0.18300914339553775, -0.143190416889369... |
707.2027 | Workspace and Assembly modes in Fully-Parallel Manipulators : A
Descriptive Study | The goal of this paper is to explain, using a typical example, the
distribution of the different assembly modes in the workspace and their
effective role in the execution of trajectories. The singular and non-singular
changes of assembly mode are described and compared to each other. The
non-singular change of assemb... | cs.RO | the goal of this paper is to explain using a typical example the distribution of the different assembly modes in the workspace and their effective role in the execution of trajectories the singular and nonsingular changes of assembly mode are described and compared to each other the nonsingular change of assembly mode ... | [['the', 'goal', 'of', 'this', 'paper', 'is', 'to', 'explain', 'using', 'a', 'typical', 'example', 'the', 'distribution', 'of', 'the', 'different', 'assembly', 'modes', 'in', 'the', 'workspace', 'and', 'their', 'effective', 'role', 'in', 'the', 'execution', 'of', 'trajectories', 'the', 'singular', 'and', 'nonsingular',... | [-0.1187834834315731, 0.09542345096089758, -0.08452839777565165, 0.05637644259213, -0.03162755605091553, -0.07552574749224551, -0.02394751387090413, 0.3804058721381249, -0.25855928097418185, -0.30426801169247336, 0.14591100258121065, -0.2436069465048685, -0.12923046410784567, 0.17427212125299, -0.08466218630460524, 0.0... |
707.2028 | Mass Outflows from Dissipative Shocks in Hot Accretion Flows | We consider stationary, axisymmetric hydrodynamic accretion flows in Kerr
geometry. As a plausible means of efficiently separating a small population of
nonthermal particles from the bulk accretion flows, we investigate the
formation of standing dissipative shocks, i.e. shocks at which fraction of the
energy, angular... | astro-ph | we consider stationary axisymmetric hydrodynamic accretion flows in kerr geometry as a plausible means of efficiently separating a small population of nonthermal particles from the bulk accretion flows we investigate the formation of standing dissipative shocks ie shocks at which fraction of the energy angular momentum... | [['we', 'consider', 'stationary', 'axisymmetric', 'hydrodynamic', 'accretion', 'flows', 'in', 'kerr', 'geometry', 'as', 'a', 'plausible', 'means', 'of', 'efficiently', 'separating', 'a', 'small', 'population', 'of', 'nonthermal', 'particles', 'from', 'the', 'bulk', 'accretion', 'flows', 'we', 'investigate', 'the', 'for... | [-0.11963564338612531, 0.17429567282457495, -0.038723785496460134, 0.11422534013578955, -0.08538297593342857, -0.08307835108403547, 0.028547903642846414, 0.3576888892477235, -0.21713569628504606, -0.31472496047902565, 0.07673285075445445, -0.27793741124109006, 0.03171419650316239, 0.2453174658124156, -0.013718909607716... |
707.2029 | Lifting SU(3)-structures to nearly parallel G_{2}-structures | Hitchin shows that half-flat SU(3)-structures on a 6-dimensional manifold M
can be lifted to parallel G_{2}-structure on the product $M\times\mathbb{R}$.
We show that Hitchin's approach can also be used to construct nearly parallel
G_{2}-structures by lifting so-called nearly half-flat structures. These
SU(3)-structu... | math.DG math-ph math.MP | hitchin shows that halfflat su3structures on a 6dimensional manifold m can be lifted to parallel g_2structure on the product mtimesmathbbr we show that hitchins approach can also be used to construct nearly parallel g_2structures by lifting socalled nearly halfflat structures these su3structures are described by pairs ... | [['hitchin', 'shows', 'that', 'halfflat', 'su3structures', 'on', 'a', '6dimensional', 'manifold', 'm', 'can', 'be', 'lifted', 'to', 'parallel', 'g_2structure', 'on', 'the', 'product', 'mtimesmathbbr', 'we', 'show', 'that', 'hitchins', 'approach', 'can', 'also', 'be', 'used', 'to', 'construct', 'nearly', 'parallel', 'g_... | [-0.2326011203906753, 0.1266520148376003, -0.05863499067385088, 0.0830463290129873, -0.13698824828659947, -0.18429133510217072, -0.10278931541199034, 0.42678047438914124, -0.2568793028931726, -0.27129377393813975, 0.1123036129146137, -0.19243606742132793, -0.16916722587563776, 0.2212624349927699, -0.10329901679334315, ... |
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