id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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709.0535 | Constructing packings in Grassmannian manifolds via alternating
projection | This paper describes a numerical method for finding good packings in
Grassmannian manifolds equipped with various metrics. This investigation also
encompasses packing in projective spaces. In each case, producing a good
packing is equivalent to constructing a matrix that has certain structural and
spectral properties... | math.MG | this paper describes a numerical method for finding good packings in grassmannian manifolds equipped with various metrics this investigation also encompasses packing in projective spaces in each case producing a good packing is equivalent to constructing a matrix that has certain structural and spectral properties by a... | [['this', 'paper', 'describes', 'a', 'numerical', 'method', 'for', 'finding', 'good', 'packings', 'in', 'grassmannian', 'manifolds', 'equipped', 'with', 'various', 'metrics', 'this', 'investigation', 'also', 'encompasses', 'packing', 'in', 'projective', 'spaces', 'in', 'each', 'case', 'producing', 'a', 'good', 'packing... | [-0.09596369781479971, 0.11062483775195169, -0.10509530992955655, 0.05225270064304829, -0.054456248345207764, -0.15928605712230312, -0.014981369978599708, 0.43513452524942076, -0.26320706886964984, -0.26283516068342916, 0.12369524836225972, -0.2593275517442384, -0.21311592847463087, 0.20540235815512622, -0.088686865285... |
709.0536 | Quantum Gravity Corrections to the One Loop Scalar Self-Mass during
Inflation | We compute the one loop corrections from quantum gravity to the
self-mass-squared of a massless, minimally coupled scalar on a locally de
Sitter background. The calculation was done using dimensional regularization
and renormalized by subtracting fourth order BPHZ counterterms. Our result
should determine whether qua... | gr-qc astro-ph hep-th | we compute the one loop corrections from quantum gravity to the selfmasssquared of a massless minimally coupled scalar on a locally de sitter background the calculation was done using dimensional regularization and renormalized by subtracting fourth order bphz counterterms our result should determine whether quantum gr... | [['we', 'compute', 'the', 'one', 'loop', 'corrections', 'from', 'quantum', 'gravity', 'to', 'the', 'selfmasssquared', 'of', 'a', 'massless', 'minimally', 'coupled', 'scalar', 'on', 'a', 'locally', 'de', 'sitter', 'background', 'the', 'calculation', 'was', 'done', 'using', 'dimensional', 'regularization', 'and', 'renorm... | [-0.13946945533940666, 0.22559702085951963, -0.14281059661063186, 0.131986871855987, -0.09948543152003958, -0.1720155043151687, -0.034910982458856314, 0.2268208856939485, -0.1473065376804586, -0.26979170105697814, 0.025937443460223444, -0.29661338831902595, -0.1402468449485145, 0.1367462212546614, -0.029282817698753717... |
709.0537 | Modeling core collapse supernovae in 2 and 3 dimensions with spectral
neutrino transport | The overwhelming evidence that the core collapse supernova mechanism is
inherently multidimensional, the complexity of the physical processes involved,
and the increasing evidence from simulations that the explosion is marginal
presents great computational challenges for the realistic modeling of this
event, particul... | astro-ph | the overwhelming evidence that the core collapse supernova mechanism is inherently multidimensional the complexity of the physical processes involved and the increasing evidence from simulations that the explosion is marginal presents great computational challenges for the realistic modeling of this event particularly ... | [['the', 'overwhelming', 'evidence', 'that', 'the', 'core', 'collapse', 'supernova', 'mechanism', 'is', 'inherently', 'multidimensional', 'the', 'complexity', 'of', 'the', 'physical', 'processes', 'involved', 'and', 'the', 'increasing', 'evidence', 'from', 'simulations', 'that', 'the', 'explosion', 'is', 'marginal', 'p... | [-0.11042408382508723, 0.13918284633511827, -0.04463471234700362, 0.06461811291074714, -0.04089213873835174, -0.08869130932915259, 0.02906399702535454, 0.35262154773392573, -0.2503927310406253, -0.31571612194392495, 0.0988942339388858, -0.2649268785404511, -0.06727342384964856, 0.15854882751425872, 0.027967171416034907... |
709.0538 | Markov-Chain Monte Carlo Methods for Simulations of Biomolecules | The computer revolution has been driven by a sustained increase of
computational speed of approximately one order of magnitude (a factor of ten)
every five years since about 1950. In natural sciences this has led to a
continuous increase of the importance of computer simulations. Major enabling
techniques are Markov ... | cond-mat.stat-mech cond-mat.soft | the computer revolution has been driven by a sustained increase of computational speed of approximately one order of magnitude a factor of ten every five years since about 1950 in natural sciences this has led to a continuous increase of the importance of computer simulations major enabling techniques are markov chain ... | [['the', 'computer', 'revolution', 'has', 'been', 'driven', 'by', 'a', 'sustained', 'increase', 'of', 'computational', 'speed', 'of', 'approximately', 'one', 'order', 'of', 'magnitude', 'a', 'factor', 'of', 'ten', 'every', 'five', 'years', 'since', 'about', '1950', 'in', 'natural', 'sciences', 'this', 'has', 'led', 'to... | [-0.07130908764963549, 0.12481862457146994, -0.06330284738696103, 0.06563508068649028, -0.025675812266991102, -0.11664333941653035, 0.021437892529245158, 0.42683535520183413, -0.2737348473602836, -0.33560528430284203, 0.16199765734801672, -0.26700315598566504, -0.13422158731259687, 0.24349590903848298, 0.00517713801263... |
709.0539 | Causal sets and conservation laws in tests of Lorentz symmetry | Many of the most important astrophysical tests of Lorentz symmetry also
assume that energy-momentum of the observed particles is exactly conserved. In
the causal set approach to quantum gravity a particular kind of Lorentz
symmetry holds but energy-momentum conservation may be violated. We show that
incorrectly assum... | gr-qc | many of the most important astrophysical tests of lorentz symmetry also assume that energymomentum of the observed particles is exactly conserved in the causal set approach to quantum gravity a particular kind of lorentz symmetry holds but energymomentum conservation may be violated we show that incorrectly assuming ex... | [['many', 'of', 'the', 'most', 'important', 'astrophysical', 'tests', 'of', 'lorentz', 'symmetry', 'also', 'assume', 'that', 'energymomentum', 'of', 'the', 'observed', 'particles', 'is', 'exactly', 'conserved', 'in', 'the', 'causal', 'set', 'approach', 'to', 'quantum', 'gravity', 'a', 'particular', 'kind', 'of', 'loren... | [-0.1684249390406078, 0.1967924238296644, -0.07712979110109867, 0.1483471415454655, -0.1716752189724725, -0.14045402349200936, -0.016287271705532104, 0.28131585788665986, -0.19603814549710868, -0.3307283033607338, 0.05645241204777504, -0.2492450850122437, -0.08844700092402268, 0.16629349635153703, -0.0211404426574555, ... |
709.054 | Implications of very rapid TeV variability in blazars | We discuss the implications of rapid (few-minute) variability in the TeV flux
of blazars, which has been observed recently with the HESS and MAGIC
telescopes. The variability timescales seen in PKS 2155-304 and Mrk 501 are
much shorter than inferred light-crossing times at the black hole horizon,
suggesting that the ... | astro-ph | we discuss the implications of rapid fewminute variability in the tev flux of blazars which has been observed recently with the hess and magic telescopes the variability timescales seen in pks 2155304 and mrk 501 are much shorter than inferred lightcrossing times at the black hole horizon suggesting that the variabilit... | [['we', 'discuss', 'the', 'implications', 'of', 'rapid', 'fewminute', 'variability', 'in', 'the', 'tev', 'flux', 'of', 'blazars', 'which', 'has', 'been', 'observed', 'recently', 'with', 'the', 'hess', 'and', 'magic', 'telescopes', 'the', 'variability', 'timescales', 'seen', 'in', 'pks', '2155304', 'and', 'mrk', '501', ... | [-0.1052476322789952, 0.16535116285899357, -0.02874802094293942, 0.16700881933481893, -0.08273818575068784, -0.08103091073301162, 0.003334910966272295, 0.42330014825024653, -0.17902573848694142, -0.34844445311267613, 0.0841362244354456, -0.28260733781080744, 0.020343894215995893, 0.23572417968575857, -0.023322062434064... |
709.0541 | Soft Spin Wave Near nu=1: Evidence for a Magnetic Instability in
Skyrmion Systems | The ground state of the two dimensional electron gas near $\nu$=1 is
investigated by inelastic light scattering measurements carried down to very
low temperatures. Away from $\nu$=1, the ferromagnetic spin wave collapses and
a new low-energy spin wave emerges below the Zeeman gap. The emergent spin wave
shows soft be... | cond-mat.mes-hall cond-mat.str-el | the ground state of the two dimensional electron gas near nu1 is investigated by inelastic light scattering measurements carried down to very low temperatures away from nu1 the ferromagnetic spin wave collapses and a new lowenergy spin wave emerges below the zeeman gap the emergent spin wave shows soft behavior as its ... | [['the', 'ground', 'state', 'of', 'the', 'two', 'dimensional', 'electron', 'gas', 'near', 'nu1', 'is', 'investigated', 'by', 'inelastic', 'light', 'scattering', 'measurements', 'carried', 'down', 'to', 'very', 'low', 'temperatures', 'away', 'from', 'nu1', 'the', 'ferromagnetic', 'spin', 'wave', 'collapses', 'and', 'a',... | [-0.20146769412106252, 0.27627235458541943, -0.0465704523497215, 0.0717692200225861, -0.02191343843835489, -0.13377869001469841, 0.07297250430680591, 0.34416738962109134, -0.23515505316012567, -0.29244536484619327, 0.014923309399008678, -0.30719091816076843, -0.024528443061811202, 0.16306210191699094, 0.140456472653235... |
709.0542 | The largest oxigen bearing organic molecule repository | We present the first detection of complex aldehydes and isomers in three
typical molecular clouds located within 200pc of the center of our Galaxy.
We find very large abundances of these complex organic molecules (COMs) in
the central molecular zone (CMZ), which we attribute to the ejection of COMs
from grain mantl... | astro-ph | we present the first detection of complex aldehydes and isomers in three typical molecular clouds located within 200pc of the center of our galaxy we find very large abundances of these complex organic molecules coms in the central molecular zone cmz which we attribute to the ejection of coms from grain mantles by shoc... | [['we', 'present', 'the', 'first', 'detection', 'of', 'complex', 'aldehydes', 'and', 'isomers', 'in', 'three', 'typical', 'molecular', 'clouds', 'located', 'within', '200pc', 'of', 'the', 'center', 'of', 'our', 'galaxy', 'we', 'find', 'very', 'large', 'abundances', 'of', 'these', 'complex', 'organic', 'molecules', 'com... | [-0.05640616143564372, 0.11313844797334768, -0.02947170744877532, 0.05649214827622961, 0.018931976824779973, 0.011091661663116535, 0.03136464404178277, 0.4227731911946208, -0.21295975682578877, -0.31217946272589103, -0.013490197804814402, -0.24662854495857442, -0.03882510347875513, 0.16189797926900162, -0.0052765628380... |
709.0543 | Stellar Wind Accretion in GX301-2: Evidence for a High-density Stream | The X-ray binary system GX301-2 consists of a neutron star in an eccentric
orbit accreting from the massive early-type star WRAY 977. It has previously
been shown that the X-ray orbital light curve is consistent with existence of a
gas stream flowing out from Wray 977 in addition to its strong stellar wind.
Here, X-r... | astro-ph | the xray binary system gx3012 consists of a neutron star in an eccentric orbit accreting from the massive earlytype star wray 977 it has previously been shown that the xray orbital light curve is consistent with existence of a gas stream flowing out from wray 977 in addition to its strong stellar wind here xray monitor... | [['the', 'xray', 'binary', 'system', 'gx3012', 'consists', 'of', 'a', 'neutron', 'star', 'in', 'an', 'eccentric', 'orbit', 'accreting', 'from', 'the', 'massive', 'earlytype', 'star', 'wray', '977', 'it', 'has', 'previously', 'been', 'shown', 'that', 'the', 'xray', 'orbital', 'light', 'curve', 'is', 'consistent', 'with'... | [-0.09654152429332415, 0.13372510102113933, -0.04383028441839722, 0.08746886761410096, -0.06466088390100258, -0.04167394840577803, 0.05921334005749424, 0.429014652678038, -0.19277777212608857, -0.3745754951039752, 0.09523753328313792, -0.32055641267359614, -0.008649059587095186, 0.21052265117052513, -0.0526436448330987... |
709.0544 | The Many Computations Interpretation (MCI) of Quantum Mechanics | Computationalism provides a framework for understanding how a mathematically
describable physical world could give rise to conscious observations without
the need for dualism. A criterion is proposed for the implementation of
computations by physical systems, which has been a problem for
computationalism. Together wi... | quant-ph | computationalism provides a framework for understanding how a mathematically describable physical world could give rise to conscious observations without the need for dualism a criterion is proposed for the implementation of computations by physical systems which has been a problem for computationalism together with an... | [['computationalism', 'provides', 'a', 'framework', 'for', 'understanding', 'how', 'a', 'mathematically', 'describable', 'physical', 'world', 'could', 'give', 'rise', 'to', 'conscious', 'observations', 'without', 'the', 'need', 'for', 'dualism', 'a', 'criterion', 'is', 'proposed', 'for', 'the', 'implementation', 'of', ... | [-0.07495694035230754, 0.059742923406719335, -0.17374777354434742, 0.11671345443874832, -0.1352503004735746, -0.17129592190689916, 0.08009935945452559, 0.3103410425250354, -0.22351740004052553, -0.2988286930950558, 0.08196937608966054, -0.19867030448579, -0.15829818895959394, 0.23676161648289729, -0.0893217131390043, 0... |
709.0545 | Did supermassive black holes form by direct collapse? | Rapid infall of gas in the nuclei of galaxies could lead to the formation of
black holes by direct collapse, without first forming stars. Black holes formed
in this way would have initial masses of a few solar masses, but would be
embedded in massive envelopes that would allow them to grow at a highly
super-Eddington... | astro-ph | rapid infall of gas in the nuclei of galaxies could lead to the formation of black holes by direct collapse without first forming stars black holes formed in this way would have initial masses of a few solar masses but would be embedded in massive envelopes that would allow them to grow at a highly supereddington rate ... | [['rapid', 'infall', 'of', 'gas', 'in', 'the', 'nuclei', 'of', 'galaxies', 'could', 'lead', 'to', 'the', 'formation', 'of', 'black', 'holes', 'by', 'direct', 'collapse', 'without', 'first', 'forming', 'stars', 'black', 'holes', 'formed', 'in', 'this', 'way', 'would', 'have', 'initial', 'masses', 'of', 'a', 'few', 'sola... | [-0.10825415694722487, 0.2137199301845551, -0.02954923960620935, 0.14213458032375795, -0.10017680188410738, -0.06223505589681981, 0.04262904484306326, 0.33888756044292717, -0.15710241485680088, -0.34494276181533096, 0.11008653248362034, -0.2503117259089532, -0.0033652780765897772, 0.20929331016423328, -0.02815495310037... |
709.0546 | Vector fields and foliations associated to groups of projective
automorphisms | We introduce and give normal forms for (one-dimensional) Riccati foliations
(vector fields) on $\ov \bc \times \bc P(2)$ and $\ov \bc \times \ov \bc^n$.
These are foliations are characterized by transversality with the generic fiber
of the first projection and we prove they are conjugate {\em in some invariant
Zarisk... | math.CV math.DS | we introduce and give normal forms for onedimensional riccati foliations vector fields on ov bc times bc p2 and ov bc times ov bcn these are foliations are characterized by transversality with the generic fiber of the first projection and we prove they are conjugate em in some invariant zariski open subset to the suspe... | [['we', 'introduce', 'and', 'give', 'normal', 'forms', 'for', 'onedimensional', 'riccati', 'foliations', 'vector', 'fields', 'on', 'ov', 'bc', 'times', 'bc', 'p2', 'and', 'ov', 'bc', 'times', 'ov', 'bcn', 'these', 'are', 'foliations', 'are', 'characterized', 'by', 'transversality', 'with', 'the', 'generic', 'fiber', 'o... | [-0.27901590604300575, 0.08958331072978952, -0.08311304691489096, 0.02699904077949382, -0.06731064562444333, -0.21851308436749536, -0.015234639292531129, 0.38715252215560114, -0.3214498957688058, -0.14930881116608227, 0.11611581675566009, -0.24008032315652128, -0.10054849580477888, 0.16670017993224232, -0.1120874613126... |
709.0547 | C^*- Actions on Stein analytic spaces with isolated singularities | Let $V$ be an irreducible complex analytic space of dimension two with normal
singularities and $\vr:\mathbb{C^*}\times V\to V$ a holomorphic action of the
group $\mathbb{C^*}$ on $V$. Denote by $\fa_\vr$ the foliation on $V$ induced
by $\vr$. The leaves of this foliation are the one-dimensional orbits of $\vr$.
%and... | math.CV math.DS | let v be an irreducible complex analytic space of dimension two with normal singularities and vrmathbbctimes vto v a holomorphic action of the group mathbbc on v denote by fa_vr the foliation on v induced by vr the leaves of this foliation are the onedimensional orbits of vr and its singularities are the fixed points o... | [['let', 'v', 'be', 'an', 'irreducible', 'complex', 'analytic', 'space', 'of', 'dimension', 'two', 'with', 'normal', 'singularities', 'and', 'vrmathbbctimes', 'vto', 'v', 'a', 'holomorphic', 'action', 'of', 'the', 'group', 'mathbbc', 'on', 'v', 'denote', 'by', 'fa_vr', 'the', 'foliation', 'on', 'v', 'induced', 'by', 'v... | [-0.21688994082311788, 0.08113450086283434, -0.08885702296015872, 0.03879793970643416, -0.06147417730100873, -0.16553807853253236, -0.030458143567382204, 0.38389034064687755, -0.27720514951632336, -0.16499908858507942, 0.08350797553553285, -0.3199607744909158, -0.14621884635750187, 0.1725801836760461, -0.11527364086818... |
709.0548 | Quantum discord and the power of one qubit | We use quantum discord to characterize the correlations present in the
quantum computational model DQC1, introduced by Knill and Laflamme [Phys. Rev.
Lett. 81, 5672 (1998)]. The model involves a collection of qubits in the
completely mixed state coupled to a single control qubit that has nonzero
purity. The initial s... | quant-ph | we use quantum discord to characterize the correlations present in the quantum computational model dqc1 introduced by knill and laflamme phys rev lett 81 5672 1998 the model involves a collection of qubits in the completely mixed state coupled to a single control qubit that has nonzero purity the initial state operatio... | [['we', 'use', 'quantum', 'discord', 'to', 'characterize', 'the', 'correlations', 'present', 'in', 'the', 'quantum', 'computational', 'model', 'dqc1', 'introduced', 'by', 'knill', 'and', 'laflamme', 'phys', 'rev', 'lett', '81', '5672', '1998', 'the', 'model', 'involves', 'a', 'collection', 'of', 'qubits', 'in', 'the', ... | [-0.1628601491264999, 0.15830375443818048, -0.05452053363621235, -0.011248537965118885, 0.04429679211601615, -0.21860719687864186, 0.07536645148321987, 0.32192091563344, -0.22142370712757112, -0.30338383945822717, -0.0155365029014647, -0.2726234526187181, -0.13004069294780493, 0.18550370023399593, -0.10515220897644759,... |
709.0549 | Explicit Connections with SU(2)-Monodromy | The pure braid group \Gamma of a quadruply-punctured Riemann sphere acts on
the SL(2,C)-moduli M of the representation variety of such sphere. The points
in M are classified into \Gamma-orbits. We show that, in this case, the
monodromy groups of many explicit solutions to the Riemann-Hilbert problem are
subgroups of ... | math.AG math.CA | the pure braid group gamma of a quadruplypunctured riemann sphere acts on the sl2cmoduli m of the representation variety of such sphere the points in m are classified into gammaorbits we show that in this case the monodromy groups of many explicit solutions to the riemannhilbert problem are subgroups of su2 most of the... | [['the', 'pure', 'braid', 'group', 'gamma', 'of', 'a', 'quadruplypunctured', 'riemann', 'sphere', 'acts', 'on', 'the', 'sl2cmoduli', 'm', 'of', 'the', 'representation', 'variety', 'of', 'such', 'sphere', 'the', 'points', 'in', 'm', 'are', 'classified', 'into', 'gammaorbits', 'we', 'show', 'that', 'in', 'this', 'case', ... | [-0.18513969537743832, 0.10208424708107486, -0.08176759073976428, 0.04864229230879573, -0.08274976048851386, -0.09688549127313309, -0.03181855974253267, 0.3950543209211901, -0.25500570854201215, -0.26874485281296073, 0.1372119912179187, -0.3057375839096494, -0.16010515658417718, 0.20410029595077503, -0.1034048200875986... |
709.055 | Possible Outlet of Test on Violation of Pauli Exclusion Principle | The present experimental tests have proved high precisely the validity of the
Pauli exclusion principle (PEP) in usual cases. The future experiments should
be combined widely with various theories of hidden and obvious violation of
PEP. Author think that known experiments and theories seem to imply the
violation at h... | physics.gen-ph | the present experimental tests have proved high precisely the validity of the pauli exclusion principle pep in usual cases the future experiments should be combined widely with various theories of hidden and obvious violation of pep author think that known experiments and theories seem to imply the violation at high en... | [['the', 'present', 'experimental', 'tests', 'have', 'proved', 'high', 'precisely', 'the', 'validity', 'of', 'the', 'pauli', 'exclusion', 'principle', 'pep', 'in', 'usual', 'cases', 'the', 'future', 'experiments', 'should', 'be', 'combined', 'widely', 'with', 'various', 'theories', 'of', 'hidden', 'and', 'obvious', 'vi... | [-0.08110210491535287, 0.18764504772885668, -0.05884721816773694, 0.1388066318254623, -0.05511849801216891, -0.16923383524199184, 0.05142204649997674, 0.305732583761108, -0.2251873824430509, -0.3316559071531988, 0.09738015230969532, -0.2765782314533596, -0.0843519539096587, 0.18754297798154407, -0.0017675625096684952, ... |
709.0551 | Quantum Gravity Phenomenology without Lorentz Invariance Violation: a
detailed proposal | We describe a scheme for the exploration of quantum gravity phenomenology
focussing on effects that could be thought as arising from a fundamental
granularity of space-time. In contrast with the simplest assumptions, such
granularity is assumed to respect Lorentz Invariance but is otherwise left
unspecified. The prop... | gr-qc hep-th | we describe a scheme for the exploration of quantum gravity phenomenology focussing on effects that could be thought as arising from a fundamental granularity of spacetime in contrast with the simplest assumptions such granularity is assumed to respect lorentz invariance but is otherwise left unspecified the proposal i... | [['we', 'describe', 'a', 'scheme', 'for', 'the', 'exploration', 'of', 'quantum', 'gravity', 'phenomenology', 'focussing', 'on', 'effects', 'that', 'could', 'be', 'thought', 'as', 'arising', 'from', 'a', 'fundamental', 'granularity', 'of', 'spacetime', 'in', 'contrast', 'with', 'the', 'simplest', 'assumptions', 'such', ... | [-0.13038812994042737, 0.16963244356864363, -0.11260055493426706, 0.10135773872238917, -0.13101308545847465, -0.16300210514353639, -0.01765071073602543, 0.3558661696765948, -0.26092110415322517, -0.2970046522336106, 0.10341102974019398, -0.20528234053539848, -0.1519029280512568, 0.16076069924160155, -0.0875382827842659... |
709.0552 | Cancer Genesis and Progression as Dynamics in Functional Landscape of
Endogenous Molecular-Cellular Network | An endogenous molecular-cellular network for both normal and abnormal
functions is assumed to exist. This endogenous network forms a nonlinear
stochastic dynamical system, with many stable attractors in its functional
landscape. Normal or abnormal robust states can be decided by this network in a
manner similar to th... | q-bio.SC q-bio.MN | an endogenous molecularcellular network for both normal and abnormal functions is assumed to exist this endogenous network forms a nonlinear stochastic dynamical system with many stable attractors in its functional landscape normal or abnormal robust states can be decided by this network in a manner similar to the neur... | [['an', 'endogenous', 'molecularcellular', 'network', 'for', 'both', 'normal', 'and', 'abnormal', 'functions', 'is', 'assumed', 'to', 'exist', 'this', 'endogenous', 'network', 'forms', 'a', 'nonlinear', 'stochastic', 'dynamical', 'system', 'with', 'many', 'stable', 'attractors', 'in', 'its', 'functional', 'landscape', ... | [-0.08096540452066078, 0.10797256180268124, -0.08414815259449235, 0.15710047083494655, -0.05803702828298147, -0.19030023244842006, 0.0469963530792754, 0.35042451878040526, -0.2797125782817602, -0.2311540786019602, 0.12391012845674178, -0.2430471367473286, -0.24831944355911045, 0.18862350470845815, -0.12465475582851197,... |
709.0553 | The On The Fly Imaging Technique | The On-The-Fly (OTF) imaging technique enables single-dish radio telescopes
to construct images of small areas of the sky with greater efficiency and
accuracy. This paper describes the practical application of the OTF imaging
technique. By way of example the implementation of the OTF imaging technique at
the NRAO 12 ... | astro-ph | the onthefly otf imaging technique enables singledish radio telescopes to construct images of small areas of the sky with greater efficiency and accuracy this paper describes the practical application of the otf imaging technique by way of example the implementation of the otf imaging technique at the nrao 12 meter tel... | [['the', 'onthefly', 'otf', 'imaging', 'technique', 'enables', 'singledish', 'radio', 'telescopes', 'to', 'construct', 'images', 'of', 'small', 'areas', 'of', 'the', 'sky', 'with', 'greater', 'efficiency', 'and', 'accuracy', 'this', 'paper', 'describes', 'the', 'practical', 'application', 'of', 'the', 'otf', 'imaging',... | [-0.08524986472553932, 0.02802371150061775, -0.021595230089643827, 0.03838657315533895, -0.09804960825982002, -0.12483130808059986, 0.008603458588298123, 0.45264229006492174, -0.19402657588227437, -0.4150401042057918, 0.16862495180505974, -0.2472368371887849, -0.12154385986236425, 0.2897505219309376, -0.065903352265461... |
709.0554 | Strong Imbalanced Turbulence | We consider stationary, forced, imbalanced, or cross-helical MHD Alfvenic
turbulence where the waves traveling in one direction have higher amplitudes
than the opposite waves. This paper is dedicated to so-called strong
turbulence, which cannot be treated perturbatively. Our main result is that the
anisotropy of the ... | astro-ph | we consider stationary forced imbalanced or crosshelical mhd alfvenic turbulence where the waves traveling in one direction have higher amplitudes than the opposite waves this paper is dedicated to socalled strong turbulence which cannot be treated perturbatively our main result is that the anisotropy of the weak waves... | [['we', 'consider', 'stationary', 'forced', 'imbalanced', 'or', 'crosshelical', 'mhd', 'alfvenic', 'turbulence', 'where', 'the', 'waves', 'traveling', 'in', 'one', 'direction', 'have', 'higher', 'amplitudes', 'than', 'the', 'opposite', 'waves', 'this', 'paper', 'is', 'dedicated', 'to', 'socalled', 'strong', 'turbulence... | [-0.1745586891770363, 0.18934879327937962, -0.08687159216031431, 0.15261410241760315, -0.11924590280279518, -0.14041802694648503, 0.0016619829935953022, 0.2926198260039091, -0.24332758279144764, -0.2692312831804156, 0.05099214303586632, -0.23107535499799997, -0.13157940971665083, 0.17239736945554615, -0.028648976743221... |
709.0555 | Applications of Cutoff Resolvent Estimates to the Wave Equation | We consider solutions to the linear wave equation on non-compact Riemannian
manifolds without boundary when the geodesic flow admits a filamentary
hyperbolic trapped set. We obtain a polynomial rate of local energy decay with
exponent depending only on the dimension.
| math.AP | we consider solutions to the linear wave equation on noncompact riemannian manifolds without boundary when the geodesic flow admits a filamentary hyperbolic trapped set we obtain a polynomial rate of local energy decay with exponent depending only on the dimension | [['we', 'consider', 'solutions', 'to', 'the', 'linear', 'wave', 'equation', 'on', 'noncompact', 'riemannian', 'manifolds', 'without', 'boundary', 'when', 'the', 'geodesic', 'flow', 'admits', 'a', 'filamentary', 'hyperbolic', 'trapped', 'set', 'we', 'obtain', 'a', 'polynomial', 'rate', 'of', 'local', 'energy', 'decay', ... | [-0.2208596252137795, 0.10187811269424855, -0.04901913459179923, 0.052948461426422, -0.1679835126924445, -0.17512016834225505, -0.024741198332048953, 0.30714236134663225, -0.2700684058945626, -0.1700511043309234, 0.13884886414161884, -0.30363665356417185, -0.07526054172776639, 0.2082358158309944, -0.02381503077049274, ... |
709.0556 | Phonon bottleneck in the low-excitation limit | The phonon-bottleneck problem in the relaxation of two-level systems (spins)
via direct phonon processes is considered numerically in the weak-excitation
limit where the Schroedinger equation for the spin-phonon system simplifies.
The solution for the relaxing spin excitation p(t), emitted phonons n_k(t),
etc. is obt... | cond-mat.stat-mech cond-mat.mtrl-sci | the phononbottleneck problem in the relaxation of twolevel systems spins via direct phonon processes is considered numerically in the weakexcitation limit where the schroedinger equation for the spinphonon system simplifies the solution for the relaxing spin excitation pt emitted phonons n_kt etc is obtained in terms o... | [['the', 'phononbottleneck', 'problem', 'in', 'the', 'relaxation', 'of', 'twolevel', 'systems', 'spins', 'via', 'direct', 'phonon', 'processes', 'is', 'considered', 'numerically', 'in', 'the', 'weakexcitation', 'limit', 'where', 'the', 'schroedinger', 'equation', 'for', 'the', 'spinphonon', 'system', 'simplifies', 'the... | [-0.1766325227225562, 0.21391440997987785, 0.011049754945748804, 0.03431954342991445, -0.029433878113659436, -0.15788277236107212, 0.0337170009945063, 0.3359324404713541, -0.28206154540331174, -0.23990362971371051, 0.019330048719155384, -0.32224055213366176, -0.035411739089032446, 0.17249709570267857, 0.072935112974693... |
709.0557 | General observations on series whose terms proceed as the sines and
cosines of multiples of angles | Translated from the Latin original, "Observationes generales circa series,
quarum termini secundum sinus vel cosinus angulorum multiplorum progrediuntur"
(1777). E655 in the Enestrom index. Euler looks at the binomial expansion
$(1+x)^n$ for $x=\cos \phi+i\sin\phi$. He does $n=$ positive and negative
integers, and $n... | math.HO math.CA | translated from the latin original observationes generales circa series quarum termini secundum sinus vel cosinus angulorum multiplorum progrediuntur 1777 e655 in the enestrom index euler looks at the binomial expansion 1xn for xcos phiisinphi he does n positive and negative integers and n12 12 and particular values of... | [['translated', 'from', 'the', 'latin', 'original', 'observationes', 'generales', 'circa', 'series', 'quarum', 'termini', 'secundum', 'sinus', 'vel', 'cosinus', 'angulorum', 'multiplorum', 'progrediuntur', '1777', 'e655', 'in', 'the', 'enestrom', 'index', 'euler', 'looks', 'at', 'the', 'binomial', 'expansion', '1xn', '... | [-0.09781940931099511, 0.12274081377489936, -0.07314071325319153, 0.06975621386386809, -0.05537447492991175, -0.2352615162020638, -0.00590886775656448, 0.24972516525581123, -0.22098029768537908, -0.23408300346428795, 0.055880286428700424, -0.3925734301973578, -0.0716554108352977, 0.11433508426749281, -0.100523588535863... |
709.0558 | Strain dependent twist-stretch elasticity in chiral filaments | Coupling between axial and torsional degrees of freedom often modifies the
conformation and expression of natural and synthetic filamentous aggregates.
Recent studies on chiral single-walled carbon nanotubes and B-DNA reveal a
reversal in the sign of the twist-stretch coupling at large strains. The
similarity in the ... | cond-mat.mtrl-sci cond-mat.soft | coupling between axial and torsional degrees of freedom often modifies the conformation and expression of natural and synthetic filamentous aggregates recent studies on chiral singlewalled carbon nanotubes and bdna reveal a reversal in the sign of the twiststretch coupling at large strains the similarity in the respons... | [['coupling', 'between', 'axial', 'and', 'torsional', 'degrees', 'of', 'freedom', 'often', 'modifies', 'the', 'conformation', 'and', 'expression', 'of', 'natural', 'and', 'synthetic', 'filamentous', 'aggregates', 'recent', 'studies', 'on', 'chiral', 'singlewalled', 'carbon', 'nanotubes', 'and', 'bdna', 'reveal', 'a', '... | [-0.16407772600525777, 0.175941617359351, -0.04983482569778001, 0.005254390494797954, -0.06565460841477717, -0.14099743521941088, 0.0407666190521129, 0.4063440739620952, -0.2966901596710586, -0.33285916986056424, 0.02711517460591116, -0.24391658919169598, -0.23091544096526884, 0.12631123293434965, 0.05017663602914111, ... |
709.0559 | New Rotating Non-Extremal Black Holes in D=5 Maximal Gauged Supergravity | We obtain new non-extremal rotating black hole solutions in maximal
five-dimensional gauged supergravity. They are characterised by five
parameters, associated with the mass, the two angular momenta, and two
independently-specifiable charge parameters. Two of the three charges
associated with the U(1)^3 Cartan subgro... | hep-th gr-qc | we obtain new nonextremal rotating black hole solutions in maximal fivedimensional gauged supergravity they are characterised by five parameters associated with the mass the two angular momenta and two independentlyspecifiable charge parameters two of the three charges associated with the u13 cartan subgroup of the so6... | [['we', 'obtain', 'new', 'nonextremal', 'rotating', 'black', 'hole', 'solutions', 'in', 'maximal', 'fivedimensional', 'gauged', 'supergravity', 'they', 'are', 'characterised', 'by', 'five', 'parameters', 'associated', 'with', 'the', 'mass', 'the', 'two', 'angular', 'momenta', 'and', 'two', 'independentlyspecifiable', '... | [-0.1823143747227251, 0.17753952868344852, -0.005785125731067224, 0.13832334358214346, -0.11176762382369027, -0.1975276780291653, -0.03837598420002244, 0.3264963001028196, -0.1528585516166496, -0.2814809324081279, 0.10959479098654668, -0.3134448219029125, -0.07786580157650957, 0.15959176131762748, -0.10506145335533772,... |
709.056 | Time-Domain Studies of Very-Large-Angle Magnetization Dynamics Excited
by Spin Transfer Torques | We describe time-domain measurements which provide new information about the
large-angle nonlinear dynamics of nanomagnets excited by spin-transfer torque
from a spin-polarized current. Sampling-oscilloscope measurements, which
average over thousands of experimental time traces, show that the mean reversal
time for s... | cond-mat.mtrl-sci | we describe timedomain measurements which provide new information about the largeangle nonlinear dynamics of nanomagnets excited by spintransfer torque from a spinpolarized current samplingoscilloscope measurements which average over thousands of experimental time traces show that the mean reversal time for spintransfe... | [['we', 'describe', 'timedomain', 'measurements', 'which', 'provide', 'new', 'information', 'about', 'the', 'largeangle', 'nonlinear', 'dynamics', 'of', 'nanomagnets', 'excited', 'by', 'spintransfer', 'torque', 'from', 'a', 'spinpolarized', 'current', 'samplingoscilloscope', 'measurements', 'which', 'average', 'over', ... | [-0.23209184179455042, 0.19338079063699115, -0.0565900171995163, 0.008544887909665703, -0.07352425747364759, -0.09569209746830165, 0.05166478423774242, 0.3852617466300726, -0.2822147034853697, -0.3450737212896347, 0.05431567916087806, -0.22367680380088859, -0.08492706680856645, 0.2657190612964332, 0.05341403718083165, ... |
709.0561 | Quantifying Stochastic Effects in Biochemical Reaction Networks using
Partitioned Leaping | "Leaping" methods show great promise for significantly accelerating
stochastic simulations of complex biochemical reaction networks. However, few
practical applications of leaping have appeared in the literature to date.
Here, we address this issue using the "partitioned leaping algorithm" (PLA)
[L.A. Harris and P. C... | q-bio.SC physics.chem-ph q-bio.QM | leaping methods show great promise for significantly accelerating stochastic simulations of complex biochemical reaction networks however few practical applications of leaping have appeared in the literature to date here we address this issue using the partitioned leaping algorithm pla la harris and p clancy j chem phy... | [['leaping', 'methods', 'show', 'great', 'promise', 'for', 'significantly', 'accelerating', 'stochastic', 'simulations', 'of', 'complex', 'biochemical', 'reaction', 'networks', 'however', 'few', 'practical', 'applications', 'of', 'leaping', 'have', 'appeared', 'in', 'the', 'literature', 'to', 'date', 'here', 'we', 'add... | [-0.0630356837911835, 0.04306546733562794, -0.06402494419655894, 0.08302130595193771, -0.08561744991596282, -0.15843659802086893, 0.061606457034308136, 0.3983327592672456, -0.26818409961908957, -0.30887747308715124, 0.0897649343197649, -0.2278859330830449, -0.2563410219964166, 0.22773379077831202, -0.11198164547828998,... |
709.0562 | Quantum Coherence Conservation by Growth in Environmental Dissipation
Rate | Quantum coherence conservation is shown to be achieved by a very high rate of
dissipation of an environmental system coupled with a principal system. This
effect is not in the list of previously-known strategies of noise suppression,
such as Zeno effect, dynamical decoupling, quantum error correction code, and
decohe... | quant-ph | quantum coherence conservation is shown to be achieved by a very high rate of dissipation of an environmental system coupled with a principal system this effect is not in the list of previouslyknown strategies of noise suppression such as zeno effect dynamical decoupling quantum error correction code and decoherence fr... | [['quantum', 'coherence', 'conservation', 'is', 'shown', 'to', 'be', 'achieved', 'by', 'a', 'very', 'high', 'rate', 'of', 'dissipation', 'of', 'an', 'environmental', 'system', 'coupled', 'with', 'a', 'principal', 'system', 'this', 'effect', 'is', 'not', 'in', 'the', 'list', 'of', 'previouslyknown', 'strategies', 'of', ... | [-0.1950119076220821, 0.1416976134457267, -0.061912214273607796, 0.039718792242720055, 0.02342777523431885, -0.2231380184131329, 0.027156208882505976, 0.3292773593363635, -0.2733423205908765, -0.288903773280928, 0.0666620527116812, -0.2665272218625197, -0.11309718962214636, 0.2260448884041038, -0.07372560040774138, 0.1... |
709.0563 | Deterministic dense coding and entanglement entropy | We present an analytical study of the standard two-party deterministic
dense-coding protocol, under which communication of perfectly distinguishable
messages takes place via a qudit from a pair of non-maximally entangled qudits
in pure state |S>. Our results include the following: (i) We prove that it is
possible for... | quant-ph | we present an analytical study of the standard twoparty deterministic densecoding protocol under which communication of perfectly distinguishable messages takes place via a qudit from a pair of nonmaximally entangled qudits in pure state s our results include the following i we prove that it is possible for a state s w... | [['we', 'present', 'an', 'analytical', 'study', 'of', 'the', 'standard', 'twoparty', 'deterministic', 'densecoding', 'protocol', 'under', 'which', 'communication', 'of', 'perfectly', 'distinguishable', 'messages', 'takes', 'place', 'via', 'a', 'qudit', 'from', 'a', 'pair', 'of', 'nonmaximally', 'entangled', 'qudits', '... | [-0.16223332522193265, 0.14278649483546538, -0.037801408755079466, -0.04186354435122981, -0.0022594485884514927, -0.25457642191942675, 0.10348974199308449, 0.2857994175196199, -0.1771292974046327, -0.271393388744757, 0.03322884009086971, -0.28189842967175344, -0.12895330222145107, 0.17025802115296126, -0.06717921634178... |
709.0564 | 3-bounded property in a triangle-free distance-regular graph | Let $\Gamma$ denote a distance-regular graph with classical parameters $(D,
b, \alpha, \beta)$ and $D\geq 3$. Assume the intersection numbers $a_1=0$ and
$a_2\not=0$. We show $\Gamma$ is 3-bounded in the sense of the article
[D-bounded distance-regular graphs, European Journal of Combinatorics(1997)18,
211-229].
| math.CO | let gamma denote a distanceregular graph with classical parameters d b alpha beta and dgeq 3 assume the intersection numbers a_10 and a_2not0 we show gamma is 3bounded in the sense of the article dbounded distanceregular graphs european journal of combinatorics199718 211229 | [['let', 'gamma', 'denote', 'a', 'distanceregular', 'graph', 'with', 'classical', 'parameters', 'd', 'b', 'alpha', 'beta', 'and', 'dgeq', '3', 'assume', 'the', 'intersection', 'numbers', 'a_10', 'and', 'a_2not0', 'we', 'show', 'gamma', 'is', '3bounded', 'in', 'the', 'sense', 'of', 'the', 'article', 'dbounded', 'distanc... | [-0.19832553143205586, 0.19396571500692517, -0.008901556179625913, 0.0012093474302673712, -0.08826736183837056, -0.22109476452460514, 0.05118653055324103, 0.3178651247173548, -0.278917497524526, -0.25088092433288695, 0.01587312432238832, -0.3537251145578921, -0.12578993039205671, 0.13479332122951745, -0.107484749658033... |
709.0565 | Orthosymplectic Lie superalgebras in superspace analogues of quantum
Kepler problems | A Schroedinger type equation on the superspace R^{D|2n} is studied, which
involves a potential inversely proportional to the negative of the osp(D|2n)
invariant "distance" away from the origin. An osp(2,D+1|2n) dynamical
supersymmetry for the system is explicitly constructed, and the bound states of
the system are sh... | math-ph hep-th math.MP math.RT | a schroedinger type equation on the superspace rd2n is studied which involves a potential inversely proportional to the negative of the ospd2n invariant distance away from the origin an osp2d12n dynamical supersymmetry for the system is explicitly constructed and the bound states of the system are shown to form an irre... | [['a', 'schroedinger', 'type', 'equation', 'on', 'the', 'superspace', 'rd2n', 'is', 'studied', 'which', 'involves', 'a', 'potential', 'inversely', 'proportional', 'to', 'the', 'negative', 'of', 'the', 'ospd2n', 'invariant', 'distance', 'away', 'from', 'the', 'origin', 'an', 'osp2d12n', 'dynamical', 'supersymmetry', 'fo... | [-0.14195703385738917, 0.08824040900630238, -0.05238716355200077, 0.04429294637453114, -0.061495566421166756, -0.09236480018562572, -0.0209956496065959, 0.29908984115477216, -0.29657390802492234, -0.255164748577531, 0.10286239619491362, -0.28109538932547495, -0.16129292142685764, 0.1567540584608566, -0.0192167124667659... |
709.0566 | Discovering Patterns in Multi-neuronal Spike Trains using the Frequent
Episode Method | Discovering the 'Neural Code' from multi-neuronal spike trains is an
important task in neuroscience. For such an analysis, it is important to
unearth interesting regularities in the spiking patterns. In this report, we
present an efficient method for automatically discovering synchrony, synfire
chains, and more gener... | cs.DB q-bio.NC | discovering the neural code from multineuronal spike trains is an important task in neuroscience for such an analysis it is important to unearth interesting regularities in the spiking patterns in this report we present an efficient method for automatically discovering synchrony synfire chains and more general sequence... | [['discovering', 'the', 'neural', 'code', 'from', 'multineuronal', 'spike', 'trains', 'is', 'an', 'important', 'task', 'in', 'neuroscience', 'for', 'such', 'an', 'analysis', 'it', 'is', 'important', 'to', 'unearth', 'interesting', 'regularities', 'in', 'the', 'spiking', 'patterns', 'in', 'this', 'report', 'we', 'presen... | [-0.08268270603268696, 0.08296340021158263, -0.06480491520387345, 0.1454488689593714, -0.06373658825097413, -0.11877919359389565, 0.06452608714522473, 0.4247803557728385, -0.2997228169749523, -0.32465772671175414, 0.09847769598428417, -0.24881594825921388, -0.2694881354940349, 0.2161229328075745, -0.07267771191766549, ... |
709.0567 | Isotopic dependence of the giant monopole resonance in the even-A
^{112-124}Sn isotopes and the asymmetry term in nuclear incompressibility | The strength distributions of the giant monopole resonance (GMR) have been
measured in the even-A Sn isotopes (A=112--124) with inelastic scattering of
400-MeV $\alpha$ particles in the angular range
$0^\circ$--$8.5^\circ$. We find that the experimentally-observed GMR energies
of the Sn isotopes are lower than the ... | nucl-ex | the strength distributions of the giant monopole resonance gmr have been measured in the evena sn isotopes a112124 with inelastic scattering of 400mev alpha particles in the angular range 0circ85circ we find that the experimentallyobserved gmr energies of the sn isotopes are lower than the values predicted by theoretic... | [['the', 'strength', 'distributions', 'of', 'the', 'giant', 'monopole', 'resonance', 'gmr', 'have', 'been', 'measured', 'in', 'the', 'evena', 'sn', 'isotopes', 'a112124', 'with', 'inelastic', 'scattering', 'of', '400mev', 'alpha', 'particles', 'in', 'the', 'angular', 'range', '0circ85circ', 'we', 'find', 'that', 'the',... | [-0.012179691898577575, 0.16886275739090728, -0.056762343237200114, 0.11604347605334854, 0.01575061777434194, -0.0762626274748222, 0.00749581112656035, 0.3599534270506871, -0.1289448221508838, -0.36734554574742345, -0.09194058730396666, -0.3687442082652374, 0.019243574235864615, 0.18856451131957525, 0.12101021920377979... |
709.0568 | Plastic flow in polycrystal states in a binary mixture | Using molecular dynamics simulation we examine dynamics in sheared
polycrystal states in a binary mixture containing 10% larger particles in two
dimensions. We find large stress fluctuations arising from sliding motions of
the particles at the grain boundaries, which occur cooperatively to release the
elastic energy ... | cond-mat.soft | using molecular dynamics simulation we examine dynamics in sheared polycrystal states in a binary mixture containing 10 larger particles in two dimensions we find large stress fluctuations arising from sliding motions of the particles at the grain boundaries which occur cooperatively to release the elastic energy store... | [['using', 'molecular', 'dynamics', 'simulation', 'we', 'examine', 'dynamics', 'in', 'sheared', 'polycrystal', 'states', 'in', 'a', 'binary', 'mixture', 'containing', '10', 'larger', 'particles', 'in', 'two', 'dimensions', 'we', 'find', 'large', 'stress', 'fluctuations', 'arising', 'from', 'sliding', 'motions', 'of', '... | [-0.15667974221287295, 0.25267763159936296, -0.05190136539458763, 0.006375732773449272, 0.0005382558185374365, -0.07472936198464594, 0.020964620597078466, 0.3679461902705953, -0.31617119116708636, -0.3153066873084754, 0.036558292365225495, -0.290348720329348, -0.08828746301587671, 0.09072751370986225, 0.050686535402201... |
709.0569 | Observations of Sunspot Oscillations in G band and Ca II H line with
Solar Optical Telescope on Hinode | Exploiting high-resolution observations made by the Solar Optical Telescope
onboard Hinode, we investigate the spatial distribution of power spectral
density of oscillatory signal in and around NOAA active region 10935. The
G-band data show that in the umbra the oscillatory power is suppressed in all
frequency ranges... | astro-ph | exploiting highresolution observations made by the solar optical telescope onboard hinode we investigate the spatial distribution of power spectral density of oscillatory signal in and around noaa active region 10935 the gband data show that in the umbra the oscillatory power is suppressed in all frequency ranges on th... | [['exploiting', 'highresolution', 'observations', 'made', 'by', 'the', 'solar', 'optical', 'telescope', 'onboard', 'hinode', 'we', 'investigate', 'the', 'spatial', 'distribution', 'of', 'power', 'spectral', 'density', 'of', 'oscillatory', 'signal', 'in', 'and', 'around', 'noaa', 'active', 'region', '10935', 'the', 'gba... | [-0.11991323496615283, 0.17279235499310652, -0.011519004302176316, 0.04749760393934586, -0.04566952107812871, -0.08213759810001828, 0.02358622302893888, 0.42477447213220204, -0.25699694466696327, -0.3155776786979688, 0.08742570447108193, -0.31889090942572956, -0.10225168159924262, 0.20317376918382635, -0.03837240473145... |
709.057 | Holographic Thermodynamics at Finite Baryon Density: Some Exact Results | We use the AdS/CFT correspondence to study the thermodynamics of massive N=2
supersymmetric hypermultiplets coupled to N=4 supersymmetric SU(Nc) Yang-Mills
theory in the limits of large Nc and large 't Hooft coupling. In particular, we
study the theory at finite baryon number density. At zero temperature, we
present ... | hep-th | we use the adscft correspondence to study the thermodynamics of massive n2 supersymmetric hypermultiplets coupled to n4 supersymmetric sunc yangmills theory in the limits of large nc and large t hooft coupling in particular we study the theory at finite baryon number density at zero temperature we present an exact expr... | [['we', 'use', 'the', 'adscft', 'correspondence', 'to', 'study', 'the', 'thermodynamics', 'of', 'massive', 'n2', 'supersymmetric', 'hypermultiplets', 'coupled', 'to', 'n4', 'supersymmetric', 'sunc', 'yangmills', 'theory', 'in', 'the', 'limits', 'of', 'large', 'nc', 'and', 'large', 't', 'hooft', 'coupling', 'in', 'parti... | [-0.13330524748364314, 0.20000973409191145, -0.033264942572295536, 0.08085318847324502, -0.03286931286277497, -0.10540326588696479, 0.0351279873145431, 0.2867087642827063, -0.14990667047687864, -0.27204335642055466, 0.011918666134835674, -0.3194289231194859, -0.10497440213123255, 0.05042764819762875, -0.003652132264610... |
709.0571 | Thermoacoustic effects in supercritical fluids near the critical point:
Resonance, piston effect, and acoustic emission and reflection | We present a general theory of thermoacoustic phenomena in supercritical
fluids near the critical point in a one-dimensional cell. We take into account
the effects of the heat conduction in the boundary walls and the bulk viscosity
near the critical point. We introduce a coefficient $Z(\omega)$ characterizing
reflect... | cond-mat.stat-mech | we present a general theory of thermoacoustic phenomena in supercritical fluids near the critical point in a onedimensional cell we take into account the effects of the heat conduction in the boundary walls and the bulk viscosity near the critical point we introduce a coefficient zomega characterizing reflection of sou... | [['we', 'present', 'a', 'general', 'theory', 'of', 'thermoacoustic', 'phenomena', 'in', 'supercritical', 'fluids', 'near', 'the', 'critical', 'point', 'in', 'a', 'onedimensional', 'cell', 'we', 'take', 'into', 'account', 'the', 'effects', 'of', 'the', 'heat', 'conduction', 'in', 'the', 'boundary', 'walls', 'and', 'the'... | [-0.16463982714507897, 0.16934680247360523, -0.05164946483968346, 0.015167329883043494, -0.04854811246397796, -0.0844219796787444, 0.06713010751965313, 0.31736816049696087, -0.3004210751444974, -0.1885955984293072, 0.11731025438466286, -0.30017173139017644, -0.13752622773392578, 0.16735663762429376, 0.00741396843548025... |
709.0572 | Separation of accelerated electrons and positrons in the relativistic
reconnection | We study an acceleration of electrons and positrons in the relativistic
magnetic field reconnection using a 2.5-D particle-in-cell electromagnetic
relativistic code. We consider the model with two current sheets and periodic
boundary conditions. The electrons and positrons are very effectively
accelerated during the ... | astro-ph | we study an acceleration of electrons and positrons in the relativistic magnetic field reconnection using a 25d particleincell electromagnetic relativistic code we consider the model with two current sheets and periodic boundary conditions the electrons and positrons are very effectively accelerated during the tearing ... | [['we', 'study', 'an', 'acceleration', 'of', 'electrons', 'and', 'positrons', 'in', 'the', 'relativistic', 'magnetic', 'field', 'reconnection', 'using', 'a', '25d', 'particleincell', 'electromagnetic', 'relativistic', 'code', 'we', 'consider', 'the', 'model', 'with', 'two', 'current', 'sheets', 'and', 'periodic', 'boun... | [-0.13866084661992592, 0.22627069638953784, -0.03725169285658806, 0.11802170794170605, 0.01156789346206342, -0.07215795875157392, -0.03297215668181519, 0.39205727341865737, -0.24042466253278746, -0.32647150272266967, -0.04468587941272066, -0.2602692807919257, -0.0071271780253728, 0.1904400902706021, 0.05667492133077411... |
709.0573 | Inhomogeneous preheating in multi-field models of cosmological
perturbation | We consider inhomogeneous preheating in multi-field models of cosmological
perturbation. After preheating, two fields are trapped at an enhanced symmetric
point. One field is an oscillating field and the other is a light field that
plays an important role in generating perturbation. In this presentation, we
consider ... | hep-ph astro-ph hep-th | we consider inhomogeneous preheating in multifield models of cosmological perturbation after preheating two fields are trapped at an enhanced symmetric point one field is an oscillating field and the other is a light field that plays an important role in generating perturbation in this presentation we consider two type... | [['we', 'consider', 'inhomogeneous', 'preheating', 'in', 'multifield', 'models', 'of', 'cosmological', 'perturbation', 'after', 'preheating', 'two', 'fields', 'are', 'trapped', 'at', 'an', 'enhanced', 'symmetric', 'point', 'one', 'field', 'is', 'an', 'oscillating', 'field', 'and', 'the', 'other', 'is', 'a', 'light', 'f... | [-0.20837431792169808, 0.207111737554078, -0.06805455992844972, 0.09422051492782141, -0.030395032973452047, -0.13180005255747926, -0.1141141130504283, 0.38926673572171816, -0.22849454889920626, -0.23523183719001034, 0.08974653188012202, -0.25274042642717676, -0.14364702942019159, 0.19705903966995802, -0.012928246996704... |
709.0574 | Solutions of nonlinear PDEs in the completion of uniform convergence
spaces | This paper deals with the solution of large classes of systems of nonlinear
partial differential equations (PDEs) in spaces of generalized functions that
are constructed as the completion of uniform convergence spaces. The existence
result for the mentioned systems of equations are obtained as an application of
a bas... | math.AP math.GN | this paper deals with the solution of large classes of systems of nonlinear partial differential equations pdes in spaces of generalized functions that are constructed as the completion of uniform convergence spaces the existence result for the mentioned systems of equations are obtained as an application of a basic ap... | [['this', 'paper', 'deals', 'with', 'the', 'solution', 'of', 'large', 'classes', 'of', 'systems', 'of', 'nonlinear', 'partial', 'differential', 'equations', 'pdes', 'in', 'spaces', 'of', 'generalized', 'functions', 'that', 'are', 'constructed', 'as', 'the', 'completion', 'of', 'uniform', 'convergence', 'spaces', 'the',... | [-0.14066832298024867, 0.047823064957750225, -0.06092261751570428, 0.10084211517144771, -0.0477535571437329, -0.0366062646266073, -0.029704586167645174, 0.31896246909163894, -0.3015246777717645, -0.2400311315645619, 0.17748937549379964, -0.23508219614159315, -0.15910994618510207, 0.20979690309613944, -0.097243359925535... |
709.0575 | Electronic Orbital Currents and Polarization in Mott Insulators | The standard view is that at low energies Mott insulators exhibit only
magnetic properties while charge degrees of freedom are frozen out as the
electrons become localized by a strong Coulomb repulsion. We demonstrate that
this is in general not true: for certain spin textures {\it spontaneous
circular electric curre... | cond-mat.str-el | the standard view is that at low energies mott insulators exhibit only magnetic properties while charge degrees of freedom are frozen out as the electrons become localized by a strong coulomb repulsion we demonstrate that this is in general not true for certain spin textures it spontaneous circular electric currents or... | [['the', 'standard', 'view', 'is', 'that', 'at', 'low', 'energies', 'mott', 'insulators', 'exhibit', 'only', 'magnetic', 'properties', 'while', 'charge', 'degrees', 'of', 'freedom', 'are', 'frozen', 'out', 'as', 'the', 'electrons', 'become', 'localized', 'by', 'a', 'strong', 'coulomb', 'repulsion', 'we', 'demonstrate',... | [-0.15718906088166426, 0.2709626837363728, -0.03169155247056874, 0.10536805128300057, -0.0407934630938118, -0.14771896796997322, 0.03665619283026763, 0.3997134795395013, -0.24500483771020146, -0.2990601335208271, 0.0268945219082253, -0.2925414891791678, -0.12299113406225273, 0.1451928867310042, 0.04110703261778037, -0.... |
709.0576 | A Spitzer Search for Water in the Transiting Exoplanet HD189733b | We present Spitzer Space Telescope observations of the extrasolar planet
HD189733b primary transit, obtained simultaneously at 3.6 and 5.8 microns with
the Infrared Array Camera. The system parameters, including planetary radius,
stellar radius, and impact parameter are derived from fits to the transit light
curves a... | astro-ph | we present spitzer space telescope observations of the extrasolar planet hd189733b primary transit obtained simultaneously at 36 and 58 microns with the infrared array camera the system parameters including planetary radius stellar radius and impact parameter are derived from fits to the transit light curves at both wa... | [['we', 'present', 'spitzer', 'space', 'telescope', 'observations', 'of', 'the', 'extrasolar', 'planet', 'hd189733b', 'primary', 'transit', 'obtained', 'simultaneously', 'at', '36', 'and', '58', 'microns', 'with', 'the', 'infrared', 'array', 'camera', 'the', 'system', 'parameters', 'including', 'planetary', 'radius', '... | [-0.09192335053376155, 0.1398446442981367, -0.05398130521462008, 0.0444192051918435, -0.08982134997313551, -0.11585849064431386, 0.06984926691075088, 0.4051323004750884, -0.1741602868096379, -0.38968599195504794, 0.1287467209958777, -0.30385998944257153, -0.06192767791435472, 0.21439089341765794, -0.08989958781603491, ... |
709.0577 | Magnetic field dependence of the electrical conductivity in V3Ge in the
vicinity of Hc2 | The phase transition from the Abrikosov state to the normal state with
superconducting fluctuations observed below the second critical field and
well-known as vortex lattice melting was one of the most popular problems in
the nineties. This problem had became popular after the discovery of high-Tc
superconductors bec... | cond-mat.supr-con cond-mat.stat-mech | the phase transition from the abrikosov state to the normal state with superconducting fluctuations observed below the second critical field and wellknown as vortex lattice melting was one of the most popular problems in the nineties this problem had became popular after the discovery of hightc superconductors because ... | [['the', 'phase', 'transition', 'from', 'the', 'abrikosov', 'state', 'to', 'the', 'normal', 'state', 'with', 'superconducting', 'fluctuations', 'observed', 'below', 'the', 'second', 'critical', 'field', 'and', 'wellknown', 'as', 'vortex', 'lattice', 'melting', 'was', 'one', 'of', 'the', 'most', 'popular', 'problems', '... | [-0.10995623298813419, 0.19318760894677792, -0.06634866228955259, 0.07233339930879663, -0.09135326648530848, -0.13701681970955112, 0.07173587047770444, 0.34561973209468483, -0.21440956459858537, -0.28468050655094584, 0.10173470333355103, -0.331033505223867, -0.12261463860561828, 0.1777957629032082, -0.02613672830593523... |
709.0578 | On the Mass-Period Distributions and Correlations of Extrasolar Planets | In addition to fitting the data of 233 extra-solar planets with power laws,
we construct a correlated mass-period distribution function of extrasolar
planets, as the first time in this field. The algorithm to generate a pair of
positively correlated beta-distributed random variables is introduced and used
for the con... | astro-ph | in addition to fitting the data of 233 extrasolar planets with power laws we construct a correlated massperiod distribution function of extrasolar planets as the first time in this field the algorithm to generate a pair of positively correlated betadistributed random variables is introduced and used for the constructio... | [['in', 'addition', 'to', 'fitting', 'the', 'data', 'of', '233', 'extrasolar', 'planets', 'with', 'power', 'laws', 'we', 'construct', 'a', 'correlated', 'massperiod', 'distribution', 'function', 'of', 'extrasolar', 'planets', 'as', 'the', 'first', 'time', 'in', 'this', 'field', 'the', 'algorithm', 'to', 'generate', 'a'... | [-0.14196483406506605, 0.13784624436491374, -0.08101308612168719, 0.14203850143604865, -0.0635940629250954, -0.05002413142938167, 0.06096216924370156, 0.34346011195773796, -0.2021122898717048, -0.3065834830246739, 0.04550398300476846, -0.30075648957389894, -0.1583364783644171, 0.18815590798760118, -0.0487720499809642, ... |
709.0579 | Berry Phase Effects in the dynamics of Dirac Electrons in Doubly Special
Relativity Framework | We consider the Doubly Special Relativity (DSR) generalization of Dirac
equation in an external potential in the Magueijo-Smolin base. The particles
obey a modified energy-momentum dispersion relation. The semiclassical
diagonalization of the Dirac Hamiltonian reveals the intrinsic Berry phase
effects in the particle... | hep-th cond-mat.other | we consider the doubly special relativity dsr generalization of dirac equation in an external potential in the magueijosmolin base the particles obey a modified energymomentum dispersion relation the semiclassical diagonalization of the dirac hamiltonian reveals the intrinsic berry phase effects in the particle dynamic... | [['we', 'consider', 'the', 'doubly', 'special', 'relativity', 'dsr', 'generalization', 'of', 'dirac', 'equation', 'in', 'an', 'external', 'potential', 'in', 'the', 'magueijosmolin', 'base', 'the', 'particles', 'obey', 'a', 'modified', 'energymomentum', 'dispersion', 'relation', 'the', 'semiclassical', 'diagonalization'... | [-0.23727102116258306, 0.17768375797029215, -0.10842844098806381, 0.1305117909796536, -0.11556091144765643, -0.16237471958580005, -0.0013564837334508245, 0.2596135075436905, -0.23542670594443652, -0.25594444695690816, -0.10399071744971232, -0.3219686910901642, -0.20190667327154765, 0.07201226569172418, -0.0076921048616... |
709.058 | Computer Simulation on Terahertz Emission from Intrinsic Josephson
Junctions of High-T_c Superconductors | Solving coupled nonlinear sine-Gordon equations and Maxwell equations
numerically, we study the electromagnetic and superconducting properties of the
single crystal of high-$T_c$ superconductor $\rm{Bi_2Sr_2CaCu_2O_{8+\delta}}$
with a static magnetic field applied parallel to the $ab$-plane and a dc
current fed in al... | cond-mat.supr-con cond-mat.other | solving coupled nonlinear sinegordon equations and maxwell equations numerically we study the electromagnetic and superconducting properties of the single crystal of hight_c superconductor rmbi_2sr_2cacu_2o_8delta with a static magnetic field applied parallel to the abplane and a dc current fed in along the caxis cavit... | [['solving', 'coupled', 'nonlinear', 'sinegordon', 'equations', 'and', 'maxwell', 'equations', 'numerically', 'we', 'study', 'the', 'electromagnetic', 'and', 'superconducting', 'properties', 'of', 'the', 'single', 'crystal', 'of', 'hight_c', 'superconductor', 'rmbi_2sr_2cacu_2o_8delta', 'with', 'a', 'static', 'magnetic... | [-0.22372636718684535, 0.21324835864610028, 0.005398488345836262, 0.008206735870030084, -0.10871954523569462, -0.12785500706652703, 0.0031194409583830862, 0.3971184529364109, -0.25869504486219685, -0.287456637310843, -0.008581567559056707, -0.27878660029614144, -0.06404376042174917, 0.23641772517590848, 0.0904809667557... |
709.0581 | Determining the Minimal Length Scale of the Generalized Uncertainty
Principle from the Entropy-Area Relationship | We derive the formula of the black hole entropy with a minimal length of the
Planck size by counting quantum modes of scalar fields in the vicinity of the
black hole horizon, taking into account the generalized uncertainty principle
(GUP). This formula is applied to some intriguing examples of black holes - the
Schwa... | hep-th gr-qc hep-ph | we derive the formula of the black hole entropy with a minimal length of the planck size by counting quantum modes of scalar fields in the vicinity of the black hole horizon taking into account the generalized uncertainty principle gup this formula is applied to some intriguing examples of black holes the schwarzschild... | [['we', 'derive', 'the', 'formula', 'of', 'the', 'black', 'hole', 'entropy', 'with', 'a', 'minimal', 'length', 'of', 'the', 'planck', 'size', 'by', 'counting', 'quantum', 'modes', 'of', 'scalar', 'fields', 'in', 'the', 'vicinity', 'of', 'the', 'black', 'hole', 'horizon', 'taking', 'into', 'account', 'the', 'generalized... | [-0.16417404640116728, 0.12792357367230578, -0.08505835007876157, 0.18090761593193747, -0.09371389087289572, -0.166937848480884, 0.012389080037828536, 0.19884355646092444, -0.17075776405399665, -0.29966036360710857, 0.07911180422524922, -0.3423610380571336, -0.06139589482918382, 0.2174464472127147, -0.06051688748644665... |
709.0582 | Kinematics of deformable media | We investigate the kinematics of deformations in two and three dimensional
media by explicitly solving (analytically) the evolution equations
(Raychaudhuri equations) for the expansion, shear and rotation associated with
the deformations. The analytical solutions allow us to study the dependence of
the kinematical qu... | physics.class-ph gr-qc hep-th | we investigate the kinematics of deformations in two and three dimensional media by explicitly solving analytically the evolution equations raychaudhuri equations for the expansion shear and rotation associated with the deformations the analytical solutions allow us to study the dependence of the kinematical quantities... | [['we', 'investigate', 'the', 'kinematics', 'of', 'deformations', 'in', 'two', 'and', 'three', 'dimensional', 'media', 'by', 'explicitly', 'solving', 'analytically', 'the', 'evolution', 'equations', 'raychaudhuri', 'equations', 'for', 'the', 'expansion', 'shear', 'and', 'rotation', 'associated', 'with', 'the', 'deforma... | [-0.13966759139964102, 0.08770349804385036, -0.11469687978901408, 0.08609697673761961, -0.05906221709287196, -0.07279055218632315, -0.040929188554668254, 0.36064097106310666, -0.24478228163777613, -0.23923667118880057, 0.13726508365738588, -0.24668755251389252, -0.151000567723303, 0.17915668496496828, -0.02923277662336... |
709.0583 | Spiral model, jamming percolation and glass-jamming transitions | The Spiral Model (SM) corresponds to a new class of kinetically constrained
models introduced in joint works with D.S. Fisher [8,9]. They provide the first
example of finite dimensional models with an ideal glass-jamming transition.
This is due to an underlying jamming percolation transition which has
unconventional ... | cond-mat.stat-mech | the spiral model sm corresponds to a new class of kinetically constrained models introduced in joint works with ds fisher 89 they provide the first example of finite dimensional models with an ideal glassjamming transition this is due to an underlying jamming percolation transition which has unconventional features it ... | [['the', 'spiral', 'model', 'sm', 'corresponds', 'to', 'a', 'new', 'class', 'of', 'kinetically', 'constrained', 'models', 'introduced', 'in', 'joint', 'works', 'with', 'ds', 'fisher', '89', 'they', 'provide', 'the', 'first', 'example', 'of', 'finite', 'dimensional', 'models', 'with', 'an', 'ideal', 'glassjamming', 'tra... | [-0.07082601570160979, 0.12601510444400102, -0.10635259235077056, 0.056800862455114336, -0.09840070222432179, -0.15583438070185868, 0.06376384823896183, 0.3207986672380779, -0.22177135026692574, -0.26589324084463817, 0.07690500517492183, -0.2918578740209341, -0.14872908466977292, 0.12601794625817123, -0.038435027479988... |
709.0584 | An approximate model for the adhesive contact of rough viscoelastic
surfaces | Surface roughness is known to easily suppress the adhesion of elastic
surfaces. Here a simple model for the contact of \emph{viscoelastic} rough
surfaces with significant levels of adhesion is presented. This approach is
derived from our previous model [E. Barthel and G. Haiat {\em Langmuir}, 18
9362 2002] for the ad... | cond-mat.soft | surface roughness is known to easily suppress the adhesion of elastic surfaces here a simple model for the contact of emphviscoelastic rough surfaces with significant levels of adhesion is presented this approach is derived from our previous model e barthel and g haiat em langmuir 18 9362 2002 for the adhesive contact ... | [['surface', 'roughness', 'is', 'known', 'to', 'easily', 'suppress', 'the', 'adhesion', 'of', 'elastic', 'surfaces', 'here', 'a', 'simple', 'model', 'for', 'the', 'contact', 'of', 'emphviscoelastic', 'rough', 'surfaces', 'with', 'significant', 'levels', 'of', 'adhesion', 'is', 'presented', 'this', 'approach', 'is', 'de... | [-0.11411374826929059, 0.1288955533926365, -0.11755526125552537, 0.02884411276149415, -0.08530614630190952, -0.18170848009311527, 0.031641077381842166, 0.3833843405911888, -0.2860605022616927, -0.2943422874516767, -0.006878872236668848, -0.24657020206306723, -0.20442690292670243, 0.19971584136584314, -0.083023485855833... |
709.0585 | The Black Hole Mass and Extreme Orbital Structure in NGC1399 | The largest galaxies, and in particular central galaxies in clusters, offer
unique insight into understanding the mechanism for the growth of nuclear black
holes. We present Hubble Space Telescope kinematics for NGC1399, the central
galaxy in Fornax. We find the best-fit model contains a black hole of 5.1 +-0.7
x 10^... | astro-ph | the largest galaxies and in particular central galaxies in clusters offer unique insight into understanding the mechanism for the growth of nuclear black holes we present hubble space telescope kinematics for ngc1399 the central galaxy in fornax we find the bestfit model contains a black hole of 51 07 x 108 msun at a d... | [['the', 'largest', 'galaxies', 'and', 'in', 'particular', 'central', 'galaxies', 'in', 'clusters', 'offer', 'unique', 'insight', 'into', 'understanding', 'the', 'mechanism', 'for', 'the', 'growth', 'of', 'nuclear', 'black', 'holes', 'we', 'present', 'hubble', 'space', 'telescope', 'kinematics', 'for', 'ngc1399', 'the'... | [-0.12466336502300868, 0.0601034519325378, -0.10670791090050914, 0.08623123263550293, -0.058073412030879186, -0.06269253353049686, 0.029826088880009233, 0.36932260457549737, -0.17658270290682473, -0.32337851893067, 0.035438830055736836, -0.31003443195753877, -0.014367970158289894, 0.21096374927767475, -0.00460143350850... |
709.0586 | Embedding Brans-Dicke gravity into electroweak theory | We argue that a version of the four dimensional Brans-Dicke theory can be
embedded in the standard flat spacetime electroweak theory. The embedding
involves a change of variables that separates the isospin from the hypercharge
in the electroweak theory.
| hep-ph gr-qc hep-th | we argue that a version of the four dimensional bransdicke theory can be embedded in the standard flat spacetime electroweak theory the embedding involves a change of variables that separates the isospin from the hypercharge in the electroweak theory | [['we', 'argue', 'that', 'a', 'version', 'of', 'the', 'four', 'dimensional', 'bransdicke', 'theory', 'can', 'be', 'embedded', 'in', 'the', 'standard', 'flat', 'spacetime', 'electroweak', 'theory', 'the', 'embedding', 'involves', 'a', 'change', 'of', 'variables', 'that', 'separates', 'the', 'isospin', 'from', 'the', 'hy... | [-0.10831986774857609, 0.21628188692892975, -0.1393732411476473, 0.1207024954402676, -0.051978436418068714, -0.13650914498915276, -0.004387463010155046, 0.27952498285911787, -0.23491542815015867, -0.22865814606671053, 0.01702568423934281, -0.24065142425780112, -0.14423324449513203, 0.06391016454794086, -0.0556990616978... |
709.0587 | What can we learn from fluctuations of particle ratios? | We explain how fluctuations of ratios can constrain and falsify the
statistical model of particle production in heavy ion collisions, using $K/\pi$
fluctuations as an example. We define an observable capable of determining
which statistical model, if any, governs freeze-out in ultrarelativistic heavy
ion collisions. ... | nucl-th hep-ex hep-ph nucl-ex | we explain how fluctuations of ratios can constrain and falsify the statistical model of particle production in heavy ion collisions using kpi fluctuations as an example we define an observable capable of determining which statistical model if any governs freezeout in ultrarelativistic heavy ion collisions we calculate... | [['we', 'explain', 'how', 'fluctuations', 'of', 'ratios', 'can', 'constrain', 'and', 'falsify', 'the', 'statistical', 'model', 'of', 'particle', 'production', 'in', 'heavy', 'ion', 'collisions', 'using', 'kpi', 'fluctuations', 'as', 'an', 'example', 'we', 'define', 'an', 'observable', 'capable', 'of', 'determining', 'w... | [-0.0459212347366292, 0.2640904928931492, -0.18059725330414755, 0.1462703619741323, 0.015493378925155725, -0.13387025007669698, 0.009103587668216387, 0.28672679060983736, -0.24432230769157015, -0.2771601915630876, -0.03476401360008545, -0.2990561198591199, -0.002194180181064945, 0.11670931648101236, 0.02147069019234634... |
709.0588 | Optimization of Short Coherent Control Pulses | The coherent control of small quantum system is considered. For a two-level
system coupled to an arbitrary bath we consider a pulse of finite duration. We
derive the leading and the next-leading order corrections to the evolution
operator due to the non-commutation of the pulse and the bath Hamiltonian. The
condition... | quant-ph cond-mat.mes-hall cond-mat.str-el | the coherent control of small quantum system is considered for a twolevel system coupled to an arbitrary bath we consider a pulse of finite duration we derive the leading and the nextleading order corrections to the evolution operator due to the noncommutation of the pulse and the bath hamiltonian the conditions are co... | [['the', 'coherent', 'control', 'of', 'small', 'quantum', 'system', 'is', 'considered', 'for', 'a', 'twolevel', 'system', 'coupled', 'to', 'an', 'arbitrary', 'bath', 'we', 'consider', 'a', 'pulse', 'of', 'finite', 'duration', 'we', 'derive', 'the', 'leading', 'and', 'the', 'nextleading', 'order', 'corrections', 'to', '... | [-0.17950735794865105, 0.20261769625218745, -0.09381605684757233, 0.0688041118675307, 0.00377754410665023, -0.15073356214808684, 0.005276776343099263, 0.37647811952365995, -0.25072322043028905, -0.2603900757656522, 0.05529824838724804, -0.2762173739459672, -0.05055597014342473, 0.1795042932244043, -0.024273914182941392... |
709.0589 | Temporary behavior of 'persistent' current in normal rings | In equilibrium, the number of conduction electrons in a solid substance
depends on the conformation of the atoms in the substance. When a magnetic
field is applied, it takes time for the system to come to a new equilibrium
with a new conformation. During such times, current may flow. But, unless
superconduction is in... | cond-mat.str-el cond-mat.supr-con | in equilibrium the number of conduction electrons in a solid substance depends on the conformation of the atoms in the substance when a magnetic field is applied it takes time for the system to come to a new equilibrium with a new conformation during such times current may flow but unless superconduction is involved th... | [['in', 'equilibrium', 'the', 'number', 'of', 'conduction', 'electrons', 'in', 'a', 'solid', 'substance', 'depends', 'on', 'the', 'conformation', 'of', 'the', 'atoms', 'in', 'the', 'substance', 'when', 'a', 'magnetic', 'field', 'is', 'applied', 'it', 'takes', 'time', 'for', 'the', 'system', 'to', 'come', 'to', 'a', 'ne... | [-0.16160748981063172, 0.21586469565798186, -0.05471352353998566, 0.02097317406500961, -0.016967915626289912, -0.14317670551753497, 0.03789317408352619, 0.343648087563394, -0.2573010939161611, -0.27226581532932537, 0.0697401382892593, -0.25721017266564733, -0.04915324828434217, 0.20546795131898002, -0.01892816800553399... |
709.059 | SUBARU Near-Infrared Multi-Color Images of Class II Young Stellar
Object, RNO91 | We conducted sub-arcsecond near-infrared imaging observations of RNO91 with
CIAO mounted on the SUBARU 8.2 m telescope. We present our JHK band data along
with optical images, which when considered together reveal a complex
circumstellar structure. We examined the colors of associated nebula and
compared the geometry... | astro-ph | we conducted subarcsecond nearinfrared imaging observations of rno91 with ciao mounted on the subaru 82 m telescope we present our jhk band data along with optical images which when considered together reveal a complex circumstellar structure we examined the colors of associated nebula and compared the geometry of the ... | [['we', 'conducted', 'subarcsecond', 'nearinfrared', 'imaging', 'observations', 'of', 'rno91', 'with', 'ciao', 'mounted', 'on', 'the', 'subaru', '82', 'm', 'telescope', 'we', 'present', 'our', 'jhk', 'band', 'data', 'along', 'with', 'optical', 'images', 'which', 'when', 'considered', 'together', 'reveal', 'a', 'complex... | [-0.06757126078329177, 0.02392575881853654, -0.08944739792623117, 0.029240744744482287, -0.12211561395111037, -0.09071847104704847, 0.0036291331728445547, 0.490908401853898, -0.20863396694356412, -0.32295432246527545, 0.08217541625421933, -0.284134701507933, -0.06889379916018715, 0.15312109627286155, -0.072407475107591... |
709.0591 | Utility function estimation: the entropy approach | The maximum entropy principle can be used to assign utility values when only
partial information is available about the decision maker's preferences. In
order to obtain such utility values it is necessary to establish an analogy
between probability and utility through the notion of a utility density
function. Accordi... | q-fin.ST physics.data-an | the maximum entropy principle can be used to assign utility values when only partial information is available about the decision makers preferences in order to obtain such utility values it is necessary to establish an analogy between probability and utility through the notion of a utility density function according to... | [['the', 'maximum', 'entropy', 'principle', 'can', 'be', 'used', 'to', 'assign', 'utility', 'values', 'when', 'only', 'partial', 'information', 'is', 'available', 'about', 'the', 'decision', 'makers', 'preferences', 'in', 'order', 'to', 'obtain', 'such', 'utility', 'values', 'it', 'is', 'necessary', 'to', 'establish', ... | [-0.04859197808423472, 0.0004299096139699319, -0.09358894311283764, 0.1038595090485423, -0.17981237982840914, -0.08585195694804976, 0.15049169907517929, 0.36271798551866885, -0.2783612563017462, -0.3277844205474187, 0.08929440419336683, -0.3050730327095248, -0.15877183786360546, 0.1116106649174502, -0.1831497620104959,... |
709.0592 | Transport through a multiply connected interacting meso-system using the
Keldysh formalism | We apply the Keldysh formalism in order to derive a current formula easy to
use for a system with many sites, one of which is interacting. The main
technical challenge is to deal with the lesser Green function. It turns out
that, in the case of the left-right symmetry, the knowledge of the lesser Green
function is no... | cond-mat.mes-hall cond-mat.str-el | we apply the keldysh formalism in order to derive a current formula easy to use for a system with many sites one of which is interacting the main technical challenge is to deal with the lesser green function it turns out that in the case of the leftright symmetry the knowledge of the lesser green function is not necess... | [['we', 'apply', 'the', 'keldysh', 'formalism', 'in', 'order', 'to', 'derive', 'a', 'current', 'formula', 'easy', 'to', 'use', 'for', 'a', 'system', 'with', 'many', 'sites', 'one', 'of', 'which', 'is', 'interacting', 'the', 'main', 'technical', 'challenge', 'is', 'to', 'deal', 'with', 'the', 'lesser', 'green', 'functio... | [-0.1256699921317679, 0.07441854441455925, -0.10192009037016087, 0.11212985961194061, -0.07070344898766799, -0.11009808217034969, 0.017300485842223344, 0.34225616030784145, -0.2179916920634752, -0.28247574364370986, 0.08410277197054548, -0.24980150462982997, -0.1645864851051967, 0.2000320376461525, -0.02643787294422110... |
709.0593 | Electron spin manipulation and resonator readout in a double quantum dot
nano-electromechanical system | Magnetically coupling a nano-mechanical resonator to a double quantum dot
confining two electrons can enable the manipulation of a single electron spin
and the readout of the resonator's natural frequency. When the Larmor frequency
matches the resonator frequency, the electron spin in one of the dots can be
selective... | cond-mat.mes-hall | magnetically coupling a nanomechanical resonator to a double quantum dot confining two electrons can enable the manipulation of a single electron spin and the readout of the resonators natural frequency when the larmor frequency matches the resonator frequency the electron spin in one of the dots can be selectively fli... | [['magnetically', 'coupling', 'a', 'nanomechanical', 'resonator', 'to', 'a', 'double', 'quantum', 'dot', 'confining', 'two', 'electrons', 'can', 'enable', 'the', 'manipulation', 'of', 'a', 'single', 'electron', 'spin', 'and', 'the', 'readout', 'of', 'the', 'resonators', 'natural', 'frequency', 'when', 'the', 'larmor', ... | [-0.16696590188531632, 0.30719257247106857, 0.028403449803590775, -0.060063999405703006, -0.021714318779308395, -0.2417839808636401, 0.048260838348777535, 0.37936670494725905, -0.26468533619183554, -0.2689520202307816, -0.014307013798381639, -0.26168114336274834, -0.01084205844854734, 0.2622236182172614, 0.012530528126... |
709.0594 | Transient quantum evolution of 2D electrons under photoexcitation of a
deep center | We have considered the ballistic propagation of the 2D electron Wigner
distribution, which is excited by an ultrashort optical pulse from a
short-range impurity into the first quantized subband of a selectively-doped
heterostructure with high mobility. Transient ionization of a deep local state
into a continuum condu... | cond-mat.other cond-mat.stat-mech | we have considered the ballistic propagation of the 2d electron wigner distribution which is excited by an ultrashort optical pulse from a shortrange impurity into the first quantized subband of a selectivelydoped heterostructure with high mobility transient ionization of a deep local state into a continuum conduction ... | [['we', 'have', 'considered', 'the', 'ballistic', 'propagation', 'of', 'the', '2d', 'electron', 'wigner', 'distribution', 'which', 'is', 'excited', 'by', 'an', 'ultrashort', 'optical', 'pulse', 'from', 'a', 'shortrange', 'impurity', 'into', 'the', 'first', 'quantized', 'subband', 'of', 'a', 'selectivelydoped', 'heteros... | [-0.12232382089830934, 0.18804385067822296, -0.10378470958676189, 0.031657584269996736, -0.0046186429646331816, -0.1128174617094919, 0.015768096481915562, 0.3828860783949494, -0.3085350186843425, -0.24013163306284696, -0.006918831062503159, -0.2795381345623173, -0.10052961902692914, 0.15220111941918732, 0.0326096088904... |
709.0595 | Observables in multi-detector analyses of supernova neutrinos | This paper has been withdrawn by the author, due to errors in the figures.
| hep-ph | this paper has been withdrawn by the author due to errors in the figures | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'author', 'due', 'to', 'errors', 'in', 'the', 'figures']] | [-0.10006661912692445, -0.020335858754281486, -0.11206320513572011, -0.06369040657799425, -0.08331371311630521, -0.012484078029436725, 0.002345973700617573, 0.32606036961078644, -0.25192813761532307, -0.4037838280200958, 0.12276170671352052, -0.34405405739588396, -0.15419600917292492, 0.09646940763507571, -0.3588278229... |
709.0596 | Bayesian Inversion of Stokes Profiles | [abridged] Inversion techniques are the most powerful methods to obtain
information about the thermodynamical and magnetic properties of solar and
stellar atmospheres. In the last years, we have witnessed the development of
highly sophisticated inversion codes that are now widely applied to
spectro-polarimetric obser... | astro-ph | abridged inversion techniques are the most powerful methods to obtain information about the thermodynamical and magnetic properties of solar and stellar atmospheres in the last years we have witnessed the development of highly sophisticated inversion codes that are now widely applied to spectropolarimetric observations... | [['abridged', 'inversion', 'techniques', 'are', 'the', 'most', 'powerful', 'methods', 'to', 'obtain', 'information', 'about', 'the', 'thermodynamical', 'and', 'magnetic', 'properties', 'of', 'solar', 'and', 'stellar', 'atmospheres', 'in', 'the', 'last', 'years', 'we', 'have', 'witnessed', 'the', 'development', 'of', 'h... | [-0.02544678888521176, 0.054543530496480655, -0.09369047880958183, 0.13869084839019027, -0.1015863628799926, -0.11857468153286471, 0.0404850735766701, 0.4151621500710886, -0.26306367924611784, -0.3383677823293251, 0.14066202249836146, -0.23721792343636905, -0.1116293255588562, 0.2368628881305052, -0.03377670468762517, ... |
709.0597 | Painlev\'e scheme | In this note, we review the notion of Painlev\'e scheme of the sixth
Painlev\'e equation from the viewpoint of accessible singular point and its
local index in the Hirzebruch surface of degree two ${\Sigma_2}$. The key
method is Painlev\'e $\alpha$-method for each accessible singular point. Giving
a Painlev\'e scheme... | math.GM | in this note we review the notion of painleve scheme of the sixth painleve equation from the viewpoint of accessible singular point and its local index in the hirzebruch surface of degree two sigma_2 the key method is painleve alphamethod for each accessible singular point giving a painleve scheme in the differential s... | [['in', 'this', 'note', 'we', 'review', 'the', 'notion', 'of', 'painleve', 'scheme', 'of', 'the', 'sixth', 'painleve', 'equation', 'from', 'the', 'viewpoint', 'of', 'accessible', 'singular', 'point', 'and', 'its', 'local', 'index', 'in', 'the', 'hirzebruch', 'surface', 'of', 'degree', 'two', 'sigma_2', 'the', 'key', 'm... | [-0.21224880438561725, 0.0055963038590497675, -0.07312184059580343, 0.027229245608895027, -0.06562362459026673, -0.22912263328753477, -0.030872738689381993, 0.26427180287057317, -0.2977248808220688, -0.2044012031386054, 0.07149632838328031, -0.29814704379017376, -0.19414870331962222, 0.1590947428372054, -0.064999803556... |
709.0598 | Asymptotic expansion and central limit theorem for quadratic variations
of Gaussian processes | Cohen, Guyon, Perrin and Pontier have given assumptions under which the
second-order quadratic variations of a Gaussian process converge almost surely
to a deterministic limit. In this paper we present two new convergence results
about these variations: the first is a deterministic asymptotic expansion; the
second is... | math.PR | cohen guyon perrin and pontier have given assumptions under which the secondorder quadratic variations of a gaussian process converge almost surely to a deterministic limit in this paper we present two new convergence results about these variations the first is a deterministic asymptotic expansion the second is a centr... | [['cohen', 'guyon', 'perrin', 'and', 'pontier', 'have', 'given', 'assumptions', 'under', 'which', 'the', 'secondorder', 'quadratic', 'variations', 'of', 'a', 'gaussian', 'process', 'converge', 'almost', 'surely', 'to', 'a', 'deterministic', 'limit', 'in', 'this', 'paper', 'we', 'present', 'two', 'new', 'convergence', '... | [-0.09296146292013652, 0.09757092771487254, -0.14370949171610514, 0.05714971402754931, -0.09036294128181356, -0.09516708988865669, 0.047503473235393, 0.3508481488168014, -0.3001088811592622, -0.21729203571113898, 0.1293079081665245, -0.24530500208846096, -0.19173312592531808, 0.1710943113165823, -0.13819765952895535, 0... |
709.0599 | On Universal Properties of Capacity-Approaching LDPC Ensembles | This paper is focused on the derivation of some universal properties of
capacity-approaching low-density parity-check (LDPC) code ensembles whose
transmission takes place over memoryless binary-input output-symmetric (MBIOS)
channels. Properties of the degree distributions, graphical complexity and the
number of fund... | cs.IT math.IT | this paper is focused on the derivation of some universal properties of capacityapproaching lowdensity paritycheck ldpc code ensembles whose transmission takes place over memoryless binaryinput outputsymmetric mbios channels properties of the degree distributions graphical complexity and the number of fundamental cycle... | [['this', 'paper', 'is', 'focused', 'on', 'the', 'derivation', 'of', 'some', 'universal', 'properties', 'of', 'capacityapproaching', 'lowdensity', 'paritycheck', 'ldpc', 'code', 'ensembles', 'whose', 'transmission', 'takes', 'place', 'over', 'memoryless', 'binaryinput', 'outputsymmetric', 'mbios', 'channels', 'properti... | [-0.1995626531081979, 0.08023267243870824, -0.07391124490044407, 0.10077000589084786, -0.03439331609453704, -0.25878896267480545, 0.09865198175397677, 0.4080271801332364, -0.2701176622913949, -0.2619387980720431, 0.1281580740944608, -0.21391068112507866, -0.16023041645719394, 0.23147735489985427, -0.11289887714350746, ... |
709.06 | Morita Type Equivalences and Reflexive Algebras | Two unital operator algebras A, B are called Delta-equivalent if there exists
an equivalence functor between the categories A-mod and B-mod which "extends"
to a *-functor implementing an equivalence between the categories A-dmod and
B-dmod. Here A-mod denotes the category of normal representations of A and
A-dmod den... | math.OA math.FA | two unital operator algebras a b are called deltaequivalent if there exists an equivalence functor between the categories amod and bmod which extends to a functor implementing an equivalence between the categories admod and bdmod here amod denotes the category of normal representations of a and admod denotes the catego... | [['two', 'unital', 'operator', 'algebras', 'a', 'b', 'are', 'called', 'deltaequivalent', 'if', 'there', 'exists', 'an', 'equivalence', 'functor', 'between', 'the', 'categories', 'amod', 'and', 'bmod', 'which', 'extends', 'to', 'a', 'functor', 'implementing', 'an', 'equivalence', 'between', 'the', 'categories', 'admod',... | [-0.15480945748036978, 0.07858483907412593, -0.05086142898143567, 0.05881857899492895, -0.08813359293625835, -0.1620569887388613, -0.04509719668829948, 0.3955069157803796, -0.45399656682515266, -0.14274617095391468, 0.09301351021120767, -0.28706892464278727, -0.14934828028217265, 0.12963016131489546, -0.208919256512728... |
709.0601 | Pulse-Bandwidth Dependence of Coherent Phase Control of
Resonance-Mediated (2+1) Three-Photon Absorption | We study in detail coherent phase control of femtosecond resonance-mediated
(2+1) three-photon absorption and its dependence on the spectral bandwidth of
the excitation pulse. The regime is the weak-field regime of third perturbative
order. The corresponding interference mechanism involves a group of
three-photon exc... | physics.atom-ph physics.chem-ph | we study in detail coherent phase control of femtosecond resonancemediated 21 threephoton absorption and its dependence on the spectral bandwidth of the excitation pulse the regime is the weakfield regime of third perturbative order the corresponding interference mechanism involves a group of threephoton excitation pat... | [['we', 'study', 'in', 'detail', 'coherent', 'phase', 'control', 'of', 'femtosecond', 'resonancemediated', '21', 'threephoton', 'absorption', 'and', 'its', 'dependence', 'on', 'the', 'spectral', 'bandwidth', 'of', 'the', 'excitation', 'pulse', 'the', 'regime', 'is', 'the', 'weakfield', 'regime', 'of', 'third', 'perturb... | [-0.13619579041066268, 0.14472731412072037, -0.03513758565447685, -0.008269296723681138, -0.0017380393582625666, -0.11105760032702508, 0.06892406633562422, 0.47274546631598385, -0.22146189617721931, -0.28907849334612273, 0.018804474079988195, -0.27682630362265837, -0.101240939065895, 0.22101419527535798, 0.023427236373... |
709.0602 | Arbitrary precision composite pulses for NMR quantum computing | We discuss the implementation of arbitrary precision composite pulses
developed using the methods of Brown et al. [Phys. Rev. A 70 (2004) 052318]. We
give explicit results for pulse sequences designed to tackle both the simple
case of pulse length errors and for the more complex case of off-resonance
errors. The resu... | quant-ph | we discuss the implementation of arbitrary precision composite pulses developed using the methods of brown et al phys rev a 70 2004 052318 we give explicit results for pulse sequences designed to tackle both the simple case of pulse length errors and for the more complex case of offresonance errors the results are deve... | [['we', 'discuss', 'the', 'implementation', 'of', 'arbitrary', 'precision', 'composite', 'pulses', 'developed', 'using', 'the', 'methods', 'of', 'brown', 'et', 'al', 'phys', 'rev', 'a', '70', '2004', '052318', 'we', 'give', 'explicit', 'results', 'for', 'pulse', 'sequences', 'designed', 'to', 'tackle', 'both', 'the', '... | [-0.07410556760116188, 0.09527257615839367, -0.04352578233037867, 0.05295545335358648, -0.06390289919200673, -0.14482286452913462, 0.036842809722466924, 0.40977374551845575, -0.14804854537290868, -0.3373903824266658, 0.04242793997965141, -0.18746783172906334, -0.1584277880767277, 0.3119662367919488, -0.1347130861462601... |
709.0603 | What is interesting in eta and eta' Meson Decays? | An introduction to the physics of eta and eta' meson decays is given. A
historical account of the discovery of the mesons is presented. It is followed
by an overview and classification of the common decay modes and the relevance
of the mesons for modern hadron and particle physics. In more detail the
hadronic decay m... | nucl-ex | an introduction to the physics of eta and eta meson decays is given a historical account of the discovery of the mesons is presented it is followed by an overview and classification of the common decay modes and the relevance of the mesons for modern hadron and particle physics in more detail the hadronic decay modes a... | [['an', 'introduction', 'to', 'the', 'physics', 'of', 'eta', 'and', 'eta', 'meson', 'decays', 'is', 'given', 'a', 'historical', 'account', 'of', 'the', 'discovery', 'of', 'the', 'mesons', 'is', 'presented', 'it', 'is', 'followed', 'by', 'an', 'overview', 'and', 'classification', 'of', 'the', 'common', 'decay', 'modes',... | [-0.05781599457040229, 0.22880591876004944, -0.10539399421904036, 0.13863015565295173, -0.04235662516927527, -0.12105713280478633, -0.0030814648070122286, 0.27835232466058707, -0.21733251510448354, -0.18794106822260606, 0.030669896658109402, -0.3563265961604894, -0.057851755430781714, 0.1873185272461244, 0.047131017711... |
709.0604 | A MERLIN Study of 6 GHz Excited-state OH & 6.7 GHz Methanol Masers in
ON1 | MERLIN observations of 6.668-GHz methanol and both 6.031- and 6.035-GHz
hydroxyl (OH) emission from the massive star-formation region ON1 are
presented. These are the first methanol observations made in full polarization
using 5 antennas of MERLIN, giving high resolution and sensitivity to extended
emission. Maser fe... | astro-ph | merlin observations of 6668ghz methanol and both 6031 and 6035ghz hydroxyl oh emission from the massive starformation region on1 are presented these are the first methanol observations made in full polarization using 5 antennas of merlin giving high resolution and sensitivity to extended emission maser features are fou... | [['merlin', 'observations', 'of', '6668ghz', 'methanol', 'and', 'both', '6031', 'and', '6035ghz', 'hydroxyl', 'oh', 'emission', 'from', 'the', 'massive', 'starformation', 'region', 'on1', 'are', 'presented', 'these', 'are', 'the', 'first', 'methanol', 'observations', 'made', 'in', 'full', 'polarization', 'using', '5', ... | [-0.11823421284310702, 0.08039949589392507, 0.08199533008244689, 0.012891454782845464, -0.06509067692102556, -0.11128412403074876, 0.0629448765500283, 0.48428082528404115, -0.17839015430079463, -0.3567464523320229, -0.0006486077270144883, -0.2584043135695114, 0.02870964401750111, 0.13627011166097014, 0.0565269881442683... |
709.0605 | AC-induced superfluidity | We argue that a system of ultracold bosonic atoms in a tilted optical lattice
can become superfluid in response to resonant AC forcing. Among others, this
allows one to prepare a Bose-Einstein condensate in a state associated with a
negative effective mass. Our reasoning is backed by both exact numerical
simulations ... | cond-mat.other | we argue that a system of ultracold bosonic atoms in a tilted optical lattice can become superfluid in response to resonant ac forcing among others this allows one to prepare a boseeinstein condensate in a state associated with a negative effective mass our reasoning is backed by both exact numerical simulations for sy... | [['we', 'argue', 'that', 'a', 'system', 'of', 'ultracold', 'bosonic', 'atoms', 'in', 'a', 'tilted', 'optical', 'lattice', 'can', 'become', 'superfluid', 'in', 'response', 'to', 'resonant', 'ac', 'forcing', 'among', 'others', 'this', 'allows', 'one', 'to', 'prepare', 'a', 'boseeinstein', 'condensate', 'in', 'a', 'state'... | [-0.1681075463214746, 0.20861138622634687, -0.08565214403833334, 0.010375143866986037, -0.026437699909393604, -0.17517428866659218, 0.09627149150921749, 0.36553619217414124, -0.18620369751006366, -0.25595734999156916, 0.025885755212332766, -0.3106393187989642, -0.09739128827618865, 0.2067650814827245, 0.010537318656077... |
709.0606 | Force induced stretched state: Effects of temperature | A model of self avoiding walks with suitable constraint has been developed to
study the effect of temperature on a single stranded DNA (ssDNA) in the
constant force ensemble. Our exact calculations for small chains show that the
extension (reaction co-ordinate) may increase or decrease with the temperature
depending ... | cond-mat.stat-mech cond-mat.soft | a model of self avoiding walks with suitable constraint has been developed to study the effect of temperature on a single stranded dna ssdna in the constant force ensemble our exact calculations for small chains show that the extension reaction coordinate may increase or decrease with the temperature depending upon the... | [['a', 'model', 'of', 'self', 'avoiding', 'walks', 'with', 'suitable', 'constraint', 'has', 'been', 'developed', 'to', 'study', 'the', 'effect', 'of', 'temperature', 'on', 'a', 'single', 'stranded', 'dna', 'ssdna', 'in', 'the', 'constant', 'force', 'ensemble', 'our', 'exact', 'calculations', 'for', 'small', 'chains', '... | [-0.12999508316522534, 0.15593986504853413, -0.08447556908845112, -0.006886616101653515, -0.061263928673218324, -0.16392128840545664, 0.06400342836174407, 0.37201625188883347, -0.24987477671850142, -0.298592526394921, 0.009504734763958127, -0.2431399000785019, -0.14518550320976426, 0.16893319187898048, 0.02029139622515... |
709.0607 | Current-induced cleaning of graphene | A simple yet highly reproducible method to suppress contamination of graphene
at low temperature inside the cryostat is presented. The method consists of
applying a current of several mA through the graphene device, which is here
typically a few $\mu$m wide. This ultra-high current density is shown to remove
contamin... | cond-mat.other cond-mat.mtrl-sci | a simple yet highly reproducible method to suppress contamination of graphene at low temperature inside the cryostat is presented the method consists of applying a current of several ma through the graphene device which is here typically a few mum wide this ultrahigh current density is shown to remove contamination ads... | [['a', 'simple', 'yet', 'highly', 'reproducible', 'method', 'to', 'suppress', 'contamination', 'of', 'graphene', 'at', 'low', 'temperature', 'inside', 'the', 'cryostat', 'is', 'presented', 'the', 'method', 'consists', 'of', 'applying', 'a', 'current', 'of', 'several', 'ma', 'through', 'the', 'graphene', 'device', 'whic... | [-0.09912084579542509, 0.16618217116244782, -0.04976326927979603, -0.01790357522672203, -0.026491064040772158, -0.1645901521299908, 0.06827737630724355, 0.3962845533948254, -0.24388419313609233, -0.3209296125619684, 0.04726667210091779, -0.27346646735145724, -0.1476819269290125, 0.2633455573167238, -0.03783275253702829... |
709.0608 | The New Science of Gravitational Waves | A brief survey is presented of new science that will emerge during the
decades ahead from direct detection of gravitational radiation. Interferometers
on earth and in space will probe the universe in an entirely new way by
directly sensing motions of distant matter over a range of more than a million
in frequency. Th... | astro-ph gr-qc | a brief survey is presented of new science that will emerge during the decades ahead from direct detection of gravitational radiation interferometers on earth and in space will probe the universe in an entirely new way by directly sensing motions of distant matter over a range of more than a million in frequency the mo... | [['a', 'brief', 'survey', 'is', 'presented', 'of', 'new', 'science', 'that', 'will', 'emerge', 'during', 'the', 'decades', 'ahead', 'from', 'direct', 'detection', 'of', 'gravitational', 'radiation', 'interferometers', 'on', 'earth', 'and', 'in', 'space', 'will', 'probe', 'the', 'universe', 'in', 'an', 'entirely', 'new'... | [-0.10934880722763612, 0.18281283976840415, -0.06801171176872838, 0.09868246390396962, -0.11218162132233071, -0.07769255362412271, 0.010365806285537675, 0.31198281212709844, -0.2062131293561025, -0.34127990655704504, 0.0917073827060651, -0.3158951646894113, -0.09518422112968336, 0.27264981033577995, -0.0144339679617486... |
709.0609 | Topological spin-Hall current in waveguided zinc-blende semiconductors
with Dresselhaus spin-orbit coupling | We describe an intrinsic spin-Hall effect in $n$-type bulk zinc-blende
semiconductors with topological origin. When electron transport is confined to
a waveguide structure, and the applied electric field is such that the spins of
electrons remain as eigenstates of the Dresselhaus spin-orbit field with
negligible subb... | cond-mat.mes-hall | we describe an intrinsic spinhall effect in ntype bulk zincblende semiconductors with topological origin when electron transport is confined to a waveguide structure and the applied electric field is such that the spins of electrons remain as eigenstates of the dresselhaus spinorbit field with negligible subband mixing... | [['we', 'describe', 'an', 'intrinsic', 'spinhall', 'effect', 'in', 'ntype', 'bulk', 'zincblende', 'semiconductors', 'with', 'topological', 'origin', 'when', 'electron', 'transport', 'is', 'confined', 'to', 'a', 'waveguide', 'structure', 'and', 'the', 'applied', 'electric', 'field', 'is', 'such', 'that', 'the', 'spins',... | [-0.17816210003908384, 0.25868442562866467, -0.04039291424507445, 0.054109349721958015, -0.09029707437042486, -0.138210861122405, -0.02158598558215255, 0.3956185468557206, -0.3074584855782715, -0.2742646816948598, -0.01840795017461377, -0.2812761411578818, -0.1234763456953012, 0.20143632845614445, 0.007206484520892528,... |
709.061 | Environments of z>5 quasars: searching for protoclusters at
submillimetre wavelengths | The most massive haloes at high redshift are expected, according to
hierarchical cosmologies, to reside in the most biased density fields. If
powerful active galactic nuclei (AGN) are expected to exist anywhere in the
early Universe (z>5), it is within these massive haloes. The most luminous of
these AGN, powered by ... | astro-ph | the most massive haloes at high redshift are expected according to hierarchical cosmologies to reside in the most biased density fields if powerful active galactic nuclei agn are expected to exist anywhere in the early universe z5 it is within these massive haloes the most luminous of these agn powered by supermassive ... | [['the', 'most', 'massive', 'haloes', 'at', 'high', 'redshift', 'are', 'expected', 'according', 'to', 'hierarchical', 'cosmologies', 'to', 'reside', 'in', 'the', 'most', 'biased', 'density', 'fields', 'if', 'powerful', 'active', 'galactic', 'nuclei', 'agn', 'are', 'expected', 'to', 'exist', 'anywhere', 'in', 'the', 'ea... | [-0.05490823714321557, 0.1088890034407567, -0.03348376047243631, 0.15968964606090674, -0.10369981861968693, -0.05139229782561603, 0.009167843147505092, 0.45985368446401825, -0.04791521320031291, -0.3628619684415176, 0.05463288882737036, -0.3492369647904521, -0.019513750010855202, 0.15518889757021848, 0.0281490497055180... |
709.0611 | Holographic Indeterminacy, Uncertainty and Noise | A theory is developed to describe the nonlocal effect of spacetime
quantization on position measurements transverse to macroscopic separations.
Spacetime quantum states close to a classical null trajectory are approximated
by plane wavefunctions of Planck wavelength (l_P) reference beams; these are
used to connect tr... | astro-ph gr-qc hep-th | a theory is developed to describe the nonlocal effect of spacetime quantization on position measurements transverse to macroscopic separations spacetime quantum states close to a classical null trajectory are approximated by plane wavefunctions of planck wavelength l_p reference beams these are used to connect transver... | [['a', 'theory', 'is', 'developed', 'to', 'describe', 'the', 'nonlocal', 'effect', 'of', 'spacetime', 'quantization', 'on', 'position', 'measurements', 'transverse', 'to', 'macroscopic', 'separations', 'spacetime', 'quantum', 'states', 'close', 'to', 'a', 'classical', 'null', 'trajectory', 'are', 'approximated', 'by', ... | [-0.16723628958094527, 0.20471151111996733, -0.12201001707051712, 0.10163807855067054, -0.07410190331310415, -0.17398235363758763, -0.01529071052011039, 0.30833403031680395, -0.21918277493122415, -0.30008941581102344, 0.006753730862824755, -0.2957481608715501, -0.04245715352061035, 0.16622915016672446, -0.0589210889857... |
709.0612 | Information Equation of State | Landauer's principle is applied to information in the universe. Once stars
began forming, the increasing proportion of matter at high stellar temperatures
compensated for the expanding universe to provide a near constant information
energy density. The information equation of state was close to the dark energy
value,... | astro-ph | landauers principle is applied to information in the universe once stars began forming the increasing proportion of matter at high stellar temperatures compensated for the expanding universe to provide a near constant information energy density the information equation of state was close to the dark energy value w 1 fo... | [['landauers', 'principle', 'is', 'applied', 'to', 'information', 'in', 'the', 'universe', 'once', 'stars', 'began', 'forming', 'the', 'increasing', 'proportion', 'of', 'matter', 'at', 'high', 'stellar', 'temperatures', 'compensated', 'for', 'the', 'expanding', 'universe', 'to', 'provide', 'a', 'near', 'constant', 'inf... | [-0.11279902079674814, 0.1563830116347942, -0.084428947678368, 0.13687243410843491, -0.10010903233861816, -0.1136109300672875, 0.0790059235578935, 0.3370138539733099, -0.2597433426251103, -0.3721729490007939, 0.06948906201287172, -0.28706041488663425, 0.04150949562234538, 0.16510912816239787, -0.004247251159189805, -0.... |
709.0613 | Complementarity and uncertainty relations for matter wave interferometry | We establish a rigorous quantitative connection between (i) the
interferometric duality relation for which-way information and fringe
visibility and (ii) Heisenberg's uncertainty relation for position and modular
momentum. We apply our theory to atom interferometry, wherein spontaneously
emitted photons provide which... | quant-ph | we establish a rigorous quantitative connection between i the interferometric duality relation for whichway information and fringe visibility and ii heisenbergs uncertainty relation for position and modular momentum we apply our theory to atom interferometry wherein spontaneously emitted photons provide which way infor... | [['we', 'establish', 'a', 'rigorous', 'quantitative', 'connection', 'between', 'i', 'the', 'interferometric', 'duality', 'relation', 'for', 'whichway', 'information', 'and', 'fringe', 'visibility', 'and', 'ii', 'heisenbergs', 'uncertainty', 'relation', 'for', 'position', 'and', 'modular', 'momentum', 'we', 'apply', 'ou... | [-0.10338928496154647, 0.09368492631157013, -0.1362706022337079, 0.11878791507677472, -0.15006584497644904, -0.1951181943824684, 0.09124535789790873, 0.3758675961501219, -0.2718846485526724, -0.3659982184075158, 0.013404804585275777, -0.29187669918279757, -0.12097523155777405, 0.14173767396079545, -0.0668426147436328, ... |
709.0614 | Dynamical parton distributions of the nucleon and very small-x physics | Utilizing recent DIS measurements (F_{2,L}) and data on dilepton and
high-E_{T} jet production we determine the dynamical parton distributions of
the nucleon generated radiatively from valence-like positive input
distributions at optimally chosen low resolution scales. These are compared
with `standard' distributions... | hep-ph | utilizing recent dis measurements f_2l and data on dilepton and highe_t jet production we determine the dynamical parton distributions of the nucleon generated radiatively from valencelike positive input distributions at optimally chosen low resolution scales these are compared with standard distributions generated fro... | [['utilizing', 'recent', 'dis', 'measurements', 'f_2l', 'and', 'data', 'on', 'dilepton', 'and', 'highe_t', 'jet', 'production', 'we', 'determine', 'the', 'dynamical', 'parton', 'distributions', 'of', 'the', 'nucleon', 'generated', 'radiatively', 'from', 'valencelike', 'positive', 'input', 'distributions', 'at', 'optima... | [-0.028531573512875795, 0.20108732131828788, -0.10516471783666097, 0.1846495616527004, -0.027440246102179735, -0.05301128559788504, -0.018205235490952227, 0.3914919459609357, -0.23097695013550856, -0.29677618243767107, 0.04646486166566042, -0.30753107020588777, 0.010564453579940413, 0.1908385341219206, 0.00669548188079... |
709.0615 | Frequency-Domain Coherent Control of Femtosecond Two-Photon Absorption:
Intermediate-Field vs. Weak-Field Regime | Coherent control of femtosecond two-photon absorption in the
intermediate-field regime is analyzed in detail in the powerful frequency
domain using an extended 4th-order perturbative description. The corresponding
absorption is coherently induced by the weak-field non-resonant two-photon
transitions as well as by fou... | physics.atom-ph physics.chem-ph | coherent control of femtosecond twophoton absorption in the intermediatefield regime is analyzed in detail in the powerful frequency domain using an extended 4thorder perturbative description the corresponding absorption is coherently induced by the weakfield nonresonant twophoton transitions as well as by fourphoton t... | [['coherent', 'control', 'of', 'femtosecond', 'twophoton', 'absorption', 'in', 'the', 'intermediatefield', 'regime', 'is', 'analyzed', 'in', 'detail', 'in', 'the', 'powerful', 'frequency', 'domain', 'using', 'an', 'extended', '4thorder', 'perturbative', 'description', 'the', 'corresponding', 'absorption', 'is', 'cohere... | [-0.13387870687739292, 0.18303426296226558, -0.043130454572295786, 0.05635726710066332, 0.001406566681046235, -0.13493544771861202, 0.07008883846867689, 0.4155604465115339, -0.23909137299970576, -0.2898366308133853, -0.004844612130349068, -0.2895012746400487, -0.08126170748207522, 0.21673340681954323, 0.061543595371417... |
709.0616 | Vacuum shell in the Schwarzschild-de Sitter world | We construct the classification scheme for all possible evolution scenarios
and find the corresponding global geometries for dynamics of a thin spherical
vacuum shell in the Schwarzschild-de Sitter metric. This configuration is
suitable for the modelling of vacuum bubbles arising during cosmological phase
transitions... | gr-qc hep-ph | we construct the classification scheme for all possible evolution scenarios and find the corresponding global geometries for dynamics of a thin spherical vacuum shell in the schwarzschildde sitter metric this configuration is suitable for the modelling of vacuum bubbles arising during cosmological phase transitions in ... | [['we', 'construct', 'the', 'classification', 'scheme', 'for', 'all', 'possible', 'evolution', 'scenarios', 'and', 'find', 'the', 'corresponding', 'global', 'geometries', 'for', 'dynamics', 'of', 'a', 'thin', 'spherical', 'vacuum', 'shell', 'in', 'the', 'schwarzschildde', 'sitter', 'metric', 'this', 'configuration', 'i... | [-0.12867502063671324, 0.08713356497761932, -0.12285499120170766, 0.08433620073892018, -0.045282960859464205, -0.09580947044602733, -0.006438607810699242, 0.32065615820837146, -0.20808635431619243, -0.26673448971532127, 0.13183145963789974, -0.24277118030697742, -0.05555617344129751, 0.11854883925890193, -0.00258240340... |
709.0617 | Widom-Rowlinson model (continuum and lattice) | This is a short review about liquid-vapor and crystalline phase transitions
in continuum and lattice Widom-Rowlinson models.
| cond-mat.stat-mech | this is a short review about liquidvapor and crystalline phase transitions in continuum and lattice widomrowlinson models | [['this', 'is', 'a', 'short', 'review', 'about', 'liquidvapor', 'and', 'crystalline', 'phase', 'transitions', 'in', 'continuum', 'and', 'lattice', 'widomrowlinson', 'models']] | [-0.12369876360411153, 0.23932281366604216, -0.11834411739426501, 0.041573536089238, -0.013136652900892146, -0.16296525362550335, 0.11150006423978244, 0.47730084815446067, -0.19810657104586854, -0.18227282758144772, 0.12858332257361754, -0.2570678538040203, -0.1529651090283604, 0.026004540240939927, -0.0103591265814269... |
709.0618 | Microwave surface resistance of pristine and neutron-irradiated MgB2
samples in magnetic field | We report on the microwave surface resistance of two polycrystalline Mg11B2
samples; one consists of pristine material, the other has been irradiated at
very high neutron fluence. It has already been reported that in the strongly
irradiated sample the two gaps merge into a single value. The mw surface
resistance has ... | cond-mat.supr-con | we report on the microwave surface resistance of two polycrystalline mg11b2 samples one consists of pristine material the other has been irradiated at very high neutron fluence it has already been reported that in the strongly irradiated sample the two gaps merge into a single value the mw surface resistance has been m... | [['we', 'report', 'on', 'the', 'microwave', 'surface', 'resistance', 'of', 'two', 'polycrystalline', 'mg11b2', 'samples', 'one', 'consists', 'of', 'pristine', 'material', 'the', 'other', 'has', 'been', 'irradiated', 'at', 'very', 'high', 'neutron', 'fluence', 'it', 'has', 'already', 'been', 'reported', 'that', 'in', 't... | [-0.07547491941867131, 0.1557372404142682, -0.08414509357618434, 0.02999941591772118, -0.0041308239395064965, -0.11250413062583123, 0.041207099735204665, 0.3778600658263479, -0.21693858612860953, -0.3541627372907741, 0.06490915308906031, -0.30189726849618764, -0.04302370802100216, 0.24566559415842806, 0.007126038228826... |
709.0619 | Physical Characteristics of a Dark Cloud in an Early Stage of Star
Formation toward NGC 7538: an Outer Galaxy Infrared Dark Cloud? | In the inner parts of the Galaxy the Infrared Dark Clouds (IRDCs) are
presently believed to be the progenitors of massive stars and star clusters.
Many of them are predominantly devoid of active star formation and for now they
represent the earliest observed stages of massive star formation. Their Outer
Galaxy counte... | astro-ph | in the inner parts of the galaxy the infrared dark clouds irdcs are presently believed to be the progenitors of massive stars and star clusters many of them are predominantly devoid of active star formation and for now they represent the earliest observed stages of massive star formation their outer galaxy counterparts... | [['in', 'the', 'inner', 'parts', 'of', 'the', 'galaxy', 'the', 'infrared', 'dark', 'clouds', 'irdcs', 'are', 'presently', 'believed', 'to', 'be', 'the', 'progenitors', 'of', 'massive', 'stars', 'and', 'star', 'clusters', 'many', 'of', 'them', 'are', 'predominantly', 'devoid', 'of', 'active', 'star', 'formation', 'and',... | [-0.11368754112055493, 0.15629560780806442, -0.04456988143685617, 0.10723548602606905, -0.060295918648408955, -0.021537751386865256, 0.008527691753809912, 0.4159587113219395, -0.15085252202606123, -0.32733010160491655, 0.07331013797921243, -0.24897388900189024, -0.024666162689722944, 0.15477392029613582, 0.021068213677... |
709.062 | Asymptotic normality for the counting process of weak records and
\delta-records in discrete models | Let $\{X_n,n\ge1\}$ be a sequence of independent and identically distributed
random variables, taking non-negative integer values, and call $X_n$ a
$\delta$-record if $X_n>\max\{X_1,...,X_{n-1}\}+\delta$, where $\delta$ is an
integer constant. We use martingale arguments to show that the counting process
of $\delta$-... | math.PR | let x_nnge1 be a sequence of independent and identically distributed random variables taking nonnegative integer values and call x_n a deltarecord if x_nmaxx_1x_n1delta where delta is an integer constant we use martingale arguments to show that the counting process of deltarecords among the first n observations suitabl... | [['let', 'x_nnge1', 'be', 'a', 'sequence', 'of', 'independent', 'and', 'identically', 'distributed', 'random', 'variables', 'taking', 'nonnegative', 'integer', 'values', 'and', 'call', 'x_n', 'a', 'deltarecord', 'if', 'x_nmaxx_1x_n1delta', 'where', 'delta', 'is', 'an', 'integer', 'constant', 'we', 'use', 'martingale', ... | [-0.17973953845507618, 0.18091630937949468, -0.09040718378304545, 0.0032786570791358827, -0.040066319121631666, -0.175417302906124, 0.0707635487196967, 0.3432626680874113, -0.31435760694430837, -0.21922706611065276, 0.13365558307416348, -0.2898122971849655, -0.08014177473317553, 0.16542499429031984, -0.0865506378780883... |
709.0621 | Strong size evolution of the most massive galaxies since z~2 | Using the combined capabilities of the large near-infrared Palomar/DEEP-2
survey, and the superb resolution of the ACS HST camera, we explore the size
evolution of 831 very massive galaxies (M*>10^{11}h_{70}^{-2}M_sun) since z~2.
We split our sample according to their light concentration using the Sersic
index n. At ... | astro-ph | using the combined capabilities of the large nearinfrared palomardeep2 survey and the superb resolution of the acs hst camera we explore the size evolution of 831 very massive galaxies m1011h_702m_sun since z2 we split our sample according to their light concentration using the sersic index n at a given stellar mass bo... | [['using', 'the', 'combined', 'capabilities', 'of', 'the', 'large', 'nearinfrared', 'palomardeep2', 'survey', 'and', 'the', 'superb', 'resolution', 'of', 'the', 'acs', 'hst', 'camera', 'we', 'explore', 'the', 'size', 'evolution', 'of', '831', 'very', 'massive', 'galaxies', 'm1011h_702m_sun', 'since', 'z2', 'we', 'split... | [-0.07327296469456461, 0.12253769005046171, -0.06843114531297675, 0.11232555546945043, -0.07853081800653051, -0.05690461406073369, 0.003512275421492043, 0.43757790951606107, -0.1119391007540638, -0.40588777431848405, 0.0815310027623234, -0.30907974991029785, -0.02041525934028494, 0.18915402970828032, -0.032506425781963... |
709.0622 | Poisson-type deviation inequalities for curved continuous-time Markov
chains | In this paper, we present new Poisson-type deviation inequalities for
continuous-time Markov chains whose Wasserstein curvature or $\Gamma$-curvature
is bounded below. Although these two curvatures are equivalent for Brownian
motion on Riemannian manifolds, they are not comparable in discrete settings
and yield diffe... | math.PR | in this paper we present new poissontype deviation inequalities for continuoustime markov chains whose wasserstein curvature or gammacurvature is bounded below although these two curvatures are equivalent for brownian motion on riemannian manifolds they are not comparable in discrete settings and yield different deviat... | [['in', 'this', 'paper', 'we', 'present', 'new', 'poissontype', 'deviation', 'inequalities', 'for', 'continuoustime', 'markov', 'chains', 'whose', 'wasserstein', 'curvature', 'or', 'gammacurvature', 'is', 'bounded', 'below', 'although', 'these', 'two', 'curvatures', 'are', 'equivalent', 'for', 'brownian', 'motion', 'on... | [-0.09950502485233714, 0.15980367995306424, -0.02913833713126785, 0.1374984546299509, -0.04745652570343781, -0.18534063371806975, 0.012241744921150868, 0.41548861505660584, -0.2774991848453031, -0.22753002214798235, 0.1691421797741356, -0.30494226443361705, -0.11411882451796011, 0.23510090453262494, -0.1379828787620777... |
709.0623 | Evaporation and condensation of spherical interstellar clouds.
Self-consistent models with saturated heat conduction and cooling | Shortened version: The fate of IS clouds embedded in a hot tenuous medium
depends on whether the clouds suffer from evaporation or whether material
condensates onto them. Analytical solutions for the rate of evaporative mass
loss from an isolated spherical cloud embedded in a hot tenuous gas are deduced
by Cowie & Mc... | astro-ph | shortened version the fate of is clouds embedded in a hot tenuous medium depends on whether the clouds suffer from evaporation or whether material condensates onto them analytical solutions for the rate of evaporative mass loss from an isolated spherical cloud embedded in a hot tenuous gas are deduced by cowie mckee 19... | [['shortened', 'version', 'the', 'fate', 'of', 'is', 'clouds', 'embedded', 'in', 'a', 'hot', 'tenuous', 'medium', 'depends', 'on', 'whether', 'the', 'clouds', 'suffer', 'from', 'evaporation', 'or', 'whether', 'material', 'condensates', 'onto', 'them', 'analytical', 'solutions', 'for', 'the', 'rate', 'of', 'evaporative'... | [-0.08998044376778934, 0.18561216303309064, -0.042656334284693, 0.07961806798612492, -0.03867389695098003, -0.06973783984780312, 0.024142361485606268, 0.35482449966172375, -0.23894907628289527, -0.3072631688788533, 0.09669082968030125, -0.28948994206562123, 0.002062172930163797, 0.19848025384152101, 0.00540725719623474... |
709.0624 | On Faster Integer Calculations using Non-Arithmetic Primitives | The unit cost model is both convenient and largely realistic for describing
integer decision algorithms over (+,*). Additional operations like division
with remainder or bitwise conjunction, although equally supported by computing
hardware, may lead to a considerable drop in complexity. We show a variety of
concrete ... | cs.DS | the unit cost model is both convenient and largely realistic for describing integer decision algorithms over additional operations like division with remainder or bitwise conjunction although equally supported by computing hardware may lead to a considerable drop in complexity we show a variety of concrete problems to ... | [['the', 'unit', 'cost', 'model', 'is', 'both', 'convenient', 'and', 'largely', 'realistic', 'for', 'describing', 'integer', 'decision', 'algorithms', 'over', 'additional', 'operations', 'like', 'division', 'with', 'remainder', 'or', 'bitwise', 'conjunction', 'although', 'equally', 'supported', 'by', 'computing', 'hard... | [-0.1308752681539094, 0.052580613554139635, -0.05168723298820777, 0.07145728168701279, -0.08686330337550933, -0.2044504866224982, 0.09869998435379337, 0.41326150894796443, -0.29978253004156935, -0.3277229780994229, 0.1707835509343136, -0.20605666818633928, -0.18342844402551714, 0.3053184355790648, -0.13408258141381507,... |
709.0625 | Efficient Implementation of the AI-REML Iteration for Variance Component
QTL Analysis | Regions in the genome that affect complex traits, quantitative trait loci
(QTL), can be identified using statistical analysis of genetic and phenotypic
data. When restricted maximum-likelihood (REML) models are used, the mapping
procedure is normally computationally demanding. We develop a new efficient
computational... | q-bio.QM q-bio.OT | regions in the genome that affect complex traits quantitative trait loci qtl can be identified using statistical analysis of genetic and phenotypic data when restricted maximumlikelihood reml models are used the mapping procedure is normally computationally demanding we develop a new efficient computational scheme for ... | [['regions', 'in', 'the', 'genome', 'that', 'affect', 'complex', 'traits', 'quantitative', 'trait', 'loci', 'qtl', 'can', 'be', 'identified', 'using', 'statistical', 'analysis', 'of', 'genetic', 'and', 'phenotypic', 'data', 'when', 'restricted', 'maximumlikelihood', 'reml', 'models', 'are', 'used', 'the', 'mapping', 'p... | [-0.0350116134157006, 0.00013006452583406213, -0.1273782531139236, 0.12045157875253602, -0.07402386231957085, -0.1592682879564569, 0.05133760565490632, 0.4053751211964859, -0.2943712708294251, -0.2723930187335929, 0.13852835560814952, -0.2049830640203454, -0.1904743045243382, 0.20198540122295092, -0.07445954423948373, ... |
709.0626 | Consistency and robustness of kernel-based regression in convex risk
minimization | We investigate statistical properties for a broad class of modern
kernel-based regression (KBR) methods. These kernel methods were developed
during the last decade and are inspired by convex risk minimization in
infinite-dimensional Hilbert spaces. One leading example is support vector
regression. We first describe t... | math.ST stat.TH | we investigate statistical properties for a broad class of modern kernelbased regression kbr methods these kernel methods were developed during the last decade and are inspired by convex risk minimization in infinitedimensional hilbert spaces one leading example is support vector regression we first describe the relati... | [['we', 'investigate', 'statistical', 'properties', 'for', 'a', 'broad', 'class', 'of', 'modern', 'kernelbased', 'regression', 'kbr', 'methods', 'these', 'kernel', 'methods', 'were', 'developed', 'during', 'the', 'last', 'decade', 'and', 'are', 'inspired', 'by', 'convex', 'risk', 'minimization', 'in', 'infinitedimensio... | [-0.009565050299796794, 0.008578625878964375, -0.12029503964137261, 0.12301317954761604, -0.09999868043034879, -0.14746230267280458, 0.036190269352089056, 0.42820519298388093, -0.2775006424635649, -0.2604930759864111, 0.12937731336683547, -0.27128615561154446, -0.18659003670601285, 0.20166463982405178, -0.0765180169434... |
709.0627 | On It\^{o}'s formula for elliptic diffusion processes | Bardina and Jolis [Stochastic process. Appl. 69 (1997) 83--109] prove an
extension of It\^{o}'s formula for $F(X_t,t)$, where $F(x,t)$ has a locally
square-integrable derivative in $x$ that satisfies a mild continuity condition
in $t$ and $X$ is a one-dimensional diffusion process such that the law of
$X_t$ has a den... | math.PR | bardina and jolis stochastic process appl 69 1997 83109 prove an extension of itos formula for fx_tt where fxt has a locally squareintegrable derivative in x that satisfies a mild continuity condition in t and x is a onedimensional diffusion process such that the law of x_t has a density satisfying certain properties t... | [['bardina', 'and', 'jolis', 'stochastic', 'process', 'appl', '69', '1997', '83109', 'prove', 'an', 'extension', 'of', 'itos', 'formula', 'for', 'fx_tt', 'where', 'fxt', 'has', 'a', 'locally', 'squareintegrable', 'derivative', 'in', 'x', 'that', 'satisfies', 'a', 'mild', 'continuity', 'condition', 'in', 't', 'and', 'x'... | [-0.1408838994987309, 0.07518976516381372, -0.1293373477095738, 0.024613989817124093, -0.07320345433428883, -0.11014709743857384, 0.026933698754757644, 0.35764973021112384, -0.3114596876502037, -0.2168641263828613, 0.10307772703282535, -0.24842505192384123, -0.15384435012936593, 0.17562227469682692, -0.1131032563615590... |
709.0628 | Lagrangian Investigation of Two-Dimensional Decaying Turbulence | We present a numerical investigation of two-dimensional decaying turbulence
in the Lagrangian framework. Focusing on single particle statistics, we
investigate Lagrangian trajectories in a freely evolving turbulent velocity
field. The dynamical evolution of the tracer particles is strongly dominated by
the emergence ... | physics.flu-dyn | we present a numerical investigation of twodimensional decaying turbulence in the lagrangian framework focusing on single particle statistics we investigate lagrangian trajectories in a freely evolving turbulent velocity field the dynamical evolution of the tracer particles is strongly dominated by the emergence and ev... | [['we', 'present', 'a', 'numerical', 'investigation', 'of', 'twodimensional', 'decaying', 'turbulence', 'in', 'the', 'lagrangian', 'framework', 'focusing', 'on', 'single', 'particle', 'statistics', 'we', 'investigate', 'lagrangian', 'trajectories', 'in', 'a', 'freely', 'evolving', 'turbulent', 'velocity', 'field', 'the... | [-0.1923049126911792, 0.1775083753396757, -0.14742147673096043, 0.11344788298738422, -0.032915364287327976, -0.06819286847749026, -0.052695961567224, 0.3361892501008697, -0.2547289612120949, -0.24885469797300175, 0.03217468303919304, -0.24161468567326666, -0.13357753948075696, 0.19734043207281501, 0.03818518379703164, ... |
709.0629 | Antisymmetric rank--2 tensor unparticle physics | We present the phenomenology of antisymmetric rank-2 tensor unparticle
operator ${\cal O}_{\cal U,A}^{\mu\nu}$ with scaling dimension $d_{\cal U}$. We
consider the physical effects of operator $O_{\cal U,A}^{\mu\nu}$ in $Z^0$
boson invisible decays $Z^0 \to {\cal U}$, $Z^0 \to b \bar{b}$ channel, the
electroweak prec... | hep-ph | we present the phenomenology of antisymmetric rank2 tensor unparticle operator cal o_cal uamunu with scaling dimension d_cal u we consider the physical effects of operator o_cal uamunu in z0 boson invisible decays z0 to cal u z0 to b barb channel the electroweak precision observable s parameter and the muon anomalous m... | [['we', 'present', 'the', 'phenomenology', 'of', 'antisymmetric', 'rank2', 'tensor', 'unparticle', 'operator', 'cal', 'o_cal', 'uamunu', 'with', 'scaling', 'dimension', 'd_cal', 'u', 'we', 'consider', 'the', 'physical', 'effects', 'of', 'operator', 'o_cal', 'uamunu', 'in', 'z0', 'boson', 'invisible', 'decays', 'z0', 't... | [-0.17636783994612093, 0.25772879847675456, 0.03539343689178638, 0.12410743043226262, -0.11280349663174744, -0.24403936312705649, 0.024585423589409957, 0.2756498242787858, -0.2505428969384508, -0.23438039987433887, 0.007519715828887114, -0.35879939877764977, 0.054237274510838776, 0.09976135975367914, 0.1073521300687963... |
709.063 | The basic K nuclear cluster K- pp and its enhanced formation in the p +
p -> K+ + X reaction | We have studied the structure of K- pp nuclear cluster comprehensively by
solving this three-body system exactly in a variational method starting from
the Ansatz that the Lambda(1405) resonance (Lambda*) is a K-p bound state. We
have found that our original prediction for the presence of K-pp as a compact
bound syste... | nucl-th | we have studied the structure of k pp nuclear cluster comprehensively by solving this threebody system exactly in a variational method starting from the ansatz that the lambda1405 resonance lambda is a kp bound state we have found that our original prediction for the presence of kpp as a compact bound system with m 232... | [['we', 'have', 'studied', 'the', 'structure', 'of', 'k', 'pp', 'nuclear', 'cluster', 'comprehensively', 'by', 'solving', 'this', 'threebody', 'system', 'exactly', 'in', 'a', 'variational', 'method', 'starting', 'from', 'the', 'ansatz', 'that', 'the', 'lambda1405', 'resonance', 'lambda', 'is', 'a', 'kp', 'bound', 'stat... | [-0.14289470095201537, 0.19022610790711814, -0.08884738619389916, 0.07188871183586315, 0.0025504367888171337, -0.16829425286656866, 0.057837243675727, 0.33720925820172964, -0.2380379450817903, -0.30901006523547975, -0.04862536321196592, -0.290826081213626, -0.05582907423116867, 0.11192829202380822, 0.11266301287846132,... |
709.0631 | Massive stars: their contribution to energy and element budget in
chemo-dynamical galaxy evolution | Here results of numerical radiation hydrodynamical simulations are presented
which explore the energetic impact of massive stars on the interstellar medium.
We study the evolution of the ambient gas around isolated massive stars in the
mass range between 15 and 85 Msun in order to analyze the formation of
structures ... | astro-ph | here results of numerical radiation hydrodynamical simulations are presented which explore the energetic impact of massive stars on the interstellar medium we study the evolution of the ambient gas around isolated massive stars in the mass range between 15 and 85 msun in order to analyze the formation of structures and... | [['here', 'results', 'of', 'numerical', 'radiation', 'hydrodynamical', 'simulations', 'are', 'presented', 'which', 'explore', 'the', 'energetic', 'impact', 'of', 'massive', 'stars', 'on', 'the', 'interstellar', 'medium', 'we', 'study', 'the', 'evolution', 'of', 'the', 'ambient', 'gas', 'around', 'isolated', 'massive', ... | [-0.0608753720264455, 0.14276393694757036, -0.033509838584965715, 0.11854558908065277, -0.058432645987098415, -0.009349559658827881, 0.03754959090535218, 0.40486669773235917, -0.17136336797848345, -0.3824754444649443, 0.07917572533575973, -0.28874903756950515, -0.004199610765014464, 0.16687800583119194, 0.0366031675152... |
709.0632 | Bogoliubov angle and visualization of particle-hole mixture in
superconductors | Superconducting excitations --Bogoliubov quasiparticles -- are the quantum
mechanical mixture of negatively charged electron (-e) and positively charged
hole (+e). Depending on the applied voltage bias in STM one can sample the
particle and hole content of such a superconducting excitation. Recent Scanning
Tunneling ... | cond-mat.supr-con cond-mat.str-el | superconducting excitations bogoliubov quasiparticles are the quantum mechanical mixture of negatively charged electron e and positively charged hole e depending on the applied voltage bias in stm one can sample the particle and hole content of such a superconducting excitation recent scanning tunneling microscope stm ... | [['superconducting', 'excitations', 'bogoliubov', 'quasiparticles', 'are', 'the', 'quantum', 'mechanical', 'mixture', 'of', 'negatively', 'charged', 'electron', 'e', 'and', 'positively', 'charged', 'hole', 'e', 'depending', 'on', 'the', 'applied', 'voltage', 'bias', 'in', 'stm', 'one', 'can', 'sample', 'the', 'particle... | [-0.16598398634364123, 0.2389948098067889, -0.11551547536658029, 0.10101617982290095, -0.05977091268967774, -0.18772627691617289, 0.11462786364221766, 0.34622572893855597, -0.24911027776319428, -0.2719598836923218, -0.05941910543222517, -0.3378573932651579, -0.0574590925358783, 0.17251835953007522, -0.00324826149038423... |
709.0633 | INTEGRAL observations of the Small Magellanic Cloud | The first INTEGRAL observations of the Small Magellanic Cloud (carried out in
2003) are reported in which two sources are clearly detected. The first source,
SMC X-1, shows a hard X-ray eclipse and measurements of its pulse period
indicate a continuation of the long-term spin-up now covering ~30 years. The
second sou... | astro-ph | the first integral observations of the small magellanic cloud carried out in 2003 are reported in which two sources are clearly detected the first source smc x1 shows a hard xray eclipse and measurements of its pulse period indicate a continuation of the longterm spinup now covering 30 years the second source is likely... | [['the', 'first', 'integral', 'observations', 'of', 'the', 'small', 'magellanic', 'cloud', 'carried', 'out', 'in', '2003', 'are', 'reported', 'in', 'which', 'two', 'sources', 'are', 'clearly', 'detected', 'the', 'first', 'source', 'smc', 'x1', 'shows', 'a', 'hard', 'xray', 'eclipse', 'and', 'measurements', 'of', 'its',... | [-0.1550637434955051, 0.0740530439175335, -0.08710503978871328, 0.11494940798729658, -0.09989803875868693, -0.1182528998045785, 0.08769531973615982, 0.4634670425394131, -0.24031596825378695, -0.33290098264611273, 0.15930283338990237, -0.30380297838818543, -0.046566525288287176, 0.258560031921379, -0.0530503373268212, 0... |
709.0634 | Detectors for Cosmic Rays on Ground and in Space | The origin of the cosmic rays has been a great mystery since they were
discovered by Victor Hess in 1912. AGASA's observation of ultra-high-energy
cosmic-rays (UHECR) possibly beyond the GZK (Greisen, Zatsepin and Kuzmin)
cutoff stimulated the field in great deal. In addition, Kamiokande's detection
of neutrinos from... | physics.ins-det | the origin of the cosmic rays has been a great mystery since they were discovered by victor hess in 1912 agasas observation of ultrahighenergy cosmicrays uhecr possibly beyond the gzk greisen zatsepin and kuzmin cutoff stimulated the field in great deal in addition kamiokandes detection of neutrinos from sn1987a and th... | [['the', 'origin', 'of', 'the', 'cosmic', 'rays', 'has', 'been', 'a', 'great', 'mystery', 'since', 'they', 'were', 'discovered', 'by', 'victor', 'hess', 'in', '1912', 'agasas', 'observation', 'of', 'ultrahighenergy', 'cosmicrays', 'uhecr', 'possibly', 'beyond', 'the', 'gzk', 'greisen', 'zatsepin', 'and', 'kuzmin', 'cut... | [-0.03819717152663917, 0.253875613042756, -0.0578468922059983, 0.20285190186627647, -0.12363863834179938, -0.026901863534551332, -0.039304747202378865, 0.38103913315297927, -0.2093073124298826, -0.3745262490092393, -0.01445795764995958, -0.38737314145957286, 0.013159097285996027, 0.2388023371767143, 0.02287556196268483... |
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