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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709.1135 | Parameter estimation in diagonalizable bilinear stochastic parabolic
equations | A parameter estimation problem is considered for a stochastic parabolic
equation with multiplicative noise under the assumption that the equation can
be reduced to an infinite system of uncoupled diffusion processes. From the
point of view of classical statistics, this problem turns out to be singular
not only for th... | math.PR math.ST stat.TH | a parameter estimation problem is considered for a stochastic parabolic equation with multiplicative noise under the assumption that the equation can be reduced to an infinite system of uncoupled diffusion processes from the point of view of classical statistics this problem turns out to be singular not only for the or... | [['a', 'parameter', 'estimation', 'problem', 'is', 'considered', 'for', 'a', 'stochastic', 'parabolic', 'equation', 'with', 'multiplicative', 'noise', 'under', 'the', 'assumption', 'that', 'the', 'equation', 'can', 'be', 'reduced', 'to', 'an', 'infinite', 'system', 'of', 'uncoupled', 'diffusion', 'processes', 'from', '... | [-0.064780217261581, 0.030088802481368915, -0.1253434954216726, 0.08369826002001583, -0.09037702399339662, -0.18932543366204901, 0.03788484421457691, 0.30405149743499527, -0.3716205601280286, -0.22544766583266745, 0.1696935007755409, -0.22827980573098344, -0.1601520127459732, 0.23043544226920748, -0.11152506124856601, ... |
709.1136 | Long Term Radio Monitoring of SN 1993J | We present our observations of the radio emission from supernova (SN) 1993J,
in M 81 (NGC 3031), made with the VLA, from 90 to 0.7 cm, as well as numerous
measurements from other telescopes. The combined data set constitutes probably
the most detailed set of measurements ever established for any SN outside of
the Loc... | astro-ph | we present our observations of the radio emission from supernova sn 1993j in m 81 ngc 3031 made with the vla from 90 to 07 cm as well as numerous measurements from other telescopes the combined data set constitutes probably the most detailed set of measurements ever established for any sn outside of the local group in ... | [['we', 'present', 'our', 'observations', 'of', 'the', 'radio', 'emission', 'from', 'supernova', 'sn', '1993j', 'in', 'm', '81', 'ngc', '3031', 'made', 'with', 'the', 'vla', 'from', '90', 'to', '07', 'cm', 'as', 'well', 'as', 'numerous', 'measurements', 'from', 'other', 'telescopes', 'the', 'combined', 'data', 'set', '... | [-0.055148917357795514, 0.10518921411768137, -0.08144359484184097, 0.07517180004323377, -0.07683385607870576, -0.1213705117244236, 0.063221239019964, 0.437949313610842, -0.20101732226364302, -0.33140465949450226, 0.11363154682206196, -0.29624527006294815, -0.00036815623363423903, 0.2131309846562511, -0.0055810083062029... |
709.1137 | Looking for Super-Earths in the HD 189733 System: A Search for Transits
in Most Space-Based Photometry | We have made a comprehensive transit search for exoplanets down to ~1.5 - 2
Earth radii in the HD 189733 system, based on 21-days of nearly uninterrupted
broadband optical photometry obtained with the MOST (Microvariability &
Oscillations of STars) satellite in 2006. We have searched these data for
realistic limb-dar... | astro-ph | we have made a comprehensive transit search for exoplanets down to 15 2 earth radii in the hd 189733 system based on 21days of nearly uninterrupted broadband optical photometry obtained with the most microvariability oscillations of stars satellite in 2006 we have searched these data for realistic limbdarkened transits... | [['we', 'have', 'made', 'a', 'comprehensive', 'transit', 'search', 'for', 'exoplanets', 'down', 'to', '15', '2', 'earth', 'radii', 'in', 'the', 'hd', '189733', 'system', 'based', 'on', '21days', 'of', 'nearly', 'uninterrupted', 'broadband', 'optical', 'photometry', 'obtained', 'with', 'the', 'most', 'microvariability',... | [-0.08174839922576212, 0.1622751303453697, -0.08060494782403112, 0.042876299638010096, -0.13777022040012527, -0.13650463299418333, 0.13109311404186882, 0.3458588552486617, -0.1129243251911248, -0.3946233780356124, 0.09460971687440178, -0.3671652049853947, -0.042440200679993725, 0.24328688330133447, -0.11457951553747989... |
709.1138 | Characterizing Heavy-Tailed Distributions Induced by Retransmissions | Consider a generic data unit of random size L that needs to be transmitted
over a channel of unit capacity. The channel availability dynamics is modeled
as an i.i.d. sequence {A, A_i},i>0 that is independent of L. During each period
of time that the channel becomes available, say A_i, we attempt to transmit the
data ... | math.PR | consider a generic data unit of random size l that needs to be transmitted over a channel of unit capacity the channel availability dynamics is modeled as an iid sequence a a_ii0 that is independent of l during each period of time that the channel becomes available say a_i we attempt to transmit the data unit if la_i t... | [['consider', 'a', 'generic', 'data', 'unit', 'of', 'random', 'size', 'l', 'that', 'needs', 'to', 'be', 'transmitted', 'over', 'a', 'channel', 'of', 'unit', 'capacity', 'the', 'channel', 'availability', 'dynamics', 'is', 'modeled', 'as', 'an', 'iid', 'sequence', 'a', 'a_ii0', 'that', 'is', 'independent', 'of', 'l', 'du... | [-0.17152326040714166, 0.10190663737653882, -0.08069681559636473, 0.025843401944801603, -0.03625330034090312, -0.15088760772288887, 0.09053054450010661, 0.36813906809990193, -0.2962312462320755, -0.28254439607382076, 0.11878651215473197, -0.2804055913762234, -0.1526983745124671, 0.1437272463170771, -0.07341182698682763... |
709.1139 | Cosmic String Detection via Microlensing of Stars | Cosmic superstrings are produced towards the end of the brane inflation. If
the string tension is low enough, loops tend to be relatively long-lived. The
resultant string network is expected to contain many loops which are smaller
than typical Galactic scales. Cosmic expansion damps the center of mass motion
of the l... | astro-ph gr-qc | cosmic superstrings are produced towards the end of the brane inflation if the string tension is low enough loops tend to be relatively longlived the resultant string network is expected to contain many loops which are smaller than typical galactic scales cosmic expansion damps the center of mass motion of the loops wh... | [['cosmic', 'superstrings', 'are', 'produced', 'towards', 'the', 'end', 'of', 'the', 'brane', 'inflation', 'if', 'the', 'string', 'tension', 'is', 'low', 'enough', 'loops', 'tend', 'to', 'be', 'relatively', 'longlived', 'the', 'resultant', 'string', 'network', 'is', 'expected', 'to', 'contain', 'many', 'loops', 'which'... | [-0.1629609613477279, 0.18594670803358304, -0.06620459769648022, 0.12644635516595534, -0.13470517590782052, -0.10020020228954471, 0.017372928397461195, 0.3476352069973643, -0.22194287265798576, -0.34093954100659707, 0.0718601616274573, -0.284418009439241, -0.044933378422912965, 0.20082601771228076, -0.02511927479193447... |
709.114 | Interaction Correction of Conductivity Near a Ferromagnetic Quantum
Critical Point | We calculate the temperature dependence of conductivity due to interaction
correction for a disordered itinerant electron system close to a ferromagnetic
quantum critical point which occurs due to a spin density wave instability. In
the quantum critical regime, the crossover between diffusive and ballistic
transport ... | cond-mat.str-el cond-mat.dis-nn | we calculate the temperature dependence of conductivity due to interaction correction for a disordered itinerant electron system close to a ferromagnetic quantum critical point which occurs due to a spin density wave instability in the quantum critical regime the crossover between diffusive and ballistic transport occu... | [['we', 'calculate', 'the', 'temperature', 'dependence', 'of', 'conductivity', 'due', 'to', 'interaction', 'correction', 'for', 'a', 'disordered', 'itinerant', 'electron', 'system', 'close', 'to', 'a', 'ferromagnetic', 'quantum', 'critical', 'point', 'which', 'occurs', 'due', 'to', 'a', 'spin', 'density', 'wave', 'inst... | [-0.17978724640483656, 0.26766467015258966, -0.06592217928109069, 0.051797229480774455, 0.0028310783766210077, -0.18229816674410054, 0.07903421617578715, 0.2724301734007895, -0.2824952976219356, -0.22810745210076372, 0.0140440483589191, -0.3565258394430081, -0.08608837685237328, 0.20107709807654223, 0.0697561085720857,... |
709.1141 | Explicit Rational Solution of the KZ Equation (example) | We investigate the Knizhnik-Zamolodchikov linear differential system. The
coefficients of this system are rational functions. We have proved that the
solution of the KZ system is rational when k is equal to two and n is equal to
three (see [5]) . In this paper, we construct the corresponding solution in the
explicit ... | math.CA math-ph math.MP | we investigate the knizhnikzamolodchikov linear differential system the coefficients of this system are rational functions we have proved that the solution of the kz system is rational when k is equal to two and n is equal to three see 5 in this paper we construct the corresponding solution in the explicit form | [['we', 'investigate', 'the', 'knizhnikzamolodchikov', 'linear', 'differential', 'system', 'the', 'coefficients', 'of', 'this', 'system', 'are', 'rational', 'functions', 'we', 'have', 'proved', 'that', 'the', 'solution', 'of', 'the', 'kz', 'system', 'is', 'rational', 'when', 'k', 'is', 'equal', 'to', 'two', 'and', 'n',... | [-0.20877588083440402, 0.02944970461935297, -0.07864301238771317, 0.03469465825188343, -0.037862823617135014, -0.14884147863343078, -0.03515529359980785, 0.3099954407310711, -0.29775418130294334, -0.2377050960401319, 0.10733525920220001, -0.32081487438342765, -0.20490593460985934, 0.16632672849128832, -0.03801472119565... |
709.1142 | Quantum expanders from any classical Cayley graph expander | We give a simple recipe for translating walks on Cayley graphs of a group G
into a quantum operation on any irrep of G. Most properties of the classical
walk carry over to the quantum operation: degree becomes the number of Kraus
operators, the spectral gap becomes the gap of the quantum operation (viewed as
a linear... | quant-ph | we give a simple recipe for translating walks on cayley graphs of a group g into a quantum operation on any irrep of g most properties of the classical walk carry over to the quantum operation degree becomes the number of kraus operators the spectral gap becomes the gap of the quantum operation viewed as a linear map o... | [['we', 'give', 'a', 'simple', 'recipe', 'for', 'translating', 'walks', 'on', 'cayley', 'graphs', 'of', 'a', 'group', 'g', 'into', 'a', 'quantum', 'operation', 'on', 'any', 'irrep', 'of', 'g', 'most', 'properties', 'of', 'the', 'classical', 'walk', 'carry', 'over', 'to', 'the', 'quantum', 'operation', 'degree', 'become... | [-0.1901098403539176, 0.1625369769676278, -0.12138323359014024, 0.03885462346176306, -0.0784044755201432, -0.1475021837367898, 0.06304745022650986, 0.40643294442977224, -0.2769614710749704, -0.23316874160830464, 0.13327252919719154, -0.247095819819896, -0.15312725049221798, 0.24613158389748563, -0.06756863598490045, 0.... |
709.1143 | Dynamics of femtosecond magnetization reversal induced by circularly
polarized light in the presence of fluctuations and dissipation | Magnetization reversal by a femtosecond circularly polarized laser pulse has
been recently demonstrated in rare-earth doped transition metals (RE-TM). The
switching mechanism has been attributed to an inverse Faraday effect and
thermal effects. Based on the parameters provided in the experimental work, we
show that t... | cond-mat.mtrl-sci | magnetization reversal by a femtosecond circularly polarized laser pulse has been recently demonstrated in rareearth doped transition metals retm the switching mechanism has been attributed to an inverse faraday effect and thermal effects based on the parameters provided in the experimental work we show that this claim... | [['magnetization', 'reversal', 'by', 'a', 'femtosecond', 'circularly', 'polarized', 'laser', 'pulse', 'has', 'been', 'recently', 'demonstrated', 'in', 'rareearth', 'doped', 'transition', 'metals', 'retm', 'the', 'switching', 'mechanism', 'has', 'been', 'attributed', 'to', 'an', 'inverse', 'faraday', 'effect', 'and', 't... | [-0.13240655276136912, 0.17198082726418962, -0.06897614493481512, 0.012575684739248373, -0.0675341528423918, -0.10675051311651866, 0.07076162593136352, 0.4156673387662182, -0.25155867591909153, -0.30976397394225363, 0.009386004089771551, -0.27522732774969344, -0.10822395728976746, 0.19382552919735208, 0.001348476281495... |
709.1144 | Cosmic Microwave Background Statistics for a Direction-Dependent
Primordial Power Spectrum | Statistical isotropy of primordial perturbations is a common assumption in
cosmology, but it is an assumption that should be tested. To this end, we
develop cosmic microwave background statistics for a primordial power spectrum
that depends on the direction, as well as the magnitude, of the Fourier
wavevector. We fir... | astro-ph | statistical isotropy of primordial perturbations is a common assumption in cosmology but it is an assumption that should be tested to this end we develop cosmic microwave background statistics for a primordial power spectrum that depends on the direction as well as the magnitude of the fourier wavevector we first consi... | [['statistical', 'isotropy', 'of', 'primordial', 'perturbations', 'is', 'a', 'common', 'assumption', 'in', 'cosmology', 'but', 'it', 'is', 'an', 'assumption', 'that', 'should', 'be', 'tested', 'to', 'this', 'end', 'we', 'develop', 'cosmic', 'microwave', 'background', 'statistics', 'for', 'a', 'primordial', 'power', 'sp... | [-0.12305661921138661, 0.13656352015700227, -0.12774263926996635, 0.07691615073171516, -0.08369320447628315, -0.06066452589674065, -0.04007932842136003, 0.3262085625471977, -0.25941207090464347, -0.28549172283293534, 0.0908991232021855, -0.2773475269643733, -0.09706991782161192, 0.21873349271392306, 0.00107210080425899... |
709.1145 | Precise radial velocities of giant stars. III. Spectroscopic stellar
parameters | Context: A radial velocity survey of about 380 G and K giant stars is ongoing
at Lick observatory. For each star we have a high signal to noise ratio
template spectrum, which we use to determine spectroscopic stellar parameters.
Aim: The aim of this paper is to present spectroscopic stellar parameters, i.e.
effective... | astro-ph | context a radial velocity survey of about 380 g and k giant stars is ongoing at lick observatory for each star we have a high signal to noise ratio template spectrum which we use to determine spectroscopic stellar parameters aim the aim of this paper is to present spectroscopic stellar parameters ie effective temperatu... | [['context', 'a', 'radial', 'velocity', 'survey', 'of', 'about', '380', 'g', 'and', 'k', 'giant', 'stars', 'is', 'ongoing', 'at', 'lick', 'observatory', 'for', 'each', 'star', 'we', 'have', 'a', 'high', 'signal', 'to', 'noise', 'ratio', 'template', 'spectrum', 'which', 'we', 'use', 'to', 'determine', 'spectroscopic', '... | [-0.05440452423859522, 0.14899360466687958, -0.05379266543347483, 0.06089326764706149, -0.09459535296441524, -0.08044419260124007, 0.09018216178111987, 0.4233380541632402, -0.11866586181899996, -0.4153696330766856, 0.02361972897442979, -0.2976775186721383, -0.003504959827739517, 0.21841575609207395, -0.0636108841987441... |
709.1146 | The influence of polaron size on the conductivity of poly-DNA | The velocity of polaron migration in the long poly-DNA chain (~40 base pairs)
in an applied electric field has been studied within a polaron model. We found
that the polaron velocity strongly depends on the polaron size. A small polaron
shows a slow propagation and strong tolerance to the electric field, while a
larg... | cond-mat.soft | the velocity of polaron migration in the long polydna chain 40 base pairs in an applied electric field has been studied within a polaron model we found that the polaron velocity strongly depends on the polaron size a small polaron shows a slow propagation and strong tolerance to the electric field while a large polaron... | [['the', 'velocity', 'of', 'polaron', 'migration', 'in', 'the', 'long', 'polydna', 'chain', '40', 'base', 'pairs', 'in', 'an', 'applied', 'electric', 'field', 'has', 'been', 'studied', 'within', 'a', 'polaron', 'model', 'we', 'found', 'that', 'the', 'polaron', 'velocity', 'strongly', 'depends', 'on', 'the', 'polaron', ... | [-0.15983103293717463, 0.20653102461368147, -0.039971732138160694, 0.07077547007468232, -0.0335997921077812, -0.15510373981298006, 0.059356539165898364, 0.39626415648517455, -0.2624314134306413, -0.25618757022188066, -0.007279997170120081, -0.23500853820525586, -0.08083888933686738, 0.16215947095522695, -0.000917597262... |
709.1147 | Physical interpretation of the near-infrared colours of low redshift
galaxies | We use empirical techniques to interpret the near-infrared colours of a
sample of 5800 galaxies drawn from Sloan Digital Sky Survey (SDSS) main
spectroscopic sample with YJHK photometry from the UK Infrared Deep Sky Survey
(UKIDSS) data release one. We study correlations between near-IR colours
measured within SDSS f... | astro-ph | we use empirical techniques to interpret the nearinfrared colours of a sample of 5800 galaxies drawn from sloan digital sky survey sdss main spectroscopic sample with yjhk photometry from the uk infrared deep sky survey ukidss data release one we study correlations between nearir colours measured within sdss fibre and ... | [['we', 'use', 'empirical', 'techniques', 'to', 'interpret', 'the', 'nearinfrared', 'colours', 'of', 'a', 'sample', 'of', '5800', 'galaxies', 'drawn', 'from', 'sloan', 'digital', 'sky', 'survey', 'sdss', 'main', 'spectroscopic', 'sample', 'with', 'yjhk', 'photometry', 'from', 'the', 'uk', 'infrared', 'deep', 'sky', 'su... | [0.045067159331070805, 0.09092398205357728, -0.11585547501869109, 0.12100635840249435, -0.12789408369308528, -0.05721203471731373, 0.035616316811355124, 0.5114795066001949, -0.08755623879678683, -0.3395111408676003, 0.007740883403652464, -0.32922987079694016, -0.023777480456737284, 0.19133252649614058, -0.1063208947110... |
709.1148 | Surface tank-treading: propulsion of Purcell's toroidal swimmer | In this work we address the "smoking ring" propulsion technique, originally
proposed by E. M. Purcell. We first consider self-locomotion of a
doughnut-shaped swimmer powered by surface tank-treading. Different modes of
surface motion are assumed and propulsion velocity and swimming efficiency are
determined. The swim... | physics.flu-dyn physics.bio-ph | in this work we address the smoking ring propulsion technique originally proposed by e m purcell we first consider selflocomotion of a doughnutshaped swimmer powered by surface tanktreading different modes of surface motion are assumed and propulsion velocity and swimming efficiency are determined the swimmer is propel... | [['in', 'this', 'work', 'we', 'address', 'the', 'smoking', 'ring', 'propulsion', 'technique', 'originally', 'proposed', 'by', 'e', 'm', 'purcell', 'we', 'first', 'consider', 'selflocomotion', 'of', 'a', 'doughnutshaped', 'swimmer', 'powered', 'by', 'surface', 'tanktreading', 'different', 'modes', 'of', 'surface', 'moti... | [-0.1781169980872489, 0.16609146665765107, -0.0633952525011929, -0.02645438929300456, -0.10850466299868589, -0.1715889718416812, -0.012384016213140317, 0.3812558576464653, -0.2443766705924645, -0.3200029285624623, 0.02081972038338011, -0.17258323277014176, -0.16548287864508374, 0.24433466720095437, -0.10405365755515439... |
709.1149 | Representing probabilistic data via ontological models | Ontological models are attempts to quantitatively describe the results of a
probabilistic theory, such as Quantum Mechanics, in a framework exhibiting an
explicit realism-based underpinning. Unlike either the well known
quasi-probability representations, or the "r-p" vector formalism, these models
are contextual and ... | quant-ph | ontological models are attempts to quantitatively describe the results of a probabilistic theory such as quantum mechanics in a framework exhibiting an explicit realismbased underpinning unlike either the well known quasiprobability representations or the rp vector formalism these models are contextual and by definitio... | [['ontological', 'models', 'are', 'attempts', 'to', 'quantitatively', 'describe', 'the', 'results', 'of', 'a', 'probabilistic', 'theory', 'such', 'as', 'quantum', 'mechanics', 'in', 'a', 'framework', 'exhibiting', 'an', 'explicit', 'realismbased', 'underpinning', 'unlike', 'either', 'the', 'well', 'known', 'quasiprobab... | [-0.06252918588571658, 0.09878375023642909, -0.1120796057360553, 0.1227952921133144, -0.05283178870999956, -0.15147676948164526, 0.044839033608210004, 0.348236521469965, -0.26768234614219055, -0.31835979228354483, 0.0758128431793111, -0.2416341449955338, -0.20919179749732505, 0.1576438651704038, -0.0780233229025688, 0.... |
709.115 | Beyond Two Dark Energy Parameters | Our ignorance of the dark energy is generally described by a two-parameter
equation of state. In these approaches a particular {\it ad hoc} functional
form is assumed, and only two independent parameters are incorporated. We
propose a model-independent, multi-parameter approach to fitting the dark
energy, and show th... | astro-ph | our ignorance of the dark energy is generally described by a twoparameter equation of state in these approaches a particular it ad hoc functional form is assumed and only two independent parameters are incorporated we propose a modelindependent multiparameter approach to fitting the dark energy and show that nextgenera... | [['our', 'ignorance', 'of', 'the', 'dark', 'energy', 'is', 'generally', 'described', 'by', 'a', 'twoparameter', 'equation', 'of', 'state', 'in', 'these', 'approaches', 'a', 'particular', 'it', 'ad', 'hoc', 'functional', 'form', 'is', 'assumed', 'and', 'only', 'two', 'independent', 'parameters', 'are', 'incorporated', '... | [-0.10933647380685822, 0.09311647676319505, -0.10192590539736557, 0.11588053805220018, -0.13187389710219577, -0.13550483110399605, 0.028414851731213275, 0.3626236850444305, -0.21089708854075676, -0.3540039429499302, 0.07481971187128995, -0.2629899540916085, -0.07138643808381555, 0.20602751594560686, -0.0096767046100770... |
709.1151 | Euler-Bernoulli beams from a symmetry standpoint-characterization of
equivalent equations | We completely solve the equivalence problem for Euler-Bernoulli equation
using Lie symmetry analysis. We show that the quotient of the symmetry Lie
algebra of the Bernoulli equation by the infinite-dimensional Lie algebra
spanned by solution symmetries is a representation of one of the following Lie
algebras: $2A_1$,... | math.AP | we completely solve the equivalence problem for eulerbernoulli equation using lie symmetry analysis we show that the quotient of the symmetry lie algebra of the bernoulli equation by the infinitedimensional lie algebra spanned by solution symmetries is a representation of one of the following lie algebras 2a_1 a_1oplus... | [['we', 'completely', 'solve', 'the', 'equivalence', 'problem', 'for', 'eulerbernoulli', 'equation', 'using', 'lie', 'symmetry', 'analysis', 'we', 'show', 'that', 'the', 'quotient', 'of', 'the', 'symmetry', 'lie', 'algebra', 'of', 'the', 'bernoulli', 'equation', 'by', 'the', 'infinitedimensional', 'lie', 'algebra', 'sp... | [-0.1569895403870837, 0.1226950041762277, -0.041386869075916155, 0.04332849083460887, -0.15318181833866587, -0.15459013451881548, -0.014811636984070882, 0.3197553833139109, -0.31686986020662167, -0.23043326802546793, 0.10279975939378579, -0.23064561436656228, -0.1207208366596457, 0.13044820105201227, -0.064118943437240... |
709.1152 | Power-law Signatures and Patchiness in Genechip Oligonucleotide
Microarrays | . Genechip oligonucleotide microarrays have been used widely for
transcriptional profiling of a large number of genes in a given paradigm. Gene
expression estimation precedes biological inference and is given as a complex
combination of atomic entities on the array called probes. These probe
intensities are further c... | q-bio.GN q-bio.QM | genechip oligonucleotide microarrays have been used widely for transcriptional profiling of a large number of genes in a given paradigm gene expression estimation precedes biological inference and is given as a complex combination of atomic entities on the array called probes these probe intensities are further classif... | [['genechip', 'oligonucleotide', 'microarrays', 'have', 'been', 'used', 'widely', 'for', 'transcriptional', 'profiling', 'of', 'a', 'large', 'number', 'of', 'genes', 'in', 'a', 'given', 'paradigm', 'gene', 'expression', 'estimation', 'precedes', 'biological', 'inference', 'and', 'is', 'given', 'as', 'a', 'complex', 'co... | [-0.0802490439623241, 0.08679912600923201, -0.04442264523100237, 0.13453239620550825, -0.03128193048599722, -0.16268286187330197, 0.017439013586283244, 0.39965275988496585, -0.24903899983599267, -0.3357994899025251, 0.05606681352946907, -0.3084489354028784, -0.13222780227942135, 0.2213077522268326, -0.01160133167266331... |
709.1153 | Cross-correlation Weak Lensing of SDSS Galaxy Clusters I: Measurements | This is the first in a series of papers on the weak lensing effect caused by
clusters of galaxies in Sloan Digital Sky Survey. The photometrically selected
cluster sample, known as MaxBCG, includes ~130,000 objects between redshift 0.1
and 0.3, ranging in size from small groups to massive clusters. We split the
clust... | astro-ph | this is the first in a series of papers on the weak lensing effect caused by clusters of galaxies in sloan digital sky survey the photometrically selected cluster sample known as maxbcg includes 130000 objects between redshift 01 and 03 ranging in size from small groups to massive clusters we split the clusters into bi... | [['this', 'is', 'the', 'first', 'in', 'a', 'series', 'of', 'papers', 'on', 'the', 'weak', 'lensing', 'effect', 'caused', 'by', 'clusters', 'of', 'galaxies', 'in', 'sloan', 'digital', 'sky', 'survey', 'the', 'photometrically', 'selected', 'cluster', 'sample', 'known', 'as', 'maxbcg', 'includes', '130000', 'objects', 'be... | [-0.05300034676748705, 0.08727007819083236, -0.05883090342775596, 0.1117749127662111, -0.0710910346391064, -0.03270457234791657, 0.04094259731324488, 0.4247497364384714, -0.19785800964009725, -0.4057173775886054, 0.05081340386004372, -0.3245012532798988, -0.0193486553484853, 0.1952517101106843, -0.015340870620516932, -... |
709.1154 | Brauer-Manin obstructions to integral points | We study Brauer-Manin obstructions to integral points on open subsets of the
projective plane.
| math.AG math.NT | we study brauermanin obstructions to integral points on open subsets of the projective plane | [['we', 'study', 'brauermanin', 'obstructions', 'to', 'integral', 'points', 'on', 'open', 'subsets', 'of', 'the', 'projective', 'plane']] | [-0.3598753570445946, -0.10811125240953905, -0.09120032084839684, 0.1540790204224842, -0.16897517362875597, -0.01037772957767759, 0.15567776118405163, 0.33848124529634205, -0.36067010728376253, -0.17489022122962133, 0.10297248628921807, -0.32297859134684714, -0.12441008484789304, 0.2408744167270405, -0.2049481872735279... |
709.1155 | iso-spectral Euler-Bernoulli beams \`a la Sophus Lie | We obtain iso-spectral Euler-Bernoulli beams by using factorization and Lie
symmetry techniques. The canonical Euler-Bernoulli beam operator is factorized
as the product of a second-order linear differential operator and its adjoint.
The factors are then reversed to obtain iso-spectral beams. The factorization
is pos... | math.AP | we obtain isospectral eulerbernoulli beams by using factorization and lie symmetry techniques the canonical eulerbernoulli beam operator is factorized as the product of a secondorder linear differential operator and its adjoint the factors are then reversed to obtain isospectral beams the factorization is possible prov... | [['we', 'obtain', 'isospectral', 'eulerbernoulli', 'beams', 'by', 'using', 'factorization', 'and', 'lie', 'symmetry', 'techniques', 'the', 'canonical', 'eulerbernoulli', 'beam', 'operator', 'is', 'factorized', 'as', 'the', 'product', 'of', 'a', 'secondorder', 'linear', 'differential', 'operator', 'and', 'its', 'adjoint... | [-0.1569534542368999, 0.04453590754533838, -0.11233856177894525, 0.05680848389651135, -0.152508827766255, -0.16364713676810905, -0.07310230194653836, 0.326187193930789, -0.3454702976916808, -0.20920568224088362, 0.12353391239263883, -0.2870911886698446, -0.15471901925583512, 0.1543098189560925, -0.03133307468786013, 0.... |
709.1156 | Hypervelocity Stars from the Andromeda Galaxy | Hypervelocity stars (HVSs) discovered in the Milky Way (MW) halo are thought
to be ejected from near the massive black hole (MBH) at the galactic centre. In
this paper we investigate the spatial and velocity distributions of the HVSs
which are expected to be similarly produced in the Andromeda galaxy (M31). We
consid... | astro-ph | hypervelocity stars hvss discovered in the milky way mw halo are thought to be ejected from near the massive black hole mbh at the galactic centre in this paper we investigate the spatial and velocity distributions of the hvss which are expected to be similarly produced in the andromeda galaxy m31 we consider three dif... | [['hypervelocity', 'stars', 'hvss', 'discovered', 'in', 'the', 'milky', 'way', 'mw', 'halo', 'are', 'thought', 'to', 'be', 'ejected', 'from', 'near', 'the', 'massive', 'black', 'hole', 'mbh', 'at', 'the', 'galactic', 'centre', 'in', 'this', 'paper', 'we', 'investigate', 'the', 'spatial', 'and', 'velocity', 'distributio... | [-0.08494244068992976, 0.15362838677066776, -0.09837453773335708, 0.17835539068625147, -0.1372153754560522, -0.008255238928099215, 0.0703555815259319, 0.36600772555736516, -0.1746627755994769, -0.3706613295779447, -0.04585622958480739, -0.3100318652898194, 0.007258942535501502, 0.23462968905030293, -0.03700347223907317... |
709.1157 | Impact of slepton generation mixing on the search for sneutrinos | We perform a systematic study of sneutrino production and decays in the
Minimal Supersymmetric Standard Model (MSSM) with slepton generation mixing. We
study both fermionic decays like sneutrino \to l^- chargino^+, nu neutralino
and bosonic decays such as sneutrino \to slepton^- H^+, slepton^- W^+. We show
that the e... | hep-ph hep-ex | we perform a systematic study of sneutrino production and decays in the minimal supersymmetric standard model mssm with slepton generation mixing we study both fermionic decays like sneutrino to l chargino nu neutralino and bosonic decays such as sneutrino to slepton h slepton w we show that the effect of slepton gener... | [['we', 'perform', 'a', 'systematic', 'study', 'of', 'sneutrino', 'production', 'and', 'decays', 'in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'with', 'slepton', 'generation', 'mixing', 'we', 'study', 'both', 'fermionic', 'decays', 'like', 'sneutrino', 'to', 'l', 'chargino', 'nu', 'neutralino',... | [-0.08118497946898603, 0.30985867772283704, 0.023776029718196035, 0.22310740124478012, -0.08988588236463375, -0.19759524908537665, 0.046622647385463185, 0.3102976398852964, -0.21698653120069933, -0.25957577782643276, 0.014851229860343866, -0.3113346367429655, 0.06808260220906928, 0.15837527002092514, 0.0817995956366579... |
709.1158 | Measuring the mean and scatter of the X-ray luminosity -- optical
richness relation for maxBCG galaxy clusters | Determining the scaling relations between galaxy cluster observables requires
large samples of uniformly observed clusters. We measure the mean X-ray
luminosity--optical richness (L_X--N_200) relation for an approximately
volume-limited sample of more than 17,000 optically-selected clusters from the
maxBCG catalog sp... | astro-ph | determining the scaling relations between galaxy cluster observables requires large samples of uniformly observed clusters we measure the mean xray luminosityoptical richness l_xn_200 relation for an approximately volumelimited sample of more than 17000 opticallyselected clusters from the maxbcg catalog spanning the re... | [['determining', 'the', 'scaling', 'relations', 'between', 'galaxy', 'cluster', 'observables', 'requires', 'large', 'samples', 'of', 'uniformly', 'observed', 'clusters', 'we', 'measure', 'the', 'mean', 'xray', 'luminosityoptical', 'richness', 'l_xn_200', 'relation', 'for', 'an', 'approximately', 'volumelimited', 'sampl... | [-0.0038837364223275155, 0.11574276388001822, -0.06689568277566234, 0.1826971679195167, -0.09455933236848024, -0.019798047172960388, 0.11901467555926282, 0.5193230020533125, -0.18514617200637887, -0.4243926520582782, 0.009263582778000554, -0.4193440350726337, 0.024327545887538153, 0.22199057712214745, -0.00565601977609... |
709.1159 | Cross-correlation Weak Lensing of SDSS galaxy Clusters II: Cluster
Density Profiles and the Mass--Richness Relation | We interpret and model the statistical weak lensing measurements around
130,000 groups and clusters of galaxies in the Sloan Digital Sky Survey
presented by Sheldon et al. 2007 (Paper I). We present non-parametric
inversions of the 2D shear profiles to the mean 3D cluster density and mass
profiles in bins of both opt... | astro-ph | we interpret and model the statistical weak lensing measurements around 130000 groups and clusters of galaxies in the sloan digital sky survey presented by sheldon et al 2007 paper i we present nonparametric inversions of the 2d shear profiles to the mean 3d cluster density and mass profiles in bins of both optical ric... | [['we', 'interpret', 'and', 'model', 'the', 'statistical', 'weak', 'lensing', 'measurements', 'around', '130000', 'groups', 'and', 'clusters', 'of', 'galaxies', 'in', 'the', 'sloan', 'digital', 'sky', 'survey', 'presented', 'by', 'sheldon', 'et', 'al', '2007', 'paper', 'i', 'we', 'present', 'nonparametric', 'inversions... | [-0.04044230649014935, 0.06713584406922261, -0.07698760214218593, 0.12930539224449872, -0.10840758999606974, -0.01236120481432105, 0.038853521372032074, 0.4125697155552054, -0.18374983867397532, -0.40177260739383874, 0.04764584592474556, -0.3178858484348489, -0.031032906964861065, 0.19963541818274447, 0.004325417995763... |
709.116 | The Relativistic Factor in the Orbital Dynamics of Point Masses | There is a growing population of relativistically relevant minor bodies in
the Solar System and a growing population of massive extrasolar planets with
orbits very close to the central star where relativistic effects should have
some signature. Our purpose is to review how general relativity affects the
orbital dynam... | astro-ph | there is a growing population of relativistically relevant minor bodies in the solar system and a growing population of massive extrasolar planets with orbits very close to the central star where relativistic effects should have some signature our purpose is to review how general relativity affects the orbital dynamics... | [['there', 'is', 'a', 'growing', 'population', 'of', 'relativistically', 'relevant', 'minor', 'bodies', 'in', 'the', 'solar', 'system', 'and', 'a', 'growing', 'population', 'of', 'massive', 'extrasolar', 'planets', 'with', 'orbits', 'very', 'close', 'to', 'the', 'central', 'star', 'where', 'relativistic', 'effects', 's... | [-0.13837922087730598, 0.13712881066688787, -0.06437509877758325, 0.13027655916141317, -0.05446407577587494, -0.09070535501889845, -0.00013325446577250495, 0.3076928274514795, -0.19176641643020792, -0.3258156767838823, 0.06909997371167736, -0.2620429664734423, -0.11894022584579152, 0.25100428454331825, -0.0521355552955... |
709.1161 | Fabrication and Characterization of Two-Dimensional Photonic Crystal
Microcavities in Nanocrystalline Diamond | Diamond-based photonic devices offer exceptional opportunity to study cavity
QED at room temperature. Here we report fabrication and optical
characterization of high quality photonic crystal (PC) microcavities based on
nanocrystalline diamond. Fundamental modes near the emission wavelength of
negatively charged nitro... | cond-mat.mtrl-sci | diamondbased photonic devices offer exceptional opportunity to study cavity qed at room temperature here we report fabrication and optical characterization of high quality photonic crystal pc microcavities based on nanocrystalline diamond fundamental modes near the emission wavelength of negatively charged nitrogenvaca... | [['diamondbased', 'photonic', 'devices', 'offer', 'exceptional', 'opportunity', 'to', 'study', 'cavity', 'qed', 'at', 'room', 'temperature', 'here', 'we', 'report', 'fabrication', 'and', 'optical', 'characterization', 'of', 'high', 'quality', 'photonic', 'crystal', 'pc', 'microcavities', 'based', 'on', 'nanocrystalline... | [-0.1161250081640901, 0.15233509839163162, -0.037504854122137964, -0.053572824403090635, -0.03716243006541239, -0.168174448296971, 0.06284044176451668, 0.5561677841469646, -0.13097448027110659, -0.3369071232955321, 0.05053869607945671, -0.33152147570702556, -0.06507649546256289, 0.24391610711245448, 0.03050705256464425... |
709.1162 | Cross-correlation Weak Lensing of SDSS Galaxy Clusters III:
Mass-to-light Ratios | We present measurements of the excess mass-to-light ratio measured
aroundMaxBCG galaxy clusters observed in the SDSS. This red sequence cluster
sample includes objects from small groups with masses ranging from ~5x10^{12}
to ~10^{15} M_{sun}/h. Using cross-correlation weak lensing, we measure the
excess mass density ... | astro-ph | we present measurements of the excess masstolight ratio measured aroundmaxbcg galaxy clusters observed in the sdss this red sequence cluster sample includes objects from small groups with masses ranging from 5x1012 to 1015 m_sunh using crosscorrelation weak lensing we measure the excess mass density profile above the u... | [['we', 'present', 'measurements', 'of', 'the', 'excess', 'masstolight', 'ratio', 'measured', 'aroundmaxbcg', 'galaxy', 'clusters', 'observed', 'in', 'the', 'sdss', 'this', 'red', 'sequence', 'cluster', 'sample', 'includes', 'objects', 'from', 'small', 'groups', 'with', 'masses', 'ranging', 'from', '5x1012', 'to', '101... | [-0.05589722134636859, 0.1019705415165204, -0.10100610140278056, 0.11027561318613864, -0.035123960740479375, -0.06532050015720989, 0.040742478652374396, 0.39582103672454555, -0.19719817058262296, -0.4020577689591534, 0.04866072250146941, -0.3085840918274933, 0.006542050160254554, 0.15428433744851122, -0.027987857573456... |
709.1163 | The electronic properties of graphene | This article reviews the basic theoretical aspects of graphene, a one atom
thick allotrope of carbon, with unusual two-dimensional Dirac-like electronic
excitations. The Dirac electrons can be controlled by application of external
electric and magnetic fields, or by altering sample geometry and/or topology.
We show t... | cond-mat.other | this article reviews the basic theoretical aspects of graphene a one atom thick allotrope of carbon with unusual twodimensional diraclike electronic excitations the dirac electrons can be controlled by application of external electric and magnetic fields or by altering sample geometry andor topology we show that the di... | [['this', 'article', 'reviews', 'the', 'basic', 'theoretical', 'aspects', 'of', 'graphene', 'a', 'one', 'atom', 'thick', 'allotrope', 'of', 'carbon', 'with', 'unusual', 'twodimensional', 'diraclike', 'electronic', 'excitations', 'the', 'dirac', 'electrons', 'can', 'be', 'controlled', 'by', 'application', 'of', 'externa... | [-0.1823193058911441, 0.212671177113341, -0.03011134432745166, 0.025750042704453666, -0.060183412774611075, -0.17095241680457865, 0.06616818669515298, 0.4308615328231152, -0.3089533382486822, -0.31609828828199615, -0.037012115988097546, -0.33555102008867305, -0.19757370222478, 0.13072140647462852, 0.03056103564069971, ... |
709.1164 | The Nature of the Dense Core Population in the Pipe Nebula: Thermal
Cores Under Pressure | In this paper we present the results of a systematic investigation of an
entire population of starless dust cores within a single molecular cloud.
Analysis of extinction data shows the cores to be dense objects characterized
by a narrow range of density. Analysis of C18O and NH3 molecular-line
observations reveals ve... | astro-ph | in this paper we present the results of a systematic investigation of an entire population of starless dust cores within a single molecular cloud analysis of extinction data shows the cores to be dense objects characterized by a narrow range of density analysis of c18o and nh3 molecularline observations reveals very na... | [['in', 'this', 'paper', 'we', 'present', 'the', 'results', 'of', 'a', 'systematic', 'investigation', 'of', 'an', 'entire', 'population', 'of', 'starless', 'dust', 'cores', 'within', 'a', 'single', 'molecular', 'cloud', 'analysis', 'of', 'extinction', 'data', 'shows', 'the', 'cores', 'to', 'be', 'dense', 'objects', 'ch... | [-0.12288308535607939, 0.15876836339409944, -0.06672278156959995, 0.020849498973733362, -0.013658291078981064, -0.019532233471788157, 0.04476475361863979, 0.3785371924491806, -0.229891902616752, -0.33489078807987327, 0.08034797318598269, -0.21004816360234851, -0.014162690091729423, 0.1507030299989209, 0.034663881616628... |
709.1165 | On a class of weighted anisotropic Sobolev inequalities | In this article, motivated by a work of Caffarelli and Cordoba in phase
transitions analysis, we prove new weighted anisotropic Sobolev type
inequalities, that is Sobolev type inequalities where different derivatives
have different weight functions. The inequalities we are dealing with, are also
intimately connected ... | math.AP math.FA | in this article motivated by a work of caffarelli and cordoba in phase transitions analysis we prove new weighted anisotropic sobolev type inequalities that is sobolev type inequalities where different derivatives have different weight functions the inequalities we are dealing with are also intimately connected to weig... | [['in', 'this', 'article', 'motivated', 'by', 'a', 'work', 'of', 'caffarelli', 'and', 'cordoba', 'in', 'phase', 'transitions', 'analysis', 'we', 'prove', 'new', 'weighted', 'anisotropic', 'sobolev', 'type', 'inequalities', 'that', 'is', 'sobolev', 'type', 'inequalities', 'where', 'different', 'derivatives', 'have', 'di... | [-0.09803857912610293, 0.11660362872930215, -0.027407227984456495, 0.09591519379827598, -0.09486233553255752, -0.16046654096334778, -0.006396320986404883, 0.34403544140204917, -0.3230680142100736, -0.18410916786344178, 0.12726932226276372, -0.32266510948868454, -0.12749179560625185, 0.20285476994725454, -0.114267933905... |
709.1166 | An Optimal Linear Time Algorithm for Quasi-Monotonic Segmentation | Monotonicity is a simple yet significant qualitative characteristic. We
consider the problem of segmenting a sequence in up to K segments. We want
segments to be as monotonic as possible and to alternate signs. We propose a
quality metric for this problem using the l_inf norm, and we present an optimal
linear time al... | cs.DB | monotonicity is a simple yet significant qualitative characteristic we consider the problem of segmenting a sequence in up to k segments we want segments to be as monotonic as possible and to alternate signs we propose a quality metric for this problem using the l_inf norm and we present an optimal linear time algorith... | [['monotonicity', 'is', 'a', 'simple', 'yet', 'significant', 'qualitative', 'characteristic', 'we', 'consider', 'the', 'problem', 'of', 'segmenting', 'a', 'sequence', 'in', 'up', 'to', 'k', 'segments', 'we', 'want', 'segments', 'to', 'be', 'as', 'monotonic', 'as', 'possible', 'and', 'to', 'alternate', 'signs', 'we', 'p... | [-0.10573623343206019, 0.014978111090176672, -0.08859578128806234, 0.050653603124696, -0.10078718669895924, -0.1485881974623926, 0.07768298081324262, 0.4906287847367008, -0.267702968997172, -0.29326647052549615, 0.06819844610712994, -0.25067649522911656, -0.1903677508420418, 0.1856264192775815, -0.11212714927155623, 0.... |
709.1167 | Using RDF to Model the Structure and Process of Systems | Many systems can be described in terms of networks of discrete elements and
their various relationships to one another. A semantic network, or
multi-relational network, is a directed labeled graph consisting of a
heterogeneous set of entities connected by a heterogeneous set of
relationships. Semantic networks serve ... | cs.AI | many systems can be described in terms of networks of discrete elements and their various relationships to one another a semantic network or multirelational network is a directed labeled graph consisting of a heterogeneous set of entities connected by a heterogeneous set of relationships semantic networks serve as a pr... | [['many', 'systems', 'can', 'be', 'described', 'in', 'terms', 'of', 'networks', 'of', 'discrete', 'elements', 'and', 'their', 'various', 'relationships', 'to', 'one', 'another', 'a', 'semantic', 'network', 'or', 'multirelational', 'network', 'is', 'a', 'directed', 'labeled', 'graph', 'consisting', 'of', 'a', 'heterogen... | [-0.09568613943660018, -0.0026973340123006267, -0.019952606944087355, 0.09698571527553076, -0.1501039597151984, -0.12061492006988883, 0.029563619198029956, 0.419775193950129, -0.33270932517332064, -0.35831189532952673, 0.06527088943066754, -0.2649720720971182, -0.15791079082332465, 0.18957288981135395, -0.0857108959119... |
709.1168 | Supersymmetric Giant Graviton Solutions in AdS_3 | We parameterize all classical probe brane configurations that preserve 4
supersymmetries in (a) the extremal D1-D5 geometry, (b) the extremal D1-D5-P
geometry, (c) the smooth D1-D5 solutions proposed by Lunin and Mathur and (d)
global $AdS_3 \times S_3 \times T^4/K3$. These configurations consist of D1
branes, D5 bra... | hep-th | we parameterize all classical probe brane configurations that preserve 4 supersymmetries in a the extremal d1d5 geometry b the extremal d1d5p geometry c the smooth d1d5 solutions proposed by lunin and mathur and d global ads_3 times s_3 times t4k3 these configurations consist of d1 branes d5 branes and bound states of ... | [['we', 'parameterize', 'all', 'classical', 'probe', 'brane', 'configurations', 'that', 'preserve', '4', 'supersymmetries', 'in', 'a', 'the', 'extremal', 'd1d5', 'geometry', 'b', 'the', 'extremal', 'd1d5p', 'geometry', 'c', 'the', 'smooth', 'd1d5', 'solutions', 'proposed', 'by', 'lunin', 'and', 'mathur', 'and', 'd', 'g... | [-0.16100066374573443, 0.14487995380129884, -0.04990994257128073, 0.1027523498031466, -0.05708529379270557, -0.2043018219837298, -0.014684356874527616, 0.2805080348250663, -0.1472142324394857, -0.22189113119513623, 0.13171349270511806, -0.31164877619594333, -0.13670387411515952, 0.083040924604413, -0.08064923253469816,... |
709.1169 | The K+K+ Scattering Length from Lattice QCD | The K+K+ scattering length is calculated in fully-dynamical lattice QCD with
domain-wall valence quarks on the MILC asqtad-improved gauge configurations
with rooted staggered sea quarks. Three-flavor mixed-action chiral perturbation
theory at next-to-leading order, which includes the leading effects of the
finite lat... | hep-lat hep-ph nucl-th | the kk scattering length is calculated in fullydynamical lattice qcd with domainwall valence quarks on the milc asqtadimproved gauge configurations with rooted staggered sea quarks threeflavor mixedaction chiral perturbation theory at nexttoleading order which includes the leading effects of the finite lattice spacing ... | [['the', 'kk', 'scattering', 'length', 'is', 'calculated', 'in', 'fullydynamical', 'lattice', 'qcd', 'with', 'domainwall', 'valence', 'quarks', 'on', 'the', 'milc', 'asqtadimproved', 'gauge', 'configurations', 'with', 'rooted', 'staggered', 'sea', 'quarks', 'threeflavor', 'mixedaction', 'chiral', 'perturbation', 'theor... | [-0.10239002480482062, 0.32579148542756836, -0.11034241763874889, 0.08035923655765752, -0.024008241873234512, -0.03711888328194618, 0.09698793451456975, 0.3845627062767744, -0.1356541972917815, -0.21449865569670995, 0.021939013795927168, -0.3488017300268014, 0.002579729904731115, 0.03570225455177327, 0.0626534555604060... |
709.117 | Inflation from Wrapped Branes | We show that the use of higher dimensional wrapped branes can significantly
extend the inflaton field range compared to brane inflation models which use
D3-branes. We construct a simple inflationary model in terms of 5-branes
wrapping a 2-cycle and traveling towards the tip of the Klebanov-Strassler
throat. Inflation... | hep-th astro-ph | we show that the use of higher dimensional wrapped branes can significantly extend the inflaton field range compared to brane inflation models which use d3branes we construct a simple inflationary model in terms of 5branes wrapping a 2cycle and traveling towards the tip of the klebanovstrassler throat inflation ends wh... | [['we', 'show', 'that', 'the', 'use', 'of', 'higher', 'dimensional', 'wrapped', 'branes', 'can', 'significantly', 'extend', 'the', 'inflaton', 'field', 'range', 'compared', 'to', 'brane', 'inflation', 'models', 'which', 'use', 'd3branes', 'we', 'construct', 'a', 'simple', 'inflationary', 'model', 'in', 'terms', 'of', '... | [-0.17082211241848488, 0.13091747688181768, -0.10673895945650673, 0.1456337130474031, -0.1205117774204673, -0.17816028897171823, -0.0188579994806515, 0.2914325040721587, -0.19288110658178262, -0.24758780969602762, 0.08416591879419948, -0.2568938471463935, -0.1388358622789383, 0.1335182049067987, -0.08474338175582379, -... |
709.1171 | Counting Giant Gravitons in AdS_3 | We quantize the set of all quarter BPS brane probe solutions in global AdS_3
\times S^3 \times T^4/K3 found in arxiv:0709.1168 [hep-th]. We show that,
generically, these solutions give rise to states in discrete representations of
the SL(2,R) WZW model on AdS_3. Our procedure provides us with a detailed
description o... | hep-th | we quantize the set of all quarter bps brane probe solutions in global ads_3 times s3 times t4k3 found in arxiv07091168 hepth we show that generically these solutions give rise to states in discrete representations of the sl2r wzw model on ads_3 our procedure provides us with a detailed description of the low energy 14... | [['we', 'quantize', 'the', 'set', 'of', 'all', 'quarter', 'bps', 'brane', 'probe', 'solutions', 'in', 'global', 'ads_3', 'times', 's3', 'times', 't4k3', 'found', 'in', 'arxiv07091168', 'hepth', 'we', 'show', 'that', 'generically', 'these', 'solutions', 'give', 'rise', 'to', 'states', 'in', 'discrete', 'representations'... | [-0.14021241437074936, 0.14174924239454914, -0.062443002464506264, 0.12434844218381307, -0.035976757882386, -0.14063723832870761, 0.0262619927623114, 0.3036538963345532, -0.1844021677747815, -0.3121361721719721, 0.08962255740861692, -0.31019333270406296, -0.10766235361723396, 0.14819519037051784, -0.05460585165813476, ... |
709.1172 | Galaxy Evolution and Star Formation Efficiency in the Last Half of the
Universe | We present the results of a CO(1-0) emission survey with the IRAM 30m of 30
galaxies at moderate redshift (z ~ 0.2-0.6) to explore galaxy evolution and in
particular the star formation efficiency, in the redshift range filling the gap
between local and very high-z objects. Our detection rate is about 50%. One of
the ... | astro-ph | we present the results of a co10 emission survey with the iram 30m of 30 galaxies at moderate redshift z 0206 to explore galaxy evolution and in particular the star formation efficiency in the redshift range filling the gap between local and very highz objects our detection rate is about 50 one of the bright objects wa... | [['we', 'present', 'the', 'results', 'of', 'a', 'co10', 'emission', 'survey', 'with', 'the', 'iram', '30m', 'of', '30', 'galaxies', 'at', 'moderate', 'redshift', 'z', '0206', 'to', 'explore', 'galaxy', 'evolution', 'and', 'in', 'particular', 'the', 'star', 'formation', 'efficiency', 'in', 'the', 'redshift', 'range', 'f... | [-0.0710487936750393, 0.06339897204042327, -0.01912215022920546, 0.08065219558669592, -0.05100454482969574, -0.07564641969193789, 0.0448212189917368, 0.4492959520694884, -0.11083446968219836, -0.40757591529664666, 0.056692903858228505, -0.3128438675522127, 0.017108359259807252, 0.13203861145302653, 0.03294165013357997,... |
709.1173 | When--and how--can a cellular automaton be rewritten as a lattice gas? | Both cellular automata (CA) and lattice-gas automata (LG) provide finite
algorithmic presentations for certain classes of infinite dynamical systems
studied by symbolic dynamics; it is customary to use the term `cellular
automaton' or `lattice gas' for the dynamic system itself as well as for its
presentation. The tw... | nlin.CG | both cellular automata ca and latticegas automata lg provide finite algorithmic presentations for certain classes of infinite dynamical systems studied by symbolic dynamics it is customary to use the term cellular automaton or lattice gas for the dynamic system itself as well as for its presentation the two kinds of pr... | [['both', 'cellular', 'automata', 'ca', 'and', 'latticegas', 'automata', 'lg', 'provide', 'finite', 'algorithmic', 'presentations', 'for', 'certain', 'classes', 'of', 'infinite', 'dynamical', 'systems', 'studied', 'by', 'symbolic', 'dynamics', 'it', 'is', 'customary', 'to', 'use', 'the', 'term', 'cellular', 'automaton'... | [-0.08536524304737603, 0.12278372540758752, -0.033086917777450715, 0.09525184801884223, -0.054765105186676495, -0.17693077648695255, 0.05881813059285359, 0.3626593940967352, -0.2677776889611815, -0.27933613328377205, 0.12022389435560955, -0.2466679995461386, -0.16789954306405722, 0.22356918545401827, -0.071055334413421... |
709.1174 | Electrochemically Top Gated Graphene: Monitoring Dopants by Raman
Scattering | We demonstrate electrochemical top gating of graphene by using a solid
polymer electrolyte. This allows to reach much higher electron and hole doping
than standard back gating. In-situ Raman measurements monitor the doping. The G
peak stiffens and sharpens for both electron and hole doping, while the 2D peak
shows a ... | cond-mat.mtrl-sci | we demonstrate electrochemical top gating of graphene by using a solid polymer electrolyte this allows to reach much higher electron and hole doping than standard back gating insitu raman measurements monitor the doping the g peak stiffens and sharpens for both electron and hole doping while the 2d peak shows a differe... | [['we', 'demonstrate', 'electrochemical', 'top', 'gating', 'of', 'graphene', 'by', 'using', 'a', 'solid', 'polymer', 'electrolyte', 'this', 'allows', 'to', 'reach', 'much', 'higher', 'electron', 'and', 'hole', 'doping', 'than', 'standard', 'back', 'gating', 'insitu', 'raman', 'measurements', 'monitor', 'the', 'doping',... | [-0.10526673473219761, 0.15128353903781416, -0.025739235583716623, 0.04324670849958303, -0.03860950705917977, -0.21543143229837727, 0.14110884469875143, 0.3955015229486574, -0.23526908744009226, -0.3048271498107535, -0.016875139558614475, -0.36018351436325435, -0.053206932314810905, 0.21022717557906165, -0.006196894110... |
709.1175 | Multiple fluxoid transitions in mesoscopic superconducting rings | The authors report magnetic measurements of fluxoid transitions in
mesoscopic, superconducting aluminum rings. The transitions are induced by
applying a flux to the ring so that the induced supercurrent approaches the
critical current. In a temperature range near $T_c$, only a single fluxoid
enters or leaves at a tim... | cond-mat.supr-con | the authors report magnetic measurements of fluxoid transitions in mesoscopic superconducting aluminum rings the transitions are induced by applying a flux to the ring so that the induced supercurrent approaches the critical current in a temperature range near t_c only a single fluxoid enters or leaves at a time leadin... | [['the', 'authors', 'report', 'magnetic', 'measurements', 'of', 'fluxoid', 'transitions', 'in', 'mesoscopic', 'superconducting', 'aluminum', 'rings', 'the', 'transitions', 'are', 'induced', 'by', 'applying', 'a', 'flux', 'to', 'the', 'ring', 'so', 'that', 'the', 'induced', 'supercurrent', 'approaches', 'the', 'critical... | [-0.1387453753649418, 0.23331178325436097, -0.08441442038810296, 0.05037222034465388, -0.027220027534652958, -0.15102250836521602, 0.10587255345412912, 0.3187484066186325, -0.2538070674757842, -0.2989310728479847, 0.08503922652754692, -0.30117688671411047, -0.04704904351919461, 0.18219991762144155, 0.04874541232590195,... |
709.1176 | On equitable zero sums | It is well-known that any sequence of at least N integers contains a
subsequence whose sum is 0 (mod N). However, there can be very few subsequences
with this property (e.g. if the initial sequence is just N 1's, then there is
only one subsequence). When the length L of the sequence is much longer, we
might expect th... | math.CO math.NT | it is wellknown that any sequence of at least n integers contains a subsequence whose sum is 0 mod n however there can be very few subsequences with this property eg if the initial sequence is just n 1s then there is only one subsequence when the length l of the sequence is much longer we might expect that there are 2l... | [['it', 'is', 'wellknown', 'that', 'any', 'sequence', 'of', 'at', 'least', 'n', 'integers', 'contains', 'a', 'subsequence', 'whose', 'sum', 'is', '0', 'mod', 'n', 'however', 'there', 'can', 'be', 'very', 'few', 'subsequences', 'with', 'this', 'property', 'eg', 'if', 'the', 'initial', 'sequence', 'is', 'just', 'n', '1s'... | [-0.20497997378874006, 0.21713925868045242, -0.08115357406451508, 0.04141008622316418, -0.027518135105668935, -0.22986207152434596, 0.016997554029909556, 0.40766686855138023, -0.33528760106613237, -0.24097679225219923, 0.10191420295847241, -0.3779799908568913, -0.08842432680433955, 0.11686781153195736, -0.0547119793834... |
709.1177 | Magnetowave Induced Plasma Wakefield Acceleration for Ultra High Energy
Cosmic Rays | Magnetowave induced plasma wakefield acceleration (MPWA) in a relativistic
astrophysical outflow has been proposed as a viable mechanism for the
acceleration of cosmic particles to ultra high energies. Here we present
simulation results that clearly demonstrate the viability of this mechanism for
the first time. We i... | astro-ph | magnetowave induced plasma wakefield acceleration mpwa in a relativistic astrophysical outflow has been proposed as a viable mechanism for the acceleration of cosmic particles to ultra high energies here we present simulation results that clearly demonstrate the viability of this mechanism for the first time we invoke ... | [['magnetowave', 'induced', 'plasma', 'wakefield', 'acceleration', 'mpwa', 'in', 'a', 'relativistic', 'astrophysical', 'outflow', 'has', 'been', 'proposed', 'as', 'a', 'viable', 'mechanism', 'for', 'the', 'acceleration', 'of', 'cosmic', 'particles', 'to', 'ultra', 'high', 'energies', 'here', 'we', 'present', 'simulatio... | [-0.11099137018761064, 0.2619182087011381, -0.06695557633836746, 0.1346548504084667, -0.06180822650870133, -0.07717778376586194, 0.0027690445108769033, 0.4498755716933654, -0.22387046113204306, -0.30345516921315563, -0.028386368024218667, -0.20726306601347896, 0.013241744011194788, 0.26310228854497403, 0.01208308671051... |
709.1178 | The Trigonometric Parallax of the Brown Dwarf Planetary System 2MASSW
J1207334-393254 | We have measured a trigonometric parallax to the young brown dwarf 2MASSW
J1207334-393254. The distance [54.0 (+3.2,-2.8) pc] and space motion confirm
membership in the TW Hydrae Association. The primary is a ~25 M_jup brown
dwarf. We discuss the "planetary mass" secondary, which is certainly below the
deuterium-burn... | astro-ph | we have measured a trigonometric parallax to the young brown dwarf 2massw j1207334393254 the distance 540 3228 pc and space motion confirm membership in the tw hydrae association the primary is a 25 m_jup brown dwarf we discuss the planetary mass secondary which is certainly below the deuteriumburning limit but whose c... | [['we', 'have', 'measured', 'a', 'trigonometric', 'parallax', 'to', 'the', 'young', 'brown', 'dwarf', '2massw', 'j1207334393254', 'the', 'distance', '540', '3228', 'pc', 'and', 'space', 'motion', 'confirm', 'membership', 'in', 'the', 'tw', 'hydrae', 'association', 'the', 'primary', 'is', 'a', '25', 'm_jup', 'brown', 'd... | [-0.09157821246481035, 0.11277083796449006, -0.09750559748499654, 0.09291141596986563, -0.18638323699997272, -0.08762147548441135, 0.15001942721755768, 0.3824947171669919, -0.17045457003405318, -0.4057698154647369, 0.05131648848691839, -0.25208952233515447, -0.01292520044671619, 0.16997440634258965, -0.202205345260154,... |
709.1179 | Inelastic X-ray Scattering Study of Phonons in Superconducting CaC6 | We investigate the dispersion and temperature dependence of a number of
phonons in the recently discovered superconductor CaC6 utilizing inelastic
x-ray scattering. Four [00L] and two ab-plane phonon modes are observed, and
measured at temperatures both above and below T_c. In general, our measurements
of phonon disp... | cond-mat.supr-con | we investigate the dispersion and temperature dependence of a number of phonons in the recently discovered superconductor cac6 utilizing inelastic xray scattering four 00l and two abplane phonon modes are observed and measured at temperatures both above and below t_c in general our measurements of phonon dispersions ar... | [['we', 'investigate', 'the', 'dispersion', 'and', 'temperature', 'dependence', 'of', 'a', 'number', 'of', 'phonons', 'in', 'the', 'recently', 'discovered', 'superconductor', 'cac6', 'utilizing', 'inelastic', 'xray', 'scattering', 'four', '00l', 'and', 'two', 'abplane', 'phonon', 'modes', 'are', 'observed', 'and', 'mea... | [-0.1431515546259927, 0.20061152952714076, -0.07577908861304761, 0.04151205356374346, -0.04232054773498984, -0.08217148000246607, 0.1051576757397247, 0.42113304762717557, -0.22311199970963394, -0.30726265503714484, -0.029344295743880245, -0.4076836099437274, -0.08366168855333372, 0.2334451702350349, 0.05817266151893372... |
709.118 | Variable stars in the Open Cluster M11 (NGC 6705) | V-band time-series CCD photometric observations of the intermediate-age open
cluster M11 were performed to search for variable stars. Using these
time-series data, we carefully examined light variations of all stars in the
observing field. A total of 82 variable stars were discovered, of which 39
stars had been detec... | astro-ph | vband timeseries ccd photometric observations of the intermediateage open cluster m11 were performed to search for variable stars using these timeseries data we carefully examined light variations of all stars in the observing field a total of 82 variable stars were discovered of which 39 stars had been detected recent... | [['vband', 'timeseries', 'ccd', 'photometric', 'observations', 'of', 'the', 'intermediateage', 'open', 'cluster', 'm11', 'were', 'performed', 'to', 'search', 'for', 'variable', 'stars', 'using', 'these', 'timeseries', 'data', 'we', 'carefully', 'examined', 'light', 'variations', 'of', 'all', 'stars', 'in', 'the', 'obse... | [-0.08976841273377775, 0.140184597886243, -0.09580357998886423, 0.07633225308932565, -0.19570281118393648, -0.10512408555400357, 0.20627419266069458, 0.42066073784804464, -0.12124966191618729, -0.40705004221180807, 0.04257824003926126, -0.344914421772685, -0.05481138044313018, 0.25519033458958557, -0.1413744336320166, ... |
709.1181 | Isotopy for extended affine Lie algebras and Lie tori | Centreless Lie tori have been used by E. Neher to construct all extended
affine Lie algebras (EALAs). In this article, we study notions of isotopes and
isotopy for centreless Lie tori, and we use these notions, along with Neher's
construction, to show that there is a 1-1 correspondence between centreless Lie
tori up ... | math.RA math.OA | centreless lie tori have been used by e neher to construct all extended affine lie algebras ealas in this article we study notions of isotopes and isotopy for centreless lie tori and we use these notions along with nehers construction to show that there is a 11 correspondence between centreless lie tori up to isotopy a... | [['centreless', 'lie', 'tori', 'have', 'been', 'used', 'by', 'e', 'neher', 'to', 'construct', 'all', 'extended', 'affine', 'lie', 'algebras', 'ealas', 'in', 'this', 'article', 'we', 'study', 'notions', 'of', 'isotopes', 'and', 'isotopy', 'for', 'centreless', 'lie', 'tori', 'and', 'we', 'use', 'these', 'notions', 'along... | [-0.16469808586782986, 0.08672707305578965, -0.05007646207457348, 0.08096669208739073, -0.1179803442660599, -0.14041593566897415, -0.027314417532855465, 0.4383728304697621, -0.30814171845634136, -0.2563871683132264, 0.0950444333232759, -0.23119319010105344, -0.14905847442156125, 0.20465723191267782, -0.1729131146123813... |
709.1182 | Near-Infrared Variability in the 2MASS Calibration Fields: A Search for
Planetary Transit Candidates | The 2MASS photometric calibration observations cover ~6 square degrees on the
sky in 35 "calibration fields" each sampled in nominal photometric conditions
between 562 and 3692 times during the four years of the 2MASS mission. We
compile a catalog of variables from the calibration observations to search for
M dwarfs ... | astro-ph | the 2mass photometric calibration observations cover 6 square degrees on the sky in 35 calibration fields each sampled in nominal photometric conditions between 562 and 3692 times during the four years of the 2mass mission we compile a catalog of variables from the calibration observations to search for m dwarfs transi... | [['the', '2mass', 'photometric', 'calibration', 'observations', 'cover', '6', 'square', 'degrees', 'on', 'the', 'sky', 'in', '35', 'calibration', 'fields', 'each', 'sampled', 'in', 'nominal', 'photometric', 'conditions', 'between', '562', 'and', '3692', 'times', 'during', 'the', 'four', 'years', 'of', 'the', '2mass', '... | [-0.10231356675663561, 0.12264741247738986, -0.05487384329613883, 0.05134380676363613, -0.1209989313433385, -0.06523522582160783, 0.15235149949177296, 0.3936951572952025, -0.12838691538519353, -0.4443707268539013, 0.11668872006132505, -0.37382334145699064, -0.05077812594747372, 0.23670997736546412, -0.09272188644892737... |
709.1183 | The Scientific Manuscripts left Unpublished by Ettore Majorana (with
outlines of his life and work) | We present a panoramic view of the main scientific manuscripts left
unpublished by the brightest Italian theoretical physicist of the XX century,
Ettore Majorana. We deal in particular: (i) with his very original "study"
notes (the so-called "Volumetti"), already published by us in English, in 2003,
c/o Kluwer Acad.P... | physics.hist-ph physics.gen-ph | we present a panoramic view of the main scientific manuscripts left unpublished by the brightest italian theoretical physicist of the xx century ettore majorana we deal in particular i with his very original study notes the socalled volumetti already published by us in english in 2003 co kluwer acadpress dordrecht bost... | [['we', 'present', 'a', 'panoramic', 'view', 'of', 'the', 'main', 'scientific', 'manuscripts', 'left', 'unpublished', 'by', 'the', 'brightest', 'italian', 'theoretical', 'physicist', 'of', 'the', 'xx', 'century', 'ettore', 'majorana', 'we', 'deal', 'in', 'particular', 'i', 'with', 'his', 'very', 'original', 'study', 'n... | [-0.042474589739407445, 0.07778875038463952, -0.05977967939976178, 0.07773759808830469, -0.1700891264219904, -0.1320895833535049, 0.07497234211253191, 0.28089571464806795, -0.16493725732832415, -0.33871233011183294, 0.1103212979888909, -0.3477242935796657, -0.12396283450247601, 0.16769278853913605, -0.18395733593998453... |
709.1184 | A refinement of Sharkovskii's theorem on orbit types characterized by
two parameters | The so-called type problem or forcing problem is considered as a way to
generalize Sharkovskii's theorem. In this paper, by focusing on certain types
of orbits, we obtain a solution of the type problem, which gives a refinement
of Sharkovskii's theorem on orbit types characterized by two parameters.
| math.DS | the socalled type problem or forcing problem is considered as a way to generalize sharkovskiis theorem in this paper by focusing on certain types of orbits we obtain a solution of the type problem which gives a refinement of sharkovskiis theorem on orbit types characterized by two parameters | [['the', 'socalled', 'type', 'problem', 'or', 'forcing', 'problem', 'is', 'considered', 'as', 'a', 'way', 'to', 'generalize', 'sharkovskiis', 'theorem', 'in', 'this', 'paper', 'by', 'focusing', 'on', 'certain', 'types', 'of', 'orbits', 'we', 'obtain', 'a', 'solution', 'of', 'the', 'type', 'problem', 'which', 'gives', '... | [-0.16980803909245878, 0.040436934175280236, -0.08505040434344362, 0.06207853101659566, -0.08237582045452048, -0.12674886125023477, 0.07951923890262454, 0.25425495331486064, -0.29296867925828946, -0.3025159309230124, 0.1445865982605028, -0.1824577373530095, -0.16341036820570784, 0.2516254361592776, -0.14173153648152947... |
709.1185 | Orbit equivalence of one-sided subshifts and the associated C^*-algebras | A $\lambda$-graph system ${\frak L}$ is a generalization of a finite labeled
graph and presents a subshift. We will prove that the topological dynamical
systems $(X_{{\frak L}_1},\sigma_{{\frak L}_1})$ and $(X_{{\frak
L}_2},\sigma_{{\frak L}_2})$ for $\lambda$-graph systems ${\frak L}_1$ and
${\frak L}_2$ are continu... | math.OA math.DS | a lambdagraph system frak l is a generalization of a finite labeled graph and presents a subshift we will prove that the topological dynamical systems x_frak l_1sigma_frak l_1 and x_frak l_2sigma_frak l_2 for lambdagraph systems frak l_1 and frak l_2 are continuously orbit equivalent if and only if there exists an isom... | [['a', 'lambdagraph', 'system', 'frak', 'l', 'is', 'a', 'generalization', 'of', 'a', 'finite', 'labeled', 'graph', 'and', 'presents', 'a', 'subshift', 'we', 'will', 'prove', 'that', 'the', 'topological', 'dynamical', 'systems', 'x_frak', 'l_1sigma_frak', 'l_1', 'and', 'x_frak', 'l_2sigma_frak', 'l_2', 'for', 'lambdagra... | [-0.19825260930741995, 0.16332014771873896, -0.020870692739894583, 0.10957726044777655, -0.037285716414956725, -0.23825890325518892, -0.005842291173856642, 0.4585760092457472, -0.41395848029750887, -0.09147902969192019, 0.1418654656706583, -0.3605881744711581, -0.11515121232970792, 0.13207903871375878, -0.1951916603355... |
709.1186 | Entropy of the Schwarzschild-de Sitter Black Hole due to arbitrary spin
fields in different Coordinates | By using the Newman-Penrose formalism and the improved thin-layer ``brick
wall'' approach, the statistical-mechanical entropies of the Schwarzschild-de
Sitter black hole arising from quantum massless arbitrary spin fields are
studied in the Painlev\'e and Lemaitre coordinates. Although the metrics in
both the Painlev... | gr-qc hep-th | by using the newmanpenrose formalism and the improved thinlayer brick wall approach the statisticalmechanical entropies of the schwarzschildde sitter black hole arising from quantum massless arbitrary spin fields are studied in the painleve and lemaitre coordinates although the metrics in both the painleve and the lema... | [['by', 'using', 'the', 'newmanpenrose', 'formalism', 'and', 'the', 'improved', 'thinlayer', 'brick', 'wall', 'approach', 'the', 'statisticalmechanical', 'entropies', 'of', 'the', 'schwarzschildde', 'sitter', 'black', 'hole', 'arising', 'from', 'quantum', 'massless', 'arbitrary', 'spin', 'fields', 'are', 'studied', 'in... | [-0.1374733303056424, 0.0958410216304642, -0.08633862986756735, 0.09595104467954083, -0.08173467997596207, -0.1855711985087718, -0.08503672517892198, 0.30250675933637533, -0.1762550373124071, -0.21344899572993078, 0.05080531584379454, -0.31216699212610005, -0.119483736882278, 0.14337812748552492, -0.056111897919775854,... |
709.1187 | A spin-dependent local moment approach to the Anderson impurity model | We present an extension of the local moment approach to the Anderson impurity
model with spin-dependent hybridization. By employing the two-self-energy
description, as originally proposed by Logan and co-workers, we applied the
symmetry restoration condition for the case with spin-dependent hybridization.
Self-consis... | cond-mat.str-el | we present an extension of the local moment approach to the anderson impurity model with spindependent hybridization by employing the twoselfenergy description as originally proposed by logan and coworkers we applied the symmetry restoration condition for the case with spindependent hybridization selfconsistent ground ... | [['we', 'present', 'an', 'extension', 'of', 'the', 'local', 'moment', 'approach', 'to', 'the', 'anderson', 'impurity', 'model', 'with', 'spindependent', 'hybridization', 'by', 'employing', 'the', 'twoselfenergy', 'description', 'as', 'originally', 'proposed', 'by', 'logan', 'and', 'coworkers', 'we', 'applied', 'the', '... | [-0.08142093968331471, 0.07976246128630177, -0.06301778990068826, 0.04714155930426271, -0.025304164630414426, -0.12943972933545023, 0.06677459554757452, 0.35793520040253457, -0.21996290209146493, -0.34626084180741473, -0.011849722564059856, -0.29141629949725906, -0.11803413298109482, 0.1659491453694458, 0.0319069182184... |
709.1188 | Particle Velocity Fluctuations in Steady State Sedimentation:
Stratification Controlled Correlations | The structure and dynamics of steady state sedimentation of semi-concentrated
($\phi=0.10$) monodisperse spheres are studied in liquid fluidized beds. Laser
turbidity and particle imaging methods are used to measure the particle
velocity fluctuations and the steady state concentration profiles. Using a wide
range of ... | physics.flu-dyn | the structure and dynamics of steady state sedimentation of semiconcentrated phi010 monodisperse spheres are studied in liquid fluidized beds laser turbidity and particle imaging methods are used to measure the particle velocity fluctuations and the steady state concentration profiles using a wide range of particle and... | [['the', 'structure', 'and', 'dynamics', 'of', 'steady', 'state', 'sedimentation', 'of', 'semiconcentrated', 'phi010', 'monodisperse', 'spheres', 'are', 'studied', 'in', 'liquid', 'fluidized', 'beds', 'laser', 'turbidity', 'and', 'particle', 'imaging', 'methods', 'are', 'used', 'to', 'measure', 'the', 'particle', 'velo... | [-0.10795912521641926, 0.18342292388198805, -0.10035876522179123, 0.0572098966177726, 0.04082513983040804, -0.12119146883793053, -0.02924166920803528, 0.37017907399195626, -0.25127398496769787, -0.30537039982638436, 0.023142061440548936, -0.2901064699128922, -0.08828259283445185, 0.17106291249488567, 0.0125032193020280... |
709.1189 | Effect of THz-radiation on Behavior of Male Mice | Effect of terahertz radiation (3.6 THz, 81.5 mkm,15 mV) on some behavioral
patterns of intact mice has been investigated. In home cage mice demonstrated
avoidance of laser ray and enhanced replacement activity in free behavior.
Animals irradiated during 30 minutes manifested an increased level of anxiety,
which was e... | q-bio.OT | effect of terahertz radiation 36 thz 815 mkm15 mv on some behavioral patterns of intact mice has been investigated in home cage mice demonstrated avoidance of laser ray and enhanced replacement activity in free behavior animals irradiated during 30 minutes manifested an increased level of anxiety which was evaluated in... | [['effect', 'of', 'terahertz', 'radiation', '36', 'thz', '815', 'mkm15', 'mv', 'on', 'some', 'behavioral', 'patterns', 'of', 'intact', 'mice', 'has', 'been', 'investigated', 'in', 'home', 'cage', 'mice', 'demonstrated', 'avoidance', 'of', 'laser', 'ray', 'and', 'enhanced', 'replacement', 'activity', 'in', 'free', 'beha... | [-0.08768458731504063, 0.20318413504731833, -0.021031010556587224, 0.04766268450451099, -0.0049427827559727225, -0.11077286752919524, 0.05469420023451922, 0.44155691014760634, -0.19012476918208648, -0.3671041183110516, 0.021559487209434354, -0.30843771654339036, -0.11533260702202885, 0.22428750574304643, -0.11921721674... |
709.119 | Belief-Propagation for Weighted b-Matchings on Arbitrary Graphs and its
Relation to Linear Programs with Integer Solutions | We consider the general problem of finding the minimum weight $\bm$-matching
on arbitrary graphs. We prove that, whenever the linear programming (LP)
relaxation of the problem has no fractional solutions, then the belief
propagation (BP) algorithm converges to the correct solution. We also show that
when the LP relax... | cs.IT cs.AI math.IT | we consider the general problem of finding the minimum weight bmmatching on arbitrary graphs we prove that whenever the linear programming lp relaxation of the problem has no fractional solutions then the belief propagation bp algorithm converges to the correct solution we also show that when the lp relaxation has a fr... | [['we', 'consider', 'the', 'general', 'problem', 'of', 'finding', 'the', 'minimum', 'weight', 'bmmatching', 'on', 'arbitrary', 'graphs', 'we', 'prove', 'that', 'whenever', 'the', 'linear', 'programming', 'lp', 'relaxation', 'of', 'the', 'problem', 'has', 'no', 'fractional', 'solutions', 'then', 'the', 'belief', 'propag... | [-0.12212887791048904, -0.015522300548117991, -0.11472187840568644, 0.06546693872188225, -0.10738223042808004, -0.14220036055983884, 0.0649948255256652, 0.3695503070322028, -0.3307495991686372, -0.29495468387954993, 0.15025981428619423, -0.2284652167879097, -0.19178863574092933, 0.18546358945330124, -0.0775788583942539... |
709.1191 | Thom polynomials of invariant cones, Schur functions, and positivity | We generalize the notion of Thom polynomials from singularities of maps
between two complex manifolds to invariant cones in representations, and
collections of vector bundles. We prove that the generalized Thom polynomials,
expanded in the products of Schur functions of the bundles, have nonnegative
coefficients. For... | math.AG math.SG | we generalize the notion of thom polynomials from singularities of maps between two complex manifolds to invariant cones in representations and collections of vector bundles we prove that the generalized thom polynomials expanded in the products of schur functions of the bundles have nonnegative coefficients for classi... | [['we', 'generalize', 'the', 'notion', 'of', 'thom', 'polynomials', 'from', 'singularities', 'of', 'maps', 'between', 'two', 'complex', 'manifolds', 'to', 'invariant', 'cones', 'in', 'representations', 'and', 'collections', 'of', 'vector', 'bundles', 'we', 'prove', 'that', 'the', 'generalized', 'thom', 'polynomials', '... | [-0.19193348525113416, 0.04261433120148562, -0.1050647032506036, 0.1269085374112166, -0.1046813259907495, -0.13129592793271075, -0.04895470458371886, 0.332900390371509, -0.3627657522929126, -0.13590604692012415, 0.07602490027483295, -0.24785894904842323, -0.2302351804696366, 0.18054454204166073, -0.16487159042340843, 0... |
709.1192 | K-H_2 Quasi-molecular absorption detected in the T-dwarf epsilon Indi Ba | T-type dwarfs present a broad and shallow absorption feature centred around
6950 A in the blue wing of the K doublet at 0.77 micron which resembles in
depth and shape the satellite absorption predicted by detailed collisional
broadening profiles. In our previous work, the predicted line satellite
position was however... | astro-ph | ttype dwarfs present a broad and shallow absorption feature centred around 6950 a in the blue wing of the k doublet at 077 micron which resembles in depth and shape the satellite absorption predicted by detailed collisional broadening profiles in our previous work the predicted line satellite position was however somew... | [['ttype', 'dwarfs', 'present', 'a', 'broad', 'and', 'shallow', 'absorption', 'feature', 'centred', 'around', '6950', 'a', 'in', 'the', 'blue', 'wing', 'of', 'the', 'k', 'doublet', 'at', '077', 'micron', 'which', 'resembles', 'in', 'depth', 'and', 'shape', 'the', 'satellite', 'absorption', 'predicted', 'by', 'detailed'... | [-0.051567655857652425, 0.11344552628193262, -0.06824682500890711, 0.07195414985530078, -0.05613129355690696, -0.1294275645827028, 0.07377097856930712, 0.4043650387938727, -0.1738539774753471, -0.3360558731125837, 0.009431020098061047, -0.2700144442170858, -0.07518110303030963, 0.1600620638202368, -0.0699835948205807, ... |
709.1193 | Hard exclusive processes with photons | Virtual photons have proven to be very efficient probes of the hadronic
structure, mostly through deep inelastic scattering and related processes. The
advent of high luminosity lepton beams has allowed to enlarge the studied
processes to hard exclusive reactions, such as deeply virtual Compton
scattering and the elec... | hep-ph nucl-th | virtual photons have proven to be very efficient probes of the hadronic structure mostly through deep inelastic scattering and related processes the advent of high luminosity lepton beams has allowed to enlarge the studied processes to hard exclusive reactions such as deeply virtual compton scattering and the electropr... | [['virtual', 'photons', 'have', 'proven', 'to', 'be', 'very', 'efficient', 'probes', 'of', 'the', 'hadronic', 'structure', 'mostly', 'through', 'deep', 'inelastic', 'scattering', 'and', 'related', 'processes', 'the', 'advent', 'of', 'high', 'luminosity', 'lepton', 'beams', 'has', 'allowed', 'to', 'enlarge', 'the', 'stu... | [-0.02967735813876641, 0.20741797455896935, -0.11984088958875425, 0.1533933842767273, -0.11814619603472343, -0.11249963318308194, 0.03755683249429516, 0.44102060541078664, -0.25020903610772843, -0.24601933082052763, 0.0183831274330589, -0.3112904846911197, -0.0394618165159625, 0.17637232300299016, 0.05630291337687252, ... |
709.1194 | Nonlinear diffusion from Einstein's master equation | We generalize Einstein's master equation for random walk processes by
considering that the probability for a particle at position $r$ to make a jump
of length $j$ lattice sites, $P_j(r)$ is a functional of the particle
distribution function $f(r,t)$. By multiscale expansion, we obtain a
generalized advection-diffusio... | cond-mat.stat-mech | we generalize einsteins master equation for random walk processes by considering that the probability for a particle at position r to make a jump of length j lattice sites p_jr is a functional of the particle distribution function frt by multiscale expansion we obtain a generalized advectiondiffusion equation we show t... | [['we', 'generalize', 'einsteins', 'master', 'equation', 'for', 'random', 'walk', 'processes', 'by', 'considering', 'that', 'the', 'probability', 'for', 'a', 'particle', 'at', 'position', 'r', 'to', 'make', 'a', 'jump', 'of', 'length', 'j', 'lattice', 'sites', 'p_jr', 'is', 'a', 'functional', 'of', 'the', 'particle', '... | [-0.1033863133786676, 0.119380734835823, -0.11818059088590627, 0.0695136664309897, -0.06827339288563683, -0.1631277185255805, -0.010223524575121701, 0.31096249729251635, -0.25833563250847735, -0.24981248199294967, 0.06229831312174121, -0.3137775053807463, -0.1347044700326828, 0.16451341264003602, 0.019523070046964745, ... |
709.1195 | Selective advantage for sexual reproduction with random haploid fusion | This paper develops a simplified set of models describing asexual and sexual
replication in unicel- lular diploid organisms. The models assume organisms
whose genomes consist of two chromosomes, where each chromosome is assumed to
be functional if it is equal to some master sequence $ \sigma_0 $, and
non-functional o... | q-bio.PE q-bio.CB | this paper develops a simplified set of models describing asexual and sexual replication in unicel lular diploid organisms the models assume organisms whose genomes consist of two chromosomes where each chromosome is assumed to be functional if it is equal to some master sequence sigma_0 and nonfunctional otherwise the... | [['this', 'paper', 'develops', 'a', 'simplified', 'set', 'of', 'models', 'describing', 'asexual', 'and', 'sexual', 'replication', 'in', 'unicel', 'lular', 'diploid', 'organisms', 'the', 'models', 'assume', 'organisms', 'whose', 'genomes', 'consist', 'of', 'two', 'chromosomes', 'where', 'each', 'chromosome', 'is', 'assu... | [-0.09217249628099085, 0.17255706213592334, -0.07750954597653237, 0.06207506574693654, -0.021950601964125606, -0.2087684461773971, 0.11595649657025586, 0.3846710522610472, -0.2635763417442899, -0.21056086712068559, 0.05187942162929311, -0.21207271516670598, -0.18863902368092797, 0.12169991778696317, -0.1183166747787661... |
709.1196 | Combination of inverse spectral transform method and method of
characteristics: deformed Pohlmeyer equation | We apply a version of the dressing method to a system of four dimensional
nonlinear Partial Differential Equations (PDEs), which contains both Pohlmeyer
equation (i.e. nonlinear PDE integrable by the Inverse Spectral Transform
Method) and nonlinear matrix PDE integrable by the method of characteristics as
particular ... | nlin.SI | we apply a version of the dressing method to a system of four dimensional nonlinear partial differential equations pdes which contains both pohlmeyer equation ie nonlinear pde integrable by the inverse spectral transform method and nonlinear matrix pde integrable by the method of characteristics as particular reduction... | [['we', 'apply', 'a', 'version', 'of', 'the', 'dressing', 'method', 'to', 'a', 'system', 'of', 'four', 'dimensional', 'nonlinear', 'partial', 'differential', 'equations', 'pdes', 'which', 'contains', 'both', 'pohlmeyer', 'equation', 'ie', 'nonlinear', 'pde', 'integrable', 'by', 'the', 'inverse', 'spectral', 'transform'... | [-0.07268539672860733, -0.010445615953918045, -0.06460220640740143, 0.07570894525941604, -0.14003866631537676, -0.18313915631733835, -0.10238345429444543, 0.28074744544350183, -0.33992289705201983, -0.2483200406243738, 0.17803091852245137, -0.31089767278172076, -0.24550071781357893, 0.2308381956178122, -0.0421810371850... |
709.1197 | An efficient algorithm finds noticeable trends and examples concerning
the \v{C}erny conjecture | A word w is called synchronizing (recurrent, reset, directed) word of a
deterministic finite automaton (DFA) if w sends all states of the automaton on
a unique state. Jan Cerny had found in 1964 a sequence of n-state complete DFA
with shortest synchronizing word of length (n-1)^2. He had conjectured that it
is an upp... | cs.DM | a word w is called synchronizing recurrent reset directed word of a deterministic finite automaton dfa if w sends all states of the automaton on a unique state jan cerny had found in 1964 a sequence of nstate complete dfa with shortest synchronizing word of length n12 he had conjectured that it is an upper bound for th... | [['a', 'word', 'w', 'is', 'called', 'synchronizing', 'recurrent', 'reset', 'directed', 'word', 'of', 'a', 'deterministic', 'finite', 'automaton', 'dfa', 'if', 'w', 'sends', 'all', 'states', 'of', 'the', 'automaton', 'on', 'a', 'unique', 'state', 'jan', 'cerny', 'had', 'found', 'in', '1964', 'a', 'sequence', 'of', 'nsta... | [-0.16628680977365273, 0.21483478448050825, -0.016409084604251698, 0.12406826583969104, -0.07517683883955659, -0.22477535102624707, 0.1426024828986048, 0.3667049260463479, -0.2868928945255141, -0.2758284022890811, 0.07188256509124226, -0.33041071764540014, -0.1181716698324741, 0.23351766583834624, -0.09540471056649505,... |
709.1198 | Complex Projection of Quasianti-Hermitian Quaternionic Hamiltonian
Dynamics | We characterize the subclass of quasianti-Hermitian quaternionic Hamiltonian
dynamics such that their complex projections are one-parameter semigroup
dynamics in the space of complex quasi-Hermitian density matrices. As an
example, the complex projection of a spin-1/2 system in a constant
quasianti-Hermitian quaterni... | math-ph math.MP quant-ph | we characterize the subclass of quasiantihermitian quaternionic hamiltonian dynamics such that their complex projections are oneparameter semigroup dynamics in the space of complex quasihermitian density matrices as an example the complex projection of a spin12 system in a constant quasiantihermitian quaternionic poten... | [['we', 'characterize', 'the', 'subclass', 'of', 'quasiantihermitian', 'quaternionic', 'hamiltonian', 'dynamics', 'such', 'that', 'their', 'complex', 'projections', 'are', 'oneparameter', 'semigroup', 'dynamics', 'in', 'the', 'space', 'of', 'complex', 'quasihermitian', 'density', 'matrices', 'as', 'an', 'example', 'the... | [-0.19567515950819309, 0.13509318284691704, -0.0172778339527378, 0.11526897722400133, -0.045450307725166735, -0.12505101545883174, -0.07852695747913624, 0.3715986998921091, -0.31611759636805137, -0.1605544669225558, 0.10951315173985098, -0.2778622889679603, -0.23746554892171512, 0.1682972085916183, -0.01920808088669384... |
709.1199 | Generalized Misner-Sharp quasi-local mass in Einstein-Gauss-Bonnet
gravity | We investigate properties of a quasi-local mass in a higher-dimensional
spacetime having symmetries corresponding to the isomertries of an
$(n-2)$-dimensional maximally symmetric space in Einstein-Gauss-Bonnet gravity
in the presence of a cosmological constant. We assume that the Gauss-Bonnet
coupling constant is non... | hep-th gr-qc | we investigate properties of a quasilocal mass in a higherdimensional spacetime having symmetries corresponding to the isomertries of an n2dimensional maximally symmetric space in einsteingaussbonnet gravity in the presence of a cosmological constant we assume that the gaussbonnet coupling constant is nonnegative the q... | [['we', 'investigate', 'properties', 'of', 'a', 'quasilocal', 'mass', 'in', 'a', 'higherdimensional', 'spacetime', 'having', 'symmetries', 'corresponding', 'to', 'the', 'isomertries', 'of', 'an', 'n2dimensional', 'maximally', 'symmetric', 'space', 'in', 'einsteingaussbonnet', 'gravity', 'in', 'the', 'presence', 'of', '... | [-0.17259117205054458, 0.12401696596472613, -0.06811045750819014, 0.07971752057546354, -0.07546069767260183, -0.1421026004379434, -0.023678109832767365, 0.2895536809331383, -0.19506979022258522, -0.25817770228785075, 0.06068619771755457, -0.2696883201906128, -0.0791552533370863, 0.12982648405435998, -0.0663277112376109... |
709.12 | Role of the cooling rate in the stability of the superconducting phase
of (TMTSF)_2ClO_4 | The noncentrosymmetric ClO$_4$ anions of the organic superconductor
(TMTSF)$_2$ClO$_4$ order below 24K. The size of domains where the anions are
ordered is substantially dependent on the cooling rate which is a key parameter
for the stability of the low temperature electronic ground states. We study the
effect of the... | cond-mat.supr-con cond-mat.str-el | the noncentrosymmetric clo_4 anions of the organic superconductor tmtsf_2clo_4 order below 24k the size of domains where the anions are ordered is substantially dependent on the cooling rate which is a key parameter for the stability of the low temperature electronic ground states we study the effect of the cooling rat... | [['the', 'noncentrosymmetric', 'clo_4', 'anions', 'of', 'the', 'organic', 'superconductor', 'tmtsf_2clo_4', 'order', 'below', '24k', 'the', 'size', 'of', 'domains', 'where', 'the', 'anions', 'are', 'ordered', 'is', 'substantially', 'dependent', 'on', 'the', 'cooling', 'rate', 'which', 'is', 'a', 'key', 'parameter', 'fo... | [-0.16642212616473748, 0.21904647623887286, -0.02979984374299723, 0.009410743935101587, -0.01264840812412634, -0.08970900813195233, 0.11066710101416295, 0.32739368226611987, -0.2168690638670038, -0.2848122880483667, 0.04995320377202006, -0.30569159554336994, -0.03514147252038432, 0.17226080240652664, 0.0510935228351930... |
709.1201 | On the Proof Complexity of Deep Inference | We obtain two results about the proof complexity of deep inference: 1)
deep-inference proof systems are as powerful as Frege ones, even when both are
extended with the Tseitin extension rule or with the substitution rule; 2)
there are analytic deep-inference proof systems that exhibit an exponential
speed-up over ana... | cs.CC cs.LO math.LO | we obtain two results about the proof complexity of deep inference 1 deepinference proof systems are as powerful as frege ones even when both are extended with the tseitin extension rule or with the substitution rule 2 there are analytic deepinference proof systems that exhibit an exponential speedup over analytic gent... | [['we', 'obtain', 'two', 'results', 'about', 'the', 'proof', 'complexity', 'of', 'deep', 'inference', '1', 'deepinference', 'proof', 'systems', 'are', 'as', 'powerful', 'as', 'frege', 'ones', 'even', 'when', 'both', 'are', 'extended', 'with', 'the', 'tseitin', 'extension', 'rule', 'or', 'with', 'the', 'substitution', '... | [-0.11438327614348709, 0.035779108291567434, -0.12372125861676116, 0.1599425134951608, -0.09272459682011813, -0.2424582539028243, 0.04190323273079437, 0.36265910442983895, -0.25173851246373696, -0.3054443403359568, 0.1833574613311181, -0.2620623883578861, -0.15684543685628133, 0.270535175717158, -0.034533873727349076, ... |
709.1202 | Towards Z_2-protected gauge--Higgs unification | In theories with flux compactification in eight or higher dimensions, the
extra-dimensional components of the gauge field may be regarded as the Higgs
field candidates. We suggest a way to protect these components from getting
large tree-level masses by imposing a $Z_2$-symmetry acting on compact
manifolds and backgr... | hep-ph hep-th | in theories with flux compactification in eight or higher dimensions the extradimensional components of the gauge field may be regarded as the higgs field candidates we suggest a way to protect these components from getting large treelevel masses by imposing a z_2symmetry acting on compact manifolds and background fiel... | [['in', 'theories', 'with', 'flux', 'compactification', 'in', 'eight', 'or', 'higher', 'dimensions', 'the', 'extradimensional', 'components', 'of', 'the', 'gauge', 'field', 'may', 'be', 'regarded', 'as', 'the', 'higgs', 'field', 'candidates', 'we', 'suggest', 'a', 'way', 'to', 'protect', 'these', 'components', 'from', ... | [-0.13603223436206702, 0.265928506790126, -0.05724638259633765, 0.11392601804815417, -0.08456644656510688, -0.1827532551976562, 0.012737996963074157, 0.32019116988665136, -0.19545342176999958, -0.3165614371413182, 0.07842380459492904, -0.2698849254730539, -0.07915938127457668, 0.16376256208187429, 0.001910256061580826,... |
709.1203 | Searches for New Physics by the H1 Experiment at HERA | The high energy program of the HERA $ep$ collider ended in March 2007, where
data equivalent to an integrated luminosity of $\sim$ 0.5 fb$^{-1}$ has been
collected by the H1 experiment. In this context, some of the most recent
results from H1 about searches for new phenomena are presented.
| hep-ex | the high energy program of the hera ep collider ended in march 2007 where data equivalent to an integrated luminosity of sim 05 fb1 has been collected by the h1 experiment in this context some of the most recent results from h1 about searches for new phenomena are presented | [['the', 'high', 'energy', 'program', 'of', 'the', 'hera', 'ep', 'collider', 'ended', 'in', 'march', '2007', 'where', 'data', 'equivalent', 'to', 'an', 'integrated', 'luminosity', 'of', 'sim', '05', 'fb1', 'has', 'been', 'collected', 'by', 'the', 'h1', 'experiment', 'in', 'this', 'context', 'some', 'of', 'the', 'most',... | [-0.01604521639493047, 0.08658513702643436, -0.08949210657262985, 0.099509815806618, -0.061026093787608704, -0.03669796499889344, -0.05960782581693208, 0.3692379183687118, -0.17665273691670094, -0.3918958435272228, 0.14248989991444563, -0.3935932558105916, 0.042957602981097846, 0.23625608343555002, 0.03525667763030042,... |
709.1204 | Harmonic ultrafilters | A set of natural numbers will be called \emph{harmonic} if the reciprocals of
its elements form a divergent series. An ultrafilter of the natural numbers
will he called \emph{harmonic} if all each members are harmonic sets. The
harmonic ultrafilters are shown to constitute a compact semigroup under the
Glazer additio... | math.CO | a set of natural numbers will be called emphharmonic if the reciprocals of its elements form a divergent series an ultrafilter of the natural numbers will he called emphharmonic if all each members are harmonic sets the harmonic ultrafilters are shown to constitute a compact semigroup under the glazer addition and its ... | [['a', 'set', 'of', 'natural', 'numbers', 'will', 'be', 'called', 'emphharmonic', 'if', 'the', 'reciprocals', 'of', 'its', 'elements', 'form', 'a', 'divergent', 'series', 'an', 'ultrafilter', 'of', 'the', 'natural', 'numbers', 'will', 'he', 'called', 'emphharmonic', 'if', 'all', 'each', 'members', 'are', 'harmonic', 's... | [-0.14448638550495704, 0.16589953672093968, -0.08443004047715819, 0.05405155491301572, -0.11205478432866467, -0.08734666924415664, -0.004825285731137476, 0.29514710082636253, -0.29610147084677957, -0.16952747564351597, 0.11301699228578718, -0.3322088507233889, -0.15388102043274934, 0.23109832175632383, -0.1337187789568... |
709.1205 | Normalisation Control in Deep Inference via Atomic Flows | We introduce `atomic flows': they are graphs obtained from derivations by
tracing atom occurrences and forgetting the logical structure. We study simple
manipulations of atomic flows that correspond to complex reductions on
derivations. This allows us to prove, for propositional logic, a new and very
general normalis... | math.LO cs.LO | we introduce atomic flows they are graphs obtained from derivations by tracing atom occurrences and forgetting the logical structure we study simple manipulations of atomic flows that correspond to complex reductions on derivations this allows us to prove for propositional logic a new and very general normalisation the... | [['we', 'introduce', 'atomic', 'flows', 'they', 'are', 'graphs', 'obtained', 'from', 'derivations', 'by', 'tracing', 'atom', 'occurrences', 'and', 'forgetting', 'the', 'logical', 'structure', 'we', 'study', 'simple', 'manipulations', 'of', 'atomic', 'flows', 'that', 'correspond', 'to', 'complex', 'reductions', 'on', 'd... | [-0.09512829241782217, 0.09966935417305062, -0.12109839462585026, 0.13238760088795737, -0.16405394326354708, -0.1845098416801662, 0.056928061665178484, 0.39098512100416327, -0.2686653259180246, -0.28404577988229934, 0.06767774837733727, -0.22144521770620015, -0.13439061728516413, 0.2086998035872145, -0.1036297115347077... |
709.1206 | Superconductivity and Spin gap in the zigzag chain t-J model simulating
a CuO double chain in Pr_2Ba_4Cu_7O_15-delta | Using the numerical diagonalization method, we examine the one-dimensional
t_1-t_2-J_1-J_2 model (zigzag chain t-J model) which represents an effective
model for metallic CuO double chain in the superconductor
Pr_2Ba_4Cu_7O_15-\delta. Based on the Tomonaga-Luttinger liquid theory, we
calculate the Luttinger-liquid pa... | cond-mat.supr-con cond-mat.str-el | using the numerical diagonalization method we examine the onedimensional t_1t_2j_1j_2 model zigzag chain tj model which represents an effective model for metallic cuo double chain in the superconductor pr_2ba_4cu_7o_15delta based on the tomonagaluttinger liquid theory we calculate the luttingerliquid parameter k_rho as... | [['using', 'the', 'numerical', 'diagonalization', 'method', 'we', 'examine', 'the', 'onedimensional', 't_1t_2j_1j_2', 'model', 'zigzag', 'chain', 'tj', 'model', 'which', 'represents', 'an', 'effective', 'model', 'for', 'metallic', 'cuo', 'double', 'chain', 'in', 'the', 'superconductor', 'pr_2ba_4cu_7o_15delta', 'based'... | [-0.16732184449210763, 0.18507691773948995, -0.04065375913730787, 0.04196488025499586, -0.004007777383547447, -0.14043083228526337, 0.08483304109562985, 0.34468126622604506, -0.23933188096204247, -0.273506939212102, 0.04489180848681375, -0.3066625181898361, -0.1063982564973723, 0.15803943763003606, 0.07511716192869917,... |
709.1207 | The P versus NP Brief | This paper discusses why P and NP are likely to be different. It analyses the
essence of the concepts and points out that P and NP might be diverse by sheer
definition. It also speculates that P and NP may be unequal due to natural
laws.
| cs.CC | this paper discusses why p and np are likely to be different it analyses the essence of the concepts and points out that p and np might be diverse by sheer definition it also speculates that p and np may be unequal due to natural laws | [['this', 'paper', 'discusses', 'why', 'p', 'and', 'np', 'are', 'likely', 'to', 'be', 'different', 'it', 'analyses', 'the', 'essence', 'of', 'the', 'concepts', 'and', 'points', 'out', 'that', 'p', 'and', 'np', 'might', 'be', 'diverse', 'by', 'sheer', 'definition', 'it', 'also', 'speculates', 'that', 'p', 'and', 'np', '... | [-0.07979176485020181, 0.17542815649800975, -0.1328714437296857, 0.14789487144899677, -0.11766178043478209, -0.20623044066293084, 0.07147057202857231, 0.27860075360892905, -0.3363687355557214, -0.3579155177525852, 0.05150366513787404, -0.257651434806378, -0.1891123661366494, 0.15477674673108952, -0.10789841126002696, 0... |
709.1208 | The measurement errors in the Swift-UVOT and XMM-OM | The probability of photon measurement in some photon counting
instrumentation, such as the Optical Monitor on the XMM-Newton satellite, and
the UVOT on the Swift satellite, does not follow a Poisson distribution due to
the detector characteristics, but a Binomial distribution. For a single-pixel
approximation, an exp... | astro-ph | the probability of photon measurement in some photon counting instrumentation such as the optical monitor on the xmmnewton satellite and the uvot on the swift satellite does not follow a poisson distribution due to the detector characteristics but a binomial distribution for a singlepixel approximation an expression wa... | [['the', 'probability', 'of', 'photon', 'measurement', 'in', 'some', 'photon', 'counting', 'instrumentation', 'such', 'as', 'the', 'optical', 'monitor', 'on', 'the', 'xmmnewton', 'satellite', 'and', 'the', 'uvot', 'on', 'the', 'swift', 'satellite', 'does', 'not', 'follow', 'a', 'poisson', 'distribution', 'due', 'to', '... | [-0.0799295183197186, 0.08990183319131057, -0.08956293671644319, 0.10618884658884849, -0.03162098898787365, -0.08777608200646589, 0.09764792376728816, 0.3773226857046101, -0.2146118021087077, -0.36779896095917325, 0.057852700198173665, -0.33113369962774986, -0.038271645466997246, 0.28251402814237175, -0.105783520201134... |
709.1209 | Primitive Characters and Permutation Characters of Solvable Groups | Let X be an irreducible, primitive complex character of the finite solvable
group G, and let X* denote the complex conjugate character. If the degree X(1)
is odd, then we show how to associate to X in a unique way, a conjugacy class
of subgroups U of G for which X*X = (1_U)^G, the permutation character on the
cosets ... | math.RT | let x be an irreducible primitive complex character of the finite solvable group g and let x denote the complex conjugate character if the degree x1 is odd then we show how to associate to x in a unique way a conjugacy class of subgroups u of g for which xx 1_ug the permutation character on the cosets of u we investiga... | [['let', 'x', 'be', 'an', 'irreducible', 'primitive', 'complex', 'character', 'of', 'the', 'finite', 'solvable', 'group', 'g', 'and', 'let', 'x', 'denote', 'the', 'complex', 'conjugate', 'character', 'if', 'the', 'degree', 'x1', 'is', 'odd', 'then', 'we', 'show', 'how', 'to', 'associate', 'to', 'x', 'in', 'a', 'unique'... | [-0.21302588496215735, 0.11325606338228865, -0.08917132044753319, -0.008409732870191713, -0.12455164162512822, -0.15508103143730306, 0.03998736112932615, 0.36239853963444507, -0.3985094942529745, -0.19312793226939143, 0.04340946657916154, -0.28860416987179954, -0.1034482785064397, 0.1942587200245714, -0.081253519340689... |
709.121 | Hermitian conjugate measurement | We propose a new class of probabilistic reversing operations on the state of
a system that was disturbed by a weak measurement. It can approximately recover
the original state from the disturbed state especially with an additional
information gain using the Hermitian conjugate of the measurement operator. We
illustra... | quant-ph | we propose a new class of probabilistic reversing operations on the state of a system that was disturbed by a weak measurement it can approximately recover the original state from the disturbed state especially with an additional information gain using the hermitian conjugate of the measurement operator we illustrate t... | [['we', 'propose', 'a', 'new', 'class', 'of', 'probabilistic', 'reversing', 'operations', 'on', 'the', 'state', 'of', 'a', 'system', 'that', 'was', 'disturbed', 'by', 'a', 'weak', 'measurement', 'it', 'can', 'approximately', 'recover', 'the', 'original', 'state', 'from', 'the', 'disturbed', 'state', 'especially', 'with... | [-0.12794931117761216, 0.1335765448121511, -0.059606836548037063, 0.005581262982355392, -0.024748379709104037, -0.14173789357063266, 0.08563811049502039, 0.3604147923083938, -0.28641375500176636, -0.31400328226463525, 0.11460635687310096, -0.26453933652908523, -0.12018135715542096, 0.17737181298434734, -0.0609960321536... |
709.1211 | Likelihood ratios and Bayesian inference for Poisson channels | In recent years, infinite-dimensional methods have been introduced for the
Gaussian channels estimation. The aim of this paper is to study the application
of similar methods to Poisson channels. In particular we compute the Bayesian
estimator of a Poisson channel using the likelihood ratio and the discrete
Malliavin ... | cs.IT math.IT math.ST stat.TH | in recent years infinitedimensional methods have been introduced for the gaussian channels estimation the aim of this paper is to study the application of similar methods to poisson channels in particular we compute the bayesian estimator of a poisson channel using the likelihood ratio and the discrete malliavin gradie... | [['in', 'recent', 'years', 'infinitedimensional', 'methods', 'have', 'been', 'introduced', 'for', 'the', 'gaussian', 'channels', 'estimation', 'the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'study', 'the', 'application', 'of', 'similar', 'methods', 'to', 'poisson', 'channels', 'in', 'particular', 'we', 'compute', 'th... | [-0.07435905422023106, -0.0015908776775381101, -0.12461139251495425, 0.08181819494130421, -0.06286043710310325, -0.14087242885518855, 0.04671196232247384, 0.37976952704870814, -0.28770322571987306, -0.2697340019621721, 0.147879115303665, -0.21093555383175333, -0.1993125669144651, 0.19050180644697778, -0.120482274707598... |
709.1212 | Distinctive features in the quantum sub-dynamics of bipartite systems | Distinctive features in the sub-dynamics of an interacting bipartite system
are explored. The sub-dynamic Heisenberg operators are introduced in a novel
way leading to the quasi-particle-like concept in the respective subsystems.
This formulation is illustrated using the known exact solutions of the generic
(Jaynes -... | quant-ph | distinctive features in the subdynamics of an interacting bipartite system are explored the subdynamic heisenberg operators are introduced in a novel way leading to the quasiparticlelike concept in the respective subsystems this formulation is illustrated using the known exact solutions of the generic jaynes cummings m... | [['distinctive', 'features', 'in', 'the', 'subdynamics', 'of', 'an', 'interacting', 'bipartite', 'system', 'are', 'explored', 'the', 'subdynamic', 'heisenberg', 'operators', 'are', 'introduced', 'in', 'a', 'novel', 'way', 'leading', 'to', 'the', 'quasiparticlelike', 'concept', 'in', 'the', 'respective', 'subsystems', '... | [-0.1633509215266843, 0.18705987154763923, -0.07474919162424547, 0.05982884778308549, -0.03138600863471982, -0.15337156754962744, -0.03243841521796726, 0.30217480767695676, -0.2531947856148084, -0.26722564095897333, 0.05096108203509911, -0.29469440617554243, -0.14622010339406274, 0.17023007300615842, -0.013785210203024... |
709.1213 | Locating the zeros of partial sums of exp(z) with Riemann-Hilbert
methods | In this paper we derive uniform asymptotic expansions for the partial sums of
the exponential series. We indicate how this information will be used in a
later publication to obtain full and explicitly computable asymptotic
expansions with error bounds for all zeros of the Taylor polynomials
$p_{n-1}(z) = \sum_{k=0}^{... | math.CA math.CV | in this paper we derive uniform asymptotic expansions for the partial sums of the exponential series we indicate how this information will be used in a later publication to obtain full and explicitly computable asymptotic expansions with error bounds for all zeros of the taylor polynomials p_n1z sum_k0n1 zk k our proof... | [['in', 'this', 'paper', 'we', 'derive', 'uniform', 'asymptotic', 'expansions', 'for', 'the', 'partial', 'sums', 'of', 'the', 'exponential', 'series', 'we', 'indicate', 'how', 'this', 'information', 'will', 'be', 'used', 'in', 'a', 'later', 'publication', 'to', 'obtain', 'full', 'and', 'explicitly', 'computable', 'asym... | [-0.12990530144525778, -0.0016866745714284052, -0.17459968887184055, 0.06740650103465919, -0.06560378368311656, -0.05395381619145564, 0.07299893123093446, 0.30605437134930846, -0.252095302989826, -0.21311829788097686, 0.12865577877922102, -0.26436113373060294, -0.18611948916671472, 0.22394149550108597, -0.0520344311328... |
709.1214 | Statistical mechanical theory of an oscillating isolated system. The
relaxation to equilibrium | In this contribution we show that a suitably defined nonequilibrium entropy
of an N-body isolated system is not a constant of the motion in general and its
variation is bounded, the bounds determined by the thermodynamic entropy, i.e.,
the equilibrium entropy. We define the nonequilibrium entropy as a convex
function... | cond-mat.stat-mech | in this contribution we show that a suitably defined nonequilibrium entropy of an nbody isolated system is not a constant of the motion in general and its variation is bounded the bounds determined by the thermodynamic entropy ie the equilibrium entropy we define the nonequilibrium entropy as a convex functional of the... | [['in', 'this', 'contribution', 'we', 'show', 'that', 'a', 'suitably', 'defined', 'nonequilibrium', 'entropy', 'of', 'an', 'nbody', 'isolated', 'system', 'is', 'not', 'a', 'constant', 'of', 'the', 'motion', 'in', 'general', 'and', 'its', 'variation', 'is', 'bounded', 'the', 'bounds', 'determined', 'by', 'the', 'thermod... | [-0.11950772149470922, 0.14696600717814992, -0.16532374920636833, 0.10170542700303213, 0.025162951611678735, -0.0973363125731594, 0.0439195216885794, 0.2540852600865275, -0.30280475067758117, -0.23504581420778115, 0.015076059313865256, -0.29265169298415566, -0.13028580541983595, 0.15259451211090677, -0.0335377047140865... |
709.1215 | Haar expectations of ratios of random characteristic polynomials | We compute Haar ensemble averages of ratios of random characteristic
polynomials for the classical Lie groups K = O(N), SO(N), and USp(N). To that
end, we start from the Clifford-Weyl algebera in its canonical realization on
the complex of holomorphic differential forms for a C-vector space V. From it
we construct th... | math-ph math.MP | we compute haar ensemble averages of ratios of random characteristic polynomials for the classical lie groups k on son and uspn to that end we start from the cliffordweyl algebera in its canonical realization on the complex of holomorphic differential forms for a cvector space v from it we construct the fock representa... | [['we', 'compute', 'haar', 'ensemble', 'averages', 'of', 'ratios', 'of', 'random', 'characteristic', 'polynomials', 'for', 'the', 'classical', 'lie', 'groups', 'k', 'on', 'son', 'and', 'uspn', 'to', 'that', 'end', 'we', 'start', 'from', 'the', 'cliffordweyl', 'algebera', 'in', 'its', 'canonical', 'realization', 'on', '... | [-0.16719097434262553, 0.08470986170208467, -0.08434626812781076, 0.015048016424478842, -0.09898254906769886, -0.11527413288767199, 0.01594931297153833, 0.34611239342624883, -0.30762796189652825, -0.21181929569661498, 0.09020523814368529, -0.24306186204907076, -0.15574482852409793, 0.15431629347588763, -0.0976183596104... |
709.1216 | The Persian-Toledan Astronomical Connection and the European Renaissance | This paper aims at presenting a brief overview of astronomical exchanges
between the Eastern and Western parts of the Islamic world from the 8th to 14th
century. These cultural interactions were in fact vaster involving Persian,
Indian, Greek, and Chinese traditions. I will particularly focus on some
interesting rela... | astro-ph | this paper aims at presenting a brief overview of astronomical exchanges between the eastern and western parts of the islamic world from the 8th to 14th century these cultural interactions were in fact vaster involving persian indian greek and chinese traditions i will particularly focus on some interesting relations b... | [['this', 'paper', 'aims', 'at', 'presenting', 'a', 'brief', 'overview', 'of', 'astronomical', 'exchanges', 'between', 'the', 'eastern', 'and', 'western', 'parts', 'of', 'the', 'islamic', 'world', 'from', 'the', '8th', 'to', '14th', 'century', 'these', 'cultural', 'interactions', 'were', 'in', 'fact', 'vaster', 'involv... | [-0.0755217302049327, 0.1053586414274879, -0.0942881867783562, 0.10440892859861557, -0.14321879958574715, -0.055253766164677136, -0.0036257419030731306, 0.347665751619567, -0.19721571597047788, -0.3493294829251961, 0.15797448406119347, -0.3438970802499093, -0.1438519812376103, 0.21119319362283295, -0.12343335911754964,... |
709.1217 | High-field vortices in Josephson junctions with alternating critical
current density | We study long Josephson junctions with the critical current density
alternating along the junction. New equilibrium states, which we call the field
synchronized or FS states, are shown to exist if the applied field is from
narrow intervals centered around equidistant series of resonant fields, $H_m$.
The values of $H... | cond-mat.supr-con | we study long josephson junctions with the critical current density alternating along the junction new equilibrium states which we call the field synchronized or fs states are shown to exist if the applied field is from narrow intervals centered around equidistant series of resonant fields h_m the values of h_m are muc... | [['we', 'study', 'long', 'josephson', 'junctions', 'with', 'the', 'critical', 'current', 'density', 'alternating', 'along', 'the', 'junction', 'new', 'equilibrium', 'states', 'which', 'we', 'call', 'the', 'field', 'synchronized', 'or', 'fs', 'states', 'are', 'shown', 'to', 'exist', 'if', 'the', 'applied', 'field', 'is'... | [-0.2802799563501375, 0.25380681870188304, -0.004446354204857791, 0.034873106612616944, -0.006530347613065883, -0.14656497820245998, 0.039173469266474796, 0.3787549577653408, -0.24858830147595318, -0.26781607613795333, 0.027954888110118054, -0.30852287742826673, -0.030195230169704667, 0.18731534741646438, 0.00957756683... |
709.1218 | Electroweak symmetry breaking and cold dark matter from strongly
interacting hidden sector | We consider a hidden sector with a vectorlike confining gauge theory like QCD
with $N_{h,c}$ colors and $N_{h,f}$ light quarks ${\cal Q}_h$ in the hidden
sector. Then a scale $\Lambda_H$ would be generated by dimensional
transmutation, and chiral symmetry breaking occurs in the hidden sector. This
scale $\Lambda_H$ c... | hep-ph | we consider a hidden sector with a vectorlike confining gauge theory like qcd with n_hc colors and n_hf light quarks cal q_h in the hidden sector then a scale lambda_h would be generated by dimensional transmutation and chiral symmetry breaking occurs in the hidden sector this scale lambda_h can play a role of the sm h... | [['we', 'consider', 'a', 'hidden', 'sector', 'with', 'a', 'vectorlike', 'confining', 'gauge', 'theory', 'like', 'qcd', 'with', 'n_hc', 'colors', 'and', 'n_hf', 'light', 'quarks', 'cal', 'q_h', 'in', 'the', 'hidden', 'sector', 'then', 'a', 'scale', 'lambda_h', 'would', 'be', 'generated', 'by', 'dimensional', 'transmutat... | [-0.15031772014632258, 0.3642496719499523, -0.08426904818921718, 0.17979814245185446, -0.12971700203411704, -0.1631792756148948, 0.00741597382189214, 0.29736943642459457, -0.23321706661954522, -0.30154847029491133, 0.055604133136649525, -0.2607903601074556, -0.018487152143245353, -0.025900493271622527, 0.07693023344870... |
709.1219 | Relaxation dynamics of aftershocks after large volatility shocks in the
SSEC index | The relaxation dynamics of aftershocks after large volatility shocks are
investigated based on two high-frequency data sets of the Shanghai Stock
Exchange Composite (SSEC) index. Compared with previous relevant work, we have
defined main financial shocks based on large volatilities rather than large
crashes. We find ... | q-fin.ST physics.soc-ph | the relaxation dynamics of aftershocks after large volatility shocks are investigated based on two highfrequency data sets of the shanghai stock exchange composite ssec index compared with previous relevant work we have defined main financial shocks based on large volatilities rather than large crashes we find that the... | [['the', 'relaxation', 'dynamics', 'of', 'aftershocks', 'after', 'large', 'volatility', 'shocks', 'are', 'investigated', 'based', 'on', 'two', 'highfrequency', 'data', 'sets', 'of', 'the', 'shanghai', 'stock', 'exchange', 'composite', 'ssec', 'index', 'compared', 'with', 'previous', 'relevant', 'work', 'we', 'have', 'd... | [-0.055272522625391896, 0.13622351283126552, -0.07982035519798165, 0.17051578666711145, -0.05817917509095581, -0.11303133296415857, 0.06412447038734251, 0.3541922088550485, -0.2363086693596257, -0.2911988282940634, 0.16129616427478258, -0.3603641356341541, -0.11534631351899842, 0.2774799514197461, -0.04579860956873745,... |
709.122 | Surface solitons in left-handed metamaterials | A theory of self-induced transparency of surface TM-mode propagating along a
interface separating conventional and left-handed metamaterials is developed. A
transition layer sandwiched between connected media is described using a model
of a two-dimensional gas of quantum dots. Explicit analytical expressions for a
su... | physics.optics physics.gen-ph | a theory of selfinduced transparency of surface tmmode propagating along a interface separating conventional and lefthanded metamaterials is developed a transition layer sandwiched between connected media is described using a model of a twodimensional gas of quantum dots explicit analytical expressions for a surface op... | [['a', 'theory', 'of', 'selfinduced', 'transparency', 'of', 'surface', 'tmmode', 'propagating', 'along', 'a', 'interface', 'separating', 'conventional', 'and', 'lefthanded', 'metamaterials', 'is', 'developed', 'a', 'transition', 'layer', 'sandwiched', 'between', 'connected', 'media', 'is', 'described', 'using', 'a', 'm... | [-0.176135020380196, 0.2070944540056528, -0.036041148358444665, -0.013269784642319543, -0.04586767192528236, -0.1578270076481881, 0.03538124373652881, 0.4005234895420133, -0.24289984142809523, -0.27774744782158556, 0.04522988994779321, -0.2893114987916003, -0.14045259816225106, 0.2231985886430587, 0.04956108705122389, ... |
709.1221 | Anomalous Lineshapes and Aging Effects in Two-Dimensional Correlation
Spectroscopy | Multitime correlation functions provide useful probes for the ensembles of
trajectories underlying the stochastic dynamics of complex systems. These can
be obtained by measuring their optical response to sequences of ultrashort
optical pulse. Using the continuous time random walk model for spectral
diffusion, we anal... | cond-mat.soft | multitime correlation functions provide useful probes for the ensembles of trajectories underlying the stochastic dynamics of complex systems these can be obtained by measuring their optical response to sequences of ultrashort optical pulse using the continuous time random walk model for spectral diffusion we analyze t... | [['multitime', 'correlation', 'functions', 'provide', 'useful', 'probes', 'for', 'the', 'ensembles', 'of', 'trajectories', 'underlying', 'the', 'stochastic', 'dynamics', 'of', 'complex', 'systems', 'these', 'can', 'be', 'obtained', 'by', 'measuring', 'their', 'optical', 'response', 'to', 'sequences', 'of', 'ultrashort'... | [-0.129037756173143, 0.20159384442636244, -0.1397725073574572, 0.09720106256692347, 0.009695753183142088, -0.16036456270549115, -0.010596365554345826, 0.44044316595069843, -0.3106460642106462, -0.26350095251224714, 0.0657012374728162, -0.24793383333656827, -0.13792952388008634, 0.1913441180200823, 0.052356039533520686,... |
709.1222 | Energetic Electrons and Nuclear Transmutations in Exploding Wires | Nuclear transmutations and fast neutrons have been observed to emerge from
large electrical current pulses passing through wire filaments which are
induced to explode. The nuclear reactions may be explained as inverse beta
transitions of energetic electrons absorbed either directly by single protons
in Hydrogen or by... | nucl-th | nuclear transmutations and fast neutrons have been observed to emerge from large electrical current pulses passing through wire filaments which are induced to explode the nuclear reactions may be explained as inverse beta transitions of energetic electrons absorbed either directly by single protons in hydrogen or by pr... | [['nuclear', 'transmutations', 'and', 'fast', 'neutrons', 'have', 'been', 'observed', 'to', 'emerge', 'from', 'large', 'electrical', 'current', 'pulses', 'passing', 'through', 'wire', 'filaments', 'which', 'are', 'induced', 'to', 'explode', 'the', 'nuclear', 'reactions', 'may', 'be', 'explained', 'as', 'inverse', 'beta... | [-0.06116717903157628, 0.26667070884366323, -0.057026558341526416, 0.12914890720233674, -0.031166339693777943, -0.1175123704019526, 0.03711912966244956, 0.4077814961001821, -0.25910046618634897, -0.3400730488237238, 0.015102523875280018, -0.27716649112284836, -0.01457436714851617, 0.19663737092743266, 0.024588579143717... |
709.1223 | Group-theoretic Methods for Bounding the Exponent of Matrix
Multiplication | The (asymptotic) complexity of matrix multiplication (over the complex field)
is measured by a real parameter w > 0, called the exponent of matrix
multiplication (over the complex field), which is defined to be the smallest
real number w > 0 such that for an arbitrary degree of precision > 0, two n by
n complex matri... | math.GR math.RT | the asymptotic complexity of matrix multiplication over the complex field is measured by a real parameter w 0 called the exponent of matrix multiplication over the complex field which is defined to be the smallest real number w 0 such that for an arbitrary degree of precision 0 two n by n complex matrices can be multip... | [['the', 'asymptotic', 'complexity', 'of', 'matrix', 'multiplication', 'over', 'the', 'complex', 'field', 'is', 'measured', 'by', 'a', 'real', 'parameter', 'w', '0', 'called', 'the', 'exponent', 'of', 'matrix', 'multiplication', 'over', 'the', 'complex', 'field', 'which', 'is', 'defined', 'to', 'be', 'the', 'smallest',... | [-0.10761836360912179, 0.11689774964529123, -0.06053622523042905, 0.028374053991015984, -0.026202711218502373, -0.16788304564962764, 0.06259085695547063, 0.3445311591924516, -0.2733023015486452, -0.35720422869955903, 0.1041939528931288, -0.23650080994524256, -0.14518368441202825, 0.24203742227752897, -0.057032433301490... |
709.1224 | Magnetized strange quark matter and magnetized strange quark stars | Strange quark matter could be found in the core of neutron stars or forming
strange quark stars. As is well known, these astrophysical objects are endowed
with strong magnetic fields which affect the microscopic properties of matter
and modify the macroscopic properties of the system. In this paper we study the
role ... | astro-ph nucl-th | strange quark matter could be found in the core of neutron stars or forming strange quark stars as is well known these astrophysical objects are endowed with strong magnetic fields which affect the microscopic properties of matter and modify the macroscopic properties of the system in this paper we study the role of a ... | [['strange', 'quark', 'matter', 'could', 'be', 'found', 'in', 'the', 'core', 'of', 'neutron', 'stars', 'or', 'forming', 'strange', 'quark', 'stars', 'as', 'is', 'well', 'known', 'these', 'astrophysical', 'objects', 'are', 'endowed', 'with', 'strong', 'magnetic', 'fields', 'which', 'affect', 'the', 'microscopic', 'prope... | [-0.14726824809926087, 0.27597547550400947, -0.06617890800543719, 0.10384114508319432, -0.07455151119410135, -0.05375828888441483, 0.057534299247308546, 0.3232212883601193, -0.1960210374241574, -0.35885304217260305, -0.005486123257135745, -0.2797668532019468, -0.001831571305197456, 0.1353987421749977, 0.043220821613941... |
709.1225 | Holographic phase transitions at finite chemical potential | Recently holographic techniques have been used to study the thermal
properties of N=2 super-Yang-Mills theory, with gauge group SU(Nc) and coupled
to Nf << Nc flavours of fundamental matter, at large Nc and large 't Hooft
coupling. Here we consider the phase diagram as a function of temperature and
baryon chemical po... | hep-th | recently holographic techniques have been used to study the thermal properties of n2 superyangmills theory with gauge group sunc and coupled to nf nc flavours of fundamental matter at large nc and large t hooft coupling here we consider the phase diagram as a function of temperature and baryon chemical potential mu for... | [['recently', 'holographic', 'techniques', 'have', 'been', 'used', 'to', 'study', 'the', 'thermal', 'properties', 'of', 'n2', 'superyangmills', 'theory', 'with', 'gauge', 'group', 'sunc', 'and', 'coupled', 'to', 'nf', 'nc', 'flavours', 'of', 'fundamental', 'matter', 'at', 'large', 'nc', 'and', 'large', 't', 'hooft', 'c... | [-0.12937955327669348, 0.2519191374569603, -0.0762272240744361, 0.033818142814928384, 0.013496190062027395, -0.13115781976834057, 0.08224947843792313, 0.3240348169228106, -0.15232505354898299, -0.27723037649503374, 0.03421995730054983, -0.2936846393299854, -0.09340975546520057, 0.05946396440854223, 0.045264852073503746... |
709.1226 | On the implications of a dilaton in gauge theory | Some recent work on the implications of a dilaton in 4d gauge theories are
revisited. In part I of this paper we see how an effective dilaton coupling to
gauge kinetic term provides a simple attractive mechanism to generate
confinement. In particular, we put emphasis on the derivation of confining
analytical solution... | hep-ph | some recent work on the implications of a dilaton in 4d gauge theories are revisited in part i of this paper we see how an effective dilaton coupling to gauge kinetic term provides a simple attractive mechanism to generate confinement in particular we put emphasis on the derivation of confining analytical solutions and... | [['some', 'recent', 'work', 'on', 'the', 'implications', 'of', 'a', 'dilaton', 'in', '4d', 'gauge', 'theories', 'are', 'revisited', 'in', 'part', 'i', 'of', 'this', 'paper', 'we', 'see', 'how', 'an', 'effective', 'dilaton', 'coupling', 'to', 'gauge', 'kinetic', 'term', 'provides', 'a', 'simple', 'attractive', 'mechanis... | [-0.125556693134532, 0.1674615284986843, -0.12847201677211442, 0.11180845838814911, -0.11754348340538182, -0.2025234077650146, 0.034166486575776915, 0.3358535983075364, -0.2074229716119834, -0.24694606986194223, 0.020828661805277048, -0.2555540956462882, -0.1759292202837327, 0.1125774394012518, -0.027770042990749123, 0... |
709.1227 | Efficient Algorithms for Node Disjoint Subgraph Homeomorphism
Determination | Recently, great efforts have been dedicated to researches on the management
of large scale graph based data such as WWW, social networks, biological
networks. In the study of graph based data management, node disjoint subgraph
homeomorphism relation between graphs is more suitable than (sub)graph
isomorphism in many ... | cs.DS cs.DB | recently great efforts have been dedicated to researches on the management of large scale graph based data such as www social networks biological networks in the study of graph based data management node disjoint subgraph homeomorphism relation between graphs is more suitable than subgraph isomorphism in many cases esp... | [['recently', 'great', 'efforts', 'have', 'been', 'dedicated', 'to', 'researches', 'on', 'the', 'management', 'of', 'large', 'scale', 'graph', 'based', 'data', 'such', 'as', 'www', 'social', 'networks', 'biological', 'networks', 'in', 'the', 'study', 'of', 'graph', 'based', 'data', 'management', 'node', 'disjoint', 'su... | [-0.11972453749502379, 0.042127694967134366, -0.025569550590315723, 0.09643107993692598, -0.16310811940039618, -0.1794853461033199, 0.06380337679857963, 0.47777088695917935, -0.24983094938472597, -0.35049553375403564, 0.1394285143148462, -0.29328290390891626, -0.16680597293580993, 0.18568417951396174, -0.10564012560815... |
709.1228 | Koszul duality for Operads | This is a copy of the article by the same authors published in Duke Math. J.
(1994).
| math.AG math.QA | this is a copy of the article by the same authors published in duke math j 1994 | [['this', 'is', 'a', 'copy', 'of', 'the', 'article', 'by', 'the', 'same', 'authors', 'published', 'in', 'duke', 'math', 'j', '1994']] | [-0.06314419505789, 0.010431628235999276, -0.08734714148073074, -0.08007954082944814, -0.0982440767042777, 0.001487987910342567, 0.10826731560861363, 0.2549460587256095, -0.15484921174014316, -0.3554244674742222, 0.09735011064228327, -0.3054544960751253, -0.13495275860323624, 0.08104287153657745, -0.27569815116550994, ... |
709.1229 | Outer Billiards on Kites | Outer billiards is a simple dynamical system based on a convex planar shape.
The Moser-Neumann question, first posed by B.H. Neumann around 1960, asks if
there exists a planar shape for which outer billiards has an unbounded orbit.
The first half of this monograph proves that outer billiards has an unbounded
orbit de... | math.DS | outer billiards is a simple dynamical system based on a convex planar shape the moserneumann question first posed by bh neumann around 1960 asks if there exists a planar shape for which outer billiards has an unbounded orbit the first half of this monograph proves that outer billiards has an unbounded orbit defined rel... | [['outer', 'billiards', 'is', 'a', 'simple', 'dynamical', 'system', 'based', 'on', 'a', 'convex', 'planar', 'shape', 'the', 'moserneumann', 'question', 'first', 'posed', 'by', 'bh', 'neumann', 'around', '1960', 'asks', 'if', 'there', 'exists', 'a', 'planar', 'shape', 'for', 'which', 'outer', 'billiards', 'has', 'an', '... | [-0.19127863825595906, 0.058495528978177204, -0.09297189905693562, 0.06008023617323488, -0.07737946725081138, -0.12214349822145244, 0.013338537758280491, 0.3028189763808141, -0.2815108647658329, -0.23192288527257163, 0.11703088519902065, -0.2962497253982543, -0.1530116251308535, 0.23656313302766147, -0.1448215790783408... |
709.123 | Exciton formation in graphene bilayer | Exciton instability in graphene bilayer systems is studied in the case of a
short-ranged Coulomb interaction and a finite voltage difference between the
layers. Self-consistent exciton gap equations are derived and solved
numerically and analytically under controlled approximation. We obtain that a
critical strength ... | cond-mat.str-el cond-mat.mtrl-sci | exciton instability in graphene bilayer systems is studied in the case of a shortranged coulomb interaction and a finite voltage difference between the layers selfconsistent exciton gap equations are derived and solved numerically and analytically under controlled approximation we obtain that a critical strength of the... | [['exciton', 'instability', 'in', 'graphene', 'bilayer', 'systems', 'is', 'studied', 'in', 'the', 'case', 'of', 'a', 'shortranged', 'coulomb', 'interaction', 'and', 'a', 'finite', 'voltage', 'difference', 'between', 'the', 'layers', 'selfconsistent', 'exciton', 'gap', 'equations', 'are', 'derived', 'and', 'solved', 'nu... | [-0.2286169118413778, 0.17224837839762897, -0.007113913967184825, 0.07797126127056114, 0.04039776869985747, -0.15079223852579113, 0.10387571531105531, 0.38600932025950246, -0.28062972747912146, -0.2764647169140716, -0.06500043001421409, -0.2719913783135556, -0.13738071195117824, 0.17825110581996914, 0.09767744135213634... |
709.1231 | Connexions with totally skew-symmetric torsion and nearly-Kaehler
geometry | We study almost Hermitian structures admitting a Hermitian connexion with
totally skew-symmetric torsion or equivalently, those almost Hermitian
structures with totally skew-symmetric Nijenhuis tensor. We investigate up to
what extent the Nijenhuis tensor fails to be parallel with respect to the
characteristic connex... | math.DG | we study almost hermitian structures admitting a hermitian connexion with totally skewsymmetric torsion or equivalently those almost hermitian structures with totally skewsymmetric nijenhuis tensor we investigate up to what extent the nijenhuis tensor fails to be parallel with respect to the characteristic connexion th... | [['we', 'study', 'almost', 'hermitian', 'structures', 'admitting', 'a', 'hermitian', 'connexion', 'with', 'totally', 'skewsymmetric', 'torsion', 'or', 'equivalently', 'those', 'almost', 'hermitian', 'structures', 'with', 'totally', 'skewsymmetric', 'nijenhuis', 'tensor', 'we', 'investigate', 'up', 'to', 'what', 'extent... | [-0.19757621720081184, 0.10458305650089127, -0.05493446210601244, 0.061429521241449715, -0.1710450672825058, -0.1368965960825872, -0.11059285040540867, 0.38590923547800854, -0.332499990009714, -0.19918957262661824, 0.07692693556337729, -0.24641495442623834, -0.23341373055443976, 0.10897895464595093, -0.0881214339863957... |
709.1232 | Functional determinants for general self-adjoint extensions of
Laplace-type operators resulting from the generalized cone | In this article we consider the zeta regularized determinant of Laplace-type
operators on the generalized cone. For {\it arbitrary} self-adjoint extensions
of a matrix of singular ordinary differential operators modelled on the
generalized cone, a closed expression for the determinant is given. The result
involves a ... | math-ph hep-th math.MP | in this article we consider the zeta regularized determinant of laplacetype operators on the generalized cone for it arbitrary selfadjoint extensions of a matrix of singular ordinary differential operators modelled on the generalized cone a closed expression for the determinant is given the result involves a determinan... | [['in', 'this', 'article', 'we', 'consider', 'the', 'zeta', 'regularized', 'determinant', 'of', 'laplacetype', 'operators', 'on', 'the', 'generalized', 'cone', 'for', 'it', 'arbitrary', 'selfadjoint', 'extensions', 'of', 'a', 'matrix', 'of', 'singular', 'ordinary', 'differential', 'operators', 'modelled', 'on', 'the', ... | [-0.14581802538920713, 0.04084815174736342, -0.050466449530526564, 0.11272238199084174, -0.11709983688510525, -0.13240037161337498, -0.038689302056669615, 0.28349007150301564, -0.3183746139805477, -0.16372315052789277, 0.11986028589084387, -0.2763723653848641, -0.19614764175136, 0.19818452652543783, -0.0725531313599696... |
709.1233 | Confinement and the second vortex of the SU(4) gauge group | We study the potential between static SU(4) sources using the Model of Thick
Center Vortices. Such vortices are characterized by the center elements
$z_1=\mathrm i$ and $z_2=z_1^2$. Fitting the ratios of string tensions to those
obtained in Monte-Carlo calculations of lattice QCD we get $f_2>f_1^2$, where
$f_n$ is th... | hep-ph | we study the potential between static su4 sources using the model of thick center vortices such vortices are characterized by the center elements z_1mathrm i and z_2z_12 fitting the ratios of string tensions to those obtained in montecarlo calculations of lattice qcd we get f_2f_12 where f_n is the probability that a v... | [['we', 'study', 'the', 'potential', 'between', 'static', 'su4', 'sources', 'using', 'the', 'model', 'of', 'thick', 'center', 'vortices', 'such', 'vortices', 'are', 'characterized', 'by', 'the', 'center', 'elements', 'z_1mathrm', 'i', 'and', 'z_2z_12', 'fitting', 'the', 'ratios', 'of', 'string', 'tensions', 'to', 'thos... | [-0.17797982469425502, 0.16409680113937644, -0.050091019865260066, 0.06089201714585434, -0.021076428378561895, -0.11901846364791314, 0.0535311000730214, 0.3619496892150267, -0.23040474549564252, -0.2472115943477635, 0.06756351445380777, -0.30702506661056034, -0.05629399651942034, 0.138895197951197, 0.018126944085605532... |
709.1234 | A constrained-transport magnetohydrodynamics algorithm with
near-spectral resolution | Numerical simulations including magnetic fields have become important in many
fields of astrophysics. Evolution of magnetic fields by the constrained
transport algorithm preserves magnetic divergence to machine precision, and
thus represents one preferred method for the inclusion of magnetic fields in
simulations. We... | astro-ph | numerical simulations including magnetic fields have become important in many fields of astrophysics evolution of magnetic fields by the constrained transport algorithm preserves magnetic divergence to machine precision and thus represents one preferred method for the inclusion of magnetic fields in simulations we show... | [['numerical', 'simulations', 'including', 'magnetic', 'fields', 'have', 'become', 'important', 'in', 'many', 'fields', 'of', 'astrophysics', 'evolution', 'of', 'magnetic', 'fields', 'by', 'the', 'constrained', 'transport', 'algorithm', 'preserves', 'magnetic', 'divergence', 'to', 'machine', 'precision', 'and', 'thus',... | [-0.1034295249828687, 0.12131685018620775, -0.10561078866966855, 0.07545617780061034, -0.0850147969879048, -0.13363240009914182, -0.019996470909114487, 0.43172921987701646, -0.29329070108740224, -0.3306391365964961, 0.0949651009080677, -0.20628340733208642, -0.0874328777126777, 0.27491941478288506, -0.02638558095020259... |
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