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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707.033 | An Algebra of Quantum Processes | We introduce an algebra qCCS of pure quantum processes in which no classical
data is involved, communications by moving quantum states physically are
allowed, and computations is modeled by super-operators. An operational
semantics of qCCS is presented in terms of (non-probabilistic) labeled
transition systems. Stron... | quant-ph | we introduce an algebra qccs of pure quantum processes in which no classical data is involved communications by moving quantum states physically are allowed and computations is modeled by superoperators an operational semantics of qccs is presented in terms of nonprobabilistic labeled transition systems strong bisimula... | [['we', 'introduce', 'an', 'algebra', 'qccs', 'of', 'pure', 'quantum', 'processes', 'in', 'which', 'no', 'classical', 'data', 'is', 'involved', 'communications', 'by', 'moving', 'quantum', 'states', 'physically', 'are', 'allowed', 'and', 'computations', 'is', 'modeled', 'by', 'superoperators', 'an', 'operational', 'sem... | [-0.17892915481792354, 0.10062511803787458, -0.07525070773710202, 0.10927627002678403, -0.05790200682425099, -0.16580064553006485, 0.07365812006794774, 0.3603454836212644, -0.3172181083355099, -0.284028889023608, 0.06936816658282358, -0.22775687562676555, -0.13309462190209603, 0.1861810865059563, -0.06593957982450531, ... |
707.0331 | Target mass corrections and twist-3 in the nucleon spin structure
functions | The Nachtmann moment is employed to study the contribution of twist-3
operator to the nucleon spin structure functions. Target mass corrections to
the Cornwall-Norton moments of the spin structure functions $g_{1,2}$ are
discussed. It is found that the corrections play a sizeable role to the
contribution of the twist... | hep-ph | the nachtmann moment is employed to study the contribution of twist3 operator to the nucleon spin structure functions target mass corrections to the cornwallnorton moments of the spin structure functions g_12 are discussed it is found that the corrections play a sizeable role to the contribution of the twist3 tilde d_2... | [['the', 'nachtmann', 'moment', 'is', 'employed', 'to', 'study', 'the', 'contribution', 'of', 'twist3', 'operator', 'to', 'the', 'nucleon', 'spin', 'structure', 'functions', 'target', 'mass', 'corrections', 'to', 'the', 'cornwallnorton', 'moments', 'of', 'the', 'spin', 'structure', 'functions', 'g_12', 'are', 'discusse... | [-0.10367550535334481, 0.16906805419259602, -0.09113148027272136, 0.19209406792651862, -0.06060949236551231, 0.029459970253002312, -0.03844630038171696, 0.3374428462099146, -0.25437062326818705, -0.19998575822898634, -0.03370964006279354, -0.3626168892994799, -0.0696690538488501, 0.09723807440173847, 0.1093194765314735... |
707.0332 | Melting of the vortex lattice in layered superconductors | The structure function of the vortex lattice of layered superconductor is
calculated to one-loop order. Based on a phenomenological melting criterion
concerning the Debye-Waller factor, we calculate the melting line of the vortex
lattice, and compare our results to Monte Carlo simulation and experiment. We
find that ... | cond-mat.supr-con cond-mat.stat-mech | the structure function of the vortex lattice of layered superconductor is calculated to oneloop order based on a phenomenological melting criterion concerning the debyewaller factor we calculate the melting line of the vortex lattice and compare our results to monte carlo simulation and experiment we find that our resu... | [['the', 'structure', 'function', 'of', 'the', 'vortex', 'lattice', 'of', 'layered', 'superconductor', 'is', 'calculated', 'to', 'oneloop', 'order', 'based', 'on', 'a', 'phenomenological', 'melting', 'criterion', 'concerning', 'the', 'debyewaller', 'factor', 'we', 'calculate', 'the', 'melting', 'line', 'of', 'the', 'vo... | [-0.06456831769972313, 0.0993060687636366, -0.12151844459926574, 0.07415836660060804, -0.03162071140619313, -0.06536505788723689, 0.1058717857273977, 0.4209415717277585, -0.18382022239086104, -0.2890449732360316, 0.033450202928379, -0.33282067589234654, -0.10497204555062259, 0.22184722764962694, 0.08655423968576076, 0.... |
707.0333 | The radius and mass of the subgiant star bet Hyi from interferometry and
asteroseismology | We have used the Sydney University Stellar Interferometer (SUSI) to measure
the angular diameter of beta Hydri. This star is a nearby G2 subgiant whose
mean density was recently measured with high precision using asteroseismology.
We determine the radius and effective temperature of the star to be
1.814+/-0.017 R_sun... | astro-ph | we have used the sydney university stellar interferometer susi to measure the angular diameter of beta hydri this star is a nearby g2 subgiant whose mean density was recently measured with high precision using asteroseismology we determine the radius and effective temperature of the star to be 18140017 r_sun 09 and 587... | [['we', 'have', 'used', 'the', 'sydney', 'university', 'stellar', 'interferometer', 'susi', 'to', 'measure', 'the', 'angular', 'diameter', 'of', 'beta', 'hydri', 'this', 'star', 'is', 'a', 'nearby', 'g2', 'subgiant', 'whose', 'mean', 'density', 'was', 'recently', 'measured', 'with', 'high', 'precision', 'using', 'aster... | [-0.04220501615526972, 0.1361802095555488, -0.11183491845925649, 0.047978527266981506, -0.09456119612839661, -0.08846814940242391, 0.09120476460431523, 0.3734159028124914, -0.13149130856618285, -0.4092002379985755, 0.09677586502603892, -0.2828115749646697, -0.032473094618916024, 0.23006820443429446, -0.0559173711052719... |
707.0334 | Implementation of three-qubit Grover search in cavity QED | Using resonant interaction of three Rydberg atoms with a single-mode
microwave cavity, we consider a realization of three-qubit Grover search
algorithm in the presence of weak cavity decay, based on a previous idea for
three-qubit quantum gate [Phys. Rev. A 73, 064304 (2006)]. We simulate the
searching process under ... | quant-ph | using resonant interaction of three rydberg atoms with a singlemode microwave cavity we consider a realization of threequbit grover search algorithm in the presence of weak cavity decay based on a previous idea for threequbit quantum gate phys rev a 73 064304 2006 we simulate the searching process under the influence o... | [['using', 'resonant', 'interaction', 'of', 'three', 'rydberg', 'atoms', 'with', 'a', 'singlemode', 'microwave', 'cavity', 'we', 'consider', 'a', 'realization', 'of', 'threequbit', 'grover', 'search', 'algorithm', 'in', 'the', 'presence', 'of', 'weak', 'cavity', 'decay', 'based', 'on', 'a', 'previous', 'idea', 'for', '... | [-0.13652293502407917, 0.15560499973156872, -0.025374451367294087, -0.05137482709172165, 0.014779473786406658, -0.2061860043774633, 0.12617420327630552, 0.3928623316809535, -0.18981149845948334, -0.32380689515403527, -0.0009469993795980426, -0.21753018730155685, -0.0887649155797108, 0.2551121719592415, -0.0069301627795... |
707.0335 | Label-setting methods for Multimode Stochastic Shortest Path problems on
graphs | Stochastic shortest path (SSP) problems arise in a variety of discrete
stochastic control contexts. An optimal solutions to such a problem is
typically computed using the value function, which can be found by solving the
corresponding dynamic programming equations. In the deterministic case, these
equations can be of... | math.OC math.NA | stochastic shortest path ssp problems arise in a variety of discrete stochastic control contexts an optimal solutions to such a problem is typically computed using the value function which can be found by solving the corresponding dynamic programming equations in the deterministic case these equations can be often solv... | [['stochastic', 'shortest', 'path', 'ssp', 'problems', 'arise', 'in', 'a', 'variety', 'of', 'discrete', 'stochastic', 'control', 'contexts', 'an', 'optimal', 'solutions', 'to', 'such', 'a', 'problem', 'is', 'typically', 'computed', 'using', 'the', 'value', 'function', 'which', 'can', 'be', 'found', 'by', 'solving', 'th... | [-0.09326543545350433, 0.019002240012632683, -0.0747842997610569, 0.09751597999408841, -0.11102186115272343, -0.14409639091044665, 0.014968321926891804, 0.3819176261499524, -0.35429510386288166, -0.31464329409599306, 0.1558488170495257, -0.1982485517412424, -0.20918680047616361, 0.26169396917521953, -0.0921538128964603... |
707.0336 | Pricing Options on Defaultable Stocks | In this note, we develop stock option price approximations for a model which
takes both the risk o default and the stochastic volatility into account. We
also let the intensity of defaults be influenced by the volatility. We show
that it might be possible to infer the risk neutral default intensity from the
stock opt... | cs.CE | in this note we develop stock option price approximations for a model which takes both the risk o default and the stochastic volatility into account we also let the intensity of defaults be influenced by the volatility we show that it might be possible to infer the risk neutral default intensity from the stock option p... | [['in', 'this', 'note', 'we', 'develop', 'stock', 'option', 'price', 'approximations', 'for', 'a', 'model', 'which', 'takes', 'both', 'the', 'risk', 'o', 'default', 'and', 'the', 'stochastic', 'volatility', 'into', 'account', 'we', 'also', 'let', 'the', 'intensity', 'of', 'defaults', 'be', 'influenced', 'by', 'the', 'v... | [-0.004508176218584046, 0.015336693496456966, -0.12806726810060912, 0.2335271842993779, -0.10069159426734792, -0.12632788570497083, 0.15460891959567866, 0.45584383137054274, -0.32204586085401943, -0.22340213916860185, 0.1809417840359766, -0.28630925174844496, -0.0996520861748371, 0.1893482963693001, -0.1508234525309154... |
707.0337 | Stability, Reactivity, and Aromaticity of Compounds of a Multivalent
Superatom | In this communication we analyze the stability, reactivity and possible
aromatic behavior of two recently reported clusters (Reveles J. U.; Khanna S.
N.; Roach P. J.; Castleman A. W. jr. Proc. Natl. Acad. Sci, 2006, 103, 18405),
viz., Al7C- and Al7O- in the light of the principles of the maximum hardness
and minimum ... | physics.atm-clus physics.chem-ph | in this communication we analyze the stability reactivity and possible aromatic behavior of two recently reported clusters reveles j u khanna s n roach p j castleman a w jr proc natl acad sci 2006 103 18405 viz al7c and al7o in the light of the principles of the maximum hardness and minimum electrophilicity as well as ... | [['in', 'this', 'communication', 'we', 'analyze', 'the', 'stability', 'reactivity', 'and', 'possible', 'aromatic', 'behavior', 'of', 'two', 'recently', 'reported', 'clusters', 'reveles', 'j', 'u', 'khanna', 's', 'n', 'roach', 'p', 'j', 'castleman', 'a', 'w', 'jr', 'proc', 'natl', 'acad', 'sci', '2006', '103', '18405', ... | [-0.14539758507804623, 0.09609292847393401, 0.0082544787337297, -0.03261560999290568, 0.007379198258196743, -0.133955117290968, 0.14188120671515836, 0.3005289749587597, -0.2301185599403809, -0.3691636620667474, 0.01585272767837962, -0.30729918226053743, -0.11394419325595914, 0.11305576846292563, -0.06655871792664302, 0... |
707.0338 | Integral pinched 3-manifolds are space forms | In this paper we prove that, under an explicit integral pinching assumption
between the $L^2$-norm of the Ricci curvature and the $L^2$-norm of the scalar
curvature, a closed 3-manifold with positive scalar curvature admits an
Einstein metric with positive curvature. In particular this implies that the
manifold is di... | math.DG math.AP | in this paper we prove that under an explicit integral pinching assumption between the l2norm of the ricci curvature and the l2norm of the scalar curvature a closed 3manifold with positive scalar curvature admits an einstein metric with positive curvature in particular this implies that the manifold is diffeomorphic to... | [['in', 'this', 'paper', 'we', 'prove', 'that', 'under', 'an', 'explicit', 'integral', 'pinching', 'assumption', 'between', 'the', 'l2norm', 'of', 'the', 'ricci', 'curvature', 'and', 'the', 'l2norm', 'of', 'the', 'scalar', 'curvature', 'a', 'closed', '3manifold', 'with', 'positive', 'scalar', 'curvature', 'admits', 'an... | [-0.2736316065896641, 0.05763203930162655, -0.10826311937787315, 0.0628916445675052, -0.13018963072787632, -0.14768760808828202, -0.1570350592257455, 0.33591719899665223, -0.24669554247097536, -0.1555641028352759, 0.10089076737534594, -0.28079920185052537, -0.19543864716013723, 0.12336389893157916, -0.1553063791583885,... |
707.0339 | The BSSN formulation is a partially constrained evolution system | Relativistic simulations in 3+1 dimensions typically monitor the Hamiltonian
and momentum constraints during evolution, with significant violations of these
constraints indicating the presence of instabilities. In this paper we rewrite
the momentum constraints as first-order evolution equations, and show that the
pop... | gr-qc | relativistic simulations in 31 dimensions typically monitor the hamiltonian and momentum constraints during evolution with significant violations of these constraints indicating the presence of instabilities in this paper we rewrite the momentum constraints as firstorder evolution equations and show that the popular bs... | [['relativistic', 'simulations', 'in', '31', 'dimensions', 'typically', 'monitor', 'the', 'hamiltonian', 'and', 'momentum', 'constraints', 'during', 'evolution', 'with', 'significant', 'violations', 'of', 'these', 'constraints', 'indicating', 'the', 'presence', 'of', 'instabilities', 'in', 'this', 'paper', 'we', 'rewri... | [-0.15416917685223253, 0.07212636855087783, -0.12150896763380029, 0.07184974086244199, -0.09260668512433767, -0.08493101108500636, -0.05432923028925679, 0.2533248681513789, -0.2318770042865684, -0.36455343207834584, 0.06437396613642034, -0.2371602441692774, -0.14191828133832468, 0.13748418652501546, -0.0332001121469626... |
707.034 | Asymptotic enumeration of sparse nonnegative integer matrices with
specified row and column sums | Let \svec = (s_1,...,s_m) and \tvec = (t_1,...,t_n) be vectors of nonnegative
integer-valued functions of m,n with equal sum S = sum_{i=1}^m s_i =
sum_{j=1}^n t_j. Let M(\svec,\tvec) be the number of m*n matrices with
nonnegative integer entries such that the i-th row has row sum s_i and the j-th
column has column su... | math.CO math.ST stat.TH | let svec s_1s_m and tvec t_1t_n be vectors of nonnegative integervalued functions of mn with equal sum s sum_i1m s_i sum_j1n t_j let msvectvec be the number of mn matrices with nonnegative integer entries such that the ith row has row sum s_i and the jth column has column sum t_j for all ij such matrices occur in many ... | [['let', 'svec', 's_1s_m', 'and', 'tvec', 't_1t_n', 'be', 'vectors', 'of', 'nonnegative', 'integervalued', 'functions', 'of', 'mn', 'with', 'equal', 'sum', 's', 'sum_i1m', 's_i', 'sum_j1n', 't_j', 'let', 'msvectvec', 'be', 'the', 'number', 'of', 'mn', 'matrices', 'with', 'nonnegative', 'integer', 'entries', 'such', 'th... | [-0.1560589194887821, 0.1538171601223778, 0.04148231713992098, -0.02057991665336072, -0.03121271279860311, -0.1885270103616987, 0.040421659672800564, 0.3434694147558871, -0.28901711881510705, -0.2285536769603998, 0.11883506491261112, -0.326797424616026, -0.1207374771753245, 0.08990377259458074, -0.0868154872636895, 0.0... |
707.0341 | Considering boundary conditions for black hole entropy in loop quantum
gravity | We argue for black hole entropy in loop quantum gravity (LQG) by taking into
account the interpretation that there is no other side of the horizon. This
gives new values for the Barbero-Immirzi parameter which are fairly larger than
those considered before. We also discuss its consequences.
| hep-th gr-qc | we argue for black hole entropy in loop quantum gravity lqg by taking into account the interpretation that there is no other side of the horizon this gives new values for the barberoimmirzi parameter which are fairly larger than those considered before we also discuss its consequences | [['we', 'argue', 'for', 'black', 'hole', 'entropy', 'in', 'loop', 'quantum', 'gravity', 'lqg', 'by', 'taking', 'into', 'account', 'the', 'interpretation', 'that', 'there', 'is', 'no', 'other', 'side', 'of', 'the', 'horizon', 'this', 'gives', 'new', 'values', 'for', 'the', 'barberoimmirzi', 'parameter', 'which', 'are', ... | [-0.13907596377774756, 0.1475147562933729, -0.1184137429487198, 0.14649644771471937, -0.10382938111557606, -0.19706789121784746, 0.03253688779659569, 0.3140368822248692, -0.18059112131595612, -0.26190791588197365, 0.11265020558679913, -0.26077086682570105, -0.09760791267407068, 0.25411327143615864, -0.08386899752819792... |
707.0342 | Spin-orbit-assisted electron-phonon interaction and the magnetophonon
resonance in semiconductor quantum wells | We introduce a spin-orbit assisted electron-phonon (e-ph) coupling mechanism
for carriers in semiconductor quantum wells and predict qualitatively the form
and shape of anticrossings between the cyclotron resonance (CR) and optical (LO
and TO) phonons. Since this e-ph interaction involves the electron spin it
makes t... | cond-mat.mes-hall | we introduce a spinorbit assisted electronphonon eph coupling mechanism for carriers in semiconductor quantum wells and predict qualitatively the form and shape of anticrossings between the cyclotron resonance cr and optical lo and to phonons since this eph interaction involves the electron spin it makes the predicted ... | [['we', 'introduce', 'a', 'spinorbit', 'assisted', 'electronphonon', 'eph', 'coupling', 'mechanism', 'for', 'carriers', 'in', 'semiconductor', 'quantum', 'wells', 'and', 'predict', 'qualitatively', 'the', 'form', 'and', 'shape', 'of', 'anticrossings', 'between', 'the', 'cyclotron', 'resonance', 'cr', 'and', 'optical', ... | [-0.16026343001528823, 0.19275137532933323, -0.004608419070492929, 0.09269459268126859, -0.009908309881401652, -0.20719483083308632, 0.07421697991024424, 0.40673460244242826, -0.26106861556199057, -0.2773914201212908, -0.10891435286655689, -0.3092829440928884, -0.1407317537744877, 0.2133470164584135, 0.0921158601404793... |
707.0343 | Particle interference as a test of Lorentz-violating electrodynamics | In Lorentz-violating electrodynamics a steady current (and similarly a static
charge) generates both static magnetic and electric fields. These induced
fields, acting on interfering particles, change the interference pattern. We
find that particle interference experiments are sensitive to small Lorentz
violating effe... | hep-ph quant-ph | in lorentzviolating electrodynamics a steady current and similarly a static charge generates both static magnetic and electric fields these induced fields acting on interfering particles change the interference pattern we find that particle interference experiments are sensitive to small lorentz violating effects and t... | [['in', 'lorentzviolating', 'electrodynamics', 'a', 'steady', 'current', 'and', 'similarly', 'a', 'static', 'charge', 'generates', 'both', 'static', 'magnetic', 'and', 'electric', 'fields', 'these', 'induced', 'fields', 'acting', 'on', 'interfering', 'particles', 'change', 'the', 'interference', 'pattern', 'we', 'find'... | [-0.20360951912256756, 0.29640428261232693, -0.013939291380146253, 0.12353217173534047, -0.13739597360004804, -0.14508222422695585, 0.029648834161759754, 0.34232213580980897, -0.20363056021077292, -0.3501513552452837, 0.009153415987384506, -0.2836572520235287, -0.13178875322254108, 0.18656733100942802, 0.00118880611262... |
707.0344 | Large deviations for symmetrised empirical measures | In this paper we prove a Large Deviation Principle for the sequence of
symmetrised empirical measures $\frac{1}{n} \sum_{i=1}^{n}
\delta_{(X^n_i,X^n_{\sigma_n(i)})}$ where $\sigma_n$ is a random permutation
and $((X_i^n)_{1 \leq i \leq n})_{n \geq 1}$ is a triangular array of random
variables with suitable properties... | math.PR | in this paper we prove a large deviation principle for the sequence of symmetrised empirical measures frac1n sum_i1n delta_xn_ixn_sigma_ni where sigma_n is a random permutation and x_in_1 leq i leq n_n geq 1 is a triangular array of random variables with suitable properties as an application we show how this result all... | [['in', 'this', 'paper', 'we', 'prove', 'a', 'large', 'deviation', 'principle', 'for', 'the', 'sequence', 'of', 'symmetrised', 'empirical', 'measures', 'frac1n', 'sum_i1n', 'delta_xn_ixn_sigma_ni', 'where', 'sigma_n', 'is', 'a', 'random', 'permutation', 'and', 'x_in_1', 'leq', 'i', 'leq', 'n_n', 'geq', '1', 'is', 'a', ... | [-0.11767267184736936, 0.1422336211352545, -0.06873660880491893, 0.07274493122932271, -0.002021346453820234, -0.12242102324017796, 0.051944513194451945, 0.3570494496304056, -0.3209305301416611, -0.2532757983097564, 0.11087906202537588, -0.28980950190895743, -0.1569505303328776, 0.1484453703911192, -0.11919871760883193,... |
707.0345 | Thermal rounding of the depinning transition | We study thermal effects at the depinning transition by numerical simulations
of driven one-dimensional elastic interfaces in a disordered medium. We find
that the velocity of the interface, evaluated at the critical depinning force,
can be correctly described with the power law $v\sim T^\psi$, where $\psi$ is
the th... | cond-mat.stat-mech cond-mat.dis-nn | we study thermal effects at the depinning transition by numerical simulations of driven onedimensional elastic interfaces in a disordered medium we find that the velocity of the interface evaluated at the critical depinning force can be correctly described with the power law vsim tpsi where psi is the thermal exponent ... | [['we', 'study', 'thermal', 'effects', 'at', 'the', 'depinning', 'transition', 'by', 'numerical', 'simulations', 'of', 'driven', 'onedimensional', 'elastic', 'interfaces', 'in', 'a', 'disordered', 'medium', 'we', 'find', 'that', 'the', 'velocity', 'of', 'the', 'interface', 'evaluated', 'at', 'the', 'critical', 'depinni... | [-0.14615941838997923, 0.18204075419367954, -0.08455691010031048, -0.01527937838462877, -0.026224114092898, -0.11461313333232663, 0.020303039434306985, 0.3523053787037129, -0.275918645041927, -0.263037690185482, 0.04660150288940183, -0.3187048858915061, -0.10024610824022395, 0.20999637493698659, 0.07850799438036327, 0.... |
707.0346 | The one-dimensional Schr\"{o}dinger-Newton equations | We prove an existence and uniqueness result for ground states of
one-dimensional Schr\"{o}dinger-Newton equations.
| math-ph math.MP | we prove an existence and uniqueness result for ground states of onedimensional schrodingernewton equations | [['we', 'prove', 'an', 'existence', 'and', 'uniqueness', 'result', 'for', 'ground', 'states', 'of', 'onedimensional', 'schrodingernewton', 'equations']] | [-0.20657049545219966, 0.07304363618875089, -0.07772076968103647, 0.07396944139951042, 0.010558949783444405, -0.13327967335603066, -0.035153301166636605, 0.22250014556837933, -0.2925602208290781, -0.20513979398778506, 0.09964925739248949, -0.3010204125727926, -0.08277353271842003, 0.13389943274004118, 0.008671740735215... |
707.0347 | Gauss-Bonnet Gravity with Scalar Field in Four Dimensions | We give all exact solutions of the Einstein-Gauss-Bonnet Field Equations
coupled with a scalar field in four dimensions under certain assumptions.
| gr-qc hep-th | we give all exact solutions of the einsteingaussbonnet field equations coupled with a scalar field in four dimensions under certain assumptions | [['we', 'give', 'all', 'exact', 'solutions', 'of', 'the', 'einsteingaussbonnet', 'field', 'equations', 'coupled', 'with', 'a', 'scalar', 'field', 'in', 'four', 'dimensions', 'under', 'certain', 'assumptions']] | [-0.27157131644586724, 0.10155949737167075, -0.03774251975119114, 0.03698018973781949, -0.07447216701915577, -0.2244052063629386, -0.1114307851308868, 0.24936554274920905, -0.10143960897056829, -0.27475421875715256, 0.11954360232976753, -0.23239082506015188, -0.16290798561558836, 0.12316887896685373, 0.0222544220852709... |
707.0348 | Self-Organized Characteristics of the International System | Various self-organized characteristics of the international system can be
identified with the help of a complexity science perspective. The perspective
discussed in this article is based on various complexity science concepts and
theories, and concepts related to ecology and ecosystems. It can be argued that
the Grea... | nlin.AO | various selforganized characteristics of the international system can be identified with the help of a complexity science perspective the perspective discussed in this article is based on various complexity science concepts and theories and concepts related to ecology and ecosystems it can be argued that the great powe... | [['various', 'selforganized', 'characteristics', 'of', 'the', 'international', 'system', 'can', 'be', 'identified', 'with', 'the', 'help', 'of', 'a', 'complexity', 'science', 'perspective', 'the', 'perspective', 'discussed', 'in', 'this', 'article', 'is', 'based', 'on', 'various', 'complexity', 'science', 'concepts', '... | [-0.11902513733907004, 0.13069661760237067, -0.13824855721613857, 0.044991660200906024, -0.04434906396615718, -0.08808046612289867, 0.04398801867833494, 0.3019880874448323, -0.2839195006626791, -0.3237625582675849, 0.1300382784492935, -0.26934154917752107, -0.2360422101574451, 0.1758799436884666, -0.07792762415899362, ... |
707.0349 | Metallic Graphene Nanodisks | We explore the electronic properties of finite-length graphene nanoribbons as
well as graphene nanodisks with various sizes and shapes in quest of metallic
ones. For this purpose it is sufficient to search zero-energy states. We find
that there exist no zero-energy states in finite-length zigzag nanoribbons
though al... | cond-mat.mes-hall cond-mat.mtrl-sci | we explore the electronic properties of finitelength graphene nanoribbons as well as graphene nanodisks with various sizes and shapes in quest of metallic ones for this purpose it is sufficient to search zeroenergy states we find that there exist no zeroenergy states in finitelength zigzag nanoribbons though all infini... | [['we', 'explore', 'the', 'electronic', 'properties', 'of', 'finitelength', 'graphene', 'nanoribbons', 'as', 'well', 'as', 'graphene', 'nanodisks', 'with', 'various', 'sizes', 'and', 'shapes', 'in', 'quest', 'of', 'metallic', 'ones', 'for', 'this', 'purpose', 'it', 'is', 'sufficient', 'to', 'search', 'zeroenergy', 'sta... | [-0.2525291646993078, 0.20998239817542083, -0.027041891307800735, 0.06983437999087565, 0.010457629327226532, -0.22890983695386474, 0.049570034018828785, 0.48390335607590207, -0.2268180419101354, -0.267383723220694, -0.008460638640926929, -0.3031610740229077, -0.17410790777568697, 0.12471654709351651, 0.0145855418640325... |
707.035 | A new concept and design of ferrite-based microwave vortex devices | In microwave resonant systems with ferrite samples, one becomes faced with
specific phase relations for the electromagnetic fields. Such specific phase
relations may lead to appearance of nontrivial states: electromagnetic
vortices. This paper provides some general ideas and design principles for
microwave devices wi... | physics.class-ph | in microwave resonant systems with ferrite samples one becomes faced with specific phase relations for the electromagnetic fields such specific phase relations may lead to appearance of nontrivial states electromagnetic vortices this paper provides some general ideas and design principles for microwave devices with the... | [['in', 'microwave', 'resonant', 'systems', 'with', 'ferrite', 'samples', 'one', 'becomes', 'faced', 'with', 'specific', 'phase', 'relations', 'for', 'the', 'electromagnetic', 'fields', 'such', 'specific', 'phase', 'relations', 'may', 'lead', 'to', 'appearance', 'of', 'nontrivial', 'states', 'electromagnetic', 'vortice... | [-0.2403815706493333, 0.21397337492089719, -0.01945581943627417, 0.03694154177355813, -0.1628975406444321, -0.13412071170751005, 0.020823330863398343, 0.37136128583612543, -0.2455773278294752, -0.3356873097557885, 0.051533518870807406, -0.3067861575788508, -0.16033501531152675, 0.23531842208467424, 0.007466260275881116... |
707.0351 | Dispersion representations for hard exclusive processes | Several hard exclusive scattering processes admit a description in terms of
generalized parton distributions and perturbative hard-scattering kernels. Both
the physical amplitude and the hard-scattering kernels fulfill dispersion
relations. We give a detailed investigation of their consistency at all orders
in pertur... | hep-ph | several hard exclusive scattering processes admit a description in terms of generalized parton distributions and perturbative hardscattering kernels both the physical amplitude and the hardscattering kernels fulfill dispersion relations we give a detailed investigation of their consistency at all orders in perturbation... | [['several', 'hard', 'exclusive', 'scattering', 'processes', 'admit', 'a', 'description', 'in', 'terms', 'of', 'generalized', 'parton', 'distributions', 'and', 'perturbative', 'hardscattering', 'kernels', 'both', 'the', 'physical', 'amplitude', 'and', 'the', 'hardscattering', 'kernels', 'fulfill', 'dispersion', 'relati... | [-0.09078306439814382, 0.14138037967763242, -0.2056373525892609, 0.1934899986606498, -0.09097937656694959, -0.07139058888022756, 0.017271598751506842, 0.37346157517241335, -0.22016932277394266, -0.23785057299952397, 0.0581278194119383, -0.27960296026591597, -0.09805553719058804, 0.17757682335273972, 0.03926177670772390... |
707.0352 | Monte Carlo simulation of pressure-induced phase transitions in
spin-crossover materials | Pressure-induced phase transitions of spin-crossover materials were simulated
by a Monte Carlo simulation in the constant pressure ensemble for the first
time. Here, as the origin of the cooperative interaction, we adopt elastic
interaction among the distortions of the lattice due to the difference of the
molecular s... | cond-mat.mtrl-sci cond-mat.stat-mech | pressureinduced phase transitions of spincrossover materials were simulated by a monte carlo simulation in the constant pressure ensemble for the first time here as the origin of the cooperative interaction we adopt elastic interaction among the distortions of the lattice due to the difference of the molecular sizes in... | [['pressureinduced', 'phase', 'transitions', 'of', 'spincrossover', 'materials', 'were', 'simulated', 'by', 'a', 'monte', 'carlo', 'simulation', 'in', 'the', 'constant', 'pressure', 'ensemble', 'for', 'the', 'first', 'time', 'here', 'as', 'the', 'origin', 'of', 'the', 'cooperative', 'interaction', 'we', 'adopt', 'elast... | [-0.12320733996642422, 0.2050834374588936, -0.05204390862581226, 0.0017967043895341633, -0.01531929683568346, -0.06508866547022102, 0.08942890310454248, 0.380694310325234, -0.27172236449929865, -0.34033361553799274, 0.031729220802527526, -0.2805142777488213, -0.11516408376078043, 0.12363901881992008, 0.0398587349219276... |
707.0353 | Intrinsic Zeeman Effect in Graphene | The intrinsic Zeeman energy is precisely one half of the cyclotron energy for
electrons in graphene. As a result a Landau-level mixing occurs to create the
energy spectrum comprised of the $4j$-fold degenerated zero-energy level and
4-fold degenerated nonzero-energy levels in the $j$-layer graphene, where
$j=1,2,3$ f... | cond-mat.mes-hall cond-mat.str-el | the intrinsic zeeman energy is precisely one half of the cyclotron energy for electrons in graphene as a result a landaulevel mixing occurs to create the energy spectrum comprised of the 4jfold degenerated zeroenergy level and 4fold degenerated nonzeroenergy levels in the jlayer graphene where j123 for monolayer bilaye... | [['the', 'intrinsic', 'zeeman', 'energy', 'is', 'precisely', 'one', 'half', 'of', 'the', 'cyclotron', 'energy', 'for', 'electrons', 'in', 'graphene', 'as', 'a', 'result', 'a', 'landaulevel', 'mixing', 'occurs', 'to', 'create', 'the', 'energy', 'spectrum', 'comprised', 'of', 'the', '4jfold', 'degenerated', 'zeroenergy',... | [-0.20317233895357367, 0.22631734345861224, 0.017093056693585535, 0.048095626264377175, 0.0544382647365115, -0.21392656121366094, 0.10031658115665346, 0.3111134452358036, -0.2206220472355991, -0.3606274300701524, -0.0867364460545924, -0.3525334571183908, -0.05233824670621388, 0.13346730616510763, 0.054155003692088005, ... |
707.0354 | Low densities in asymmetric nuclear matter | Asymmetric nuclear matter is investigated in the low density region below the
nuclear saturation density. Microscopic calculations based on the Dirac
Brueckner Hartree-Fock (DBHF) approach with realistic nucleon-nucleon
potentials are used to adjust a low density functional. This functional is
constructed on a densit... | nucl-th | asymmetric nuclear matter is investigated in the low density region below the nuclear saturation density microscopic calculations based on the dirac brueckner hartreefock dbhf approach with realistic nucleonnucleon potentials are used to adjust a low density functional this functional is constructed on a density expans... | [['asymmetric', 'nuclear', 'matter', 'is', 'investigated', 'in', 'the', 'low', 'density', 'region', 'below', 'the', 'nuclear', 'saturation', 'density', 'microscopic', 'calculations', 'based', 'on', 'the', 'dirac', 'brueckner', 'hartreefock', 'dbhf', 'approach', 'with', 'realistic', 'nucleonnucleon', 'potentials', 'are'... | [-0.08104905836490732, 0.14100100069678356, -0.1758241290891809, 0.13767150654177412, -0.045667409956371204, -0.0860286062282223, 0.013768951540735824, 0.31856380566898596, -0.21768826939654887, -0.2964202050623813, -0.0038170617492169255, -0.2908880606406811, -0.07827118989535348, 0.10611732193983082, 0.03983357129421... |
707.0355 | Evolutionary Conditions in the Dissipative MHD System Revisited | The evolutionary conditions for the dissipative continuous
magnetohydrodynamic (MHD) shocks are studied. We modify Hada's approach in the
stability analysis of the MHD shock waves. The matching conditions between
perturbed shock structure and asymptotic wave modes shows that all types of the
MHD shocks, including the... | astro-ph | the evolutionary conditions for the dissipative continuous magnetohydrodynamic mhd shocks are studied we modify hadas approach in the stability analysis of the mhd shock waves the matching conditions between perturbed shock structure and asymptotic wave modes shows that all types of the mhd shocks including the interme... | [['the', 'evolutionary', 'conditions', 'for', 'the', 'dissipative', 'continuous', 'magnetohydrodynamic', 'mhd', 'shocks', 'are', 'studied', 'we', 'modify', 'hadas', 'approach', 'in', 'the', 'stability', 'analysis', 'of', 'the', 'mhd', 'shock', 'waves', 'the', 'matching', 'conditions', 'between', 'perturbed', 'shock', '... | [-0.18848468266826654, 0.11487372256565972, -0.08792417562550067, 0.11130730949662393, -0.05344290764021155, -0.07385429600877355, -0.06592174143380751, 0.3613872098004712, -0.2934098658817155, -0.2953614263263132, 0.1141435489896269, -0.22775654618661584, -0.1312071363790892, 0.19583757420436346, 0.052885919235580205,... |
707.0356 | No Higgs at the LHC ?! A case for the ILC | I discuss the question whether it is possible that the LHC will find no
signal for the Higgs particle. It is argued that in this case singlet scalars
should be present that could play an important role in astroparticle physics. A
critical view at the existing electroweak data shows that this possibility
might be favo... | hep-ph | i discuss the question whether it is possible that the lhc will find no signal for the higgs particle it is argued that in this case singlet scalars should be present that could play an important role in astroparticle physics a critical view at the existing electroweak data shows that this possibility might be favored ... | [['i', 'discuss', 'the', 'question', 'whether', 'it', 'is', 'possible', 'that', 'the', 'lhc', 'will', 'find', 'no', 'signal', 'for', 'the', 'higgs', 'particle', 'it', 'is', 'argued', 'that', 'in', 'this', 'case', 'singlet', 'scalars', 'should', 'be', 'present', 'that', 'could', 'play', 'an', 'important', 'role', 'in', ... | [-0.08236747554729919, 0.18669295515664508, -0.08119402078886491, 0.1712653133687815, -0.09823576040012208, -0.17028354389618175, -0.03925139073446091, 0.33162626337159323, -0.24702762776507517, -0.2619728118533621, 0.07837921477275321, -0.25879378275744414, -0.12557980710187475, 0.17274967166186134, 0.0060111896034229... |
707.0357 | Relativistic Dynamics of Multi-BPS D-vortices and Straight BPS D-strings | Moduli space dynamics of multi-D-vortices from D2${\bar {\rm D}}$
(equivalently, parallel straight D-strings from D3${\bar {\rm D}}$3) is
systematically studied. For the BPS D-vortices, we show through exact
calculations that the classical motion of randomly-distributed $n$ D-vortices
is governed by a relativistic La... | hep-th astro-ph | moduli space dynamics of multidvortices from d2bar rm d equivalently parallel straight dstrings from d3bar rm d3 is systematically studied for the bps dvortices we show through exact calculations that the classical motion of randomlydistributed n dvortices is governed by a relativistic lagrangian of free massive pointp... | [['moduli', 'space', 'dynamics', 'of', 'multidvortices', 'from', 'd2bar', 'rm', 'd', 'equivalently', 'parallel', 'straight', 'dstrings', 'from', 'd3bar', 'rm', 'd3', 'is', 'systematically', 'studied', 'for', 'the', 'bps', 'dvortices', 'we', 'show', 'through', 'exact', 'calculations', 'that', 'the', 'classical', 'motion... | [-0.18122225062576153, 0.21451979029948087, -0.057098522528465236, 0.10392097560538639, -0.031381484098552216, -0.1475060827098787, -0.014044668196490214, 0.33179583565121695, -0.24771400024934162, -0.24920906006028096, 0.026454983576531373, -0.2838528408398551, -0.08936373225803818, 0.17716767716131385, 0.028053824186... |
707.0358 | Spatial correlation of linear and nonlinear electron transport in
superconducting microwave resonator: laser scanning microscopy analysis | Spatially-resolved techniques of laser scanning microscopy (LSM) have been
used to image simultaneously the spatial variations of (i) rf current flow,
J$_RF$(x,y), of (ii) areas of resistive dissipation and (iii) the sources of
microwave nonlinearity (NL) in an operating superconducting resonator. The RF
power depend... | cond-mat.supr-con cond-mat.mtrl-sci | spatiallyresolved techniques of laser scanning microscopy lsm have been used to image simultaneously the spatial variations of i rf current flow j_rfxy of ii areas of resistive dissipation and iii the sources of microwave nonlinearity nl in an operating superconducting resonator the rf power dependent spatial evolution... | [['spatiallyresolved', 'techniques', 'of', 'laser', 'scanning', 'microscopy', 'lsm', 'have', 'been', 'used', 'to', 'image', 'simultaneously', 'the', 'spatial', 'variations', 'of', 'i', 'rf', 'current', 'flow', 'j_rfxy', 'of', 'ii', 'areas', 'of', 'resistive', 'dissipation', 'and', 'iii', 'the', 'sources', 'of', 'microw... | [-0.16182886397845186, 0.13202880822913823, -0.0026164991055837774, -0.021653462003553864, -0.049962401390075684, -0.1482423953732591, 0.01841318793028214, 0.40989677573397626, -0.22551903272031154, -0.2958343567870623, 0.041346532882982456, -0.3069968126813131, -0.03465382248344543, 0.23190091678922156, 0.047137794824... |
707.0359 | SM scalar and extra singlet(s) | I discuss the question whether it is possible that the LHC will find no
signal for the Higgs boson. It is argued that in this case singlet scalars
should be present that could play an important role in astroparticle physics. A
critical view at the existing electroweak data shows that this possibility
might be favored... | hep-ph | i discuss the question whether it is possible that the lhc will find no signal for the higgs boson it is argued that in this case singlet scalars should be present that could play an important role in astroparticle physics a critical view at the existing electroweak data shows that this possibility might be favored ove... | [['i', 'discuss', 'the', 'question', 'whether', 'it', 'is', 'possible', 'that', 'the', 'lhc', 'will', 'find', 'no', 'signal', 'for', 'the', 'higgs', 'boson', 'it', 'is', 'argued', 'that', 'in', 'this', 'case', 'singlet', 'scalars', 'should', 'be', 'present', 'that', 'could', 'play', 'an', 'important', 'role', 'in', 'as... | [-0.08630810791274181, 0.1874176300387606, -0.07754295664789104, 0.1773705361835734, -0.10369785802086463, -0.17391398790091075, -0.030208963387947832, 0.3349198651172825, -0.2473306849636641, -0.25246729799923867, 0.07608551124891115, -0.2554678866715246, -0.12202199457867725, 0.17340632663674754, 0.009434944131990542... |
707.036 | Effect of Co and Fe on the inverse magnetocaloric properties of Ni-Mn-Sn | At certain compositions Ni-Mn-$X$ Heusler alloys ($X$: group IIIA-VA
elements) undergo martensitic transformations, and many of them exhibit inverse
magnetocaloric effects. In alloys where $X$ is Sn, the isothermal entropy
change is largest among the Heusler alloys, particularly in
Ni$_{50}$Mn$_{37}$Sn$_{13}$ where i... | cond-mat.mtrl-sci | at certain compositions nimnx heusler alloys x group iiiava elements undergo martensitic transformations and many of them exhibit inverse magnetocaloric effects in alloys where x is sn the isothermal entropy change is largest among the heusler alloys particularly in ni_50mn_37sn_13 where it reaches a value of 20 jkg1k1... | [['at', 'certain', 'compositions', 'nimnx', 'heusler', 'alloys', 'x', 'group', 'iiiava', 'elements', 'undergo', 'martensitic', 'transformations', 'and', 'many', 'of', 'them', 'exhibit', 'inverse', 'magnetocaloric', 'effects', 'in', 'alloys', 'where', 'x', 'is', 'sn', 'the', 'isothermal', 'entropy', 'change', 'is', 'lar... | [-0.06279032097991881, 0.18346355420831456, 0.03668742204685039, -0.022220423911548152, -0.00888596196821422, -0.10549003511804762, 0.10975958826645409, 0.39828560771358096, -0.28985240470442997, -0.3279095933828878, 0.04256927518286561, -0.40384885555308236, -0.04291351924137831, 0.1410147925735695, 0.0244150691690710... |
707.0361 | The curvature perturbation in a box | The stochastic properties of cosmological perturbations are best defined
through the Fourier expansion in a finite box. I discuss the reasons for that
with reference the curvature perturbation, and explore some issues arising from
it.
| astro-ph gr-qc hep-ph hep-th | the stochastic properties of cosmological perturbations are best defined through the fourier expansion in a finite box i discuss the reasons for that with reference the curvature perturbation and explore some issues arising from it | [['the', 'stochastic', 'properties', 'of', 'cosmological', 'perturbations', 'are', 'best', 'defined', 'through', 'the', 'fourier', 'expansion', 'in', 'a', 'finite', 'box', 'i', 'discuss', 'the', 'reasons', 'for', 'that', 'with', 'reference', 'the', 'curvature', 'perturbation', 'and', 'explore', 'some', 'issues', 'arisi... | [-0.11566617409033435, 0.0860347229987383, -0.08411939341042723, 0.10098882243037224, -0.09032138820205415, -0.07974812514813882, -0.02394982028220381, 0.3158520512815033, -0.32913266058479035, -0.23252183965274265, 0.18066050874268902, -0.29276722720158954, -0.15427863033754485, 0.15690426464758014, -0.027022934784846... |
707.0362 | On Fox and augmentation quotients of semidirect products | Let $G$ be a group which is the semidirect product of a normal subgroup $N$
and some subgroup $T$. Let $I^n(G)$, $n\ge 1$, denote the powers of the
augmentation ideal $I(G)$ of the group ring $\Z(G)$. Using homological methods
the groups $Q_n(G,H) = I^{n-1}(G)I(H)/I^{n}(G)I(H)$, $H=G,N,T$, are
functorially expressed ... | math.GR math.RA | let g be a group which is the semidirect product of a normal subgroup n and some subgroup t let ing nge 1 denote the powers of the augmentation ideal ig of the group ring zg using homological methods the groups q_ngh in1gihingih hgnt are functorially expressed in terms of enveloping algebras of certain lie rings associ... | [['let', 'g', 'be', 'a', 'group', 'which', 'is', 'the', 'semidirect', 'product', 'of', 'a', 'normal', 'subgroup', 'n', 'and', 'some', 'subgroup', 't', 'let', 'ing', 'nge', '1', 'denote', 'the', 'powers', 'of', 'the', 'augmentation', 'ideal', 'ig', 'of', 'the', 'group', 'ring', 'zg', 'using', 'homological', 'methods', '... | [-0.22384417741402482, 0.12255017049192043, -0.038417793857906564, -0.0373678259548909, -0.06571316063466869, -0.20188391010873438, -0.04918255690443382, 0.3417672373856721, -0.3563031425040341, -0.2241050765504328, 0.13875059682739835, -0.2655488517805097, -0.05260784161444544, 0.1875059494481872, -0.09641325115906389... |
707.0363 | Detecting bubbles in exotic nuclei | The occurrence of a bubble, due to an inversion of s$_{1/2}$ state with the
state usually located above, is investigated. Proton bubbles in neutron-rich
Argon isotopes are optimal candidates. Pairing effects which can play against
the bubble formation are evaluated. They cannot prevent bubble formation in
very neutro... | nucl-th nucl-ex | the occurrence of a bubble due to an inversion of s_12 state with the state usually located above is investigated proton bubbles in neutronrich argon isotopes are optimal candidates pairing effects which can play against the bubble formation are evaluated they cannot prevent bubble formation in very neutronrich argon i... | [['the', 'occurrence', 'of', 'a', 'bubble', 'due', 'to', 'an', 'inversion', 'of', 's_12', 'state', 'with', 'the', 'state', 'usually', 'located', 'above', 'is', 'investigated', 'proton', 'bubbles', 'in', 'neutronrich', 'argon', 'isotopes', 'are', 'optimal', 'candidates', 'pairing', 'effects', 'which', 'can', 'play', 'ag... | [-0.043882317364808514, 0.25231570568063366, -0.04182032448641786, 0.11345867296172814, 0.03818749124184251, -0.1049999107245557, 0.025231296799822965, 0.3580982165665112, -0.20378897986798125, -0.2819138646432707, 0.06216744454154237, -0.3380954816768115, 0.03610541895084845, 0.1529668590281455, 0.05154927932149307, 0... |
707.0364 | Polarization types of isogenous Prym-Tyurin varieties | Let p:C-->Y be a covering of smooth, projective curves which is a composition
of \pi:C-->C' of degree 2 and g:C'-->Y of degree n. Let f:X-->Y be the covering
of degree 2^n, where the curve X parametrizes the liftings in C^{(n)} of the
fibers of g:C'-->Y. Let P(X,\delta) be the associated Prym-Tyurin variety,
known to... | math.AG | let pcy be a covering of smooth projective curves which is a composition of picc of degree 2 and gcy of degree n let fxy be the covering of degree 2n where the curve x parametrizes the liftings in cn of the fibers of gcy let pxdelta be the associated prymtyurin variety known to be isogenous to the prym variety pcc most... | [['let', 'pcy', 'be', 'a', 'covering', 'of', 'smooth', 'projective', 'curves', 'which', 'is', 'a', 'composition', 'of', 'picc', 'of', 'degree', '2', 'and', 'gcy', 'of', 'degree', 'n', 'let', 'fxy', 'be', 'the', 'covering', 'of', 'degree', '2n', 'where', 'the', 'curve', 'x', 'parametrizes', 'the', 'liftings', 'in', 'cn'... | [-0.15705273934696434, 0.09056993033454726, -0.06407866981162717, -0.004546434649841323, -0.04436917919453911, -0.16654925402183313, -0.029732677853616857, 0.32707738272394193, -0.3052979322039226, -0.22176209727838408, 0.10344130112119301, -0.24368382741125638, -0.1296980591406199, 0.23981554552940934, -0.123935094050... |
707.0365 | Performance Analysis of Publish/Subscribe Systems | The Desktop Grid offers solutions to overcome several challenges and to
answer increasingly needs of scientific computing. Its technology consists
mainly in exploiting resources, geographically dispersed, to treat complex
applications needing big power of calculation and/or important storage
capacity. However, as res... | cs.DC | the desktop grid offers solutions to overcome several challenges and to answer increasingly needs of scientific computing its technology consists mainly in exploiting resources geographically dispersed to treat complex applications needing big power of calculation andor important storage capacity however as resources n... | [['the', 'desktop', 'grid', 'offers', 'solutions', 'to', 'overcome', 'several', 'challenges', 'and', 'to', 'answer', 'increasingly', 'needs', 'of', 'scientific', 'computing', 'its', 'technology', 'consists', 'mainly', 'in', 'exploiting', 'resources', 'geographically', 'dispersed', 'to', 'treat', 'complex', 'application... | [-0.16117869982442173, 0.026932090940252423, -0.025887262758586962, 0.06963632788765842, -0.09358213116856626, -0.1687969258413292, 0.06878858462098436, 0.39620408851008576, -0.2782197430705986, -0.37115260046453047, 0.12230582270048893, -0.26591754185322386, -0.11069034456532115, 0.22131089934779224, -0.11976367108320... |
707.0366 | Willmore Legendrian surfaces in pseudoconformal 5-sphere | Let $ X: M \hook S^5$ be a compact Legendrian surface in pseudoconformal(CR)
5-sphere. We introduce a pseudoconformally invariant Willmore type second order
functional $ \W(X)$, and study its critical points called Willmore Legendrian
surfaces. The fifth order structure equations show that Willmore dual can be
define... | math.DG math.AP | let x m hook s5 be a compact legendrian surface in pseudoconformalcr 5sphere we introduce a pseudoconformally invariant willmore type second order functional wx and study its critical points called willmore legendrian surfaces the fifth order structure equations show that willmore dual can be defined for a class of wil... | [['let', 'x', 'm', 'hook', 's5', 'be', 'a', 'compact', 'legendrian', 'surface', 'in', 'pseudoconformalcr', '5sphere', 'we', 'introduce', 'a', 'pseudoconformally', 'invariant', 'willmore', 'type', 'second', 'order', 'functional', 'wx', 'and', 'study', 'its', 'critical', 'points', 'called', 'willmore', 'legendrian', 'sur... | [-0.27311165458072095, 0.057421555707180466, -0.1087497841386545, 0.12956737903427454, -0.15166626611514197, -0.19219250399093593, -0.08600607363417023, 0.3432996044566314, -0.26207947433595696, -0.19882483482961694, 0.08956170861417759, -0.2662221848093454, -0.1684489277371716, 0.1713332471253741, -0.1929830683455352,... |
707.0367 | Radial Dunkl Processes : Existence and uniqueness, Hitting time, Beta
Processes and Random Matrices | We begin with the study of some properties of the radial Dunkl process
associated to a reduced root system $R$. It is shown that this diffusion is the
unique strong solution for all $t \geq 0$ of a SDE with singular drift. Then,
we study $T_0$, the first hitting time of the positive Weyl chamber : we prove,
via stoch... | math.PR | we begin with the study of some properties of the radial dunkl process associated to a reduced root system r it is shown that this diffusion is the unique strong solution for all t geq 0 of a sde with singular drift then we study t_0 the first hitting time of the positive weyl chamber we prove via stochastic calculus a... | [['we', 'begin', 'with', 'the', 'study', 'of', 'some', 'properties', 'of', 'the', 'radial', 'dunkl', 'process', 'associated', 'to', 'a', 'reduced', 'root', 'system', 'r', 'it', 'is', 'shown', 'that', 'this', 'diffusion', 'is', 'the', 'unique', 'strong', 'solution', 'for', 'all', 't', 'geq', '0', 'of', 'a', 'sde', 'with... | [-0.13531071166685055, 0.09485323946675002, -0.06951855310375243, 0.043338284313489094, -0.08307154765909376, -0.12395977664678155, 0.017416524108620764, 0.3096316696255994, -0.3277386351559392, -0.2044841137869061, 0.14610244260509955, -0.2817033142985209, -0.13037004306882052, 0.18245444354176035, -0.0778041949607026... |
707.0368 | Stochastic background of relic scalar gravitational waves from
scalar-tensor gravity | A stochastic background of relic gravitational waves is achieved by the so
called adiabatically-amplified zero-point fluctuations process derived from
early inflation. In principle, it provides a distinctive spectrum of relic
gravitational waves. In the framework of scalar-tensor gravity, we discuss the
scalar modes ... | gr-qc | a stochastic background of relic gravitational waves is achieved by the so called adiabaticallyamplified zeropoint fluctuations process derived from early inflation in principle it provides a distinctive spectrum of relic gravitational waves in the framework of scalartensor gravity we discuss the scalar modes of gravit... | [['a', 'stochastic', 'background', 'of', 'relic', 'gravitational', 'waves', 'is', 'achieved', 'by', 'the', 'so', 'called', 'adiabaticallyamplified', 'zeropoint', 'fluctuations', 'process', 'derived', 'from', 'early', 'inflation', 'in', 'principle', 'it', 'provides', 'a', 'distinctive', 'spectrum', 'of', 'relic', 'gravi... | [-0.19368072270523184, 0.1993567593073329, -0.12894036502052003, 0.12813868070292628, -0.1424616460616772, -0.060425389325246215, -0.05499038976641037, 0.23876221295302877, -0.2352086005684657, -0.2761805252006385, 0.05380063758004839, -0.27494888800459033, -0.116090590122323, 0.1732093471651658, 0.049960670531548276, ... |
707.0369 | Numerical study of the influence of an applied electrical potential on
the solidification of a binary metal alloy | In this work we study numerically the influence of a homogeneous electrical
field on the fluid and heat transfer phenomena at macroscale and mesoscale
during unidirectional solidification of a binary metal alloy. The numerical
results showed that a pulse electric discharging applied perpendicularly to the
solidificat... | cond-mat.mtrl-sci cond-mat.other | in this work we study numerically the influence of a homogeneous electrical field on the fluid and heat transfer phenomena at macroscale and mesoscale during unidirectional solidification of a binary metal alloy the numerical results showed that a pulse electric discharging applied perpendicularly to the solidification... | [['in', 'this', 'work', 'we', 'study', 'numerically', 'the', 'influence', 'of', 'a', 'homogeneous', 'electrical', 'field', 'on', 'the', 'fluid', 'and', 'heat', 'transfer', 'phenomena', 'at', 'macroscale', 'and', 'mesoscale', 'during', 'unidirectional', 'solidification', 'of', 'a', 'binary', 'metal', 'alloy', 'the', 'nu... | [-0.1376785621238948, 0.21051715789174005, -0.07897649992672676, -0.018201974576899177, -0.0411822262056474, -0.04801570186611718, 0.048354331940425106, 0.35311038652434945, -0.2787280757439549, -0.27715656936571403, 0.03582290579121233, -0.2659310093133811, -0.1251593450622356, 0.18037641429770235, -0.0052574177499155... |
707.037 | Efficient dynamical nuclear polarization in quantum dots: Temperature
dependence | We investigate in micro-photoluminescence experiments the dynamical nuclear
polarization in individual InGaAs quantum dots. Experiments carried out in an
applied magnetic field of 2T show that the nuclear polarization achieved
through the optical pumping of electron spins is increasing with the sample
temperature bet... | cond-mat.other | we investigate in microphotoluminescence experiments the dynamical nuclear polarization in individual ingaas quantum dots experiments carried out in an applied magnetic field of 2t show that the nuclear polarization achieved through the optical pumping of electron spins is increasing with the sample temperature between... | [['we', 'investigate', 'in', 'microphotoluminescence', 'experiments', 'the', 'dynamical', 'nuclear', 'polarization', 'in', 'individual', 'ingaas', 'quantum', 'dots', 'experiments', 'carried', 'out', 'in', 'an', 'applied', 'magnetic', 'field', 'of', '2t', 'show', 'that', 'the', 'nuclear', 'polarization', 'achieved', 'th... | [-0.11709680737528418, 0.19829619769717238, -0.041218844641532214, -3.431245291029059e-05, 0.037394405309376974, -0.09492428298801228, 0.07762966115149625, 0.40963057845476125, -0.24549036045070916, -0.33571434425677926, 0.025605565099145418, -0.3071283847093582, -0.018216604610816353, 0.2341221545973981, 0.07137463898... |
707.0371 | Quadratic maps between groups | The notion of quadratic maps between arbitrary groups appeared at several
places in the literature on quadratic algebra. Here a unified extensive
treatment of their properties is given; the relation with a relative version of
Passi's polynomial maps and groups of degree 2 is established and used to study
the structur... | math.GR math.RA | the notion of quadratic maps between arbitrary groups appeared at several places in the literature on quadratic algebra here a unified extensive treatment of their properties is given the relation with a relative version of passis polynomial maps and groups of degree 2 is established and used to study the structure of ... | [['the', 'notion', 'of', 'quadratic', 'maps', 'between', 'arbitrary', 'groups', 'appeared', 'at', 'several', 'places', 'in', 'the', 'literature', 'on', 'quadratic', 'algebra', 'here', 'a', 'unified', 'extensive', 'treatment', 'of', 'their', 'properties', 'is', 'given', 'the', 'relation', 'with', 'a', 'relative', 'versi... | [-0.1471111040808401, 0.02688925969853716, -0.10790217586107692, 0.060719173028186524, -0.05915903222729575, -0.06517407693460865, 0.029665208193209936, 0.34729971293852013, -0.3068872713308149, -0.30729244782079784, 0.10507112038365723, -0.24485015942943547, -0.1596256948849362, 0.2150593745118042, -0.0530755992293498... |
707.0372 | Regulators of canonical extensions are torsion: the smooth divisor case | In this paper, we prove a generalization of Reznikov's theorem which says
that the Chern-Simons classes and in particular the Deligne Chern classes (in
degrees $>1$) are torsion, of a flat bundle on a smooth complex projective
variety. We consider the case of a smooth quasi--projective variety with an
irreducible smo... | math.AG | in this paper we prove a generalization of reznikovs theorem which says that the chernsimons classes and in particular the deligne chern classes in degrees 1 are torsion of a flat bundle on a smooth complex projective variety we consider the case of a smooth quasiprojective variety with an irreducible smooth divisor at... | [['in', 'this', 'paper', 'we', 'prove', 'a', 'generalization', 'of', 'reznikovs', 'theorem', 'which', 'says', 'that', 'the', 'chernsimons', 'classes', 'and', 'in', 'particular', 'the', 'deligne', 'chern', 'classes', 'in', 'degrees', '1', 'are', 'torsion', 'of', 'a', 'flat', 'bundle', 'on', 'a', 'smooth', 'complex', 'pr... | [-0.2532795412400954, 0.07181687257404921, -0.08491295737452632, 0.03907421100641016, -0.11891952646506387, -0.18626037286053043, -0.06734050375945476, 0.2909923963949929, -0.31345514268722646, -0.17519076643674092, 0.023361053086308287, -0.19653155716396, -0.1955835074754865, 0.1739904402300369, -0.19801763966842012, ... |
707.0373 | Search for invisibly decaying Higgs bosons in e+e- -> Zoho production at
sqrt(s) = 183 - 209 GeV | A search is performed for Higgs bosons decaying into invisible final states,
produced in association with a Zo boson in e+e- collisions at energies between
183 and 209 GeV. The search is based on data samples collected by the OPAL
detector at LEP corresponding to an integrated luminosity of about 660 pb-1.
The analys... | hep-ex | a search is performed for higgs bosons decaying into invisible final states produced in association with a zo boson in ee collisions at energies between 183 and 209 gev the search is based on data samples collected by the opal detector at lep corresponding to an integrated luminosity of about 660 pb1 the analysis aims ... | [['a', 'search', 'is', 'performed', 'for', 'higgs', 'bosons', 'decaying', 'into', 'invisible', 'final', 'states', 'produced', 'in', 'association', 'with', 'a', 'zo', 'boson', 'in', 'ee', 'collisions', 'at', 'energies', 'between', '183', 'and', '209', 'gev', 'the', 'search', 'is', 'based', 'on', 'data', 'samples', 'coll... | [-0.04657178862393157, 0.2846364788101163, -0.054169057300975904, 0.18278375209520362, -0.034015526002669924, -0.1898164619905416, 0.06606174198098867, 0.31170925979828207, -0.1896086760155368, -0.2925002238219553, -0.00454996282341661, -0.3577471988611534, 0.13059430584423448, 0.15738821329734712, 0.13731365051385158,... |
707.0374 | Vibration diagnostics instrumentation for ILC | The future e-e+ 500 GeV International Linear Collider will rely on
unprecedented nanometer scale particle beam size at the interaction point, in
order to achieve the design luminosity. Tight tolerances on static and dynamic
alignment of the accelerator cavities and optical components are demanded to
transport and foc... | physics.ins-det physics.acc-ph | the future ee 500 gev international linear collider will rely on unprecedented nanometer scale particle beam size at the interaction point in order to achieve the design luminosity tight tolerances on static and dynamic alignment of the accelerator cavities and optical components are demanded to transport and focus the... | [['the', 'future', 'ee', '500', 'gev', 'international', 'linear', 'collider', 'will', 'rely', 'on', 'unprecedented', 'nanometer', 'scale', 'particle', 'beam', 'size', 'at', 'the', 'interaction', 'point', 'in', 'order', 'to', 'achieve', 'the', 'design', 'luminosity', 'tight', 'tolerances', 'on', 'static', 'and', 'dynami... | [-0.10980794442341078, 0.15517082716186725, -0.034244607083586065, 0.07326086744027169, -0.05871871449757194, -0.1634735096283907, 0.0033040963191820613, 0.43672052255376825, -0.23535817655799693, -0.34051340150776815, 0.09455551448830425, -0.28725898004310246, 0.02062689881706827, 0.23120800540701292, -0.0023206331886... |
707.0375 | Performance limits of graphene-ribbon-based field effect transistors | The performance of field effect transistors based on an single graphene
ribbon with a constriction and a single back gate are studied with the help of
atomistic models. It is shown how this scheme, unlike that of traditional
carbon-nanotube-based transistors, reduces the importance of the specifics of
the chemical bo... | cond-mat.mes-hall cond-mat.mtrl-sci | the performance of field effect transistors based on an single graphene ribbon with a constriction and a single back gate are studied with the help of atomistic models it is shown how this scheme unlike that of traditional carbonnanotubebased transistors reduces the importance of the specifics of the chemical bonding t... | [['the', 'performance', 'of', 'field', 'effect', 'transistors', 'based', 'on', 'an', 'single', 'graphene', 'ribbon', 'with', 'a', 'constriction', 'and', 'a', 'single', 'back', 'gate', 'are', 'studied', 'with', 'the', 'help', 'of', 'atomistic', 'models', 'it', 'is', 'shown', 'how', 'this', 'scheme', 'unlike', 'that', 'o... | [-0.13721286819200032, 0.09796838978902088, -0.03847804741759319, 0.008184809053200298, -0.012353376129176467, -0.2002828191127628, 0.08758418831508606, 0.4054521987214684, -0.2231075354013592, -0.28726632123813034, 0.0229926706594415, -0.24998896665871143, -0.18260853311046957, 0.2554912570863962, -0.05085994725581258... |
707.0376 | Self Improving Sobolev-Poincare Inequalities, Truncation and
Symmetrization | In a previous paper we developed a new method to obtain symmetrization
inequalities of Sobolev type for functions in $W_{0}^{1,1}(\Omega)$. In this
paper we extend our method to Sobolev functions that do not vanish at the
boundary.
| math.FA math.AP | in a previous paper we developed a new method to obtain symmetrization inequalities of sobolev type for functions in w_011omega in this paper we extend our method to sobolev functions that do not vanish at the boundary | [['in', 'a', 'previous', 'paper', 'we', 'developed', 'a', 'new', 'method', 'to', 'obtain', 'symmetrization', 'inequalities', 'of', 'sobolev', 'type', 'for', 'functions', 'in', 'w_011omega', 'in', 'this', 'paper', 'we', 'extend', 'our', 'method', 'to', 'sobolev', 'functions', 'that', 'do', 'not', 'vanish', 'at', 'the', ... | [-0.04965732802843882, 0.014671383684294092, -0.11188764033269966, 0.07400688092780507, -0.09573062116073237, -0.09109351564095253, 0.058961515321344554, 0.36612484304027426, -0.26212588718367946, -0.19463116034037536, 0.08031799835993701, -0.2244930508443051, -0.17626027290761057, 0.22317560651249047, -0.1550591417795... |
707.0377 | Analysis of Emission Shapes | Shapes of relative emission sources can be accessed by expanding shapes of
correlations at low relative velocities in pair center of mass in Cartesian
harmonics. Coefficients of expansion for correlations are related to the
respective coefficients of expansion for the sources through one dimensional
integral transfor... | nucl-th | shapes of relative emission sources can be accessed by expanding shapes of correlations at low relative velocities in pair center of mass in cartesian harmonics coefficients of expansion for correlations are related to the respective coefficients of expansion for the sources through one dimensional integral transforms ... | [['shapes', 'of', 'relative', 'emission', 'sources', 'can', 'be', 'accessed', 'by', 'expanding', 'shapes', 'of', 'correlations', 'at', 'low', 'relative', 'velocities', 'in', 'pair', 'center', 'of', 'mass', 'in', 'cartesian', 'harmonics', 'coefficients', 'of', 'expansion', 'for', 'correlations', 'are', 'related', 'to', ... | [-0.10724378292798065, 0.15134124402538873, -0.1250094469069154, 0.06419271027880313, -0.013436098492093151, -0.04727574498974718, -0.06015857826787396, 0.4073418894549832, -0.25687481438944815, -0.26762917754240334, 0.03137097150829504, -0.3725666283571627, 0.01628012995206518, 0.22638745557924267, 0.05352624610532075... |
707.0378 | CP violation in scatterings, three body processes and the Boltzmann
equations for leptogenesis | We obtain the Boltzmann equations for leptogenesis including decay and
scattering processes with two and three body initial or final states. We
present an explicit computation of the CP violating scattering asymmetries. We
analyze their possible impact in leptogenesis, and we discuss the validity of
their approximate... | hep-ph | we obtain the boltzmann equations for leptogenesis including decay and scattering processes with two and three body initial or final states we present an explicit computation of the cp violating scattering asymmetries we analyze their possible impact in leptogenesis and we discuss the validity of their approximate expr... | [['we', 'obtain', 'the', 'boltzmann', 'equations', 'for', 'leptogenesis', 'including', 'decay', 'and', 'scattering', 'processes', 'with', 'two', 'and', 'three', 'body', 'initial', 'or', 'final', 'states', 'we', 'present', 'an', 'explicit', 'computation', 'of', 'the', 'cp', 'violating', 'scattering', 'asymmetries', 'we'... | [-0.1550571049875905, 0.21259734593652582, -0.06437283466189539, 0.1269728642123531, 0.0031733150476269344, -0.09525089264066229, 0.06107666194332533, 0.27523347997276854, -0.2612371264996948, -0.2878302753219501, 0.05245318079945601, -0.27539336746458404, -0.029430471895818388, 0.10648902438916466, 0.03995608818051981... |
707.0379 | Dependence of Resonant Absorption Linewidth on Atomic Vapour Column
Thickness for D1 Line of Cs Atoms Confined in Nano-Cell | A new nano-cell with smoothly varying longitudinal thickness of the atomic
vapour layer L in the range of 350 - 5100 nm allowing to study the resonant
absorption of D1 and D2 lines of Cs atoms for thicknesses changing from L =
Lambda/2 to L = 6 Lambda with the step of Lambda/2 (Lambda = 852 nm or 894 nm
are the reson... | physics.atom-ph | a new nanocell with smoothly varying longitudinal thickness of the atomic vapour layer l in the range of 350 5100 nm allowing to study the resonant absorption of d1 and d2 lines of cs atoms for thicknesses changing from l lambda2 to l 6 lambda with the step of lambda2 lambda 852 nm or 894 nm are the resonant laser wave... | [['a', 'new', 'nanocell', 'with', 'smoothly', 'varying', 'longitudinal', 'thickness', 'of', 'the', 'atomic', 'vapour', 'layer', 'l', 'in', 'the', 'range', 'of', '350', '5100', 'nm', 'allowing', 'to', 'study', 'the', 'resonant', 'absorption', 'of', 'd1', 'and', 'd2', 'lines', 'of', 'cs', 'atoms', 'for', 'thicknesses', '... | [-0.11313863839848037, 0.20213743124853104, 0.03715120193465978, -0.01931893263421835, -0.004935268906558145, -0.2186225192868917, 0.03189128335518173, 0.4437489478459841, -0.23683330840932182, -0.3172318945886402, 0.0032366878681674696, -0.2911103014197625, 0.010878899970233346, 0.16286470606050726, 0.0647108730936682... |
707.038 | Expanding Space: the Root of all Evil? | While it remains the staple of virtually all cosmological teaching, the
concept of expanding space in explaining the increasing separation of galaxies
has recently come under fire as a dangerous idea whose application leads to the
development of confusion and the establishment of misconceptions. In this
paper, we dev... | astro-ph gr-qc physics.ed-ph | while it remains the staple of virtually all cosmological teaching the concept of expanding space in explaining the increasing separation of galaxies has recently come under fire as a dangerous idea whose application leads to the development of confusion and the establishment of misconceptions in this paper we develop ... | [['while', 'it', 'remains', 'the', 'staple', 'of', 'virtually', 'all', 'cosmological', 'teaching', 'the', 'concept', 'of', 'expanding', 'space', 'in', 'explaining', 'the', 'increasing', 'separation', 'of', 'galaxies', 'has', 'recently', 'come', 'under', 'fire', 'as', 'a', 'dangerous', 'idea', 'whose', 'application', 'l... | [-0.07423810226908695, 0.12122503825191891, -0.12842491575706322, 0.060503916637724746, -0.09655295229574616, -0.06868047053736132, 0.03308598548833248, 0.328160082274405, -0.22195820830168977, -0.2955429595029723, 0.1134024297898899, -0.21483944607623007, -0.16514862772176223, 0.18477821613628978, -0.06740781750562971... |
707.0381 | Strong and electroweak corrections to the production of Higgs+2jets via
weak interactions at the LHC | Radiative corrections of strong and electroweak interactions are presented at
next-to-leading order for the production of a Higgs boson plus two hard jets
via weak interactions at the LHC. The calculation includes all weak-boson
fusion and quark-antiquark annihilation diagrams as well as the corresponding
interferenc... | hep-ph | radiative corrections of strong and electroweak interactions are presented at nexttoleading order for the production of a higgs boson plus two hard jets via weak interactions at the lhc the calculation includes all weakboson fusion and quarkantiquark annihilation diagrams as well as the corresponding interferences the ... | [['radiative', 'corrections', 'of', 'strong', 'and', 'electroweak', 'interactions', 'are', 'presented', 'at', 'nexttoleading', 'order', 'for', 'the', 'production', 'of', 'a', 'higgs', 'boson', 'plus', 'two', 'hard', 'jets', 'via', 'weak', 'interactions', 'at', 'the', 'lhc', 'the', 'calculation', 'includes', 'all', 'wea... | [-0.08997728216490941, 0.22862219689583677, -0.033379656356070576, 0.20479621661555333, -0.025616786816196207, -0.08103157279644317, 0.0053555942480064305, 0.31757513162059087, -0.18831435388710815, -0.29536425561915775, 0.005370211398258107, -0.3585522831029569, -0.006274351796794993, 0.11578331935258272, 0.1117437073... |
707.0382 | Why are accreting T Tauri stars less luminous in X-rays than
non-accretors? | Accreting T Tauri stars are observed to be less luminous in X-rays than
non-accretors, an effect that has been detected in various star forming
regions. To explain this we have combined, for the first time, a radiative
transfer code with an accretion model that considers magnetic fields
extrapolated from surface magn... | astro-ph | accreting t tauri stars are observed to be less luminous in xrays than nonaccretors an effect that has been detected in various star forming regions to explain this we have combined for the first time a radiative transfer code with an accretion model that considers magnetic fields extrapolated from surface magnetograms... | [['accreting', 't', 'tauri', 'stars', 'are', 'observed', 'to', 'be', 'less', 'luminous', 'in', 'xrays', 'than', 'nonaccretors', 'an', 'effect', 'that', 'has', 'been', 'detected', 'in', 'various', 'star', 'forming', 'regions', 'to', 'explain', 'this', 'we', 'have', 'combined', 'for', 'the', 'first', 'time', 'a', 'radiat... | [-0.05635730526939204, 0.18664385886149096, -0.008379745673425872, 0.09317788762872982, -0.08233134414662015, -0.05685716985508499, -0.023928474747773373, 0.47415576288194367, -0.19230161772363566, -0.34020164142353365, 0.07015829111538789, -0.28230760248396736, -0.03536204998898837, 0.22925169206299492, -0.01926659159... |
707.0383 | Pair condensation of bosonic atoms induced by optical lattices | We design a model of correlated hopping for bosonic atoms in optical
lattices. Such model exhibits three kinds of phases, comprehending a Mott
insulator, a charge density wave and a pair quasi-condensate. The
implementation of the model relies on two-state atoms embedded in
state-dependent lattices and having spin-de... | cond-mat.other quant-ph | we design a model of correlated hopping for bosonic atoms in optical lattices such model exhibits three kinds of phases comprehending a mott insulator a charge density wave and a pair quasicondensate the implementation of the model relies on twostate atoms embedded in statedependent lattices and having spindependent in... | [['we', 'design', 'a', 'model', 'of', 'correlated', 'hopping', 'for', 'bosonic', 'atoms', 'in', 'optical', 'lattices', 'such', 'model', 'exhibits', 'three', 'kinds', 'of', 'phases', 'comprehending', 'a', 'mott', 'insulator', 'a', 'charge', 'density', 'wave', 'and', 'a', 'pair', 'quasicondensate', 'the', 'implementation... | [-0.18709255415680154, 0.22342196257252778, -0.06291254146240785, 0.03469798121368513, -0.020652178837917746, -0.21643633866416556, 0.07870984835483666, 0.4154856530683381, -0.20166658698581158, -0.21814790576297258, -0.0015813829759801074, -0.32214011448834623, -0.13951350336096116, 0.1673297279880249, 0.0609258449037... |
707.0384 | Ab-initio calculation of phonon dispersion curves: accelerating q point
convergence | We present a scheme for the improved description of the long-range
interatomic force constants in a more accurate way than the procedure which is
commonly used within plane-wave based density-functional perturbation-theory
calculations. Our scheme is based on the inclusion of a q point grid which is
denser in a restr... | cond-mat.mtrl-sci cond-mat.dis-nn cond-mat.mes-hall cond-mat.other cond-mat.soft cond-mat.stat-mech | we present a scheme for the improved description of the longrange interatomic force constants in a more accurate way than the procedure which is commonly used within planewave based densityfunctional perturbationtheory calculations our scheme is based on the inclusion of a q point grid which is denser in a restricted a... | [['we', 'present', 'a', 'scheme', 'for', 'the', 'improved', 'description', 'of', 'the', 'longrange', 'interatomic', 'force', 'constants', 'in', 'a', 'more', 'accurate', 'way', 'than', 'the', 'procedure', 'which', 'is', 'commonly', 'used', 'within', 'planewave', 'based', 'densityfunctional', 'perturbationtheory', 'calcu... | [-0.10212121021040545, 0.06358476390967702, -0.09744485283308492, 0.016090367115292773, -0.019159009518595983, -0.07071841818432571, 0.110920608535466, 0.39594622457171885, -0.2023541862002517, -0.26155703733390084, 0.056220565765753995, -0.25865851975597287, -0.11554357366950004, 0.2289720274970097, 0.0054780511275808... |
707.0385 | Specialization of strategies and herding behavior of trading firms in a
financial market | The understanding of complex social or economic systems is an important
scientific challenge. Here we present a comprehensive study of the Spanish
Stock Exchange showing that most financial firms trading in that market are
characterized by a resulting strategy and can be classified in groups of firms
with different s... | q-fin.ST physics.soc-ph | the understanding of complex social or economic systems is an important scientific challenge here we present a comprehensive study of the spanish stock exchange showing that most financial firms trading in that market are characterized by a resulting strategy and can be classified in groups of firms with different spec... | [['the', 'understanding', 'of', 'complex', 'social', 'or', 'economic', 'systems', 'is', 'an', 'important', 'scientific', 'challenge', 'here', 'we', 'present', 'a', 'comprehensive', 'study', 'of', 'the', 'spanish', 'stock', 'exchange', 'showing', 'that', 'most', 'financial', 'firms', 'trading', 'in', 'that', 'market', '... | [-0.12186639387870118, 0.13710787968167487, -0.09384804633667782, 0.10893436786968128, -0.0999548394410383, -0.11632386084446418, 0.09324294116647382, 0.4232798591034398, -0.266566460881482, -0.3257798183753732, 0.13204680318068268, -0.2989016645976032, -0.16540068972556451, 0.21583495900822094, -0.08613732590207032, -... |
707.0386 | BRST approach to Lagrangian formulation for mixed-symmetry fermionic
higher-spin fields | We construct a Lagrangian description of irreducible half-integer higher-spin
representations of the Poincare group with the corresponding Young tableaux
having two rows, on a basis of the BRST approach. Starting with a description
of fermionic higher-spin fields in a flat space of any dimension in terms of an
auxili... | hep-th | we construct a lagrangian description of irreducible halfinteger higherspin representations of the poincare group with the corresponding young tableaux having two rows on a basis of the brst approach starting with a description of fermionic higherspin fields in a flat space of any dimension in terms of an auxiliary foc... | [['we', 'construct', 'a', 'lagrangian', 'description', 'of', 'irreducible', 'halfinteger', 'higherspin', 'representations', 'of', 'the', 'poincare', 'group', 'with', 'the', 'corresponding', 'young', 'tableaux', 'having', 'two', 'rows', 'on', 'a', 'basis', 'of', 'the', 'brst', 'approach', 'starting', 'with', 'a', 'descr... | [-0.18026334805016622, 0.17351380069848887, -0.08493633577223829, 0.05627927435808956, -0.12136392385905816, -0.10951690894617426, -0.0263098537700834, 0.30875218801454385, -0.21896073912420885, -0.28029063881423105, 0.048829664345101616, -0.22268322737642912, -0.12171488723745852, 0.12566807015323916, -0.0297513591229... |
707.0387 | Planar Homological Mirror Symmetry | In this article, we formulate a planar limited version of the B-side in
homological mirror symmetry that formularizes Chern-Simons-type topological
open string field theory using homotopy associative algebra ($A_{\infty}$
algebra). This formulation is based on the works by Dijkgraaf and Vafa. We show
that our formula... | hep-th math.AG math.SG | in this article we formulate a planar limited version of the bside in homological mirror symmetry that formularizes chernsimonstype topological open string field theory using homotopy associative algebra a_infty algebra this formulation is based on the works by dijkgraaf and vafa we show that our formularization includ... | [['in', 'this', 'article', 'we', 'formulate', 'a', 'planar', 'limited', 'version', 'of', 'the', 'bside', 'in', 'homological', 'mirror', 'symmetry', 'that', 'formularizes', 'chernsimonstype', 'topological', 'open', 'string', 'field', 'theory', 'using', 'homotopy', 'associative', 'algebra', 'a_infty', 'algebra', 'this', ... | [-0.1461796794038523, 0.06726369920090355, -0.13512486804292761, 0.10935490914612431, -0.12902691639189062, -0.17217225235373038, -0.023186952877259845, 0.29233563350361036, -0.29606777872761775, -0.2208791882249302, 0.06798142770200903, -0.19724456561279707, -0.26571131389285035, 0.09780847178450947, -0.21165528554662... |
707.0388 | From boundary to bulk in logarithmic CFT | The analogue of the charge-conjugation modular invariant for rational
logarithmic conformal field theories is constructed. This is done by
reconstructing the bulk spectrum from a simple boundary condition (the analogue
of the Cardy `identity brane'). We apply the general method to the c_1,p
triplet models and reprodu... | hep-th math.QA | the analogue of the chargeconjugation modular invariant for rational logarithmic conformal field theories is constructed this is done by reconstructing the bulk spectrum from a simple boundary condition the analogue of the cardy identity brane we apply the general method to the c_1p triplet models and reproduce the pre... | [['the', 'analogue', 'of', 'the', 'chargeconjugation', 'modular', 'invariant', 'for', 'rational', 'logarithmic', 'conformal', 'field', 'theories', 'is', 'constructed', 'this', 'is', 'done', 'by', 'reconstructing', 'the', 'bulk', 'spectrum', 'from', 'a', 'simple', 'boundary', 'condition', 'the', 'analogue', 'of', 'the',... | [-0.10553546539180118, 0.06907655471392597, -0.1238643547942586, 0.1369304723317597, -0.07052688885704372, -0.17580758120985357, 0.0034858179941592324, 0.285419469492303, -0.23871111040245052, -0.24132670441004275, 0.07148806172362701, -0.245284198395287, -0.17817808447560107, 0.1577444883770551, -0.044779559088594934,... |
707.0389 | A remark on fractional integrals on modulation spaces | In this paper, we give the necessary and sufficient conditions for the
boundedness of fractional integral operators on the modulation spaces.
| math.FA math.AP | in this paper we give the necessary and sufficient conditions for the boundedness of fractional integral operators on the modulation spaces | [['in', 'this', 'paper', 'we', 'give', 'the', 'necessary', 'and', 'sufficient', 'conditions', 'for', 'the', 'boundedness', 'of', 'fractional', 'integral', 'operators', 'on', 'the', 'modulation', 'spaces']] | [-0.182577144620674, 0.07532881701453811, -0.06871498861749258, 0.1511373634926886, -0.08223895214143254, -0.016598157584667206, 0.013458768587692507, 0.34679194078558967, -0.24578246882274038, -0.2167577523560751, 0.2410791978361972, -0.1515312193050271, -0.1826756125582116, 0.19648571367863388, -0.1750001517967099, 0... |
707.039 | The York Map and the Role of Non-Inertial Frames in the Geometrical View
of the Gravitational Field | The role of non-inertial frames in a class of models of general relativity is
clarified by means of Dirac's theory of constraints. The identification of a
York canonical basis allows to give the interpretation of the gauge variables
as generalized inertial effects and to identify the Dirac observables of the
gravitat... | gr-qc astro-ph hep-th | the role of noninertial frames in a class of models of general relativity is clarified by means of diracs theory of constraints the identification of a york canonical basis allows to give the interpretation of the gauge variables as generalized inertial effects and to identify the dirac observables of the gravitational... | [['the', 'role', 'of', 'noninertial', 'frames', 'in', 'a', 'class', 'of', 'models', 'of', 'general', 'relativity', 'is', 'clarified', 'by', 'means', 'of', 'diracs', 'theory', 'of', 'constraints', 'the', 'identification', 'of', 'a', 'york', 'canonical', 'basis', 'allows', 'to', 'give', 'the', 'interpretation', 'of', 'th... | [-0.20067943318621498, 0.18582579983374128, -0.1286971525277023, 0.09052798376031607, -0.13238227395219848, -0.12477057092133667, 0.015621223334259316, 0.2595789378460545, -0.23844958708754607, -0.3121468417539999, 0.007170583643079675, -0.1888382108823484, -0.1548528759982195, 0.15542315578015595, -0.06748685003681616... |
707.0391 | On the $L^2$-boundedness of pseudo-differential operators and their
commutators with symbols in $\alpha$-modulation spaces | In this paper, we consider the $L^2$-boundedness of pseudo-differential
operators with symbols in $\alpha$-modulation spaces.
| math.FA math.AP | in this paper we consider the l2boundedness of pseudodifferential operators with symbols in alphamodulation spaces | [['in', 'this', 'paper', 'we', 'consider', 'the', 'l2boundedness', 'of', 'pseudodifferential', 'operators', 'with', 'symbols', 'in', 'alphamodulation', 'spaces']] | [-0.19206200192372005, 0.11185690183192491, 0.02342751274506251, 0.12173541656229644, -0.06825353902143737, -0.029547986388206483, -0.037171876857367656, 0.352484297255675, -0.29926206966241203, -0.1189727688829104, 0.16129693961702288, -0.3124686983724435, -0.20392210111021997, 0.1225108399366339, -0.27052181474864484... |
707.0392 | Measurement of the Strong Coupling alpha_s from the Four-Jet Rate in
e+e- Annihilation using JADE data | Data from e+e- annihilation into hadrons collected by the JADE experiment at
centre-of-mass energies between 14 GeV and 44 GeV are used to study the
four-jet event production rate as a function of the Durham jet algorithm's
resolution parameter ycut. The four-jet rate is compared to QCD next-to-leading
order calculat... | hep-ex | data from ee annihilation into hadrons collected by the jade experiment at centreofmass energies between 14 gev and 44 gev are used to study the fourjet event production rate as a function of the durham jet algorithms resolution parameter ycut the fourjet rate is compared to qcd nexttoleading order calculations includi... | [['data', 'from', 'ee', 'annihilation', 'into', 'hadrons', 'collected', 'by', 'the', 'jade', 'experiment', 'at', 'centreofmass', 'energies', 'between', '14', 'gev', 'and', '44', 'gev', 'are', 'used', 'to', 'study', 'the', 'fourjet', 'event', 'production', 'rate', 'as', 'a', 'function', 'of', 'the', 'durham', 'jet', 'al... | [-0.06562865736583869, 0.1227817578924199, -0.10802661430711548, 0.1608227995938311, 0.014228764586150647, -0.05219544236237804, -0.009552203141696131, 0.34943525219957033, -0.16383030305927, -0.3436894870052735, -0.02342069459768633, -0.3983854705343644, 0.1183904404224207, 0.1681931229494512, 0.11589772794395685, 0.1... |
707.0393 | Supernovae in the Subaru Deep Field: An Initial Sample, and Type Ia
Rate, out to Redshift 1.6 | Large samples of high-redshift supernovae (SNe) are potentially powerful
probes of cosmic star formation, metal enrichment, and SN physics. We present
initial results from a new deep SN survey, based on re-imaging in the R, i', z'
bands, of the 0.25 deg2 Subaru Deep Field (SDF), with the 8.2-m Subaru
telescope and Su... | astro-ph | large samples of highredshift supernovae sne are potentially powerful probes of cosmic star formation metal enrichment and sn physics we present initial results from a new deep sn survey based on reimaging in the r i z bands of the 025 deg2 subaru deep field sdf with the 82m subaru telescope and suprimecam in a single ... | [['large', 'samples', 'of', 'highredshift', 'supernovae', 'sne', 'are', 'potentially', 'powerful', 'probes', 'of', 'cosmic', 'star', 'formation', 'metal', 'enrichment', 'and', 'sn', 'physics', 'we', 'present', 'initial', 'results', 'from', 'a', 'new', 'deep', 'sn', 'survey', 'based', 'on', 'reimaging', 'in', 'the', 'r'... | [-0.03431589209671634, 0.05037946211234373, -0.05674878080046599, 0.07512045741305927, -0.12256026464039003, -0.11092468119679032, 0.11407506931084696, 0.4364406620933824, -0.1256477374386472, -0.32276475691347273, 0.04957834181092497, -0.3342926040702089, 0.0035242585138046552, 0.22919970536091644, -0.0226440603952790... |
707.0394 | Identification of candidate regulatory sequences in mammalian 3' UTRs by
statistical analysis of oligonucleotide distributions | 3' untranslated regions (3' UTRs) contain binding sites for many regulatory
elements, and in particular for microRNAs (miRNAs). The importance of
miRNA-mediated post-transcriptional regulation has become increasingly clear in
the last few years.
We propose two complementary approaches to the statistical analysis of... | q-bio.GN | 3 untranslated regions 3 utrs contain binding sites for many regulatory elements and in particular for micrornas mirnas the importance of mirnamediated posttranscriptional regulation has become increasingly clear in the last few years we propose two complementary approaches to the statistical analysis of oligonucleotid... | [['3', 'untranslated', 'regions', '3', 'utrs', 'contain', 'binding', 'sites', 'for', 'many', 'regulatory', 'elements', 'and', 'in', 'particular', 'for', 'micrornas', 'mirnas', 'the', 'importance', 'of', 'mirnamediated', 'posttranscriptional', 'regulation', 'has', 'become', 'increasingly', 'clear', 'in', 'the', 'last', ... | [-0.10498768221228742, 0.08767508805400352, 0.020589612023188517, 0.09289474254921795, 0.008863887334099183, -0.1517609530218089, 0.06560819911806343, 0.39129139786013045, -0.19917413101043516, -0.3132802290591196, 0.04723256025552893, -0.29607007117010653, -0.16837457552677593, 0.20303404696572286, -0.0245686744769605... |
707.0395 | Warm molecular hydrogen in the Spitzer SINGS galaxy sample | (simplified) Results on the properties of warm H2 in 57 normal galaxies are
derived from H2 rotational transitions, obtained as part of SINGS. This study
extends previous extragalactic surveys of H2, the most abundant constituent of
the molecular ISM, to more common systems (L_FIR = e7 to 6e10 L_sun) of all
morpholog... | astro-ph | simplified results on the properties of warm h2 in 57 normal galaxies are derived from h2 rotational transitions obtained as part of sings this study extends previous extragalactic surveys of h2 the most abundant constituent of the molecular ism to more common systems l_fir e7 to 6e10 l_sun of all morphological and nuc... | [['simplified', 'results', 'on', 'the', 'properties', 'of', 'warm', 'h2', 'in', '57', 'normal', 'galaxies', 'are', 'derived', 'from', 'h2', 'rotational', 'transitions', 'obtained', 'as', 'part', 'of', 'sings', 'this', 'study', 'extends', 'previous', 'extragalactic', 'surveys', 'of', 'h2', 'the', 'most', 'abundant', 'co... | [-0.050199592246087645, 0.12259953106057761, 0.01994026753814723, 0.07407351999641333, 0.010306235731432968, -0.04683224090459106, 0.03294306973238354, 0.45029860243425524, -0.16254835652481814, -0.3136476943930097, 0.01948640738414557, -0.31449701518044626, 0.044738931333752084, 0.13156605245121894, -0.002757391063839... |
707.0396 | Finite volume QCD at fixed topological charge | In finite volume the partition function of QCD with a given $\theta$ is a sum
of different topological sectors with a weight primarily determined by the
topological susceptibility. If a physical observable is evaluated only in a
fixed topological sector, the result deviates from the true expectation value
by an amoun... | hep-lat hep-th | in finite volume the partition function of qcd with a given theta is a sum of different topological sectors with a weight primarily determined by the topological susceptibility if a physical observable is evaluated only in a fixed topological sector the result deviates from the true expectation value by an amount propo... | [['in', 'finite', 'volume', 'the', 'partition', 'function', 'of', 'qcd', 'with', 'a', 'given', 'theta', 'is', 'a', 'sum', 'of', 'different', 'topological', 'sectors', 'with', 'a', 'weight', 'primarily', 'determined', 'by', 'the', 'topological', 'susceptibility', 'if', 'a', 'physical', 'observable', 'is', 'evaluated', '... | [-0.1520516336205657, 0.1637448567922143, -0.10311430819867248, 0.05802551877396009, -0.05131512295230533, -0.08955862296365753, 0.1042380997263266, 0.28087038087175675, -0.2713256868333297, -0.2444821727565593, 0.0782271519408958, -0.3047995634239029, -0.1269694620191499, 0.11868014536944597, -0.017696483236822706, 0.... |
707.0397 | Robust Audio Watermarking Against the D/A and A/D conversions | Audio watermarking has played an important role in multimedia security. In
many applications using audio watermarking, D/A and A/D conversions (denoted by
DA/AD in this paper) are often involved. In previous works, however, the
robustness issue of audio watermarking against the DA/AD conversions has not
drawn suffici... | cs.CR cs.MM | audio watermarking has played an important role in multimedia security in many applications using audio watermarking da and ad conversions denoted by daad in this paper are often involved in previous works however the robustness issue of audio watermarking against the daad conversions has not drawn sufficient attention... | [['audio', 'watermarking', 'has', 'played', 'an', 'important', 'role', 'in', 'multimedia', 'security', 'in', 'many', 'applications', 'using', 'audio', 'watermarking', 'da', 'and', 'ad', 'conversions', 'denoted', 'by', 'daad', 'in', 'this', 'paper', 'are', 'often', 'involved', 'in', 'previous', 'works', 'however', 'the'... | [-0.1349736019339258, 0.04630461674241815, -0.0948856548041858, 0.053592322273614185, -0.07525771374722527, -0.15660783031670655, 0.013094556552883952, 0.4106074238528975, -0.2696694757963092, -0.29649633205848036, 0.1186704398935101, -0.26776077098652257, -0.18962368524966308, 0.1915614892501828, -0.1675930992782193, ... |
707.0398 | Exchange effects on electron scattering through a quantum dot embedded
in a two-dimensional semiconductor structure | We have developed a theoretical method to study scattering processes of an
incident electron through an N-electron quantum dot (QD) embedded in a
two-dimensional (2D) semiconductor. The generalized Lippmann-Schwinger
equations including the electron-electron exchange interaction in this system
are solved for the cont... | cond-mat.other | we have developed a theoretical method to study scattering processes of an incident electron through an nelectron quantum dot qd embedded in a twodimensional 2d semiconductor the generalized lippmannschwinger equations including the electronelectron exchange interaction in this system are solved for the continuum elect... | [['we', 'have', 'developed', 'a', 'theoretical', 'method', 'to', 'study', 'scattering', 'processes', 'of', 'an', 'incident', 'electron', 'through', 'an', 'nelectron', 'quantum', 'dot', 'qd', 'embedded', 'in', 'a', 'twodimensional', '2d', 'semiconductor', 'the', 'generalized', 'lippmannschwinger', 'equations', 'includin... | [-0.0886089220099772, 0.14396591078087415, -0.05375701550122661, 0.08252636865557482, 0.04687042803658793, -0.13498115350181858, -0.004442535878236716, 0.4028403365984559, -0.25966975548071786, -0.263277704101832, -0.020300142387471472, -0.3456889973099654, -0.10774413554948599, 0.2171983073465526, 0.1218260296387598, ... |
707.0399 | Low-lying ud anti-s anti-s configurations in a non-relativistic
constituent quark model | The energies of the low-lying isoscalar and isovector ud anti-s anti-s
configurations with spin-parity J^P=0^+, 1^+, and 2^+ are calculated in a
non-relativistic constituent quark model by use of the variational method. The
contributions of various parts of the quark-quark interacting potentials
including the s-chann... | nucl-th | the energies of the lowlying isoscalar and isovector ud antis antis configurations with spinparity jp0 1 and 2 are calculated in a nonrelativistic constituent quark model by use of the variational method the contributions of various parts of the quarkquark interacting potentials including the schannel interaction are i... | [['the', 'energies', 'of', 'the', 'lowlying', 'isoscalar', 'and', 'isovector', 'ud', 'antis', 'antis', 'configurations', 'with', 'spinparity', 'jp0', '1', 'and', '2', 'are', 'calculated', 'in', 'a', 'nonrelativistic', 'constituent', 'quark', 'model', 'by', 'use', 'of', 'the', 'variational', 'method', 'the', 'contributi... | [-0.10712475064678288, 0.2502209460083192, -0.07353721285344601, 0.11231207013471808, -0.03120901191497311, -0.13112716222645543, 0.0481398307858645, 0.3444895339584767, -0.192326095156518, -0.28585345681968216, -0.003701799013346889, -0.29712533807853747, -0.028656744042321974, 0.11415360930810914, 0.10127059833500453... |
707.04 | Singular Hecke algebras, Markov traces, and HOMFLY-type invariants | We define the singular Hecke algebra ${\mathcal H} (SB_n)$ as the quotient of
the singular braid monoid algebra ${\mathbb C} (q) [SB_n]$ by the Hecke
relations $\sigma_k^2 = (q-1) \sigma_k +q$, $1 \le k\le n-1$, and define the
Markov traces on the sequence $\{{\mathcal H}(SB_n)\}_{n=1}^{+\infty}$ in the
same way as f... | math.GT math.RT | we define the singular hecke algebra mathcal h sb_n as the quotient of the singular braid monoid algebra mathbb c q sb_n by the hecke relations sigma_k2 q1 sigma_k q 1 le kle n1 and define the markov traces on the sequence mathcal hsb_n_n1infty in the same way as for the markov traces on the tower of nonsingular hecke ... | [['we', 'define', 'the', 'singular', 'hecke', 'algebra', 'mathcal', 'h', 'sb_n', 'as', 'the', 'quotient', 'of', 'the', 'singular', 'braid', 'monoid', 'algebra', 'mathbb', 'c', 'q', 'sb_n', 'by', 'the', 'hecke', 'relations', 'sigma_k2', 'q1', 'sigma_k', 'q', '1', 'le', 'kle', 'n1', 'and', 'define', 'the', 'markov', 'tra... | [-0.19021483889270213, 0.11298051453031216, -0.08847416697197684, 0.07791161310629949, -0.09541261972363797, -0.1514580007567401, -0.04506675672112784, 0.326076855034297, -0.3774930221899863, -0.18769396560627125, 0.09326533762636714, -0.27028326220968135, -0.1450098011365856, 0.1593176607312935, -0.11345353407875425, ... |
707.0401 | J.S. Bell's Concept of Local Causality | John Stewart Bell's famous 1964 theorem is widely regarded as one of the most
important developments in the foundations of physics. It has even been
described as "the most profound discovery of science." Yet even as we approach
the 50th anniversary of Bell's discovery, its meaning and implications remain
controversia... | quant-ph | john stewart bells famous 1964 theorem is widely regarded as one of the most important developments in the foundations of physics it has even been described as the most profound discovery of science yet even as we approach the 50th anniversary of bells discovery its meaning and implications remain controversial many te... | [['john', 'stewart', 'bells', 'famous', '1964', 'theorem', 'is', 'widely', 'regarded', 'as', 'one', 'of', 'the', 'most', 'important', 'developments', 'in', 'the', 'foundations', 'of', 'physics', 'it', 'has', 'even', 'been', 'described', 'as', 'the', 'most', 'profound', 'discovery', 'of', 'science', 'yet', 'even', 'as',... | [-0.04903355585978836, 0.06200224159193785, -0.17273126289725674, 0.15675179982434742, -0.1514552933854736, -0.18940329483868015, 0.04272274155899005, 0.26064223014510984, -0.232555440547033, -0.33770267490667005, 0.0802652394862784, -0.24562970152286398, -0.16577457027771503, 0.1925262507938295, -0.16222914316968545, ... |
707.0402 | The maximum output p-norm of quantum channels is not multiplicative for
any p>2 | We prove the claim made in the title by showing that approximately
randomising maps of large dimension are counterexamples to the multiplicativity
conjecture.
| quant-ph | we prove the claim made in the title by showing that approximately randomising maps of large dimension are counterexamples to the multiplicativity conjecture | [['we', 'prove', 'the', 'claim', 'made', 'in', 'the', 'title', 'by', 'showing', 'that', 'approximately', 'randomising', 'maps', 'of', 'large', 'dimension', 'are', 'counterexamples', 'to', 'the', 'multiplicativity', 'conjecture']] | [-0.1523178248468827, 0.06944231280004201, -0.04229945693489002, 0.10383623133858909, -0.0007814537207393543, -0.1240308721266363, 0.016015583649277687, 0.3432711672199809, -0.3100224568144135, -0.2725058020618947, 0.09147243249817225, -0.30012227205114195, -0.17274468047949282, 0.19457712139853317, -0.1550702414596858... |
707.0403 | Dynamical control of matter-wave tunneling in periodic potentials | We report on measurements of dynamical suppression of inter-well tunneling of
a Bose-Einstein condensate (BEC) in a strongly driven optical lattice. The
strong driving is a sinusoidal shaking of the lattice corresponding to a
time-varying linear potential, and the tunneling is measured by letting the BEC
freely expan... | cond-mat.other quant-ph | we report on measurements of dynamical suppression of interwell tunneling of a boseeinstein condensate bec in a strongly driven optical lattice the strong driving is a sinusoidal shaking of the lattice corresponding to a timevarying linear potential and the tunneling is measured by letting the bec freely expand in the ... | [['we', 'report', 'on', 'measurements', 'of', 'dynamical', 'suppression', 'of', 'interwell', 'tunneling', 'of', 'a', 'boseeinstein', 'condensate', 'bec', 'in', 'a', 'strongly', 'driven', 'optical', 'lattice', 'the', 'strong', 'driving', 'is', 'a', 'sinusoidal', 'shaking', 'of', 'the', 'lattice', 'corresponding', 'to', ... | [-0.19533364164882003, 0.26950642418639686, -0.061189244715579315, -0.0083585566299168, -0.010187928799737608, -0.14969617441251248, 0.10614543120310832, 0.3630029834328895, -0.258229508592162, -0.2347311916332527, 0.042944142722681294, -0.25408596483232304, -0.10233571255925746, 0.21917973619069805, 0.0329388569447055... |
707.0404 | Search for Direc Magnetic Monopoles in e+e- Collisions with the OPAL
Detector at LEP2 | This letter describes a direct search for pair produced magnetic monopoles in
e+e- collisions. The analysis is based on 62.7 pb^-1 of data collected with the
OPAL detector at an average centre-of-mass energy of sqrt(s)= 206.3GeV. The
monopole signal was assumed to be characterized by two back-to-back particles
with a... | hep-ex | this letter describes a direct search for pair produced magnetic monopoles in ee collisions the analysis is based on 627 pb1 of data collected with the opal detector at an average centreofmass energy of sqrts 2063gev the monopole signal was assumed to be characterized by two backtoback particles with an anomalously hig... | [['this', 'letter', 'describes', 'a', 'direct', 'search', 'for', 'pair', 'produced', 'magnetic', 'monopoles', 'in', 'ee', 'collisions', 'the', 'analysis', 'is', 'based', 'on', '627', 'pb1', 'of', 'data', 'collected', 'with', 'the', 'opal', 'detector', 'at', 'an', 'average', 'centreofmass', 'energy', 'of', 'sqrts', '206... | [-0.13304797761962137, 0.21960924925808953, -0.034942765823668905, 0.11392261985386921, -0.0002885873481217358, -0.05625983618167985, 0.022553067477260772, 0.34394144375896096, -0.11570994334263551, -0.3992794432506188, -0.007906034070417348, -0.37281808128946614, 0.09288992954051903, 0.174055633884377, 0.0676993675386... |
707.0405 | Casimir-Polder intermolecular forces in minimal length theories | Generalized uncertainty relations are known to provide a minimal length
$\hbar\sqrt{\beta}$. The effect of such minimal length in the Casimir-Polder
interactions between neutral atoms (molecules) is studied. The first order
correction term in the minimal uncertainty parameter is derived and found to
describe an attra... | hep-th hep-ph | generalized uncertainty relations are known to provide a minimal length hbarsqrtbeta the effect of such minimal length in the casimirpolder interactions between neutral atoms molecules is studied the first order correction term in the minimal uncertainty parameter is derived and found to describe an attractive potentia... | [['generalized', 'uncertainty', 'relations', 'are', 'known', 'to', 'provide', 'a', 'minimal', 'length', 'hbarsqrtbeta', 'the', 'effect', 'of', 'such', 'minimal', 'length', 'in', 'the', 'casimirpolder', 'interactions', 'between', 'neutral', 'atoms', 'molecules', 'is', 'studied', 'the', 'first', 'order', 'correction', 't... | [-0.14529796445276588, 0.12279497753891823, 0.012157081613743988, 0.1717725395108573, -0.0502128759243836, -0.13337220676088085, -0.002056473237462342, 0.32083867744077, -0.29837872778686386, -0.318869966113319, 0.025068214035127313, -0.3122632105524341, -0.1169687279034406, 0.16372086651002368, -0.007806766227198144, ... |
707.0406 | On the onset of runaway stellar collisions in dense star clusters I.
Dynamics of the first collision | We study the circumstances under which first collisions occur in young and
dense star clusters. The initial conditions for our direct $N$-body simulations
are chosen such that the clusters experience core collapse within a few million
years, before the most massive stars have left the main-sequence. It turns out
that... | astro-ph | we study the circumstances under which first collisions occur in young and dense star clusters the initial conditions for our direct nbody simulations are chosen such that the clusters experience core collapse within a few million years before the most massive stars have left the mainsequence it turns out that the firs... | [['we', 'study', 'the', 'circumstances', 'under', 'which', 'first', 'collisions', 'occur', 'in', 'young', 'and', 'dense', 'star', 'clusters', 'the', 'initial', 'conditions', 'for', 'our', 'direct', 'nbody', 'simulations', 'are', 'chosen', 'such', 'that', 'the', 'clusters', 'experience', 'core', 'collapse', 'within', 'a... | [-0.1180673229628829, 0.16824819958182397, -0.08614277211592797, 0.07053137246956244, -0.07877499904385825, -0.0306525579143465, 0.05349592022298847, 0.3528118915280994, -0.22153479852110008, -0.31772275068394745, 0.04841344258000637, -0.3014176567171321, -0.06773791972685743, 0.17841012874347975, 0.006683231028153297,... |
707.0407 | Stellar Population Gradients in Bulges along the Hubble Sequence: I. The
Data | This is the first paper presenting our long-term project aimed at studying
the nature of bulges through the analysis of their stellar population
gradients. We present deep spectroscopic observations along the minor axis and
the data reduction for a sample of 32 bulges of edge-on spiral galaxies. We
explain in detail ... | astro-ph | this is the first paper presenting our longterm project aimed at studying the nature of bulges through the analysis of their stellar population gradients we present deep spectroscopic observations along the minor axis and the data reduction for a sample of 32 bulges of edgeon spiral galaxies we explain in detail our pr... | [['this', 'is', 'the', 'first', 'paper', 'presenting', 'our', 'longterm', 'project', 'aimed', 'at', 'studying', 'the', 'nature', 'of', 'bulges', 'through', 'the', 'analysis', 'of', 'their', 'stellar', 'population', 'gradients', 'we', 'present', 'deep', 'spectroscopic', 'observations', 'along', 'the', 'minor', 'axis', '... | [-0.09235319649199332, 0.03193152871158883, -0.11035442918421716, 0.07981946394415793, -0.06633582104760127, -0.03050074011087876, 0.03882137072954591, 0.41812779924531623, -0.19613524044563216, -0.35895866780417174, 0.08262994624105993, -0.2759810896282356, -0.06632372126850394, 0.21300654587662213, -0.039911706660558... |
707.0408 | Disk-Evaporation Fed Corona: Structure and Evaporation Feature with
Magnetic Field | The disk-corona evaporation model naturally interprets many observational
phenomena in black hole X-ray binaries, such as the truncation of an accretion
disk and the spectral state transitions. On the other hand, magnetic field is
known to play an important role in transporting angular momentum and producing
viscosit... | astro-ph | the diskcorona evaporation model naturally interprets many observational phenomena in black hole xray binaries such as the truncation of an accretion disk and the spectral state transitions on the other hand magnetic field is known to play an important role in transporting angular momentum and producing viscosity in ac... | [['the', 'diskcorona', 'evaporation', 'model', 'naturally', 'interprets', 'many', 'observational', 'phenomena', 'in', 'black', 'hole', 'xray', 'binaries', 'such', 'as', 'the', 'truncation', 'of', 'an', 'accretion', 'disk', 'and', 'the', 'spectral', 'state', 'transitions', 'on', 'the', 'other', 'hand', 'magnetic', 'fiel... | [-0.10271346824608364, 0.18798432814483262, -0.011483984448188768, 0.12345354918099989, -0.054496699604164575, -0.08376945402118814, 0.02891419751598475, 0.3810131816426292, -0.2382212850941032, -0.34448100518501173, 0.09592641404607391, -0.28422458990233895, -0.021873718587088243, 0.2150481500883331, -0.01224964486117... |
707.0409 | On conformal Killing-Yano tensors for Plebanski-Demianski family of
solutions | We present the explicit expressions for the conformal Killing-Yano tensors
for the Plebanski-Demianski family of type D solutions in four dimensions. Some
physically important special cases are discussed in more detail. In particular,
it is demonstrated how the conformal Killing-Yano tensor becomes the
Killing-Yano t... | gr-qc hep-th | we present the explicit expressions for the conformal killingyano tensors for the plebanskidemianski family of type d solutions in four dimensions some physically important special cases are discussed in more detail in particular it is demonstrated how the conformal killingyano tensor becomes the killingyano tensor for... | [['we', 'present', 'the', 'explicit', 'expressions', 'for', 'the', 'conformal', 'killingyano', 'tensors', 'for', 'the', 'plebanskidemianski', 'family', 'of', 'type', 'd', 'solutions', 'in', 'four', 'dimensions', 'some', 'physically', 'important', 'special', 'cases', 'are', 'discussed', 'in', 'more', 'detail', 'in', 'pa... | [-0.14884638420520716, 0.12838063300267666, 0.0010418753395331842, 0.09030391784001361, -0.08596220238170788, -0.16849009808627705, -0.10908147456425735, 0.3560724717510097, -0.16392676721728755, -0.19357649196742796, 0.1229808705142133, -0.2652597908619974, -0.19560985077245563, 0.16110259160518134, -0.017710050252978... |
707.041 | On gas drag in a circular binary system | We investigate both analytically and numerically the motion of massless
particles orbiting primary star in a close circular binary system with
particular focus on the gas drag effects. These are the first calculations with
particles ranging in size from 1m to 10km, which account for the presence of a
tidally perturbe... | astro-ph | we investigate both analytically and numerically the motion of massless particles orbiting primary star in a close circular binary system with particular focus on the gas drag effects these are the first calculations with particles ranging in size from 1m to 10km which account for the presence of a tidally perturbed ga... | [['we', 'investigate', 'both', 'analytically', 'and', 'numerically', 'the', 'motion', 'of', 'massless', 'particles', 'orbiting', 'primary', 'star', 'in', 'a', 'close', 'circular', 'binary', 'system', 'with', 'particular', 'focus', 'on', 'the', 'gas', 'drag', 'effects', 'these', 'are', 'the', 'first', 'calculations', 'w... | [-0.1307210144986761, 0.16154551111413423, -0.07375851836062626, 0.04521458119443682, -0.030675532950358537, -0.05269856407140019, -0.01792743567507074, 0.3561879412594557, -0.21277473275220904, -0.311216113667665, 0.07063074303632744, -0.2638184570557196, -0.08401788642829042, 0.175795859423953, -0.013662978094995363,... |
707.0411 | Interference pattern of a long diffusive Josephson junction | We calculate the modulation by a magnetic field of the critical current of a
long disordered Josephson junction in the diffusive limit, i.e. when the
dimensions of the junction are larger that the elastic mean free path, and when
the length $L$ is much larger than the width $w$. Due to the averaging of the
gauge inva... | cond-mat.mes-hall | we calculate the modulation by a magnetic field of the critical current of a long disordered josephson junction in the diffusive limit ie when the dimensions of the junction are larger that the elastic mean free path and when the length l is much larger than the width w due to the averaging of the gauge invariant phase... | [['we', 'calculate', 'the', 'modulation', 'by', 'a', 'magnetic', 'field', 'of', 'the', 'critical', 'current', 'of', 'a', 'long', 'disordered', 'josephson', 'junction', 'in', 'the', 'diffusive', 'limit', 'ie', 'when', 'the', 'dimensions', 'of', 'the', 'junction', 'are', 'larger', 'that', 'the', 'elastic', 'mean', 'free'... | [-0.17550016095576523, 0.2347866718068421, -0.06818379693756904, 0.07638930977292795, -0.014390436278001682, -0.1313133770138495, 0.017119150954877604, 0.3345668539404869, -0.3025244354933232, -0.2639209346443012, 0.037329298662239906, -0.28047290929333046, -0.12019594628909216, 0.19631131260177573, 0.02724074024228832... |
707.0412 | Solution of non-singlet DGLAP evolution equation in leading order and
next-to-leading order at small-x by method of characteristics | The non-singlet structure functions have been obtained by solving
Dokshitzer-Gribov-Lipatov-Altarelli-Parisi (DGLAP) evolution equations in
leading order (LO) and next-to-leading order (NLO) at the small-x limit. Here a
Taylor series expansion has been used and then the method of characteristics
has been applied to s... | hep-ph | the nonsinglet structure functions have been obtained by solving dokshitzergribovlipatovaltarelliparisi dglap evolution equations in leading order lo and nexttoleading order nlo at the smallx limit here a taylor series expansion has been used and then the method of characteristics has been applied to solve the evolutio... | [['the', 'nonsinglet', 'structure', 'functions', 'have', 'been', 'obtained', 'by', 'solving', 'dokshitzergribovlipatovaltarelliparisi', 'dglap', 'evolution', 'equations', 'in', 'leading', 'order', 'lo', 'and', 'nexttoleading', 'order', 'nlo', 'at', 'the', 'smallx', 'limit', 'here', 'a', 'taylor', 'series', 'expansion',... | [-0.03229569039139591, 0.06822811864835561, -0.20131533596756274, 0.09275379674661843, -0.09968762104323164, -0.01488089325578242, -0.08899003578746906, 0.3388250484970994, -0.1628994643688202, -0.2840800927341229, 0.09867877679396055, -0.35997050625012544, -0.03159633825426219, 0.12949710565268016, 0.10919644723295188... |
707.0413 | Detuned Twin-Signal-Recycling for ultra-high precision interferometers | We propose a new interferometer technique for high precision phase
measurements such as those in gravitational wave detection. The technique
utilizes a pair of optically coupled resonators that provides identical
resonance conditions for the upper as well the lower phase modulation signal
sidebands. This symmetry sig... | quant-ph | we propose a new interferometer technique for high precision phase measurements such as those in gravitational wave detection the technique utilizes a pair of optically coupled resonators that provides identical resonance conditions for the upper as well the lower phase modulation signal sidebands this symmetry signifi... | [['we', 'propose', 'a', 'new', 'interferometer', 'technique', 'for', 'high', 'precision', 'phase', 'measurements', 'such', 'as', 'those', 'in', 'gravitational', 'wave', 'detection', 'the', 'technique', 'utilizes', 'a', 'pair', 'of', 'optically', 'coupled', 'resonators', 'that', 'provides', 'identical', 'resonance', 'co... | [-0.18689011133392341, 0.19157036140095443, -0.05279355427483097, 0.037153445398143956, -0.05228333492996171, -0.14553607392299456, 0.06317792733898386, 0.38163951609749347, -0.19139740005484782, -0.31965906978584824, 0.07077945250202902, -0.2489461019751616, -0.12061307784169913, 0.25145451436983424, 0.003629243711475... |
707.0414 | A computation of Poisson kernels for some standard weighted biharmonic
operators in the unit disc | We compute Poisson kernels for integer weight parameter standard weighted
biharmonic operators in the unit disc with Dirichlet boundary conditions. The
computations performed extend the supply of explicit examples of such kernels
and suggest similar formulas for these Poisson kernels to hold true in more
generality. ... | math.AP math.CA | we compute poisson kernels for integer weight parameter standard weighted biharmonic operators in the unit disc with dirichlet boundary conditions the computations performed extend the supply of explicit examples of such kernels and suggest similar formulas for these poisson kernels to hold true in more generality comp... | [['we', 'compute', 'poisson', 'kernels', 'for', 'integer', 'weight', 'parameter', 'standard', 'weighted', 'biharmonic', 'operators', 'in', 'the', 'unit', 'disc', 'with', 'dirichlet', 'boundary', 'conditions', 'the', 'computations', 'performed', 'extend', 'the', 'supply', 'of', 'explicit', 'examples', 'of', 'such', 'ker... | [-0.08414496185250138, -0.005909933882244563, -0.04479862239716922, 0.12393423384134421, -0.11539081195211512, -0.16771862045782854, 0.019965545779441374, 0.4342154398307962, -0.2719911898691523, -0.2330177703998604, 0.15169913266880153, -0.24029943355659056, -0.11567594783412198, 0.2507188396717785, -0.046360108794958... |
707.0415 | Surface Encapsulation for Low-Loss Silicon Photonics | Encapsulation layers are explored for passivating the surfaces of silicon to
reduce optical absorption in the 1500-nm wavelength band. Surface-sensitive
test structures consisting of microdisk resonators are fabricated for this
purpose. Based on previous work in silicon photovoltaics, coatings of SiNx and
SiO2 are ap... | physics.optics | encapsulation layers are explored for passivating the surfaces of silicon to reduce optical absorption in the 1500nm wavelength band surfacesensitive test structures consisting of microdisk resonators are fabricated for this purpose based on previous work in silicon photovoltaics coatings of sinx and sio2 are applied u... | [['encapsulation', 'layers', 'are', 'explored', 'for', 'passivating', 'the', 'surfaces', 'of', 'silicon', 'to', 'reduce', 'optical', 'absorption', 'in', 'the', '1500nm', 'wavelength', 'band', 'surfacesensitive', 'test', 'structures', 'consisting', 'of', 'microdisk', 'resonators', 'are', 'fabricated', 'for', 'this', 'pu... | [-0.08595270552786485, 0.1601530022691099, -0.01716389044363774, -0.07113507953923842, 0.04387237318097709, -0.20327051289911782, 0.05266411134697573, 0.5133539360700822, -0.23779505658633437, -0.31530584074314494, 0.07872261347401203, -0.28388941557887865, -0.0832494677101471, 0.20176323692371345, -0.05609009573616239... |
707.0416 | Relationship between non-exponentiality of relaxation and relaxation
time at the glass transition | By analyzing the experimental data for various glass-forming liquids and
polymers, we find that non-exponentiality $\beta$ and the relaxation time
$\tau$ are uniquely related: $\log(\tau)$ is an approximately linear function
of $1/\beta$, followed by a crossover to a higher linear slope. We rationalize
the observed r... | cond-mat.dis-nn cond-mat.soft | by analyzing the experimental data for various glassforming liquids and polymers we find that nonexponentiality beta and the relaxation time tau are uniquely related logtau is an approximately linear function of 1beta followed by a crossover to a higher linear slope we rationalize the observed relationship using a rece... | [['by', 'analyzing', 'the', 'experimental', 'data', 'for', 'various', 'glassforming', 'liquids', 'and', 'polymers', 'we', 'find', 'that', 'nonexponentiality', 'beta', 'and', 'the', 'relaxation', 'time', 'tau', 'are', 'uniquely', 'related', 'logtau', 'is', 'an', 'approximately', 'linear', 'function', 'of', '1beta', 'fol... | [-0.06955323431802053, 0.1801284428168751, -0.10309196012811019, 0.050324930232734634, -0.019958902809482353, -0.163918897545395, 0.026886797975748777, 0.3548455825791909, -0.3192047445246807, -0.26500677758684527, 0.10316005235788628, -0.2831527716121994, -0.20426921646755475, 0.14964219082433444, 0.04457153080461117,... |
707.0417 | Efficient identification of exoplanetary transit candidates from
SuperWASP light curves | Transiting extrasolar planets constitute only a small fraction of the range
of stellar systems found to display periodic, shallow dimmings in wide-field
surveys employing small-aperture camera arrays. Here we present an efficient
selection strategy for follow-up observations, derived from analysis of the
light curves... | astro-ph | transiting extrasolar planets constitute only a small fraction of the range of stellar systems found to display periodic shallow dimmings in widefield surveys employing smallaperture camera arrays here we present an efficient selection strategy for followup observations derived from analysis of the light curves of a sa... | [['transiting', 'extrasolar', 'planets', 'constitute', 'only', 'a', 'small', 'fraction', 'of', 'the', 'range', 'of', 'stellar', 'systems', 'found', 'to', 'display', 'periodic', 'shallow', 'dimmings', 'in', 'widefield', 'surveys', 'employing', 'smallaperture', 'camera', 'arrays', 'here', 'we', 'present', 'an', 'efficien... | [-0.06036216779543074, 0.09723510219376758, -0.10654838773291231, 0.10544849089510216, -0.1377590394715713, -0.1225899310063636, 0.12407742048411532, 0.3953726311916845, -0.13507354191301202, -0.3860008175885141, 0.1005266672306645, -0.30450832227909, -0.09528019986311465, 0.23558471350968416, -0.08699173913721511, 0.0... |
707.0418 | Random matrices beyond the Cartan classification | It is known that hermitean random matrix ensembles can be identified with
symmetric coset spaces of Lie groups, or else with tangent spaces of the same.
This results in a classification of random matrix ensembles as well as
applications in practical calculations of physical observables. In this paper
we show that a l... | math-ph cond-mat.mes-hall hep-ph hep-th math.MP | it is known that hermitean random matrix ensembles can be identified with symmetric coset spaces of lie groups or else with tangent spaces of the same this results in a classification of random matrix ensembles as well as applications in practical calculations of physical observables in this paper we show that a large ... | [['it', 'is', 'known', 'that', 'hermitean', 'random', 'matrix', 'ensembles', 'can', 'be', 'identified', 'with', 'symmetric', 'coset', 'spaces', 'of', 'lie', 'groups', 'or', 'else', 'with', 'tangent', 'spaces', 'of', 'the', 'same', 'this', 'results', 'in', 'a', 'classification', 'of', 'random', 'matrix', 'ensembles', 'a... | [-0.13842832550163503, 0.20332398571232604, -0.024176098683012136, 0.056873947870411466, -0.033941905245360365, -0.13216482370120028, -0.03311124831974587, 0.4161947578785644, -0.2564250788334217, -0.24164132645650618, 0.11813431010544435, -0.22381520905511695, -0.18718427054557032, 0.10343115852531586, -0.055294668511... |
707.0419 | Radiative and semileptonic decays in Chiral Perturbation Theory | I give a short overview of what has been done in radiative and semileptonic
Kaon decays in Chiral Perturbation Theory. This includes for semileptonic
decays the work which has been done to order $p^6$ including preliminary
results of isospin breaking to that order in $K_{\ell3}$. For the radiative
decays I mainly pre... | hep-ph | i give a short overview of what has been done in radiative and semileptonic kaon decays in chiral perturbation theory this includes for semileptonic decays the work which has been done to order p6 including preliminary results of isospin breaking to that order in k_ell3 for the radiative decays i mainly present some re... | [['i', 'give', 'a', 'short', 'overview', 'of', 'what', 'has', 'been', 'done', 'in', 'radiative', 'and', 'semileptonic', 'kaon', 'decays', 'in', 'chiral', 'perturbation', 'theory', 'this', 'includes', 'for', 'semileptonic', 'decays', 'the', 'work', 'which', 'has', 'been', 'done', 'to', 'order', 'p6', 'including', 'preli... | [-0.04134767352009256, 0.18522286301093369, -0.05069370378322642, 0.06217422590647214, -0.1005556620657444, -0.10864591995928564, 0.018563654378120756, 0.31027562304496253, -0.14968254723875174, -0.2070071049805345, 0.03612867076600228, -0.3384592430344943, -0.06561895447044537, 0.1264730436920092, 0.04489506378063354,... |
707.042 | Entropy of Extremal Black Holes in Two Dimension | In this paper we apply the entropy function formalism to the two-dimensional
black hole which come from the compactification of the heterotic string theory
with the dilaton coupling function. We find the Bekenstein-Hawking entropy from
the value of the entropy function at its saddle point. Also we consider higher
der... | hep-th | in this paper we apply the entropy function formalism to the twodimensional black hole which come from the compactification of the heterotic string theory with the dilaton coupling function we find the bekensteinhawking entropy from the value of the entropy function at its saddle point also we consider higher derivativ... | [['in', 'this', 'paper', 'we', 'apply', 'the', 'entropy', 'function', 'formalism', 'to', 'the', 'twodimensional', 'black', 'hole', 'which', 'come', 'from', 'the', 'compactification', 'of', 'the', 'heterotic', 'string', 'theory', 'with', 'the', 'dilaton', 'coupling', 'function', 'we', 'find', 'the', 'bekensteinhawking',... | [-0.08562888146529125, 0.0775312461286179, -0.10062458421374243, 0.1033648034853458, -0.03781169471079232, -0.12053293250878719, 0.07147880772606947, 0.24731227791415075, -0.26989727002895764, -0.23448655504821422, 0.02623429151749037, -0.33543958930248347, -0.19040182456877586, 0.11275365802056685, -0.0685364163757578... |
707.0421 | The $k$-anonymity Problem is Hard | The problem of publishing personal data without giving up privacy is becoming
increasingly important. An interesting formalization recently proposed is the
k-anonymity. This approach requires that the rows in a table are clustered in
sets of size at least k and that all the rows in a cluster become the same
tuple, af... | cs.DB cs.CC cs.DS | the problem of publishing personal data without giving up privacy is becoming increasingly important an interesting formalization recently proposed is the kanonymity this approach requires that the rows in a table are clustered in sets of size at least k and that all the rows in a cluster become the same tuple after th... | [['the', 'problem', 'of', 'publishing', 'personal', 'data', 'without', 'giving', 'up', 'privacy', 'is', 'becoming', 'increasingly', 'important', 'an', 'interesting', 'formalization', 'recently', 'proposed', 'is', 'the', 'kanonymity', 'this', 'approach', 'requires', 'that', 'the', 'rows', 'in', 'a', 'table', 'are', 'clu... | [-0.15166948739811473, 0.12481822748448299, -0.01776708831005779, 0.05270726180031871, -0.07110018327244018, -0.15051410441580965, 0.08345954174154413, 0.3617426383149761, -0.29110158200905734, -0.33618222948739696, 0.13891305432958975, -0.3269508262226162, -0.11845041295562528, 0.18020374271988035, -0.0723129885859395... |
707.0422 | Dimerization process and elementary excitations in spin-Peierls chains
coupled by frustrated interactions | We consider the ground state and the elementary excitations of an array of
spin-Peierls chains coupled by elastic and magnetic interactions. It is
expected that the effect of the magnetic interchain coupling will be to reduce
the dimerization amplitude and that of the elastic coupling will be to confine
the spin one-... | cond-mat.str-el | we consider the ground state and the elementary excitations of an array of spinpeierls chains coupled by elastic and magnetic interactions it is expected that the effect of the magnetic interchain coupling will be to reduce the dimerization amplitude and that of the elastic coupling will be to confine the spin onehalf ... | [['we', 'consider', 'the', 'ground', 'state', 'and', 'the', 'elementary', 'excitations', 'of', 'an', 'array', 'of', 'spinpeierls', 'chains', 'coupled', 'by', 'elastic', 'and', 'magnetic', 'interactions', 'it', 'is', 'expected', 'that', 'the', 'effect', 'of', 'the', 'magnetic', 'interchain', 'coupling', 'will', 'be', 't... | [-0.2264055376044578, 0.24441483451470655, -9.820275235041562e-05, 0.08762429842738331, -0.07835292522536798, -0.11954823612338966, 0.026464243688517148, 0.40258519909758533, -0.2779449588774393, -0.25067703988817003, 0.05028889803797938, -0.30763143305003826, -0.12320418023672472, 0.1383407293646289, 0.113025511516672... |
707.0423 | Inverse bremsstrahlung contributions to Drell-Yan like processes | The contribution of the sub-process $\gamma q \to q' l_1\bar{l}_2$ in
hadron-hadron interactions is considered. It is a part of one-loop electroweak
radiative corrections for the Drell-Yan production of lepton pairs at hadron
colliders. It is shown that this contribution should be taken into account
aiming at the 1% ... | hep-ph | the contribution of the subprocess gamma q to q l_1barl_2 in hadronhadron interactions is considered it is a part of oneloop electroweak radiative corrections for the drellyan production of lepton pairs at hadron colliders it is shown that this contribution should be taken into account aiming at the 1 accuracy of the d... | [['the', 'contribution', 'of', 'the', 'subprocess', 'gamma', 'q', 'to', 'q', 'l_1barl_2', 'in', 'hadronhadron', 'interactions', 'is', 'considered', 'it', 'is', 'a', 'part', 'of', 'oneloop', 'electroweak', 'radiative', 'corrections', 'for', 'the', 'drellyan', 'production', 'of', 'lepton', 'pairs', 'at', 'hadron', 'colli... | [-0.07481261168927508, 0.18784214244727548, -0.08246830814735133, 0.17735007330488647, -0.003987405722885317, -0.12191328705238128, -0.04810228664427996, 0.3425428558996803, -0.20036472390229637, -0.20349880041101495, -0.016405719201823044, -0.35221623349934816, 0.019196374669066957, 0.164778160787112, 0.11236207122990... |
707.0424 | AdS/CFT for Four-Point Amplitudes involving Gravitino Exchange | In this paper we compute the tree-level four-point scattering amplitude of
two dilatini and two axion-dilaton fields in type IIB supergravity in AdS5 x
S5. A special feature of this process is that there is an "exotic" channel in
which there are no singleparticle poles. Another novelty is that this process
involves t... | hep-th | in this paper we compute the treelevel fourpoint scattering amplitude of two dilatini and two axiondilaton fields in type iib supergravity in ads5 x s5 a special feature of this process is that there is an exotic channel in which there are no singleparticle poles another novelty is that this process involves the exchan... | [['in', 'this', 'paper', 'we', 'compute', 'the', 'treelevel', 'fourpoint', 'scattering', 'amplitude', 'of', 'two', 'dilatini', 'and', 'two', 'axiondilaton', 'fields', 'in', 'type', 'iib', 'supergravity', 'in', 'ads5', 'x', 's5', 'a', 'special', 'feature', 'of', 'this', 'process', 'is', 'that', 'there', 'is', 'an', 'exo... | [-0.18950684103599894, 0.1867496651547395, -0.04230149658832214, 0.1104869528370306, -0.040254184722567234, -0.1300599095903761, 0.0014842470343095985, 0.3080321744735527, -0.19631526546672978, -0.22040257989845383, 0.07960383749700187, -0.3007624117729474, -0.15718001555424274, 0.11556941108225383, -0.0245585045890837... |
707.0425 | Random Normal Matrices and Polynomial Curves | We show that in the large matrix limit, the eigenvalues of the normal matrix
model for matrices with spectrum inside a compact domain with a special class
of potentials homogeneously fill the interior of a polynomial curve uniquely
defined by the area of its interior domain and its exterior harmonic moments
which are... | math.QA math.PR | we show that in the large matrix limit the eigenvalues of the normal matrix model for matrices with spectrum inside a compact domain with a special class of potentials homogeneously fill the interior of a polynomial curve uniquely defined by the area of its interior domain and its exterior harmonic moments which are al... | [['we', 'show', 'that', 'in', 'the', 'large', 'matrix', 'limit', 'the', 'eigenvalues', 'of', 'the', 'normal', 'matrix', 'model', 'for', 'matrices', 'with', 'spectrum', 'inside', 'a', 'compact', 'domain', 'with', 'a', 'special', 'class', 'of', 'potentials', 'homogeneously', 'fill', 'the', 'interior', 'of', 'a', 'polynom... | [-0.12259058403438544, 0.0847618502453557, -0.04301074307479032, 0.0003678221748470589, -0.052753183764179014, -0.07567572237101493, 0.04295144125248666, 0.32082024535483067, -0.3124704992499303, -0.22749367854683786, 0.14424971576259882, -0.2379150793715674, -0.16854069370205874, 0.15559399802120286, -0.03236320681098... |
707.0426 | Multinucleon transfer reactions in closed-shell nuclei | Multinucleon transfer reactions in 40Ca+96Zr and 90Zr+208Pb have been
measured at energies close to the Coulomb barrier in a high resolution
gamma-particle coincidence experiment. The large solid angle magnetic
spectrometer PRISMA coupled to the CLARA gamma-array has been employed.
Trajectory reconstruction has been ... | nucl-ex | multinucleon transfer reactions in 40ca96zr and 90zr208pb have been measured at energies close to the coulomb barrier in a high resolution gammaparticle coincidence experiment the large solid angle magnetic spectrometer prisma coupled to the clara gammaarray has been employed trajectory reconstruction has been applied ... | [['multinucleon', 'transfer', 'reactions', 'in', '40ca96zr', 'and', '90zr208pb', 'have', 'been', 'measured', 'at', 'energies', 'close', 'to', 'the', 'coulomb', 'barrier', 'in', 'a', 'high', 'resolution', 'gammaparticle', 'coincidence', 'experiment', 'the', 'large', 'solid', 'angle', 'magnetic', 'spectrometer', 'prisma'... | [-0.09012295923808038, 0.1963072484617846, -0.042373850592142576, 0.11010723832145299, 0.023917846866728116, -0.1281880064893307, 0.01769423775086007, 0.3857413383493959, -0.20249357066306942, -0.3363529288671324, -0.021879587593031356, -0.3517922876937384, 0.011214203378013163, 0.16051339029002487, 0.0387178341428538,... |
707.0427 | Complete isometries between subspaces of noncommutative Lp-spaces | We prove some noncommutative analogues of a theorem by Plotkin and Rudin
about isometries between subspaces of Lp-spaces. Let 0<p<\infty, p not an even
integer. The main result of this paper states that in the category of unital
subspaces of noncommutative probability Lp-spaces, under some boundedness
condition, the ... | math.OA math.FA | we prove some noncommutative analogues of a theorem by plotkin and rudin about isometries between subspaces of lpspaces let 0pinfty p not an even integer the main result of this paper states that in the category of unital subspaces of noncommutative probability lpspaces under some boundedness condition the unital compl... | [['we', 'prove', 'some', 'noncommutative', 'analogues', 'of', 'a', 'theorem', 'by', 'plotkin', 'and', 'rudin', 'about', 'isometries', 'between', 'subspaces', 'of', 'lpspaces', 'let', '0pinfty', 'p', 'not', 'an', 'even', 'integer', 'the', 'main', 'result', 'of', 'this', 'paper', 'states', 'that', 'in', 'the', 'category'... | [-0.13979582269971166, 0.12457526844297372, -0.07509791510487894, 0.09674693028029369, -0.06462185410782695, -0.1771368048232521, -0.04603927144223273, 0.3123776212983935, -0.4093380759299641, -0.11130215329918224, 0.1326835605391288, -0.2715755637840066, -0.11964739058953776, 0.19872102089567292, -0.2685977518164986, ... |
707.0428 | Template-based searches for gravitational waves: efficient lattice
covering of flat parameter spaces | The construction of optimal template banks for matched-filtering searches is
an example of the sphere covering problem. For parameter spaces with
constant-coefficient metrics a (near-) optimal template bank is achieved by the
A_n* lattice, which is the best lattice-covering in dimensions n <= 5, and is
close to the b... | gr-qc | the construction of optimal template banks for matchedfiltering searches is an example of the sphere covering problem for parameter spaces with constantcoefficient metrics a near optimal template bank is achieved by the a_n lattice which is the best latticecovering in dimensions n 5 and is close to the best covering kn... | [['the', 'construction', 'of', 'optimal', 'template', 'banks', 'for', 'matchedfiltering', 'searches', 'is', 'an', 'example', 'of', 'the', 'sphere', 'covering', 'problem', 'for', 'parameter', 'spaces', 'with', 'constantcoefficient', 'metrics', 'a', 'near', 'optimal', 'template', 'bank', 'is', 'achieved', 'by', 'the', 'a... | [-0.10810138998077372, 0.04533999509705767, -0.009699424668012754, 0.08579220140793199, -0.0590644142560094, -0.169371900821874, 0.0584772402780009, 0.4202322785783073, -0.18266338623209816, -0.2840684408362469, 0.16116785560481492, -0.27370860498985683, -0.14142578462665173, 0.22465836386317792, -0.05263877320913193, ... |
707.0429 | The Axion from Five-Dimensional Supergravity | We consider the axion arising from five-dimensional supergravity in the
presence of boundaries. We find the approximate bosonic effective action to
estimate the lower bound on the "Peccei-Quinn" energy scale with a flat bulk.
With a warped bulk, one can obtain a scale within the standard window; this
puts a bound on ... | hep-ph | we consider the axion arising from fivedimensional supergravity in the presence of boundaries we find the approximate bosonic effective action to estimate the lower bound on the pecceiquinn energy scale with a flat bulk with a warped bulk one can obtain a scale within the standard window this puts a bound on the requir... | [['we', 'consider', 'the', 'axion', 'arising', 'from', 'fivedimensional', 'supergravity', 'in', 'the', 'presence', 'of', 'boundaries', 'we', 'find', 'the', 'approximate', 'bosonic', 'effective', 'action', 'to', 'estimate', 'the', 'lower', 'bound', 'on', 'the', 'pecceiquinn', 'energy', 'scale', 'with', 'a', 'flat', 'bul... | [-0.1615656815140563, 0.1681397766860969, -0.07265137546175324, 0.11228323581436758, -0.11834719131669878, -0.10192237868083312, 0.04325830958345357, 0.30553189809160197, -0.20443311316125534, -0.34932276017498226, 0.10016082924763288, -0.23280566424569663, -0.07888170845929862, 0.09543579136404921, -0.0499133216025417... |
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