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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708.2149 | When do stepwise algorithms meet subset selection criteria? | Recent results in homotopy and solution paths demonstrate that certain
well-designed greedy algorithms, with a range of values of the algorithmic
parameter, can provide solution paths to a sequence of convex optimization
problems. On the other hand, in regression many existing criteria in subset
selection (including ... | math.ST stat.TH | recent results in homotopy and solution paths demonstrate that certain welldesigned greedy algorithms with a range of values of the algorithmic parameter can provide solution paths to a sequence of convex optimization problems on the other hand in regression many existing criteria in subset selection including c_p aic ... | [['recent', 'results', 'in', 'homotopy', 'and', 'solution', 'paths', 'demonstrate', 'that', 'certain', 'welldesigned', 'greedy', 'algorithms', 'with', 'a', 'range', 'of', 'values', 'of', 'the', 'algorithmic', 'parameter', 'can', 'provide', 'solution', 'paths', 'to', 'a', 'sequence', 'of', 'convex', 'optimization', 'pro... | [-0.11950938524333415, 0.03326334847251591, -0.10187161904702216, 0.07127032074200587, -0.11430201577568817, -0.19240568290223126, 0.03640937221374501, 0.40099704292039445, -0.30771131148090425, -0.2986911447074862, 0.15859171666958036, -0.23704614562706816, -0.18619803001782226, 0.21457906845198185, -0.122209367100839... |
708.215 | Local partial likelihood estimation in proportional hazards regression | Fan, Gijbels and King [Ann. Statist. 25 (1997) 1661--1690] considered the
estimation of the risk function $\psi (x)$ in the proportional hazards model.
Their proposed estimator is based on integrating the estimated derivative
function obtained through a local version of the partial likelihood. They
proved the large s... | math.ST stat.TH | fan gijbels and king ann statist 25 1997 16611690 considered the estimation of the risk function psi x in the proportional hazards model their proposed estimator is based on integrating the estimated derivative function obtained through a local version of the partial likelihood they proved the large sample properties o... | [['fan', 'gijbels', 'and', 'king', 'ann', 'statist', '25', '1997', '16611690', 'considered', 'the', 'estimation', 'of', 'the', 'risk', 'function', 'psi', 'x', 'in', 'the', 'proportional', 'hazards', 'model', 'their', 'proposed', 'estimator', 'is', 'based', 'on', 'integrating', 'the', 'estimated', 'derivative', 'functio... | [-0.06696701177282681, -0.01836328240862703, -0.12022034413160664, 0.10105544268102154, -0.03250070671082696, -0.08373617328374096, 0.08154922231095355, 0.34512231179940106, -0.2627072982973733, -0.2931156586032381, 0.12123581855969494, -0.26927780801718487, -0.15995576125035804, 0.15524809723539865, -0.113252115106590... |
708.2151 | Mapping the distribution of luminous and dark matter in strong lensing
galaxies | We present the distribution of luminous and dark matter in a set of strong
lensing (early-type) galaxies. By combining two independent techniques -
stellar population synthesis and gravitational lensing - we can compare the
baryonic and dark matter content in these galaxies within the regions that can
be probed using... | astro-ph | we present the distribution of luminous and dark matter in a set of strong lensing earlytype galaxies by combining two independent techniques stellar population synthesis and gravitational lensing we can compare the baryonic and dark matter content in these galaxies within the regions that can be probed using the image... | [['we', 'present', 'the', 'distribution', 'of', 'luminous', 'and', 'dark', 'matter', 'in', 'a', 'set', 'of', 'strong', 'lensing', 'earlytype', 'galaxies', 'by', 'combining', 'two', 'independent', 'techniques', 'stellar', 'population', 'synthesis', 'and', 'gravitational', 'lensing', 'we', 'can', 'compare', 'the', 'baryo... | [-0.07577071054838598, 0.09831340068703867, -0.12298351476331137, 0.12841406139131223, -0.07377943070362865, -0.052146550270521806, -0.012291514175012707, 0.39948118713994824, -0.15972694011935445, -0.39038867353358203, 0.011560061407767028, -0.30991354144522726, -0.01884938527881685, 0.19020547555780165, 0.00585183460... |
708.2152 | Coupling, concentration inequalities and stochastic dynamics | In the context of interacting particle systems, we study the influence of the
action of the semigroup on the concentration property of Lipschitz functions.
As an application, this gives a new approach to estimate the relaxation speed
to equilibrium of interacting particle systems. We illustrate our approach in a
vari... | math.PR math-ph math.MP | in the context of interacting particle systems we study the influence of the action of the semigroup on the concentration property of lipschitz functions as an application this gives a new approach to estimate the relaxation speed to equilibrium of interacting particle systems we illustrate our approach in a variety of... | [['in', 'the', 'context', 'of', 'interacting', 'particle', 'systems', 'we', 'study', 'the', 'influence', 'of', 'the', 'action', 'of', 'the', 'semigroup', 'on', 'the', 'concentration', 'property', 'of', 'lipschitz', 'functions', 'as', 'an', 'application', 'this', 'gives', 'a', 'new', 'approach', 'to', 'estimate', 'the',... | [-0.09512201571136568, 0.10726903262661051, -0.11561709222512255, 0.09390805590783202, -0.05440773827361007, -0.1447536720982592, 0.026363457745776094, 0.33244913888709815, -0.27120595020723753, -0.24038198880112632, 0.09916584241878369, -0.26522983009284684, -0.14400681246178434, 0.23429503442984523, -0.03929382901446... |
708.2153 | Estimating the number of classes | Estimating the unknown number of classes in a population has numerous
important applications. In a Poisson mixture model, the problem is reduced to
estimating the odds that a class is undetected in a sample. The discontinuity
of the odds prevents the existence of locally unbiased and informative
estimators and restri... | math.ST stat.TH | estimating the unknown number of classes in a population has numerous important applications in a poisson mixture model the problem is reduced to estimating the odds that a class is undetected in a sample the discontinuity of the odds prevents the existence of locally unbiased and informative estimators and restricts c... | [['estimating', 'the', 'unknown', 'number', 'of', 'classes', 'in', 'a', 'population', 'has', 'numerous', 'important', 'applications', 'in', 'a', 'poisson', 'mixture', 'model', 'the', 'problem', 'is', 'reduced', 'to', 'estimating', 'the', 'odds', 'that', 'a', 'class', 'is', 'undetected', 'in', 'a', 'sample', 'the', 'dis... | [-0.11948692974937933, 0.08741775117919184, -0.0704070231301731, 0.15061710902955383, -0.08170451028167866, -0.14070566607576407, 0.09434481365004492, 0.34841603105573843, -0.23089509402935424, -0.3275024386520466, 0.15479787834527578, -0.24595088624719824, -0.0582256037689578, 0.21547048329375684, -0.1116111720859837,... |
708.2154 | Gain of analyticity for semilinear Schroedinger equations | We discuss gain of analyticity phenomenon of solutions to the initial value
problem for semilinear Schroedinger equations with gauge invariant
nonlinearity. We prove that if the initial data decays exponentially, then the
solution becomes real-analytic in the space variable and a Gevrey function of
order 2 in the tim... | math.AP | we discuss gain of analyticity phenomenon of solutions to the initial value problem for semilinear schroedinger equations with gauge invariant nonlinearity we prove that if the initial data decays exponentially then the solution becomes realanalytic in the space variable and a gevrey function of order 2 in the time var... | [['we', 'discuss', 'gain', 'of', 'analyticity', 'phenomenon', 'of', 'solutions', 'to', 'the', 'initial', 'value', 'problem', 'for', 'semilinear', 'schroedinger', 'equations', 'with', 'gauge', 'invariant', 'nonlinearity', 'we', 'prove', 'that', 'if', 'the', 'initial', 'data', 'decays', 'exponentially', 'then', 'the', 's... | [-0.15172001883053246, 0.07093171504498176, -0.09939166659060926, 0.0865420104102948, -0.09385451521628942, -0.1040275657716661, 0.013971011699117625, 0.31760031935305166, -0.260119901295417, -0.2305785029863891, 0.1434079503031591, -0.28916833482873744, -0.10709013093788272, 0.16618337832056942, -0.029711647603947382,... |
708.2155 | Strongly pseudoconvex domains as subvarieties of complex manifolds | In this paper (a sequel to B. Drinovec Drnovsek and F. Forstneric,
Holomorphic curves in complex spaces, Duke Math. J. 139 (2007), 203-253) we
obtain existence and approximation results for closed complex subvarieties that
are normalized by strongly pseudoconvex Stein domains. Our sufficient condition
for the existen... | math.CV math.AG | in this paper a sequel to b drinovec drnovsek and f forstneric holomorphic curves in complex spaces duke math j 139 2007 203253 we obtain existence and approximation results for closed complex subvarieties that are normalized by strongly pseudoconvex stein domains our sufficient condition for the existence of such subv... | [['in', 'this', 'paper', 'a', 'sequel', 'to', 'b', 'drinovec', 'drnovsek', 'and', 'f', 'forstneric', 'holomorphic', 'curves', 'in', 'complex', 'spaces', 'duke', 'math', 'j', '139', '2007', '203253', 'we', 'obtain', 'existence', 'and', 'approximation', 'results', 'for', 'closed', 'complex', 'subvarieties', 'that', 'are'... | [-0.1626873572022305, 0.030477039706170217, -0.04638655681992532, 0.08812795250833005, -0.10985418006021064, -0.10387667431223235, 0.004869122950367455, 0.34053739032242447, -0.23416585265658796, -0.2054074648040114, 0.10276769832580612, -0.233874707169889, -0.19187806159243337, 0.23993948351517247, -0.2055053552867320... |
708.2156 | Ordering from frustration in a strongly correlated one-dimensional
system | We study a one-dimensional extended Hubbard model with longer-range Coulomb
interactions at quarter-filling in the strong coupling limit. We find two
different charge-ordered (CO) ground states as the strength of the longer range
interactions is varied. At lower energies, these CO states drive two different
spin-orde... | cond-mat.str-el | we study a onedimensional extended hubbard model with longerrange coulomb interactions at quarterfilling in the strong coupling limit we find two different chargeordered co ground states as the strength of the longer range interactions is varied at lower energies these co states drive two different spinordered ground s... | [['we', 'study', 'a', 'onedimensional', 'extended', 'hubbard', 'model', 'with', 'longerrange', 'coulomb', 'interactions', 'at', 'quarterfilling', 'in', 'the', 'strong', 'coupling', 'limit', 'we', 'find', 'two', 'different', 'chargeordered', 'co', 'ground', 'states', 'as', 'the', 'strength', 'of', 'the', 'longer', 'rang... | [-0.2156755878328113, 0.2586856398556847, -0.026456933338340604, 0.0704367025035026, 0.005727631994523108, -0.20217126098577864, 0.1026566385582555, 0.3926085295039229, -0.2355471449525794, -0.23736961547110697, 0.01934349989387556, -0.3655614965187851, -0.10897288965061307, 0.10332227531907848, 0.1325262801896315, 0.0... |
708.2157 | Dynamics of \bar{K} and multi-\bar{K} nuclei | We report on self-consistent calculations of single-K^- nuclear states and
multi-Kbar nuclear states in 12C, 16O, 40Ca and 208Pb within the relativistic
mean-field (RMF) approach. Gradient terms motivated by the p-wave resonance
Sigma(1385) are found to play a secondary role for single-K^- nuclear systems
where the m... | nucl-th | we report on selfconsistent calculations of singlek nuclear states and multikbar nuclear states in 12c 16o 40ca and 208pb within the relativistic meanfield rmf approach gradient terms motivated by the pwave resonance sigma1385 are found to play a secondary role for singlek nuclear systems where the meanfield concept is... | [['we', 'report', 'on', 'selfconsistent', 'calculations', 'of', 'singlek', 'nuclear', 'states', 'and', 'multikbar', 'nuclear', 'states', 'in', '12c', '16o', '40ca', 'and', '208pb', 'within', 'the', 'relativistic', 'meanfield', 'rmf', 'approach', 'gradient', 'terms', 'motivated', 'by', 'the', 'pwave', 'resonance', 'sigm... | [-0.07240151994867447, 0.274280962138726, -0.04982324545589848, 0.1029307959667806, 0.03500639116959155, -0.12392105372125133, 0.09935003351304472, 0.34316226519551707, -0.1710395435976177, -0.2933102791510532, -0.10858462553294897, -0.36672854972482655, 0.009434076863404665, 0.09710859171814801, 0.1500169092956323, 0.... |
708.2158 | Clathrate hydrates as a sink of noble gases in Titan's atmosphere | We use a statistical thermodynamic approach to determine the composition of
clathrate hydrates which may form from a multiple compound gas whose
composition is similar to that of Titan's atmosphere. Assuming that noble gases
are initially present in this gas phase, we calculate the ratios of xenon,
krypton and argon ... | astro-ph | we use a statistical thermodynamic approach to determine the composition of clathrate hydrates which may form from a multiple compound gas whose composition is similar to that of titans atmosphere assuming that noble gases are initially present in this gas phase we calculate the ratios of xenon krypton and argon to spe... | [['we', 'use', 'a', 'statistical', 'thermodynamic', 'approach', 'to', 'determine', 'the', 'composition', 'of', 'clathrate', 'hydrates', 'which', 'may', 'form', 'from', 'a', 'multiple', 'compound', 'gas', 'whose', 'composition', 'is', 'similar', 'to', 'that', 'of', 'titans', 'atmosphere', 'assuming', 'that', 'noble', 'g... | [-0.014660384053095929, 0.2489369533485638, -0.03925361123876836, 0.02196112183238646, 0.07782652685703824, -0.08590754644698179, 0.05460206563738935, 0.40351533891671165, -0.2160501645507329, -0.3306320004868416, 0.07683573903727384, -0.28633443538422637, -0.0634133864861761, 0.14575156518133423, -0.005588010028337261... |
708.2159 | From frustrated insulators to correlated anisotropic metals: charge
ordering and quantum criticality in coupled chain systems | A recent study revealed the dynamics of the charge sector of a
one-dimensional quarter-filled electronic system with extended Hubbard
interactions to be that of an effective pseudospin transverse-field Ising model
(TFIM) in the strong coupling limit. With the twin motivations of studying the
co-existing charge and sp... | cond-mat.str-el | a recent study revealed the dynamics of the charge sector of a onedimensional quarterfilled electronic system with extended hubbard interactions to be that of an effective pseudospin transversefield ising model tfim in the strong coupling limit with the twin motivations of studying the coexisting charge and spin order ... | [['a', 'recent', 'study', 'revealed', 'the', 'dynamics', 'of', 'the', 'charge', 'sector', 'of', 'a', 'onedimensional', 'quarterfilled', 'electronic', 'system', 'with', 'extended', 'hubbard', 'interactions', 'to', 'be', 'that', 'of', 'an', 'effective', 'pseudospin', 'transversefield', 'ising', 'model', 'tfim', 'in', 'th... | [-0.21924442119779997, 0.22784756418765867, -0.06472663530019837, 0.06282545730489521, -0.015880649537743572, -0.1826167965057091, 0.05259287016031941, 0.34199077281832263, -0.2453930277193789, -0.2355475862971686, 0.0502467631147458, -0.3119245891307051, -0.137211288211312, 0.14090179015609186, 0.09856206095159556, 0.... |
708.216 | Rational algebraic K-theory of topological K-theory | We show that after rationalization there is a homotopy fiber sequence BBU ->
K(ku) -> K(Z). We interpret this as a correspondence between the virtual
2-vector bundles over a space X and their associated anomaly bundles over the
free loop space LX. We also rationally compute K(KU) by using the localization
sequence, a... | math.KT math.AT | we show that after rationalization there is a homotopy fiber sequence bbu kku kz we interpret this as a correspondence between the virtual 2vector bundles over a space x and their associated anomaly bundles over the free loop space lx we also rationally compute kku by using the localization sequence and kmu by a method... | [['we', 'show', 'that', 'after', 'rationalization', 'there', 'is', 'a', 'homotopy', 'fiber', 'sequence', 'bbu', 'kku', 'kz', 'we', 'interpret', 'this', 'as', 'a', 'correspondence', 'between', 'the', 'virtual', '2vector', 'bundles', 'over', 'a', 'space', 'x', 'and', 'their', 'associated', 'anomaly', 'bundles', 'over', '... | [-0.1997377678110707, 0.098827927123343, -0.09019177213795941, 0.09670348909729329, -0.05420114032038655, -0.13377445298018026, 0.06641206414377714, 0.47652417500732375, -0.3548002399382044, -0.16523755140236165, 0.07969806261635462, -0.18740052949698244, -0.22278719163331828, 0.21544177393566388, -0.13506870798491796,... |
708.2161 | Dynamic elastic properties and magnetic susceptibility across the
austenite-martensite transformation in site-disordered ferromagnetic Ni-Fe-Al
alloy | Besides permitting an accurate determination of the
ferromagnetic-to-paramagnetic phase transition temperature and the
characteristic temperatures for the beginning and end of the growth of
martensite (austenite) phase at the expense of austenite (martensite) phase
while cooling (heating), the results of an extensive... | cond-mat.mtrl-sci cond-mat.other | besides permitting an accurate determination of the ferromagnetictoparamagnetic phase transition temperature and the characteristic temperatures for the beginning and end of the growth of martensite austenite phase at the expense of austenite martensite phase while cooling heating the results of an extensive ac suscept... | [['besides', 'permitting', 'an', 'accurate', 'determination', 'of', 'the', 'ferromagnetictoparamagnetic', 'phase', 'transition', 'temperature', 'and', 'the', 'characteristic', 'temperatures', 'for', 'the', 'beginning', 'and', 'end', 'of', 'the', 'growth', 'of', 'martensite', 'austenite', 'phase', 'at', 'the', 'expense'... | [-0.15876265242695808, 0.2591012769557788, -0.06944159403770366, -0.054151895421358065, -0.03326481341682943, -0.061543841352188634, 0.14233684519311157, 0.37344959798404054, -0.2635794142418886, -0.25683831899846327, 0.10962035395880408, -0.2443753307941192, -0.12916241187019317, 0.14084814060905962, 0.014040377529343... |
708.2162 | Normal Surface Theory in Link Diagrams | This paper has been withdrawn by the author, due to a significant error in
section 4.3.1.
| math.GT | this paper has been withdrawn by the author due to a significant error in section 431 | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'author', 'due', 'to', 'a', 'significant', 'error', 'in', 'section', '431']] | [-0.11877008283045143, -0.06373786000767723, -0.09729297753074206, -0.03778180309018353, -0.06622681498993188, -0.047266099572880194, 0.03117303836188512, 0.31308686500415206, -0.20150024467147887, -0.40554738068021834, 0.09446261732227867, -0.3175840985495597, -0.1300886581884697, 0.10289573948830366, -0.3258071706513... |
708.2163 | R-separation of variables for the conformally invariant Laplace equation | The conditions for R-separation of variables for the conformally invariant
Laplace equation on an n-dimensional Riemannian manifold are determined and
compared with the conditions for the additive separation of the null geodesic
Hamilton-Jacobi equation. The case of 3-dimensions is examined in detail and it
is proven... | math-ph math.MP | the conditions for rseparation of variables for the conformally invariant laplace equation on an ndimensional riemannian manifold are determined and compared with the conditions for the additive separation of the null geodesic hamiltonjacobi equation the case of 3dimensions is examined in detail and it is proven that o... | [['the', 'conditions', 'for', 'rseparation', 'of', 'variables', 'for', 'the', 'conformally', 'invariant', 'laplace', 'equation', 'on', 'an', 'ndimensional', 'riemannian', 'manifold', 'are', 'determined', 'and', 'compared', 'with', 'the', 'conditions', 'for', 'the', 'additive', 'separation', 'of', 'the', 'null', 'geodes... | [-0.16363923804213604, 0.06465901944793587, -0.08703344835278888, 0.10231809998319173, -0.06714436252756666, -0.14694439340382814, -0.10869044357289871, 0.3346484608948231, -0.2307172306192418, -0.21616481704598603, 0.12261616542236879, -0.284983362754186, -0.113525421731174, 0.18108657357127717, -0.07798811246951422, ... |
708.2164 | Constraining Dark Energy From Splitting Angle Statistic of Strong
Gravitational Lenses | Utilizing the CLASS statistical sample, we investigate the constraint of the
splitting angle statistic of strong gravitational lenses(SGL) on the
equation-of-state parameter $w=p/\rho$ of the dark energy in the flat cold dark
matter cosmology. Through the comoving number density of dark halos described
by Press-Schec... | astro-ph | utilizing the class statistical sample we investigate the constraint of the splitting angle statistic of strong gravitational lensessgl on the equationofstate parameter wprho of the dark energy in the flat cold dark matter cosmology through the comoving number density of dark halos described by pressschechter theory da... | [['utilizing', 'the', 'class', 'statistical', 'sample', 'we', 'investigate', 'the', 'constraint', 'of', 'the', 'splitting', 'angle', 'statistic', 'of', 'strong', 'gravitational', 'lensessgl', 'on', 'the', 'equationofstate', 'parameter', 'wprho', 'of', 'the', 'dark', 'energy', 'in', 'the', 'flat', 'cold', 'dark', 'matte... | [-0.11765751681486243, 0.15395378677095187, -0.07351953227895293, 0.10676132683936962, -0.0689104225169471, -0.14680323227862282, 0.019216001268471294, 0.34319835052171604, -0.21028059452494724, -0.395426131965112, 0.03198881215970725, -0.2666393309395681, 0.04092207529205591, 0.19192023648870515, 0.06390743658189325, ... |
708.2165 | Matching with shift for one-dimensional Gibbs measures | We consider matching with shifts for Gibbsian sequences. We prove that the
maximal overlap behaves as $c\log n$, where $c$ is explicitly identified in
terms of the thermodynamic quantities (pressure) of the underlying potential.
Our approach is based on the analysis of the first and second moment of the
number of ove... | math.PR math-ph math.MP | we consider matching with shifts for gibbsian sequences we prove that the maximal overlap behaves as clog n where c is explicitly identified in terms of the thermodynamic quantities pressure of the underlying potential our approach is based on the analysis of the first and second moment of the number of overlaps of a g... | [['we', 'consider', 'matching', 'with', 'shifts', 'for', 'gibbsian', 'sequences', 'we', 'prove', 'that', 'the', 'maximal', 'overlap', 'behaves', 'as', 'clog', 'n', 'where', 'c', 'is', 'explicitly', 'identified', 'in', 'terms', 'of', 'the', 'thermodynamic', 'quantities', 'pressure', 'of', 'the', 'underlying', 'potential... | [-0.15595686886725682, 0.14978519147261976, -0.040848004884485686, 0.046055136360311215, 0.015508769499137997, -0.06684746264280485, 0.057752235517338185, 0.32453778368820035, -0.25703235317819884, -0.26260263275887286, 0.07931301855714992, -0.2939096812691007, -0.13331634487091962, 0.14752987225406936, -0.035099954011... |
708.2166 | An approximate theory for substructure propagation in clusters | The existence of dark matter can be proved in an astrophysical context by the
discovery of a system in which the observed baryons and the inferred dark
matter are spatially segregated, such as the bullet cluster (1E0657-558). The
full descriptions of the dark matter halo and X-ray gas substructure motions
are necessa... | astro-ph | the existence of dark matter can be proved in an astrophysical context by the discovery of a system in which the observed baryons and the inferred dark matter are spatially segregated such as the bullet cluster 1e0657558 the full descriptions of the dark matter halo and xray gas substructure motions are necessary to fo... | [['the', 'existence', 'of', 'dark', 'matter', 'can', 'be', 'proved', 'in', 'an', 'astrophysical', 'context', 'by', 'the', 'discovery', 'of', 'a', 'system', 'in', 'which', 'the', 'observed', 'baryons', 'and', 'the', 'inferred', 'dark', 'matter', 'are', 'spatially', 'segregated', 'such', 'as', 'the', 'bullet', 'cluster',... | [-0.08927366569593188, 0.09730645744083073, -0.15264038260905974, 0.13517623740744086, -0.0969790805176261, -0.006216635912536613, -0.01470529779251064, 0.3500609049213029, -0.23163529559218834, -0.38322028151202586, 0.03817794208655194, -0.2731633062204046, -0.022823495912035145, 0.1725879199412321, 0.0562648845175581... |
708.2167 | Thompson's renormalization group method applied to QCD at high energy
scale | We use a renormalization group method to treat QCD-vacuum behavior specially
closer to the regime of asymptotic freedom. QCD-vacuum behaves effectively like
a "paramagnetic system" of a classical theory in the sense that virtual color
charges (gluons) emerges in it as a spin effect of a paramagnetic material when
a m... | hep-ph | we use a renormalization group method to treat qcdvacuum behavior specially closer to the regime of asymptotic freedom qcdvacuum behaves effectively like a paramagnetic system of a classical theory in the sense that virtual color charges gluons emerges in it as a spin effect of a paramagnetic material when a magnetic f... | [['we', 'use', 'a', 'renormalization', 'group', 'method', 'to', 'treat', 'qcdvacuum', 'behavior', 'specially', 'closer', 'to', 'the', 'regime', 'of', 'asymptotic', 'freedom', 'qcdvacuum', 'behaves', 'effectively', 'like', 'a', 'paramagnetic', 'system', 'of', 'a', 'classical', 'theory', 'in', 'the', 'sense', 'that', 'vi... | [-0.12769722146717752, 0.22146485621830353, -0.12029088744619752, 0.07561196313296374, -0.10657404916470542, -0.1263033398828164, 0.04567385281246848, 0.32814348785660596, -0.22222127038163736, -0.28579056459995567, 0.017840029529448475, -0.28622947399457527, -0.11057023843848186, 0.1304271681343808, -0.002347859102027... |
708.2168 | Room-temperature magnetocaloric effect in La0.7Sr0.3Mn1-xM'xO3 (M'=Al,
Ti) | Magnetic entropy and adiabatic temperature changes in and above the
room-temperature region has been measured for La0.7Sr0.3Mn1-xM'xO3 (M' = Al,
Ti) by means of magnetization and heat capacity measurements in magnetic fields
up to 6 T. The magnetocaloric effect becomes largest at the ferromagnetic
ordering temperatur... | cond-mat.mtrl-sci cond-mat.str-el | magnetic entropy and adiabatic temperature changes in and above the roomtemperature region has been measured for la07sr03mn1xmxo3 m al ti by means of magnetization and heat capacity measurements in magnetic fields up to 6 t the magnetocaloric effect becomes largest at the ferromagnetic ordering temperature tc that is t... | [['magnetic', 'entropy', 'and', 'adiabatic', 'temperature', 'changes', 'in', 'and', 'above', 'the', 'roomtemperature', 'region', 'has', 'been', 'measured', 'for', 'la07sr03mn1xmxo3', 'm', 'al', 'ti', 'by', 'means', 'of', 'magnetization', 'and', 'heat', 'capacity', 'measurements', 'in', 'magnetic', 'fields', 'up', 'to',... | [-0.13321939132090907, 0.23687306535805785, 0.047888179540619136, -0.01749442959947872, -0.05295433760094907, -0.14309313176800648, 0.14580462046245474, 0.36730332867873294, -0.2747427450808426, -0.35685576216858483, 0.005792255859799503, -0.35646494976859805, -0.027877300842514923, 0.2137289794965557, 0.01241464965818... |
708.2169 | Photogalvanic effects in HgTe quantum wells | We report on the observation of the terahertz radiation induced circular
(CPGE) and linear (LPGE) photogalvanic effects in HgTe quantum wells. The
current response is well described by the phenomenological theory of CPGE and
LPGE.
| cond-mat.mes-hall | we report on the observation of the terahertz radiation induced circular cpge and linear lpge photogalvanic effects in hgte quantum wells the current response is well described by the phenomenological theory of cpge and lpge | [['we', 'report', 'on', 'the', 'observation', 'of', 'the', 'terahertz', 'radiation', 'induced', 'circular', 'cpge', 'and', 'linear', 'lpge', 'photogalvanic', 'effects', 'in', 'hgte', 'quantum', 'wells', 'the', 'current', 'response', 'is', 'well', 'described', 'by', 'the', 'phenomenological', 'theory', 'of', 'cpge', 'an... | [-0.1852520384825766, 0.21689368451812438, -0.02178321604483894, 0.006509987175065492, -0.04140742634023939, -0.11037457548081875, 0.006789714660096382, 0.365065985545516, -0.254810950585774, -0.27669355938477175, 0.0033815082794587527, -0.30764203827295983, -0.2128687151840755, 0.2403385835566691, 0.006263905171571034... |
708.217 | Future Directions of Research in Geometry: A Summary of the Panel
Discussion at the 2007 Midwest Geometry Conference | The 2007 Midwest Geometry Conference included a panel discussion devoted to
open problems and the general direction of future research in fields related to
the main themes of the conference. This paper summarizes the comments made
during the panel discussion.
| math.DG gr-qc hep-th math-ph math.MP | the 2007 midwest geometry conference included a panel discussion devoted to open problems and the general direction of future research in fields related to the main themes of the conference this paper summarizes the comments made during the panel discussion | [['the', '2007', 'midwest', 'geometry', 'conference', 'included', 'a', 'panel', 'discussion', 'devoted', 'to', 'open', 'problems', 'and', 'the', 'general', 'direction', 'of', 'future', 'research', 'in', 'fields', 'related', 'to', 'the', 'main', 'themes', 'of', 'the', 'conference', 'this', 'paper', 'summarizes', 'the', ... | [-0.11120735085569322, 0.057348932651802895, -0.014882223692256957, 0.005930300787440501, -0.18249410758726298, -0.07303523224545642, -0.006611687314580195, 0.3069678680971265, -0.21008393866941333, -0.3207120401901193, 0.1806173163553467, -0.30121364421211183, -0.16564084868878126, 0.22167725441977382, -0.159193668258... |
708.2171 | Control of laser wake field acceleration by plasma density profile | We show that both the maximum energy gain and the accelerated beam quality
can be efficiently controlled by the plasma density profile. Choosing a proper
density gradient one can uplift the dephasing limitation. When a periodic wake
field is exploited, the phase synchronism between the bunch of relativistic
particles... | physics.plasm-ph physics.acc-ph | we show that both the maximum energy gain and the accelerated beam quality can be efficiently controlled by the plasma density profile choosing a proper density gradient one can uplift the dephasing limitation when a periodic wake field is exploited the phase synchronism between the bunch of relativistic particles and ... | [['we', 'show', 'that', 'both', 'the', 'maximum', 'energy', 'gain', 'and', 'the', 'accelerated', 'beam', 'quality', 'can', 'be', 'efficiently', 'controlled', 'by', 'the', 'plasma', 'density', 'profile', 'choosing', 'a', 'proper', 'density', 'gradient', 'one', 'can', 'uplift', 'the', 'dephasing', 'limitation', 'when', '... | [-0.11464727172753543, 0.2565191165834718, -0.11441883370808675, 0.055462985103025185, -0.015134321687518493, -0.09957449365174398, 0.0022233938484564953, 0.40335856629073197, -0.28485615379243084, -0.3106787392278433, 0.04764732890118389, -0.20536090908671153, -0.0029105190930769163, 0.19246376792698808, -0.0263471975... |
708.2172 | Gravitational stability in the disk of M51 | Star formation laws, like i.e. the Schmidt law relating star formation rate
and total gas density, have been studied in several spiral galaxies but the
underlying physics are not yet well understood. M51, as a nearby face-on, grand
design spiral galaxy studied in many line transitions, is an ideal target to
study the... | astro-ph | star formation laws like ie the schmidt law relating star formation rate and total gas density have been studied in several spiral galaxies but the underlying physics are not yet well understood m51 as a nearby faceon grand design spiral galaxy studied in many line transitions is an ideal target to study the connection... | [['star', 'formation', 'laws', 'like', 'ie', 'the', 'schmidt', 'law', 'relating', 'star', 'formation', 'rate', 'and', 'total', 'gas', 'density', 'have', 'been', 'studied', 'in', 'several', 'spiral', 'galaxies', 'but', 'the', 'underlying', 'physics', 'are', 'not', 'yet', 'well', 'understood', 'm51', 'as', 'a', 'nearby',... | [-0.07772547727226785, 0.047752777040862296, -0.06847667972066702, 0.09905142130913171, -0.042651012872224885, -0.009473427641383222, 0.023192618521666226, 0.3737431512932286, -0.16240667611296566, -0.3524133116149038, 0.05896321000204287, -0.22408640437283134, -0.09689524820437015, 0.12801838183610253, -0.007293704078... |
708.2173 | Provenance as Dependency Analysis | Provenance is information recording the source, derivation, or history of
some information. Provenance tracking has been studied in a variety of
settings; however, although many design points have been explored, the
mathematical or semantic foundations of data provenance have received
comparatively little attention. ... | cs.DB cs.PL | provenance is information recording the source derivation or history of some information provenance tracking has been studied in a variety of settings however although many design points have been explored the mathematical or semantic foundations of data provenance have received comparatively little attention in this p... | [['provenance', 'is', 'information', 'recording', 'the', 'source', 'derivation', 'or', 'history', 'of', 'some', 'information', 'provenance', 'tracking', 'has', 'been', 'studied', 'in', 'a', 'variety', 'of', 'settings', 'however', 'although', 'many', 'design', 'points', 'have', 'been', 'explored', 'the', 'mathematical',... | [-0.1028796517319541, -0.01766071152697141, -0.12891216124701607, 0.09588160130891714, -0.18660832753589562, -0.10762543507709026, 0.02399812898019681, 0.39249059634266403, -0.2635952376567566, -0.32756221193719554, 0.13818256644876087, -0.24941853057542765, -0.1668811459094286, 0.18723367180608147, -0.0965165235899254... |
708.2174 | A geometric analysis of the Maxwell field in a vicinity of a multipole
particle and new special functions | A method of solving Maxwell equations in a vicinity of a multipole particle
(moving along an arbitrary trajectory) is proposed. The method is based on a
geometric construction of a trajectory-adapted coordinate system, which
simplifies considerably the equations. The solution is given in terms of a
series, where a ne... | physics.class-ph | a method of solving maxwell equations in a vicinity of a multipole particle moving along an arbitrary trajectory is proposed the method is based on a geometric construction of a trajectoryadapted coordinate system which simplifies considerably the equations the solution is given in terms of a series where a new family ... | [['a', 'method', 'of', 'solving', 'maxwell', 'equations', 'in', 'a', 'vicinity', 'of', 'a', 'multipole', 'particle', 'moving', 'along', 'an', 'arbitrary', 'trajectory', 'is', 'proposed', 'the', 'method', 'is', 'based', 'on', 'a', 'geometric', 'construction', 'of', 'a', 'trajectoryadapted', 'coordinate', 'system', 'whic... | [-0.14768618741340336, 0.06113209619605646, -0.11982972324750889, 0.009664444230100804, -0.09369646040080436, -0.08494962435001614, -0.025154306177630613, 0.26870051701285547, -0.27498344982835066, -0.28238981152916776, 0.07542913542905201, -0.243283152615052, -0.16467483242138706, 0.23325607872396792, -0.0657252400187... |
708.2175 | Cyclotron resonance photoconductivity of a two-dimensional electron gas
in HgTe quantum wells | Far-infrared cyclotron resonance photoconductivity (CRP) is investigated in
HgTe quantum wells (QWs) of various widths grown on (013) oriented GaAs
substrates. It is shown that CRP is caused by the heating of two-dimensional
electron gas (2DEG). From the resonance magnetic field strength effective
masses and their de... | cond-mat.mes-hall | farinfrared cyclotron resonance photoconductivity crp is investigated in hgte quantum wells qws of various widths grown on 013 oriented gaas substrates it is shown that crp is caused by the heating of twodimensional electron gas 2deg from the resonance magnetic field strength effective masses and their dependence on th... | [['farinfrared', 'cyclotron', 'resonance', 'photoconductivity', 'crp', 'is', 'investigated', 'in', 'hgte', 'quantum', 'wells', 'qws', 'of', 'various', 'widths', 'grown', 'on', '013', 'oriented', 'gaas', 'substrates', 'it', 'is', 'shown', 'that', 'crp', 'is', 'caused', 'by', 'the', 'heating', 'of', 'twodimensional', 'el... | [-0.1197502826833212, 0.20742774935780275, -0.026413115049699242, 0.03532258083086304, 0.006505900639778291, -0.15154946664623706, 0.05640083308738302, 0.3878052479679316, -0.19973755804584098, -0.37328467603353127, 0.0078112278822284765, -0.3298880843589948, -0.05389156386675969, 0.278727820707144, 0.00919112927464007... |
708.2176 | Link-space formalism for network analysis | We introduce the link-space formalism for analyzing network models with
degree-degree correlations. The formalism is based on a statistical description
of the fraction of links l_{i,j} connecting nodes of degrees i and j. To
demonstrate its use, we apply the framework to some pedagogical network models,
namely, rando... | physics.soc-ph | we introduce the linkspace formalism for analyzing network models with degreedegree correlations the formalism is based on a statistical description of the fraction of links l_ij connecting nodes of degrees i and j to demonstrate its use we apply the framework to some pedagogical network models namely randomattachment ... | [['we', 'introduce', 'the', 'linkspace', 'formalism', 'for', 'analyzing', 'network', 'models', 'with', 'degreedegree', 'correlations', 'the', 'formalism', 'is', 'based', 'on', 'a', 'statistical', 'description', 'of', 'the', 'fraction', 'of', 'links', 'l_ij', 'connecting', 'nodes', 'of', 'degrees', 'i', 'and', 'j', 'to'... | [-0.11440301860125761, 0.06953249240570979, -0.10123426911131655, 0.09049626058942915, -0.05167923364914148, -0.18500256068324922, 0.06746523906681309, 0.3814783951067413, -0.27378095778309414, -0.2818463937178053, 0.0020331286509030475, -0.28049557831390476, -0.22059960107986085, 0.09460038606335434, -0.00833952406144... |
708.2177 | Likelihood based inference for monotone response models | The behavior of maximum likelihood estimates (MLEs) and the likelihood ratio
statistic in a family of problems involving pointwise nonparametric estimation
of a monotone function is studied. This class of problems differs radically
from the usual parametric or semiparametric situations in that the MLE of the
monotone... | math.ST stat.TH | the behavior of maximum likelihood estimates mles and the likelihood ratio statistic in a family of problems involving pointwise nonparametric estimation of a monotone function is studied this class of problems differs radically from the usual parametric or semiparametric situations in that the mle of the monotone func... | [['the', 'behavior', 'of', 'maximum', 'likelihood', 'estimates', 'mles', 'and', 'the', 'likelihood', 'ratio', 'statistic', 'in', 'a', 'family', 'of', 'problems', 'involving', 'pointwise', 'nonparametric', 'estimation', 'of', 'a', 'monotone', 'function', 'is', 'studied', 'this', 'class', 'of', 'problems', 'differs', 'ra... | [-0.08271153259474176, 0.05100679485761422, -0.10432721455152152, 0.12282230877499128, -0.018827762048532988, -0.1432009916389295, 0.05114121972880465, 0.3236206201770416, -0.2294757984287984, -0.27401980996158315, 0.11871847104287792, -0.26967898210021835, -0.13567435906057293, 0.20728703835774345, -0.0937343125944917... |
708.2178 | The S2N2 metallicity calibrator and the abundance gradient of M 33 | We introduce the log(Ha/[SII]6717+6731) vs. log(Ha/[NII]6583) (S2N2)
diagnostic diagram as metallicity and ionisation parameter indicator for HII
regions in external galaxies. The location of HII regions in the S2N2 diagram
was studied both empirically and theoretically. We found that, for a wide range
of metalliciti... | astro-ph | we introduce the loghasii67176731 vs loghanii6583 s2n2 diagnostic diagram as metallicity and ionisation parameter indicator for hii regions in external galaxies the location of hii regions in the s2n2 diagram was studied both empirically and theoretically we found that for a wide range of metallicities the s2n2 diagram... | [['we', 'introduce', 'the', 'loghasii67176731', 'vs', 'loghanii6583', 's2n2', 'diagnostic', 'diagram', 'as', 'metallicity', 'and', 'ionisation', 'parameter', 'indicator', 'for', 'hii', 'regions', 'in', 'external', 'galaxies', 'the', 'location', 'of', 'hii', 'regions', 'in', 'the', 's2n2', 'diagram', 'was', 'studied', '... | [-0.03184242122897915, 0.06498393859139612, -0.06135579324601328, 0.12940098595915034, -0.052726029104544034, -0.034477931919836384, 0.13685718008006612, 0.47503823233658776, -0.10209117480781953, -0.3242193421568064, -0.04466977953344729, -0.2278262124552081, -0.03740355627914872, 0.21723102850556447, -0.0383331119379... |
708.2179 | A simple proof of the matrix-valued Fej\'er-Riesz theorem | A very short proof of the Fej\'er-Riesz lemma is presented in the matrix case
| math.CV | a very short proof of the fejerriesz lemma is presented in the matrix case | [['a', 'very', 'short', 'proof', 'of', 'the', 'fejerriesz', 'lemma', 'is', 'presented', 'in', 'the', 'matrix', 'case']] | [-0.17919405536460026, 0.0296793133020401, -0.15715387942535536, 0.12971899556162367, -0.04444682318717241, -0.16066799176457738, 0.027563190885952542, 0.27865388869707075, -0.24834020648683822, -0.18717826583555766, 0.17288731879255334, -0.20674044949867362, -0.16746557650289365, 0.25479572798524586, -0.12901497306302... |
708.218 | A nonparametric approach to the estimation of lengths and surface areas | The Minkowski content $L_0(G)$ of a body $G\subset{\mathbb{R}}^d$ represents
the boundary length (for $d=2$) or the surface area (for $d=3$) of $G$. A
method for estimating $L_0(G)$ is proposed. It relies on a nonparametric
estimator based on the information provided by a random sample (taken on a
rectangle containin... | math.ST stat.TH | the minkowski content l_0g of a body gsubsetmathbbrd represents the boundary length for d2 or the surface area for d3 of g a method for estimating l_0g is proposed it relies on a nonparametric estimator based on the information provided by a random sample taken on a rectangle containing g in which we are able to identi... | [['the', 'minkowski', 'content', 'l_0g', 'of', 'a', 'body', 'gsubsetmathbbrd', 'represents', 'the', 'boundary', 'length', 'for', 'd2', 'or', 'the', 'surface', 'area', 'for', 'd3', 'of', 'g', 'a', 'method', 'for', 'estimating', 'l_0g', 'is', 'proposed', 'it', 'relies', 'on', 'a', 'nonparametric', 'estimator', 'based', '... | [-0.11604856969598605, 0.022047889133801266, -0.09611073245617505, 0.06270918146379253, -0.06899448411244595, -0.12868398470728068, 0.05366449575034939, 0.38359010580699054, -0.1875224025748974, -0.2497858201267616, 0.175209946413667, -0.2920546718511958, -0.12778497598019942, 0.22731357883680992, -0.11097867597768805,... |
708.2181 | The Phase Structure of Higher-Dimensional Black Rings and Black Holes | We construct an approximate solution for an asymptotically flat, neutral,
thin rotating black ring in any dimension D>=5 by matching the near-horizon
solution for a bent boosted black string, to a linearized gravity solution away
from the horizon. The rotating black ring solution has a regular horizon of
topology S^1... | hep-th | we construct an approximate solution for an asymptotically flat neutral thin rotating black ring in any dimension d5 by matching the nearhorizon solution for a bent boosted black string to a linearized gravity solution away from the horizon the rotating black ring solution has a regular horizon of topology s1 x sd3 and... | [['we', 'construct', 'an', 'approximate', 'solution', 'for', 'an', 'asymptotically', 'flat', 'neutral', 'thin', 'rotating', 'black', 'ring', 'in', 'any', 'dimension', 'd5', 'by', 'matching', 'the', 'nearhorizon', 'solution', 'for', 'a', 'bent', 'boosted', 'black', 'string', 'to', 'a', 'linearized', 'gravity', 'solution... | [-0.21642802881813614, 0.06431237796391422, -0.06922486668610305, 0.11367434125255656, -0.06638768596683071, -0.17408606442179353, 0.015228652100266011, 0.31173174633156686, -0.16008048756885782, -0.24865279146873578, 0.09292125076957283, -0.3290993022872874, -0.09468459432498705, 0.18083906810356196, -0.06063607482670... |
708.2182 | Local rigidity in quaternionic hyperbolic space | In this note, we study deformations of quaternionic hyperbolic lattices in
larger quaternionic hyperbolic spaces and prove local rigidity results. On the
other hand, surface groups are shown to be more flexible in quaternionic
hyperbolic plane than in complex hyperbolic plane.
| math.DG | in this note we study deformations of quaternionic hyperbolic lattices in larger quaternionic hyperbolic spaces and prove local rigidity results on the other hand surface groups are shown to be more flexible in quaternionic hyperbolic plane than in complex hyperbolic plane | [['in', 'this', 'note', 'we', 'study', 'deformations', 'of', 'quaternionic', 'hyperbolic', 'lattices', 'in', 'larger', 'quaternionic', 'hyperbolic', 'spaces', 'and', 'prove', 'local', 'rigidity', 'results', 'on', 'the', 'other', 'hand', 'surface', 'groups', 'are', 'shown', 'to', 'be', 'more', 'flexible', 'in', 'quatern... | [-0.18257711199112236, 0.13466673361410092, -0.07187143567858673, 0.14228928555654952, -0.15787059495725284, -0.13633951503874325, -0.08878321548151534, 0.4271527021759894, -0.25151218707877687, -0.14516692740342965, 0.09979525403823794, -0.27642752411888866, -0.2671983875107111, 0.3117986017974412, -0.1626854942793526... |
708.2183 | Nuclear condensation and the equation of state of nuclear matter | The isothermal compression of a dilute nucleonic gas invoking cluster degrees
of freedom is studied in an equilibrium statistical model; this clusterized
system is found to be more stable than the pure nucleonic system. The equation
of state (EoS) of this matter shows features qualitatively very similar to the
one ob... | nucl-th | the isothermal compression of a dilute nucleonic gas invoking cluster degrees of freedom is studied in an equilibrium statistical model this clusterized system is found to be more stable than the pure nucleonic system the equation of state eos of this matter shows features qualitatively very similar to the one obtained... | [['the', 'isothermal', 'compression', 'of', 'a', 'dilute', 'nucleonic', 'gas', 'invoking', 'cluster', 'degrees', 'of', 'freedom', 'is', 'studied', 'in', 'an', 'equilibrium', 'statistical', 'model', 'this', 'clusterized', 'system', 'is', 'found', 'to', 'be', 'more', 'stable', 'than', 'the', 'pure', 'nucleonic', 'system'... | [-0.11377766175868631, 0.20632505772682788, -0.15390206399929374, 0.0931143116000278, 0.009888682483124132, -0.12365074844115234, 0.029531873300859407, 0.3095992509933079, -0.25178805298070195, -0.2805748410080755, 0.01742922332129997, -0.29730578392994506, -0.04712829452610629, 0.12132095866210509, 0.02424131611659497... |
708.2184 | Monte Carlo likelihood inference for missing data models | We describe a Monte Carlo method to approximate the maximum likelihood
estimate (MLE), when there are missing data and the observed data likelihood is
not available in closed form. This method uses simulated missing data that are
independent and identically distributed and independent of the observed data.
Our Monte ... | math.ST stat.TH | we describe a monte carlo method to approximate the maximum likelihood estimate mle when there are missing data and the observed data likelihood is not available in closed form this method uses simulated missing data that are independent and identically distributed and independent of the observed data our monte carlo a... | [['we', 'describe', 'a', 'monte', 'carlo', 'method', 'to', 'approximate', 'the', 'maximum', 'likelihood', 'estimate', 'mle', 'when', 'there', 'are', 'missing', 'data', 'and', 'the', 'observed', 'data', 'likelihood', 'is', 'not', 'available', 'in', 'closed', 'form', 'this', 'method', 'uses', 'simulated', 'missing', 'dat... | [-0.0565944224751244, 0.05141803972906524, -0.11126187115614475, 0.1715799827501609, -0.061402144115331965, -0.16369479322047145, 0.055907681958396335, 0.3974224567171876, -0.25586792543806414, -0.336527688825434, 0.1360412841884816, -0.3288813222596353, -0.05359059444917538, 0.18737399253640669, -0.02834888210485655, ... |
708.2185 | On combinatorial model categories | Combinatorial model categories were introduced by J. H. Smith as model
categories which are locally presentable and cofibrantly generated. He has not
published his results yet but proofs of some of them were presented by T. Beke
or D. Dugger. We are contributing to this endeavour by proving that weak
equivalences in ... | math.CT | combinatorial model categories were introduced by j h smith as model categories which are locally presentable and cofibrantly generated he has not published his results yet but proofs of some of them were presented by t beke or d dugger we are contributing to this endeavour by proving that weak equivalences in a combin... | [['combinatorial', 'model', 'categories', 'were', 'introduced', 'by', 'j', 'h', 'smith', 'as', 'model', 'categories', 'which', 'are', 'locally', 'presentable', 'and', 'cofibrantly', 'generated', 'he', 'has', 'not', 'published', 'his', 'results', 'yet', 'but', 'proofs', 'of', 'some', 'of', 'them', 'were', 'presented', '... | [-0.0777004279087713, 0.05543019068352658, -0.0632461086985328, 0.13934828607189292, -0.13459485401776997, -0.22707345145376953, 0.022918177727685386, 0.4178827560028514, -0.34377642776313666, -0.30864135316900304, 0.07144815912407294, -0.20964178420301224, -0.12560277299741535, 0.17070798289874015, -0.1714371758060076... |
708.2186 | Monodromy of a Class of Logarithmic Connections on an Elliptic Curve | The logarithmic connections studied in the paper are direct images of regular
connections on line bundles over genus-2 double covers of the elliptic curve.
We give an explicit parametrization of all such connections, determine their
monodromy, differential Galois group and the underlying rank-2 vector bundle.
The lat... | math.AG math-ph math.MP | the logarithmic connections studied in the paper are direct images of regular connections on line bundles over genus2 double covers of the elliptic curve we give an explicit parametrization of all such connections determine their monodromy differential galois group and the underlying rank2 vector bundle the latter is d... | [['the', 'logarithmic', 'connections', 'studied', 'in', 'the', 'paper', 'are', 'direct', 'images', 'of', 'regular', 'connections', 'on', 'line', 'bundles', 'over', 'genus2', 'double', 'covers', 'of', 'the', 'elliptic', 'curve', 'we', 'give', 'an', 'explicit', 'parametrization', 'of', 'all', 'such', 'connections', 'dete... | [-0.2501605584851054, 0.03290004714236587, -0.07894063330270716, 0.11141097839143066, -0.1362047787893136, -0.12624804088540498, -0.026570812947418327, 0.3690038524934503, -0.3320347602005865, -0.22668668771254236, 0.10028963715036507, -0.2544631309822568, -0.18911829098894978, 0.21045516558052574, -0.1314207086049509,... |
708.2187 | Stochastic Variational Integrators | This paper presents a continuous and discrete Lagrangian theory for
stochastic Hamiltonian systems on manifolds. The main result is to derive
stochastic governing equations for such systems from a critical point of a
stochastic action. Using this result the paper derives Langevin-type equations
for constrained mechan... | math.PR | this paper presents a continuous and discrete lagrangian theory for stochastic hamiltonian systems on manifolds the main result is to derive stochastic governing equations for such systems from a critical point of a stochastic action using this result the paper derives langevintype equations for constrained mechanical ... | [['this', 'paper', 'presents', 'a', 'continuous', 'and', 'discrete', 'lagrangian', 'theory', 'for', 'stochastic', 'hamiltonian', 'systems', 'on', 'manifolds', 'the', 'main', 'result', 'is', 'to', 'derive', 'stochastic', 'governing', 'equations', 'for', 'such', 'systems', 'from', 'a', 'critical', 'point', 'of', 'a', 'st... | [-0.1627021589900242, 0.06769751764702743, -0.10307312799520346, 0.0514050487571382, -0.07214144692380926, -0.1175120085887889, -0.0129646738322622, 0.30718944282722727, -0.32714097582519663, -0.2565817553550005, 0.11533627240942902, -0.2266382446178972, -0.22235863934854852, 0.21080527914889546, -0.09886316035842913, ... |
708.2188 | Comparison between Second Variation of Area and Second Variation of
Energy of a Minimal Surface | The conformal parameterisation of a minimal surface is harmonic. Therefore, a
minimal surface is a critical point of both the energy functional and the area
functional. In this paper, we compare the Morse index of a minimal surface as a
critical point of the area functional with its Morse index as a critical point
of... | math.DG | the conformal parameterisation of a minimal surface is harmonic therefore a minimal surface is a critical point of both the energy functional and the area functional in this paper we compare the morse index of a minimal surface as a critical point of the area functional with its morse index as a critical point of the e... | [['the', 'conformal', 'parameterisation', 'of', 'a', 'minimal', 'surface', 'is', 'harmonic', 'therefore', 'a', 'minimal', 'surface', 'is', 'a', 'critical', 'point', 'of', 'both', 'the', 'energy', 'functional', 'and', 'the', 'area', 'functional', 'in', 'this', 'paper', 'we', 'compare', 'the', 'morse', 'index', 'of', 'a'... | [-0.14560458836571652, 0.10737224527945573, -0.12158055086223077, 0.08946411746694859, -0.03715916033184459, -0.0971304973616272, 0.07385335255562249, 0.3076488870744731, -0.22376315471582664, -0.3115753700249186, 0.10024690393867447, -0.2875215095999631, -0.18318190067544465, 0.21319743849710712, -0.11320970722207034,... |
708.2189 | Reconsidering Relativistic Causality | I discuss the idea of relativistic causality, i.e. the requirement that
causal processes or signals can propagate only within the light-cone. After
briefly locating this requirement in the philosophy of causation, my main aim
is to draw philosophers' attention to the fact that it is subtle, indeed
problematic, in rel... | quant-ph | i discuss the idea of relativistic causality ie the requirement that causal processes or signals can propagate only within the lightcone after briefly locating this requirement in the philosophy of causation my main aim is to draw philosophers attention to the fact that it is subtle indeed problematic in relativistic q... | [['i', 'discuss', 'the', 'idea', 'of', 'relativistic', 'causality', 'ie', 'the', 'requirement', 'that', 'causal', 'processes', 'or', 'signals', 'can', 'propagate', 'only', 'within', 'the', 'lightcone', 'after', 'briefly', 'locating', 'this', 'requirement', 'in', 'the', 'philosophy', 'of', 'causation', 'my', 'main', 'ai... | [-0.0789608165808022, 0.12024249463074375, -0.13330895870923995, 0.16632924506161362, -0.15614118336699903, -0.1561468227393925, 0.005952332055196166, 0.332290559515357, -0.274218180000782, -0.28328897469863296, 0.06756416752934456, -0.2508211718760431, -0.20309331621043383, 0.1361329753305763, -0.12359055754262954, -0... |
708.219 | Primitive Divisors of some Lehmer-Pierce Sequences | We study the primitive divisors of the terms of $(\Delta_n)_{n \geq 1}$,
where $\Delta_n=N_{K/ \mathbb{Q}}(u^n-1)$ for $K$ a real quadratic field, and
$u>1$ a unit element of its ring of integers. The methods used allow us to find
the terms of the sequence that do not have a primitive prime divisor.
| math.NT | we study the primitive divisors of the terms of delta_n_n geq 1 where delta_nn_k mathbbqun1 for k a real quadratic field and u1 a unit element of its ring of integers the methods used allow us to find the terms of the sequence that do not have a primitive prime divisor | [['we', 'study', 'the', 'primitive', 'divisors', 'of', 'the', 'terms', 'of', 'delta_n_n', 'geq', '1', 'where', 'delta_nn_k', 'mathbbqun1', 'for', 'k', 'a', 'real', 'quadratic', 'field', 'and', 'u1', 'a', 'unit', 'element', 'of', 'its', 'ring', 'of', 'integers', 'the', 'methods', 'used', 'allow', 'us', 'to', 'find', 'th... | [-0.2065584646576705, 0.05383941746549681, -0.08990462376580884, 0.005838427226990461, -0.062085537773479395, -0.12700733069020012, 0.012891536323877517, 0.2892294766303773, -0.30395078856963664, -0.22541342892994484, 0.08438627261784859, -0.2589381462118278, -0.12753212507232092, 0.1853505723241445, -0.043941985582932... |
708.2191 | The global isoperimetric methodology applied to Kneser's Theorem | We give in the present work a new methodology that allows to give
isoperimetric proofs, for Kneser's Theorem and
Kemperman's structure Theory and most sophisticated results of this type. As
an illustration we present a new proof of Kneser's Theorem.
| math.NT | we give in the present work a new methodology that allows to give isoperimetric proofs for knesers theorem and kempermans structure theory and most sophisticated results of this type as an illustration we present a new proof of knesers theorem | [['we', 'give', 'in', 'the', 'present', 'work', 'a', 'new', 'methodology', 'that', 'allows', 'to', 'give', 'isoperimetric', 'proofs', 'for', 'knesers', 'theorem', 'and', 'kempermans', 'structure', 'theory', 'and', 'most', 'sophisticated', 'results', 'of', 'this', 'type', 'as', 'an', 'illustration', 'we', 'present', 'a'... | [-0.07498098146606935, -0.035781950360615156, -0.20685662794858217, 0.10037949344550726, -0.14043337418697774, -0.15034453012049198, 0.08334838789596688, 0.2882270317990333, -0.20426285671273944, -0.29786852761171756, 0.10881222503667232, -0.18433105480544326, -0.23303117221221328, 0.26828860798850657, -0.1450805756729... |
708.2192 | Stochastic Einstein Locality Revisited | I discuss various formulations of stochastic Einstein locality (SEL), which
is a version of the idea of relativistic causality, i.e. the idea that
influences propagate at most as fast as light. SEL is similar to Reichenbach's
Principle of the Common Cause (PCC), and Bell's Local Causality.
My main aim is to discuss... | quant-ph | i discuss various formulations of stochastic einstein locality sel which is a version of the idea of relativistic causality ie the idea that influences propagate at most as fast as light sel is similar to reichenbachs principle of the common cause pcc and bells local causality my main aim is to discuss formulations of ... | [['i', 'discuss', 'various', 'formulations', 'of', 'stochastic', 'einstein', 'locality', 'sel', 'which', 'is', 'a', 'version', 'of', 'the', 'idea', 'of', 'relativistic', 'causality', 'ie', 'the', 'idea', 'that', 'influences', 'propagate', 'at', 'most', 'as', 'fast', 'as', 'light', 'sel', 'is', 'similar', 'to', 'reichen... | [-0.0823858400392666, 0.11806471510754742, -0.12738345654766636, 0.15723796812408666, -0.09192835776675634, -0.2100741976431308, 0.003572076320015463, 0.32195838424910345, -0.22468814324783756, -0.2613278393214213, 0.07351207572572246, -0.2511583318905407, -0.15196757167862116, 0.13181872664460245, -0.13852343434656308... |
708.2193 | Focusing waves in unknown media by modified time reversal iteration | We study the wave equation in a bounded domain or on a compact Riemannian
manifold with boundary. Assume that we are given the hyperbolic
Neumann-to-Dirichlet map on the boundary corresponding to physical boundary
measurements. We consider how to focus waves, that is, how to find Neumann
boundary values so that at a ... | math.AP math.OC | we study the wave equation in a bounded domain or on a compact riemannian manifold with boundary assume that we are given the hyperbolic neumanntodirichlet map on the boundary corresponding to physical boundary measurements we consider how to focus waves that is how to find neumann boundary values so that at a given ti... | [['we', 'study', 'the', 'wave', 'equation', 'in', 'a', 'bounded', 'domain', 'or', 'on', 'a', 'compact', 'riemannian', 'manifold', 'with', 'boundary', 'assume', 'that', 'we', 'are', 'given', 'the', 'hyperbolic', 'neumanntodirichlet', 'map', 'on', 'the', 'boundary', 'corresponding', 'to', 'physical', 'boundary', 'measure... | [-0.14681116872607103, 0.10856062192951095, -0.08682676376637948, 0.00683959143759768, -0.1257303913346084, -0.11455945781389483, 0.017281121995111354, 0.38347782709428835, -0.29480423841601106, -0.21843659477551874, 0.1543736520582457, -0.2991059274759655, -0.12810779577942893, 0.16708556480030073, -0.0297982649987234... |
708.2194 | Fermionic vacuum polarization in higher-dimensional global monopole
spacetime | In this paper we analyse the vacuum polarization effects associated with a
massless fermionic field in a higher-dimensional global monopole spacetime in
the "braneworld" scenario. In this context we admit that the our Universe, the
bulk, is represented by a flat $(n-1)-$dimensional brane having a global
monopole in a... | hep-th gr-qc | in this paper we analyse the vacuum polarization effects associated with a massless fermionic field in a higherdimensional global monopole spacetime in the braneworld scenario in this context we admit that the our universe the bulk is represented by a flat n1dimensional brane having a global monopole in a extra transve... | [['in', 'this', 'paper', 'we', 'analyse', 'the', 'vacuum', 'polarization', 'effects', 'associated', 'with', 'a', 'massless', 'fermionic', 'field', 'in', 'a', 'higherdimensional', 'global', 'monopole', 'spacetime', 'in', 'the', 'braneworld', 'scenario', 'in', 'this', 'context', 'we', 'admit', 'that', 'the', 'our', 'univ... | [-0.1863299042663791, 0.13607420285015998, -0.06583152458335113, 0.09350028580332156, -0.079481503625184, -0.1029946913547588, -0.027404477632830316, 0.32663635018686155, -0.14914146675304932, -0.2692763178992659, 0.047982775648547846, -0.2455618482205377, -0.138094404220788, 0.0932047146588865, -0.038104263063745966, ... |
708.2195 | Connection between ordinary multinomials, generalized Fibonacci numbers,
partial Bell partition polynomials and convolution powers of discrete uniform
distribution | Using an explicit computable expression of ordinary multinomials, we
establish three remarkable connections, with the q-generalized Fibonacci
sequence, the exponential partial Bell partition polynomials and the density of
convolution powers of the discrete uniform distribution. Identities and various
combinatorial re... | math.CO math.PR | using an explicit computable expression of ordinary multinomials we establish three remarkable connections with the qgeneralized fibonacci sequence the exponential partial bell partition polynomials and the density of convolution powers of the discrete uniform distribution identities and various combinatorial relations... | [['using', 'an', 'explicit', 'computable', 'expression', 'of', 'ordinary', 'multinomials', 'we', 'establish', 'three', 'remarkable', 'connections', 'with', 'the', 'qgeneralized', 'fibonacci', 'sequence', 'the', 'exponential', 'partial', 'bell', 'partition', 'polynomials', 'and', 'the', 'density', 'of', 'convolution', '... | [-0.17864901191067128, 0.0797624663381222, -0.11412465359483447, 0.15841757480631627, -0.09211082836346966, -0.12052018406046998, 0.023490018657563876, 0.3026480808676708, -0.3438355951350656, -0.2587090391011554, 0.0757380042646435, -0.25399172284995164, -0.19444742013833352, 0.16743494439426632, -0.02604899080913691,... |
708.2196 | Superfluid properties of a Bose-Einstein condensate in an optical
lattice confined in a cavity | We study the effect of a one dimensional optical lattice in a cavity field
with quantum properties on the superfluid dynamics of a Bose-Einstein
condensate(BEC). In the cavity the influence of atomic backaction and the
external driving pump become important and strongly modify the optical
potential. Due to the strong... | cond-mat.stat-mech | we study the effect of a one dimensional optical lattice in a cavity field with quantum properties on the superfluid dynamics of a boseeinstein condensatebec in the cavity the influence of atomic backaction and the external driving pump become important and strongly modify the optical potential due to the strong coupli... | [['we', 'study', 'the', 'effect', 'of', 'a', 'one', 'dimensional', 'optical', 'lattice', 'in', 'a', 'cavity', 'field', 'with', 'quantum', 'properties', 'on', 'the', 'superfluid', 'dynamics', 'of', 'a', 'boseeinstein', 'condensatebec', 'in', 'the', 'cavity', 'the', 'influence', 'of', 'atomic', 'backaction', 'and', 'the'... | [-0.20358965800698386, 0.19993872908100987, -0.1066001428898131, -0.0031397574008285496, -0.028395455770110815, -0.14024549370547862, 0.05292562822146823, 0.35794206189640454, -0.2667538093833326, -0.2319789592888248, 0.024589193338695706, -0.24988890789302715, -0.1016944878410255, 0.1810885687944678, 0.045325755549783... |
708.2197 | Piecewise linear regularized solution paths | We consider the generic regularized optimization problem
$\hat{\mathsf{\beta}}(\lambda)=\arg
\min_{\beta}L({\sf{y}},X{\sf{\beta}})+\lambda J({\sf{\beta}})$. Efron, Hastie,
Johnstone and Tibshirani [Ann. Statist. 32 (2004) 407--499] have shown that for
the LASSO--that is, if $L$ is squared error loss and $J(\beta)=\|\... | math.ST stat.ML stat.TH | we consider the generic regularized optimization problem hatmathsfbetalambdaarg min_betalsfyxsfbetalambda jsfbeta efron hastie johnstone and tibshirani ann statist 32 2004 407499 have shown that for the lassothat is if l is squared error loss and jbetabeta_1 is the ell_1 norm of betathe optimal coefficient path is piec... | [['we', 'consider', 'the', 'generic', 'regularized', 'optimization', 'problem', 'hatmathsfbetalambdaarg', 'min_betalsfyxsfbetalambda', 'jsfbeta', 'efron', 'hastie', 'johnstone', 'and', 'tibshirani', 'ann', 'statist', '32', '2004', '407499', 'have', 'shown', 'that', 'for', 'the', 'lassothat', 'is', 'if', 'l', 'is', 'squ... | [-0.07797735531312355, -0.0006819441077823285, -0.058397162536721225, 0.08533095504935773, -0.1316184700044687, -0.18506989624802372, 0.01643992925164639, 0.4044210539505002, -0.3093648534068052, -0.24619662460463587, 0.12357289803458116, -0.244175542742596, -0.21417069196832017, 0.18977802651534148, -0.125268608568148... |
708.2198 | $B_2$-crystals: axioms, structure, models | We present a list of ``local'' axioms and an explicit combinatorial
construction for the regular $B_2$-crystals (crystal graphs of highest weight
integrable modules over $U_q(sp_4)$). Also a new combinatorial model for these
crystals is developed.
| math.RT math.CO | we present a list of local axioms and an explicit combinatorial construction for the regular b_2crystals crystal graphs of highest weight integrable modules over u_qsp_4 also a new combinatorial model for these crystals is developed | [['we', 'present', 'a', 'list', 'of', 'local', 'axioms', 'and', 'an', 'explicit', 'combinatorial', 'construction', 'for', 'the', 'regular', 'b_2crystals', 'crystal', 'graphs', 'of', 'highest', 'weight', 'integrable', 'modules', 'over', 'u_qsp_4', 'also', 'a', 'new', 'combinatorial', 'model', 'for', 'these', 'crystals',... | [-0.09911159574138848, 0.062439373063336294, -0.0554094732541478, 0.06870177167002112, -0.16623607210137628, -0.16181872147276546, 0.04167286574022111, 0.38776546061942074, -0.32628722048618575, -0.24764969397449133, 0.07946748603982004, -0.20093874572635148, -0.16474484437794396, 0.21909467937340113, -0.09562775328981... |
708.2199 | Curves of given $p$-rank with trivial automorphism group | Let $k$ be an algebraically closed field of characteristic $p >0$. Suppose $g
\geq 3$ and $0 \leq f \leq g$. We prove there is a smooth projective $k$-curve
of genus $g$ and $p$-rank $f$ with no non-trivial automorphisms. In addition,
we prove there is a smooth projective hyperelliptic $k$-curve of genus $g$ and
$p$-... | math.NT | let k be an algebraically closed field of characteristic p 0 suppose g geq 3 and 0 leq f leq g we prove there is a smooth projective kcurve of genus g and prank f with no nontrivial automorphisms in addition we prove there is a smooth projective hyperelliptic kcurve of genus g and prank f whose only nontrivial automorp... | [['let', 'k', 'be', 'an', 'algebraically', 'closed', 'field', 'of', 'characteristic', 'p', '0', 'suppose', 'g', 'geq', '3', 'and', '0', 'leq', 'f', 'leq', 'g', 'we', 'prove', 'there', 'is', 'a', 'smooth', 'projective', 'kcurve', 'of', 'genus', 'g', 'and', 'prank', 'f', 'with', 'no', 'nontrivial', 'automorphisms', 'in',... | [-0.3441357642984896, 0.1357655900160196, -0.10276408266575857, -0.032263314652513586, -0.11663206250289049, -0.24003203591096334, -0.02798233112058035, 0.35301866836246404, -0.32667289044836473, -0.24097231670614633, 0.001825901919215832, -0.26324774452816996, -0.1070623140134474, 0.22275652731608214, -0.1544115360419... |
708.22 | Supersymmetric and R symmetric vacua in Wess-Zumino models | In the context of supersymmetric Wess-Zumino models with an R symmetry, we
find some simple conditions on the R-charge content of the theory that imply
the presence or absence of supersymmetric and R-symmetric vacua. The main
result of this work is that the comparison between the number of R-charge 0 and
R-charge 2 s... | hep-th | in the context of supersymmetric wesszumino models with an r symmetry we find some simple conditions on the rcharge content of the theory that imply the presence or absence of supersymmetric and rsymmetric vacua the main result of this work is that the comparison between the number of rcharge 0 and rcharge 2 superfield... | [['in', 'the', 'context', 'of', 'supersymmetric', 'wesszumino', 'models', 'with', 'an', 'r', 'symmetry', 'we', 'find', 'some', 'simple', 'conditions', 'on', 'the', 'rcharge', 'content', 'of', 'the', 'theory', 'that', 'imply', 'the', 'presence', 'or', 'absence', 'of', 'supersymmetric', 'and', 'rsymmetric', 'vacua', 'the... | [-0.15575769011271545, 0.14408738755908138, -0.03567346467081314, 0.10307670006407604, -0.05800081745613939, -0.17016020303484625, 0.008813514722323116, 0.32990337054854113, -0.1748915494983801, -0.29067161471847125, 0.0877718969792253, -0.2711452810595242, -0.16055947124438646, 0.06794863060349599, -0.0424061348267759... |
708.2201 | A Modified Borel Summation Technique | We compare and contrast three different perturbative expansions for the
quartic anharmonic oscillator wavefunction and apply a modified Borel summation
technique to determine the energy eigenvalues. In the first two expansions this
provides the energy eigenvalues directly however in the third method we tune
the wavef... | quant-ph hep-th | we compare and contrast three different perturbative expansions for the quartic anharmonic oscillator wavefunction and apply a modified borel summation technique to determine the energy eigenvalues in the first two expansions this provides the energy eigenvalues directly however in the third method we tune the wavefunc... | [['we', 'compare', 'and', 'contrast', 'three', 'different', 'perturbative', 'expansions', 'for', 'the', 'quartic', 'anharmonic', 'oscillator', 'wavefunction', 'and', 'apply', 'a', 'modified', 'borel', 'summation', 'technique', 'to', 'determine', 'the', 'energy', 'eigenvalues', 'in', 'the', 'first', 'two', 'expansions',... | [-0.09564846623688936, 0.03703396555959314, -0.1155021685707782, 0.1283017926283979, -0.0814450815320015, -0.11188150492629835, 0.09023623233882799, 0.36476129744024505, -0.22981459750306038, -0.3148449628879981, 0.01675765601075476, -0.26526269447294043, -0.1001284931697661, 0.19149387308529445, -0.04460257184469984, ... |
708.2202 | Locally compact quantum groups. Radford's $S^4$ formula | Let $A$ be a finite-dimensional Hopf algebra. The left and the right
integrals on $A$ are related by means of a distinguished group-like element
$\delta$ of $A$. Similarly, there is this element $\hat\delta$ in the dual Hopf
algebra $\hat A$. Radford showed that
$$S^4(a)=\delta^{-1}(\hat\delta\triangleright a \triang... | math.QA math.OA | let a be a finitedimensional hopf algebra the left and the right integrals on a are related by means of a distinguished grouplike element delta of a similarly there is this element hatdelta in the dual hopf algebra hat a radford showed that s4adelta1hatdeltatriangleright a triangleleft hatdelta1delta for all a in a whe... | [['let', 'a', 'be', 'a', 'finitedimensional', 'hopf', 'algebra', 'the', 'left', 'and', 'the', 'right', 'integrals', 'on', 'a', 'are', 'related', 'by', 'means', 'of', 'a', 'distinguished', 'grouplike', 'element', 'delta', 'of', 'a', 'similarly', 'there', 'is', 'this', 'element', 'hatdelta', 'in', 'the', 'dual', 'hopf', ... | [-0.1316644344971994, 0.11320373484575409, -0.10722752215030293, 0.06756839632677535, -0.12116514410202701, -0.1543565937809439, 0.008958099647295764, 0.3360133746328453, -0.31582678434852923, -0.1676641784504884, 0.1404565451501791, -0.2538411906713413, -0.15111202501898838, 0.25366075833444485, -0.13604952756068087, ... |
708.2203 | Earthquake Networks, Complex | An article for the Springer Encyclopedia of Complexity and System Science
| physics.geo-ph physics.soc-ph | an article for the springer encyclopedia of complexity and system science | [['an', 'article', 'for', 'the', 'springer', 'encyclopedia', 'of', 'complexity', 'and', 'system', 'science']] | [-0.11437669565731828, -0.02466757903378245, -0.06745350473052399, -0.05634508485143835, -0.0648129480806264, -0.02582298998128284, -0.03581696291538802, 0.17664538662541995, -0.3992205770178275, -0.43649452907795255, 0.13574211451817642, -0.3077561523426663, -0.2697455883026123, 0.2723060373894193, -0.2373923274942419... |
708.2204 | Integral-Field Spectroscopy of the Post Red Supergiant IRC +10420:
evidence for an axi-symmetric wind | We present NAOMI/OASIS adaptive-optics assisted integral-field spectroscopy
of the transitional massive hypergiant IRC +10420, an extreme mass-losing star
apparently in the process of evolving from a Red Supergiant toward the
Wolf-Rayet phase. To investigate the present-day mass-loss geometry of the
star, we study th... | astro-ph | we present naomioasis adaptiveoptics assisted integralfield spectroscopy of the transitional massive hypergiant irc 10420 an extreme masslosing star apparently in the process of evolving from a red supergiant toward the wolfrayet phase to investigate the presentday massloss geometry of the star we study the appearance ... | [['we', 'present', 'naomioasis', 'adaptiveoptics', 'assisted', 'integralfield', 'spectroscopy', 'of', 'the', 'transitional', 'massive', 'hypergiant', 'irc', '10420', 'an', 'extreme', 'masslosing', 'star', 'apparently', 'in', 'the', 'process', 'of', 'evolving', 'from', 'a', 'red', 'supergiant', 'toward', 'the', 'wolfray... | [-0.08276622023353455, 0.08668304398804803, -0.08551034514555884, 0.05416986881082378, -0.10386263850563565, -0.07136477936527755, 0.06047553293538377, 0.4456437089097646, -0.17923752243339192, -0.27020965702688904, 0.07214284641168257, -0.26112733492227785, -0.11008043898458084, 0.15749850013704708, -0.076746778117179... |
708.2205 | Axisymmetric orbit models of N-body merger remnants: a dependency of
reconstructed mass on viewing angle | We model mock observations of collisionless N-body disc-disc mergers with an
axisymmetric orbit superposition program that has been used to model Coma
ellipticals. The remnants sample representatively the shapes of disc-disc
mergers including prolate, triaxial and oblate objects. The aim is to better
understand how t... | astro-ph | we model mock observations of collisionless nbody discdisc mergers with an axisymmetric orbit superposition program that has been used to model coma ellipticals the remnants sample representatively the shapes of discdisc mergers including prolate triaxial and oblate objects the aim is to better understand how the assum... | [['we', 'model', 'mock', 'observations', 'of', 'collisionless', 'nbody', 'discdisc', 'mergers', 'with', 'an', 'axisymmetric', 'orbit', 'superposition', 'program', 'that', 'has', 'been', 'used', 'to', 'model', 'coma', 'ellipticals', 'the', 'remnants', 'sample', 'representatively', 'the', 'shapes', 'of', 'discdisc', 'mer... | [-0.08510200605227577, 0.11379338139592653, -0.09395357187733883, 0.13743414855389682, -0.09562780400910587, -0.07951450348935193, -0.04271807058033085, 0.42722857412364745, -0.16672489015316522, -0.39061089133567833, 0.042264498301557506, -0.25252770797384005, -0.01743174404061089, 0.17789440284731325, -0.048614622637... |
708.2206 | Role of electrostatics in the texture of islands in free standing
ferroelectric liquid crystal films | Curved textures of ferroelectric smectic C* liquid crystals produce space
charge when they involve divergence of the spontaneous polarization field.
Impurity ions can partially screen this space charge, reducing long range
interactions to local ones. Through studies of the textures of islands on very
thin free-standi... | cond-mat.soft | curved textures of ferroelectric smectic c liquid crystals produce space charge when they involve divergence of the spontaneous polarization field impurity ions can partially screen this space charge reducing long range interactions to local ones through studies of the textures of islands on very thin freestanding smec... | [['curved', 'textures', 'of', 'ferroelectric', 'smectic', 'c', 'liquid', 'crystals', 'produce', 'space', 'charge', 'when', 'they', 'involve', 'divergence', 'of', 'the', 'spontaneous', 'polarization', 'field', 'impurity', 'ions', 'can', 'partially', 'screen', 'this', 'space', 'charge', 'reducing', 'long', 'range', 'inte... | [-0.1662281089755256, 0.2448801871223916, -0.03328256616828918, 0.04126775345479649, -0.06835809175015217, -0.13370237361466994, 0.047823388722815344, 0.4171842704376867, -0.28895979083233303, -0.29714713364298784, 0.02043864183736244, -0.27521553484632844, -0.11138960137031972, 0.09165114891197111, 0.02768105756483912... |
708.2207 | Statistical inferences for functional data | With modern technology development, functional data are being observed
frequently in many scientific fields. A popular method for analyzing such
functional data is ``smoothing first, then estimation.'' That is, statistical
inference such as estimation and hypothesis testing about functional data is
conducted based on... | math.ST stat.TH | with modern technology development functional data are being observed frequently in many scientific fields a popular method for analyzing such functional data is smoothing first then estimation that is statistical inference such as estimation and hypothesis testing about functional data is conducted based on the substi... | [['with', 'modern', 'technology', 'development', 'functional', 'data', 'are', 'being', 'observed', 'frequently', 'in', 'many', 'scientific', 'fields', 'a', 'popular', 'method', 'for', 'analyzing', 'such', 'functional', 'data', 'is', 'smoothing', 'first', 'then', 'estimation', 'that', 'is', 'statistical', 'inference', '... | [-0.06081822697694103, 0.02421439224126516, -0.11903368054233768, 0.15309348993986432, -0.06821906399585445, -0.11417100852596815, 0.06024781064026886, 0.38742879120012125, -0.25904461591228567, -0.29958361769095065, 0.1528879650458866, -0.2691995636197842, -0.1848537935504552, 0.2002607402495212, -0.06652412112905748,... |
708.2208 | Wrapping interactions at strong coupling -- the giant magnon | We derive generalized Luscher formulas for finite size corrections in a
theory with a general dispersion relation. For the AdS_5xS^5 superstring these
formulas encode leading wrapping interaction effects. We apply the generalized
mu-term formula to calculate finite size corrections to the dispersion relation
of the g... | hep-th | we derive generalized luscher formulas for finite size corrections in a theory with a general dispersion relation for the ads_5xs5 superstring these formulas encode leading wrapping interaction effects we apply the generalized muterm formula to calculate finite size corrections to the dispersion relation of the giant m... | [['we', 'derive', 'generalized', 'luscher', 'formulas', 'for', 'finite', 'size', 'corrections', 'in', 'a', 'theory', 'with', 'a', 'general', 'dispersion', 'relation', 'for', 'the', 'ads_5xs5', 'superstring', 'these', 'formulas', 'encode', 'leading', 'wrapping', 'interaction', 'effects', 'we', 'apply', 'the', 'generaliz... | [-0.15231286439082617, 0.12382003303187397, -0.09396910759016544, 0.17067128844088414, -0.10513687782132855, -0.12686773119391975, 0.06689498328301892, 0.26295158926111, -0.19310136805390837, -0.25983048726262137, 0.009716585815812532, -0.2747370911107122, -0.09308426514022299, 0.16899839661513957, 0.002147299377631478... |
708.2209 | Extremality conditions for isolated and dynamical horizons | A maximally rotating Kerr black hole is said to be extremal. In this paper we
introduce the corresponding restrictions for isolated and dynamical horizons.
These reduce to the standard notions for Kerr but in general do not require the
horizon to be either stationary or rotationally symmetric. We consider physical
im... | gr-qc | a maximally rotating kerr black hole is said to be extremal in this paper we introduce the corresponding restrictions for isolated and dynamical horizons these reduce to the standard notions for kerr but in general do not require the horizon to be either stationary or rotationally symmetric we consider physical implica... | [['a', 'maximally', 'rotating', 'kerr', 'black', 'hole', 'is', 'said', 'to', 'be', 'extremal', 'in', 'this', 'paper', 'we', 'introduce', 'the', 'corresponding', 'restrictions', 'for', 'isolated', 'and', 'dynamical', 'horizons', 'these', 'reduce', 'to', 'the', 'standard', 'notions', 'for', 'kerr', 'but', 'in', 'general'... | [-0.11186713887720451, 0.12387842470278987, -0.08716992181548967, 0.11202275440173483, -0.12074959970704174, -0.15669235866664188, -0.00032868487259396647, 0.3570430237988505, -0.22198865421210665, -0.23443365705352795, 0.16883222353821503, -0.2670190803518024, -0.12773192498561797, 0.1876375830564294, -0.1426075686202... |
708.221 | Intersection theory from duality and replica | Kontsevich's work on Airy matrix integrals has led to explicit results for
the intersection numbers of the moduli space of curves. In this article we show
that a duality between k-point functions on $N\times N$ matrices and N-point
functions of $k\times k$ matrices, plus the replica method, familiar in the
theory of ... | hep-th math-ph math.MP | kontsevichs work on airy matrix integrals has led to explicit results for the intersection numbers of the moduli space of curves in this article we show that a duality between kpoint functions on ntimes n matrices and npoint functions of ktimes k matrices plus the replica method familiar in the theory of disordered sys... | [['kontsevichs', 'work', 'on', 'airy', 'matrix', 'integrals', 'has', 'led', 'to', 'explicit', 'results', 'for', 'the', 'intersection', 'numbers', 'of', 'the', 'moduli', 'space', 'of', 'curves', 'in', 'this', 'article', 'we', 'show', 'that', 'a', 'duality', 'between', 'kpoint', 'functions', 'on', 'ntimes', 'n', 'matrice... | [-0.1572259612461572, 0.08249767256981408, -0.1313623614954732, 0.06759301732013863, -0.07170845454017963, -0.1083102200670989, 0.06707899147264099, 0.3483211794087002, -0.2645491524349137, -0.24996895572453517, 0.04320351485543514, -0.2886478705608639, -0.2298023430154889, 0.20327283506111432, -0.09226128439949725, 0.... |
708.2211 | Optical characterization of GaN by N+ implantation into GaAs at elevated
temperature | Both hexagonal wurtzite and cubic zinc blend GaN phases were synthesized in
GaAs by 50 keV N+ implantation at 400 deg C and subsequent annealing at 900 deg
C for 15 min in N2 ambient. Crystallographic structural and Raman scattering
studies revealed that GaN phases were grown for fluence above 2x1017 cm-2.
Temperatur... | cond-mat.mtrl-sci | both hexagonal wurtzite and cubic zinc blend gan phases were synthesized in gaas by 50 kev n implantation at 400 deg c and subsequent annealing at 900 deg c for 15 min in n2 ambient crystallographic structural and raman scattering studies revealed that gan phases were grown for fluence above 2x1017 cm2 temperaturedepen... | [['both', 'hexagonal', 'wurtzite', 'and', 'cubic', 'zinc', 'blend', 'gan', 'phases', 'were', 'synthesized', 'in', 'gaas', 'by', '50', 'kev', 'n', 'implantation', 'at', '400', 'deg', 'c', 'and', 'subsequent', 'annealing', 'at', '900', 'deg', 'c', 'for', '15', 'min', 'in', 'n2', 'ambient', 'crystallographic', 'structural... | [-0.041081114847347444, 0.2375191581135762, 0.08259637174244548, -0.045723108261506815, 0.05994878637546808, -0.1932841380482021, 0.12022282198052277, 0.5387579458813692, -0.2238761421830691, -0.4099005637384385, 0.009619454044330213, -0.39161000984538463, -0.03032844447165958, 0.14492116174804642, 0.07729975781979558,... |
708.2212 | Enumerative Properties of NC^B(p,q) | We determine the rank generating function, the zeta polynomial and the
Moebius function for the poset NC^B(p,q) of annular non-crossing partitions of
type B, where p and q are two positive integers. We give an alternative
treatment of some of these results in the case q=1, for which this poset is a
lattice. We also c... | math.CO math.GR | we determine the rank generating function the zeta polynomial and the moebius function for the poset ncbpq of annular noncrossing partitions of type b where p and q are two positive integers we give an alternative treatment of some of these results in the case q1 for which this poset is a lattice we also consider the g... | [['we', 'determine', 'the', 'rank', 'generating', 'function', 'the', 'zeta', 'polynomial', 'and', 'the', 'moebius', 'function', 'for', 'the', 'poset', 'ncbpq', 'of', 'annular', 'noncrossing', 'partitions', 'of', 'type', 'b', 'where', 'p', 'and', 'q', 'are', 'two', 'positive', 'integers', 'we', 'give', 'an', 'alternativ... | [-0.1875548489008318, 0.09640872557527687, -0.035152723990819035, 0.0698111557004535, -0.06581402078051778, -0.11283451555954183, 0.068466766923666, 0.30518515815629677, -0.3051731395863873, -0.21865274100290502, 0.029865936032386825, -0.24380009827368399, -0.13736300262458184, 0.14428499010117615, -0.07412117564064614... |
708.2213 | Moderate Growth Time Series for Dynamic Combinatorics Modelisation | Here, we present a family of time series with a simple growth constraint.
This family can be the basis of a model to apply to emerging computation in
business and micro-economy where global functions can be expressed from local
rules. We explicit a double statistics on these series which allows to
establish a one-to-... | cs.SC cs.MA math.CO | here we present a family of time series with a simple growth constraint this family can be the basis of a model to apply to emerging computation in business and microeconomy where global functions can be expressed from local rules we explicit a double statistics on these series which allows to establish a onetoone corr... | [['here', 'we', 'present', 'a', 'family', 'of', 'time', 'series', 'with', 'a', 'simple', 'growth', 'constraint', 'this', 'family', 'can', 'be', 'the', 'basis', 'of', 'a', 'model', 'to', 'apply', 'to', 'emerging', 'computation', 'in', 'business', 'and', 'microeconomy', 'where', 'global', 'functions', 'can', 'be', 'expre... | [-0.1135248152473778, 0.04945698019378541, -0.13349931353801175, 0.05250663920346517, -0.11262509299507528, -0.09954347560312926, 0.08589959505275545, 0.36607777921221496, -0.33417477465251033, -0.29875676076565133, 0.11184016535704008, -0.20797030114300197, -0.1888915052343356, 0.21517157975763998, -0.0326173501737669... |
708.2214 | On the p-th root of a p-adic number | We give a sufficient and necessary condition for a p-adic integer to have
p-th root in the ring of p-adic integers. The same condition holds clearly for
residues modulo p^k. We give a proof that Fermat's last theorem is false for
p-adic integers and for residues mod p^k.
| math.NT | we give a sufficient and necessary condition for a padic integer to have pth root in the ring of padic integers the same condition holds clearly for residues modulo pk we give a proof that fermats last theorem is false for padic integers and for residues mod pk | [['we', 'give', 'a', 'sufficient', 'and', 'necessary', 'condition', 'for', 'a', 'padic', 'integer', 'to', 'have', 'pth', 'root', 'in', 'the', 'ring', 'of', 'padic', 'integers', 'the', 'same', 'condition', 'holds', 'clearly', 'for', 'residues', 'modulo', 'pk', 'we', 'give', 'a', 'proof', 'that', 'fermats', 'last', 'theo... | [-0.28912753507029265, 0.04449097830123113, -0.21579572783472636, 0.11663940055344331, -0.07860941978772946, -0.19582294735785885, 0.007274683957803063, 0.2180445308816464, -0.28463359371138114, -0.18758715246804059, 0.012263751188584138, -0.2105291747720912, -0.14564609197259415, 0.22734563196233162, -0.10120350275731... |
708.2215 | Polarization rotation for light propagating non-parallel to a magnetic
field in QED vacuum and in a dilute electron gas | The rotation of the polarization vector for light propagating perpendicular
to an external constant external magnetic field $B$, is calculated in quantum
vacuum, where it leads to different photon eigenmodes of the magnetized photon
self-energy tensor for polarizations along and orthogonal to $B$ (Cotton-Mouton
effec... | hep-ph | the rotation of the polarization vector for light propagating perpendicular to an external constant external magnetic field b is calculated in quantum vacuum where it leads to different photon eigenmodes of the magnetized photon selfenergy tensor for polarizations along and orthogonal to b cottonmouton effect in qed va... | [['the', 'rotation', 'of', 'the', 'polarization', 'vector', 'for', 'light', 'propagating', 'perpendicular', 'to', 'an', 'external', 'constant', 'external', 'magnetic', 'field', 'b', 'is', 'calculated', 'in', 'quantum', 'vacuum', 'where', 'it', 'leads', 'to', 'different', 'photon', 'eigenmodes', 'of', 'the', 'magnetized... | [-0.15082128317253163, 0.2473848089758399, -0.0192916664301149, 0.04120940325747326, -0.04942608619696342, -0.10328458072680155, -0.0055521052477618795, 0.3727199307099085, -0.21868901426947657, -0.2988382077622759, 0.020208540169409657, -0.297793235617296, -0.03213812838364768, 0.21858589429933353, 0.03878359377209172... |
708.2216 | Experimental joint signal-idler quasi-distributions and photon-number
statistics for mesoscopic twin beams | Joint signal-idler photoelectron distributions of twin beams containing
several tens of photons per mode have been measured recently. Exploiting a
microscopic quantum theory for joint quasi-distributions in parametric
down-conversion developed earlier we characterize properties of twin beams in
terms of quasi-distrib... | quant-ph | joint signalidler photoelectron distributions of twin beams containing several tens of photons per mode have been measured recently exploiting a microscopic quantum theory for joint quasidistributions in parametric downconversion developed earlier we characterize properties of twin beams in terms of quasidistributions ... | [['joint', 'signalidler', 'photoelectron', 'distributions', 'of', 'twin', 'beams', 'containing', 'several', 'tens', 'of', 'photons', 'per', 'mode', 'have', 'been', 'measured', 'recently', 'exploiting', 'a', 'microscopic', 'quantum', 'theory', 'for', 'joint', 'quasidistributions', 'in', 'parametric', 'downconversion', '... | [-0.05058424256276339, 0.2135669709654686, -0.1215657086491033, 0.10441238358386873, 0.0021645921357205987, -0.1199599849232645, -0.006147520094937472, 0.4599383119493723, -0.22023207429842448, -0.32280311377052173, -0.01406672292670672, -0.296469399659538, -0.021374554660769155, 0.23745879411042012, -0.025995346502311... |
708.2217 | Ferromagnetism in cobalt doped n-GaN | Ferromagnetic ordering is reported in the post-annealed samples of Co doped
n-GaN formed by Co+ implantation. A maximum Curie temperature ~ 250K is
recorded for the sample with 8 atomic percent Co. Particle induced x-ray
emission-channeling study confirmed the substitutional Co in Ga lattice site.
Local atomic arrang... | cond-mat.mtrl-sci | ferromagnetic ordering is reported in the postannealed samples of co doped ngan formed by co implantation a maximum curie temperature 250k is recorded for the sample with 8 atomic percent co particle induced xray emissionchanneling study confirmed the substitutional co in ga lattice site local atomic arrangement around... | [['ferromagnetic', 'ordering', 'is', 'reported', 'in', 'the', 'postannealed', 'samples', 'of', 'co', 'doped', 'ngan', 'formed', 'by', 'co', 'implantation', 'a', 'maximum', 'curie', 'temperature', '250k', 'is', 'recorded', 'for', 'the', 'sample', 'with', '8', 'atomic', 'percent', 'co', 'particle', 'induced', 'xray', 'em... | [-0.11612370942492743, 0.2698407847988042, 0.116885227299094, 0.028939700990638417, 0.02742452237352326, -0.14001204450992313, 0.12112848338595517, 0.47275664372923404, -0.21210356446838863, -0.3209633438822788, -0.05769710395032087, -0.38617155877118176, -0.018372539481198467, 0.08757552318746929, 0.16815179515932058,... |
708.2218 | Tensoring with infinite-dimensional modules in $\scr O_0$ | We show that the principal block $\scr O_0$ of the BGG category $\scr O$ for
a semisimple Lie algebra $\germ g$ acts faithfully on itself via exact
endofunctors which preserve tilting modules, via right exact endofunctors which
preserve projective modules and via left exact endofunctors which preserve
injective modul... | math.RT | we show that the principal block scr o_0 of the bgg category scr o for a semisimple lie algebra germ g acts faithfully on itself via exact endofunctors which preserve tilting modules via right exact endofunctors which preserve projective modules and via left exact endofunctors which preserve injective modules the origi... | [['we', 'show', 'that', 'the', 'principal', 'block', 'scr', 'o_0', 'of', 'the', 'bgg', 'category', 'scr', 'o', 'for', 'a', 'semisimple', 'lie', 'algebra', 'germ', 'g', 'acts', 'faithfully', 'on', 'itself', 'via', 'exact', 'endofunctors', 'which', 'preserve', 'tilting', 'modules', 'via', 'right', 'exact', 'endofunctors'... | [-0.15622851493006404, -0.009196550495239948, -0.024211830738931895, 0.0733982279388742, -0.14651521509724924, -0.16667959276925434, -0.04537770666224374, 0.414580749720335, -0.4118028861047192, -0.14769621946933595, 0.10213898764394054, -0.1678186665114481, -0.14295412901026958, 0.14451953172260387, -0.178688515202057... |
708.2219 | On the $\mathbb{L}_p$-error of monotonicity constrained estimators | We aim at estimating a function $\lambda:[0,1]\to \mathbb {R}$, subject to
the constraint that it is decreasing (or increasing). We provide a unified
approach for studying the $\mathbb {L}_p$-loss of an estimator defined as the
slope of a concave (or convex) approximation of an estimator of a primitive of
$\lambda$, ... | math.ST stat.TH | we aim at estimating a function lambda01to mathbb r subject to the constraint that it is decreasing or increasing we provide a unified approach for studying the mathbb l_ploss of an estimator defined as the slope of a concave or convex approximation of an estimator of a primitive of lambda based on n observations our m... | [['we', 'aim', 'at', 'estimating', 'a', 'function', 'lambda01to', 'mathbb', 'r', 'subject', 'to', 'the', 'constraint', 'that', 'it', 'is', 'decreasing', 'or', 'increasing', 'we', 'provide', 'a', 'unified', 'approach', 'for', 'studying', 'the', 'mathbb', 'l_ploss', 'of', 'an', 'estimator', 'defined', 'as', 'the', 'slope... | [-0.09296431829635468, 0.027914897959514445, -0.1027196409187228, 0.06595067309744233, -0.026735628917877976, -0.13824383360851142, 0.031561760926302265, 0.35500735365268254, -0.2719634721870534, -0.22229700575634423, 0.13178802870728154, -0.28731030214435627, -0.16249234630474044, 0.18067104361155847, -0.1005384064224... |
708.222 | HIPPARCOS Astrometric Orbit and Evolutionary Status of HR 6046 | The previously known, 6-yr spectroscopic binary HR 6046 has been speculated
in the past to contain a compact object as the secondary. A recent study has
re-determined the orbit with great accuracy, and shown that the companion is an
evolved but otherwise normal star of nearly identical mass as the primary,
which is a... | astro-ph | the previously known 6yr spectroscopic binary hr 6046 has been speculated in the past to contain a compact object as the secondary a recent study has redetermined the orbit with great accuracy and shown that the companion is an evolved but otherwise normal star of nearly identical mass as the primary which is also a gi... | [['the', 'previously', 'known', '6yr', 'spectroscopic', 'binary', 'hr', '6046', 'has', 'been', 'speculated', 'in', 'the', 'past', 'to', 'contain', 'a', 'compact', 'object', 'as', 'the', 'secondary', 'a', 'recent', 'study', 'has', 'redetermined', 'the', 'orbit', 'with', 'great', 'accuracy', 'and', 'shown', 'that', 'the'... | [-0.09900529596965522, 0.10440097504927098, -0.10160888912118721, 0.03557244779998374, -0.10902634789954696, -0.07706631408791814, 0.06698386975245288, 0.3782317490010654, -0.178738870731033, -0.3627058269968569, 0.13185845528441736, -0.2666570890894872, -0.0836643137587797, 0.18421950199697543, -0.09605426458491875, 0... |
708.2221 | Nitrogen ion beam synthesis of InN in InP (100) at elevated temperature | InN phase is grown in crystalline InP(100) substrates by 50 keV N+
implantation at an elevated temperature of 400 deg C followed by annealing at
525 deg C in N2 ambient. Crystallographic structural and Raman scattering
studies are performed for the characterization of grown phases. Temperature-
and power-dependent ph... | cond-mat.mtrl-sci | inn phase is grown in crystalline inp100 substrates by 50 kev n implantation at an elevated temperature of 400 deg c followed by annealing at 525 deg c in n2 ambient crystallographic structural and raman scattering studies are performed for the characterization of grown phases temperature and powerdependent photolumine... | [['inn', 'phase', 'is', 'grown', 'in', 'crystalline', 'inp100', 'substrates', 'by', '50', 'kev', 'n', 'implantation', 'at', 'an', 'elevated', 'temperature', 'of', '400', 'deg', 'c', 'followed', 'by', 'annealing', 'at', '525', 'deg', 'c', 'in', 'n2', 'ambient', 'crystallographic', 'structural', 'and', 'raman', 'scatteri... | [-0.0824097727836911, 0.30866042114381387, -0.012666966852753661, -0.08490615149521334, 0.10321122995675217, -0.17914661885845626, 0.11587294134268061, 0.5236910588681958, -0.22426079867710902, -0.36855029262775596, 0.034645494395802015, -0.3404847602468244, 0.034282666733921614, 0.19732588356858943, 0.0844893066407462... |
708.2222 | On the occurrence of oscillatory modulations in the power-law behavior
of dynamic and kinetic processes in fractals | The dynamic and kinetic behavior of processes occurring in fractals with
spatial discrete scale invariance (DSI) is considered. Spatial DSI implies the
existence of a fundamental scaling ratio (b_1). We address time-dependent
physical processes, which as a consequence of the time evolution develop a
characteristic le... | cond-mat.stat-mech | the dynamic and kinetic behavior of processes occurring in fractals with spatial discrete scale invariance dsi is considered spatial dsi implies the existence of a fundamental scaling ratio b_1 we address timedependent physical processes which as a consequence of the time evolution develop a characteristic length of th... | [['the', 'dynamic', 'and', 'kinetic', 'behavior', 'of', 'processes', 'occurring', 'in', 'fractals', 'with', 'spatial', 'discrete', 'scale', 'invariance', 'dsi', 'is', 'considered', 'spatial', 'dsi', 'implies', 'the', 'existence', 'of', 'a', 'fundamental', 'scaling', 'ratio', 'b_1', 'we', 'address', 'timedependent', 'ph... | [-0.18274894968420266, 0.2120921202711761, -0.09967792327050119, 0.09117543811498036, -0.015343205061741173, -0.12414617608673871, 0.031589932643808424, 0.30643300822377206, -0.31159423860907554, -0.2573604637607932, 0.06298584918119013, -0.20494470223411917, -0.15430115231126545, 0.15288664247840644, 0.051231146685779... |
708.2223 | Tau decay and the structure of the a1 | We analyse the decay $\tau\to\pi\pi\pi\nu$ based on the recently developed
techniques to generate axial-vector resonances dynamically. Under the
assumption that the a1 is a coupled-channel meson-molecule, the spectral
function is described surprisingly well by adjusting only one free parameter.
Including, in addition... | hep-ph nucl-th | we analyse the decay tautopipipinu based on the recently developed techniques to generate axialvector resonances dynamically under the assumption that the a1 is a coupledchannel mesonmolecule the spectral function is described surprisingly well by adjusting only one free parameter including in addition an elementary a1... | [['we', 'analyse', 'the', 'decay', 'tautopipipinu', 'based', 'on', 'the', 'recently', 'developed', 'techniques', 'to', 'generate', 'axialvector', 'resonances', 'dynamically', 'under', 'the', 'assumption', 'that', 'the', 'a1', 'is', 'a', 'coupledchannel', 'mesonmolecule', 'the', 'spectral', 'function', 'is', 'described'... | [-0.07330701945592528, 0.17893681746341905, -0.09224702678013431, 0.0936523515417281, -0.06115152850828093, -0.15114213913962568, 0.029626546063176964, 0.3646965157240629, -0.23162463922863422, -0.251024063150196, 0.08346726295143447, -0.22242764772280402, -0.14209575708272218, 0.1605345102776166, -0.001113589772063752... |
708.2224 | Squeezed-light generation in a nonlinear planar waveguide with a
periodic corrugation | Two-mode nonlinear interaction (second-harmonic and second-subharmonic
generation) in a planar waveguide with a small periodic corrugation at the
surface is studied. Scattering of the interacting fields on the corrugation
leads to constructive interference that enhances the nonlinear process provided
that all the int... | quant-ph | twomode nonlinear interaction secondharmonic and secondsubharmonic generation in a planar waveguide with a small periodic corrugation at the surface is studied scattering of the interacting fields on the corrugation leads to constructive interference that enhances the nonlinear process provided that all the interaction... | [['twomode', 'nonlinear', 'interaction', 'secondharmonic', 'and', 'secondsubharmonic', 'generation', 'in', 'a', 'planar', 'waveguide', 'with', 'a', 'small', 'periodic', 'corrugation', 'at', 'the', 'surface', 'is', 'studied', 'scattering', 'of', 'the', 'interacting', 'fields', 'on', 'the', 'corrugation', 'leads', 'to', ... | [-0.15803123741995456, 0.181763825006783, -0.01834146169672157, 0.03806568604436189, -0.02418114745253047, -0.148031394294501, -0.008383229500776546, 0.44358980698987494, -0.21425735911484375, -0.2896569493811491, 0.059150133280592515, -0.2633087930031294, -0.13800094464555557, 0.2443516102814397, 0.016672285728503104,... |
708.2225 | On equimultiple modules | We study the class of equimultiple modules. In particular, we prove several
criteria for an equimultiple module to be a complete intersection and prove the
openness of the equimultiple locus of an ideal module.
| math.AC math.AG | we study the class of equimultiple modules in particular we prove several criteria for an equimultiple module to be a complete intersection and prove the openness of the equimultiple locus of an ideal module | [['we', 'study', 'the', 'class', 'of', 'equimultiple', 'modules', 'in', 'particular', 'we', 'prove', 'several', 'criteria', 'for', 'an', 'equimultiple', 'module', 'to', 'be', 'a', 'complete', 'intersection', 'and', 'prove', 'the', 'openness', 'of', 'the', 'equimultiple', 'locus', 'of', 'an', 'ideal', 'module']] | [-0.20077460856341264, -0.07085693985658616, -0.07319317963864545, 0.05162816467311453, -0.024999306471299325, -0.10254533510819516, -0.04234769063837388, 0.35094660816385465, -0.3856697054032017, -0.1257379998398178, 0.15079792748164275, -0.20266659524949157, -0.14591185455484426, 0.23794876718345812, -0.1581166246632... |
708.2226 | Coupling of frustrated Ising spins to magnetic cycloid in multiferroic
TbMnO3 | We report on diffraction measurements on multiferroic TbMnO3 which
demonstrate that the Tb- and Mn-magnetic orders are coupled below the
ferroelectric transition TFE = 28 K. For T < TFE the magnetic propagation
vectors (tau) for Tb and Mn are locked so that tauTb = tauMn, while below TNTb
= 7 K we find that tauTb and... | cond-mat.str-el cond-mat.mtrl-sci | we report on diffraction measurements on multiferroic tbmno3 which demonstrate that the tb and mnmagnetic orders are coupled below the ferroelectric transition tfe 28 k for t tfe the magnetic propagation vectors tau for tb and mn are locked so that tautb taumn while below tntb 7 k we find that tautb and taumn lockin to... | [['we', 'report', 'on', 'diffraction', 'measurements', 'on', 'multiferroic', 'tbmno3', 'which', 'demonstrate', 'that', 'the', 'tb', 'and', 'mnmagnetic', 'orders', 'are', 'coupled', 'below', 'the', 'ferroelectric', 'transition', 'tfe', '28', 'k', 'for', 't', 'tfe', 'the', 'magnetic', 'propagation', 'vectors', 'tau', 'fo... | [-0.18018692791156354, 0.24985169972205767, 0.03829143775146804, 0.018136724476789823, -0.03540851220350305, -0.14979068388038286, 0.1168532310093724, 0.3569148138485616, -0.25594883702433435, -0.2915902426466346, 0.07055659756497334, -0.33343188869184814, -0.0863469372416148, 0.12437611177119834, 0.0739650127634377, -... |
708.2227 | On local $U$-statistic processes and the estimation of densities of
functions of several sample variables | A notion of local $U$-statistic process is introduced and central limit
theorems in various norms are obtained for it. This involves the development of
several inequalities for $U$-processes that may be useful in other contexts.
This local $U$-statistic process is based on an estimator of the density of a
function of... | math.ST stat.TH | a notion of local ustatistic process is introduced and central limit theorems in various norms are obtained for it this involves the development of several inequalities for uprocesses that may be useful in other contexts this local ustatistic process is based on an estimator of the density of a function of several samp... | [['a', 'notion', 'of', 'local', 'ustatistic', 'process', 'is', 'introduced', 'and', 'central', 'limit', 'theorems', 'in', 'various', 'norms', 'are', 'obtained', 'for', 'it', 'this', 'involves', 'the', 'development', 'of', 'several', 'inequalities', 'for', 'uprocesses', 'that', 'may', 'be', 'useful', 'in', 'other', 'con... | [-0.061405276175761636, 0.03576446155260106, -0.10430380765911798, 0.0889373297634657, 0.009533460988381575, -0.07915959673457194, 0.0545199183817563, 0.33640715488514233, -0.24914794328600862, -0.28067302000221556, 0.15855936753579827, -0.22965471203937088, -0.10152722402613848, 0.2410730081718675, -0.1513087367638945... |
708.2228 | Sl(N) link homology using foams and the Kapustin-Li formula | We use foams to give a topological construction of a rational link homology
categorifying the slN link invariant, for N>3. To evaluate closed foams we use
the Kapustin-Li formula adapted to foams by Khovanov and Rozansky. We show that
for any link our homology is isomorphic to Khovanov and Rozansky's.
| math.GT math.QA | we use foams to give a topological construction of a rational link homology categorifying the sln link invariant for n3 to evaluate closed foams we use the kapustinli formula adapted to foams by khovanov and rozansky we show that for any link our homology is isomorphic to khovanov and rozanskys | [['we', 'use', 'foams', 'to', 'give', 'a', 'topological', 'construction', 'of', 'a', 'rational', 'link', 'homology', 'categorifying', 'the', 'sln', 'link', 'invariant', 'for', 'n3', 'to', 'evaluate', 'closed', 'foams', 'we', 'use', 'the', 'kapustinli', 'formula', 'adapted', 'to', 'foams', 'by', 'khovanov', 'and', 'roza... | [-0.2317351085692644, 0.07677759321406484, -0.16738567426800727, 0.14152978253434412, -0.1350837378948927, -0.234944573212415, 0.01319488325389102, 0.3646346060931683, -0.3095475487038493, -0.20284479059278965, 0.09264839376322925, -0.18136916037648917, -0.2858423212077469, 0.14952981065027415, -0.2219435714557767, -0.... |
708.2229 | Multi-phonon Raman scattering in GaN nanowires | UV Raman scattering studies show longitudinal optical (LO) mode up to 4th
order in wurtzite GaN nanowire system. Frohlich interaction of electron with
the long range electrostatic field of ionic bonded GaN gives rise to
enhancement in LO phonon modes. Good crystalline quality, as indicated by the
crystallographic as ... | cond-mat.mtrl-sci | uv raman scattering studies show longitudinal optical lo mode up to 4th order in wurtzite gan nanowire system frohlich interaction of electron with the long range electrostatic field of ionic bonded gan gives rise to enhancement in lo phonon modes good crystalline quality as indicated by the crystallographic as well as... | [['uv', 'raman', 'scattering', 'studies', 'show', 'longitudinal', 'optical', 'lo', 'mode', 'up', 'to', '4th', 'order', 'in', 'wurtzite', 'gan', 'nanowire', 'system', 'frohlich', 'interaction', 'of', 'electron', 'with', 'the', 'long', 'range', 'electrostatic', 'field', 'of', 'ionic', 'bonded', 'gan', 'gives', 'rise', 't... | [-0.07733288911220275, 0.18748660975773085, 0.012408240678671158, 0.04925843240006974, -0.016740475368906597, -0.153077508624349, -0.002233879160332052, 0.4670510598507367, -0.21723849573417714, -0.3630021626815984, -0.06325981046661343, -0.29220437421708517, -0.07559652751262642, 0.18727429721896585, 0.036220008801472... |
708.223 | Collection analysis for Horn clause programs | We consider approximating data structures with collections of the items that
they contain. For examples, lists, binary trees, tuples, etc, can be
approximated by sets or multisets of the items within them. Such approximations
can be used to provide partial correctness properties of logic programs. For
example, one mi... | cs.LO | we consider approximating data structures with collections of the items that they contain for examples lists binary trees tuples etc can be approximated by sets or multisets of the items within them such approximations can be used to provide partial correctness properties of logic programs for example one might wish to... | [['we', 'consider', 'approximating', 'data', 'structures', 'with', 'collections', 'of', 'the', 'items', 'that', 'they', 'contain', 'for', 'examples', 'lists', 'binary', 'trees', 'tuples', 'etc', 'can', 'be', 'approximated', 'by', 'sets', 'or', 'multisets', 'of', 'the', 'items', 'within', 'them', 'such', 'approximations... | [-0.09181492491593997, 0.1142609965262447, -0.06530035128379429, 0.10456672927674106, -0.1455057495392409, -0.15823857980817807, 0.0839371717325568, 0.3878174965463629, -0.33508125315076553, -0.3191290915874927, 0.12778634305155817, -0.3077100752196556, -0.07677420640783073, 0.16555805340715551, -0.08131095851246492, 0... |
708.2231 | Pathway parameter and thermonuclear functions | In the theory of thermonuclear reaction rates, analytical evaluation of
thermonuclear functions for non-resonant reactions, including cases with
cut-off and depletion of the tail of the Maxwell-Boltzmann distribution
function were considered in a series of papers by Mathai and Haubold (1988). In
the present paper we ... | cond-mat.stat-mech math.CA | in the theory of thermonuclear reaction rates analytical evaluation of thermonuclear functions for nonresonant reactions including cases with cutoff and depletion of the tail of the maxwellboltzmann distribution function were considered in a series of papers by mathai and haubold 1988 in the present paper we study more... | [['in', 'the', 'theory', 'of', 'thermonuclear', 'reaction', 'rates', 'analytical', 'evaluation', 'of', 'thermonuclear', 'functions', 'for', 'nonresonant', 'reactions', 'including', 'cases', 'with', 'cutoff', 'and', 'depletion', 'of', 'the', 'tail', 'of', 'the', 'maxwellboltzmann', 'distribution', 'function', 'were', 'c... | [-0.057841421073673155, 0.12556834765259298, -0.05857540864869201, 0.08208041934556859, 0.005635307866439063, -0.09472524437813028, 0.06581550744682631, 0.3303561980325368, -0.21011794549262813, -0.26946683236027275, 0.019791177586622296, -0.2771531629566384, -0.14099460300458697, 0.2409339479461152, -0.029670381337724... |
708.2232 | Variational quantum Monte Carlo simulations with tensor-network states | We show that the formalism of tensor-network states, such as the matrix
product states (MPS), can be used as a basis for variational quantum Monte
Carlo simulations. Using a stochastic optimization method, we demonstrate the
potential of this approach by explicit MPS calculations for the transverse
Ising chain with u... | cond-mat.str-el cond-mat.stat-mech | we show that the formalism of tensornetwork states such as the matrix product states mps can be used as a basis for variational quantum monte carlo simulations using a stochastic optimization method we demonstrate the potential of this approach by explicit mps calculations for the transverse ising chain with up to n256... | [['we', 'show', 'that', 'the', 'formalism', 'of', 'tensornetwork', 'states', 'such', 'as', 'the', 'matrix', 'product', 'states', 'mps', 'can', 'be', 'used', 'as', 'a', 'basis', 'for', 'variational', 'quantum', 'monte', 'carlo', 'simulations', 'using', 'a', 'stochastic', 'optimization', 'method', 'we', 'demonstrate', 't... | [-0.07508801626196752, 0.133659769926453, -0.08223712243974053, 0.05597979714972704, 0.04113808373464659, -0.13396596504753688, 0.06314681789808674, 0.3825907588082676, -0.27662158678867854, -0.31148268133498885, 0.11852466495292902, -0.2351194411603501, -0.13447337218288644, 0.17673149457308077, 0.07490418265903524, 0... |
708.2233 | A complement to Le Cam's theorem | This paper examines asymptotic equivalence in the sense of Le Cam between
density estimation experiments and the accompanying Poisson experiments. The
significance of asymptotic equivalence is that all asymptotically optimal
statistical procedures can be carried over from one experiment to the other.
The equivalence ... | math.ST stat.TH | this paper examines asymptotic equivalence in the sense of le cam between density estimation experiments and the accompanying poisson experiments the significance of asymptotic equivalence is that all asymptotically optimal statistical procedures can be carried over from one experiment to the other the equivalence give... | [['this', 'paper', 'examines', 'asymptotic', 'equivalence', 'in', 'the', 'sense', 'of', 'le', 'cam', 'between', 'density', 'estimation', 'experiments', 'and', 'the', 'accompanying', 'poisson', 'experiments', 'the', 'significance', 'of', 'asymptotic', 'equivalence', 'is', 'that', 'all', 'asymptotically', 'optimal', 'sta... | [-0.1379501219977805, 0.1181708980922497, -0.08536444130661566, 0.09112973468783762, -0.05538721559494133, -0.15791744796649343, 0.03562368954730881, 0.3564059676061715, -0.24705147342155537, -0.22339215211480135, 0.11224972231749204, -0.25101018739834186, -0.11710348351287746, 0.18788261204064194, -0.10864323947293263... |
708.2234 | Bose-Einstein condensation of a Knudsen gas | We reconcile a long-standing controversy regarding the transition temperature
of the Bose-Einstein condensation in a dilute interacting Bose gas, by showing
that there is a crossover between ideal gas and interacting gas. The former
corresponds to a Knudsen (or collisionless) regime, in which the mean-free-path
is mu... | cond-mat.stat-mech | we reconcile a longstanding controversy regarding the transition temperature of the boseeinstein condensation in a dilute interacting bose gas by showing that there is a crossover between ideal gas and interacting gas the former corresponds to a knudsen or collisionless regime in which the meanfreepath is much larger t... | [['we', 'reconcile', 'a', 'longstanding', 'controversy', 'regarding', 'the', 'transition', 'temperature', 'of', 'the', 'boseeinstein', 'condensation', 'in', 'a', 'dilute', 'interacting', 'bose', 'gas', 'by', 'showing', 'that', 'there', 'is', 'a', 'crossover', 'between', 'ideal', 'gas', 'and', 'interacting', 'gas', 'the... | [-0.13561568965438897, 0.22188888520420355, -0.09599379639558751, 0.041144383588508734, 0.026005266563453037, -0.13195327134273047, 0.04126410081918384, 0.2757527391137234, -0.24013835610821843, -0.2172691892975026, 0.036683942177252654, -0.33349687652662396, -0.040395888798982545, 0.14493832361466927, 0.03063949244799... |
708.2235 | Realizing modules over the homology of a DGA | Let A be a DGA over a field and X a module over H_*(A). Fix an
$A_\infty$-structure on H_*(A) making it quasi-isomorphic to A. We construct an
equivalence of categories between A_{n+1}-module structures on X and length n
Postnikov systems in the derived category of A-modules based on the bar
resolution of X. This imp... | math.AT math.RA | let a be a dga over a field and x a module over h_a fix an a_inftystructure on h_a making it quasiisomorphic to a we construct an equivalence of categories between a_n1module structures on x and length n postnikov systems in the derived category of amodules based on the bar resolution of x this implies that quasiisomor... | [['let', 'a', 'be', 'a', 'dga', 'over', 'a', 'field', 'and', 'x', 'a', 'module', 'over', 'h_a', 'fix', 'an', 'a_inftystructure', 'on', 'h_a', 'making', 'it', 'quasiisomorphic', 'to', 'a', 'we', 'construct', 'an', 'equivalence', 'of', 'categories', 'between', 'a_n1module', 'structures', 'on', 'x', 'and', 'length', 'n', ... | [-0.2222732059014714, 0.06864424067921833, -0.05217308237884952, 0.04529499234343195, -0.009235242019053054, -0.13393451175363982, -0.013211370313919224, 0.39565585804196585, -0.35941190667351525, -0.21140747304709084, 0.03667568528521971, -0.2100048145130936, -0.08222273982591531, 0.2069580626851195, -0.12113522961570... |
708.2236 | Large-order shifted 1/N expansions through the asymptotic iteration
method | The perturbation technique within the framework of the asymptotic iteration
method is used to obtain large-order shifted 1/N expansions, where N is the
number of spatial dimensions. This method is contrary to the usual
Rayleigh-Schr\"{o}dinger perturbation theory, no matrix elements need to be
calculated. The method ... | quant-ph | the perturbation technique within the framework of the asymptotic iteration method is used to obtain largeorder shifted 1n expansions where n is the number of spatial dimensions this method is contrary to the usual rayleighschrodinger perturbation theory no matrix elements need to be calculated the method is applied to... | [['the', 'perturbation', 'technique', 'within', 'the', 'framework', 'of', 'the', 'asymptotic', 'iteration', 'method', 'is', 'used', 'to', 'obtain', 'largeorder', 'shifted', '1n', 'expansions', 'where', 'n', 'is', 'the', 'number', 'of', 'spatial', 'dimensions', 'this', 'method', 'is', 'contrary', 'to', 'the', 'usual', '... | [-0.06726737815456894, 0.05523284118680749, -0.12033325104186168, 0.08223756263032556, -0.046495881941742624, -0.13064184058457612, -0.020452037147389582, 0.3288788604908265, -0.2444597291545226, -0.25468926531477615, 0.08675213367857326, -0.29620008343973986, -0.19560640870163648, 0.14706477694786513, 0.00393832860013... |
708.2237 | A generation-based particle-hole density-matrix renormalization group
study of interacting quantum dots | The particle-hole version of the density-matrix renormalization-group method
(PH-DMRG) is utilized to calculate the ground-state energy of an interacting
two-dimensional quantum dot. We show that a modification of the method, termed
generation-based PH-DMRG, leads to significant improvement of the results, and
discus... | cond-mat.dis-nn cond-mat.str-el | the particlehole version of the densitymatrix renormalizationgroup method phdmrg is utilized to calculate the groundstate energy of an interacting twodimensional quantum dot we show that a modification of the method termed generationbased phdmrg leads to significant improvement of the results and discuss its feasibilit... | [['the', 'particlehole', 'version', 'of', 'the', 'densitymatrix', 'renormalizationgroup', 'method', 'phdmrg', 'is', 'utilized', 'to', 'calculate', 'the', 'groundstate', 'energy', 'of', 'an', 'interacting', 'twodimensional', 'quantum', 'dot', 'we', 'show', 'that', 'a', 'modification', 'of', 'the', 'method', 'termed', 'g... | [-0.13130988280192532, 0.04172431041937169, -0.10088667829906375, 0.06170818717259079, 0.01561813850903177, -0.0996990862687857, 0.048378765123398525, 0.33774271963870733, -0.22792349697957778, -0.26758583506633493, 0.03461062797377336, -0.2639129684820514, -0.16504980825241014, 0.22143865098116983, -0.0029854137482571... |
708.2238 | Affleck-Dine leptogenesis via multiscalar evolution in a supersymmetric
seesaw model | A leptogenesis scenario in a supersymmetric standard model extended with
introducing right-handed neutrinos is reconsidered. Lepton asymmetry is
produced in the condensate of a right-handed sneutrino via the Affleck-Dine
mechanism. The LH_u direction develops large value due to a negative effective
mass induced by th... | hep-ph | a leptogenesis scenario in a supersymmetric standard model extended with introducing righthanded neutrinos is reconsidered lepton asymmetry is produced in the condensate of a righthanded sneutrino via the affleckdine mechanism the lh_u direction develops large value due to a negative effective mass induced by the right... | [['a', 'leptogenesis', 'scenario', 'in', 'a', 'supersymmetric', 'standard', 'model', 'extended', 'with', 'introducing', 'righthanded', 'neutrinos', 'is', 'reconsidered', 'lepton', 'asymmetry', 'is', 'produced', 'in', 'the', 'condensate', 'of', 'a', 'righthanded', 'sneutrino', 'via', 'the', 'affleckdine', 'mechanism', '... | [-0.170579761221278, 0.3840852831263186, -0.00060020844315792, 0.18512711219529326, -0.0986875294105763, -0.2131760012778658, 0.022521744243709778, 0.28467596177772686, -0.24623898966465055, -0.27119732342473024, -0.013413499921514856, -0.2503420455472135, -0.002403580878929394, 0.027593434581010625, 0.0654530874311515... |
708.2239 | Extension of thermonuclear functions through the pathway model including
Maxwell-Boltzmann and Tsallis distributions | The Maxwell-Boltzmannian approach to nuclear reaction rate theory is extended
to cover Tsallis statistics (Tsallis, 1988) and more general cases of
distribution functions. An analytical study of respective thermonuclear
functions is being conducted with the help of statistical techniques. The
pathway model, recently ... | astro-ph nucl-th | the maxwellboltzmannian approach to nuclear reaction rate theory is extended to cover tsallis statistics tsallis 1988 and more general cases of distribution functions an analytical study of respective thermonuclear functions is being conducted with the help of statistical techniques the pathway model recently introduce... | [['the', 'maxwellboltzmannian', 'approach', 'to', 'nuclear', 'reaction', 'rate', 'theory', 'is', 'extended', 'to', 'cover', 'tsallis', 'statistics', 'tsallis', '1988', 'and', 'more', 'general', 'cases', 'of', 'distribution', 'functions', 'an', 'analytical', 'study', 'of', 'respective', 'thermonuclear', 'functions', 'is... | [-0.023125749338246154, 0.06320471929670336, -0.11730653139491788, 0.13438115347905652, -0.05078237366093242, -0.09962648895832346, 0.026619868542816814, 0.31377197482177743, -0.21547225532729342, -0.22970070177689195, 0.056546717825214095, -0.26936215894175286, -0.16174174350200463, 0.2689176645388057, -0.062653992375... |
708.224 | Casimir-Polder interatomic potential between two atoms at finite
temperature and in the presence of boundary conditions | We evaluate the Casimir-Polder potential between two atoms in the presence of
an infinite perfectly conducting plate and at nonzero temperature. In order to
calculate the potential, we use a method based on equal-time spatial
correlations of the electric field, already used to evaluate the effect of
boundary conditio... | quant-ph | we evaluate the casimirpolder potential between two atoms in the presence of an infinite perfectly conducting plate and at nonzero temperature in order to calculate the potential we use a method based on equaltime spatial correlations of the electric field already used to evaluate the effect of boundary conditions on i... | [['we', 'evaluate', 'the', 'casimirpolder', 'potential', 'between', 'two', 'atoms', 'in', 'the', 'presence', 'of', 'an', 'infinite', 'perfectly', 'conducting', 'plate', 'and', 'at', 'nonzero', 'temperature', 'in', 'order', 'to', 'calculate', 'the', 'potential', 'we', 'use', 'a', 'method', 'based', 'on', 'equaltime', 's... | [-0.12497100497486892, 0.09351320889687191, -0.09320481100144822, 0.049364960655939205, -0.014706545261884326, -0.09491604217957403, 0.07116409822425863, 0.38017555480604776, -0.21490895062231938, -0.27462478388134426, 0.046715313704004766, -0.27475188994729843, -0.13461814663028931, 0.19730829309068015, 0.017515784729... |
708.2241 | Simple direct measurement of nonclassical joint signal-idler
photon-number statistics and correlation area of twin photon beams | The measurement of joint signal-idler photon-number distribution of a field
obtained from spontaneous parametric downconversion using an intensified CCD
camera is presented. It is shown that a classicality criterion is violated
directly by the measured data. Characteristic dimensions of the area of
correlation are de... | quant-ph | the measurement of joint signalidler photonnumber distribution of a field obtained from spontaneous parametric downconversion using an intensified ccd camera is presented it is shown that a classicality criterion is violated directly by the measured data characteristic dimensions of the area of correlation are determin... | [['the', 'measurement', 'of', 'joint', 'signalidler', 'photonnumber', 'distribution', 'of', 'a', 'field', 'obtained', 'from', 'spontaneous', 'parametric', 'downconversion', 'using', 'an', 'intensified', 'ccd', 'camera', 'is', 'presented', 'it', 'is', 'shown', 'that', 'a', 'classicality', 'criterion', 'is', 'violated', ... | [-0.1188855009409599, 0.15253565404826078, -0.14334423440508545, 0.054259642062243076, -0.009252977352589368, -0.16899358270689846, -0.00950332976412028, 0.37949159145355227, -0.23448056122288108, -0.2965382022038102, 0.04909336794866249, -0.2554684549570084, -0.07198359072208405, 0.2541391295939684, -0.081725026704370... |
708.2242 | Antisymmetric entangled two-photon states generated in nonlinear GaN/AlN
photonic-band-gap structures | The properties of an entangled two-photon state antisymmetric in frequencies
are studied. At a beam-splitter, two entangled photons are perfectly
anti-correlated. In addition, they cannot be detected at the same time instant
despite the fact that their detection times are confined to a narrow time
window, i.e. they a... | quant-ph | the properties of an entangled twophoton state antisymmetric in frequencies are studied at a beamsplitter two entangled photons are perfectly anticorrelated in addition they cannot be detected at the same time instant despite the fact that their detection times are confined to a narrow time window ie they are temporall... | [['the', 'properties', 'of', 'an', 'entangled', 'twophoton', 'state', 'antisymmetric', 'in', 'frequencies', 'are', 'studied', 'at', 'a', 'beamsplitter', 'two', 'entangled', 'photons', 'are', 'perfectly', 'anticorrelated', 'in', 'addition', 'they', 'can', 'not', 'be', 'detected', 'at', 'the', 'same', 'time', 'instant', ... | [-0.17733852228726635, 0.2941997693106619, -0.05094946261995764, 0.04821641107763984, 0.017250068624740215, -0.20585652939808458, -0.03784217290691475, 0.54551445047802, -0.24716824843589938, -0.24966493032094259, 0.0773236633507785, -0.2984633101567404, -0.042980293548707645, 0.20794152530299417, 0.027205959756497238,... |
708.2243 | Embedding group algebras into finite von Neumann regular rings | Let G be a group and let K be a field of characteristic zero. We shall prove
that KG can be embedded into a von Neumann unit-regular ring. In the course of
the proof, we shall obtain a result relevant to the Atiyah conjecture.
| math.RA math.GR | let g be a group and let k be a field of characteristic zero we shall prove that kg can be embedded into a von neumann unitregular ring in the course of the proof we shall obtain a result relevant to the atiyah conjecture | [['let', 'g', 'be', 'a', 'group', 'and', 'let', 'k', 'be', 'a', 'field', 'of', 'characteristic', 'zero', 'we', 'shall', 'prove', 'that', 'kg', 'can', 'be', 'embedded', 'into', 'a', 'von', 'neumann', 'unitregular', 'ring', 'in', 'the', 'course', 'of', 'the', 'proof', 'we', 'shall', 'obtain', 'a', 'result', 'relevant', '... | [-0.19548368017951195, 0.14296088816428726, -0.21164549856489015, -0.007200770207088102, -0.10459270046769896, -0.19114660645242443, -0.05262644174085422, 0.2922174136778763, -0.3202111949636178, -0.2100647967732088, 0.10359466867256825, -0.21612166612811218, -0.07905486035584049, 0.2042776898544451, -0.149404890919950... |
708.2244 | Unbiased Random Threshold Networks Are Chaotic or Critical | This paper has been withdrawn.
| cond-mat.dis-nn cond-mat.stat-mech nlin.CG q-bio.MN | this paper has been withdrawn | [['this', 'paper', 'has', 'been', 'withdrawn']] | [-0.14966976195573806, -0.11479587350040674, -0.26925536394119265, -0.2174653896363452, -0.24278417900204657, -0.06483052410185337, -0.18645338097121567, 0.4360402226448059, -0.2831330731511116, -0.34362963438034055, 0.12004837393760681, -0.3683081828057766, -0.1602430183440447, -0.10558439195156097, -0.497941048443317... |
708.2245 | Mathematical Modeling of Control Dynamical Systems | This paper has been withdrawn by the author due to a crucial mistakes.
| math-ph math.MP | this paper has been withdrawn by the author due to a crucial mistakes | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'author', 'due', 'to', 'a', 'crucial', 'mistakes']] | [-0.08223364709948118, -0.030214484351185653, -0.12351351202680515, -0.05219239588432874, -0.17892727556710059, -0.0833760960958898, 0.025227499489959043, 0.298291435608497, -0.22287339774461892, -0.3896642421873716, 0.11665532558869857, -0.2919154983873551, -0.21363361538029635, 0.035534532024310186, -0.38174736177405... |
708.2246 | Monopoles, topology of the Standard Model, and unification of
interactions at Tev scale | It is shown that unification of strong and Electroweak interactions at Tev
scale may lead to appearance of topologically stable monopoles with masses of
the order of 40 Tev. Those monopoles may play an important role in the early
Universe, at finite temperature. They may even be condensed at high enough
temperature. ... | hep-lat hep-ph | it is shown that unification of strong and electroweak interactions at tev scale may lead to appearance of topologically stable monopoles with masses of the order of 40 tev those monopoles may play an important role in the early universe at finite temperature they may even be condensed at high enough temperature the la... | [['it', 'is', 'shown', 'that', 'unification', 'of', 'strong', 'and', 'electroweak', 'interactions', 'at', 'tev', 'scale', 'may', 'lead', 'to', 'appearance', 'of', 'topologically', 'stable', 'monopoles', 'with', 'masses', 'of', 'the', 'order', 'of', '40', 'tev', 'those', 'monopoles', 'may', 'play', 'an', 'important', 'r... | [-0.1438830265936802, 0.30683601004162603, -0.09256856391567864, 0.16101194720812922, -0.046039570964151816, -0.11494788666999328, -0.033860494720659426, 0.37392778237981183, -0.21139461484046712, -0.3612922603384622, 0.09983423811706504, -0.26278159635201576, -0.04182548965177228, 0.14175080719418945, 0.03021025276111... |
708.2247 | Bridgeland-Stable Moduli Spaces for K-Trivial Surfaces | We give a natural family of Bridgeland stability conditions on the derived
category of a smooth projective complex surface S and describe ``wall-crossing
behavior'' for objects with the same invariants as $\cO_C(H)$ when H generates
Pic(S) and $C \in |H|$. If, in addition, S is a K3 or Abelian surface, we use
this de... | math.AG | we give a natural family of bridgeland stability conditions on the derived category of a smooth projective complex surface s and describe wallcrossing behavior for objects with the same invariants as co_ch when h generates pics and c in h if in addition s is a k3 or abelian surface we use this description to construct ... | [['we', 'give', 'a', 'natural', 'family', 'of', 'bridgeland', 'stability', 'conditions', 'on', 'the', 'derived', 'category', 'of', 'a', 'smooth', 'projective', 'complex', 'surface', 's', 'and', 'describe', 'wallcrossing', 'behavior', 'for', 'objects', 'with', 'the', 'same', 'invariants', 'as', 'co_ch', 'when', 'h', 'ge... | [-0.1570809363157198, 0.11060284292425519, -0.10601138664028978, 0.1309671635409036, -0.08562174777660558, -0.1406580437705802, 0.017761246192329112, 0.3398610659704734, -0.3275194984299922, -0.2461753583222788, 0.06721214874602494, -0.16884981562453572, -0.16312027027422402, 0.22339846847781672, -0.1771945376074322, -... |
708.2248 | Observation of B0 -> K*0 K*0bar and search for B0 -> K*0 K*0 | We report the observation of the b -> d penguin-dominated decay B0 -> K*0
K*0bar with a sample of 383.2 +/- 4.2 million BBbar pairs collected with the
BaBar detector at the PEP-II asymmetric-energy e^+e^- collider at the Stanford
Linear Accelerator Center. The measured branching fraction is Br(B0 -> K*0
K*0bar) = [1.... | hep-ex | we report the observation of the b d penguindominated decay b0 k0 k0bar with a sample of 3832 42 million bbbar pairs collected with the babar detector at the pepii asymmetricenergy ee collider at the stanford linear accelerator center the measured branching fraction is brb0 k0 k0bar 128035_030 011 x 106 and the fractio... | [['we', 'report', 'the', 'observation', 'of', 'the', 'b', 'd', 'penguindominated', 'decay', 'b0', 'k0', 'k0bar', 'with', 'a', 'sample', 'of', '3832', '42', 'million', 'bbbar', 'pairs', 'collected', 'with', 'the', 'babar', 'detector', 'at', 'the', 'pepii', 'asymmetricenergy', 'ee', 'collider', 'at', 'the', 'stanford', '... | [-0.16396659183170725, 0.1851160371019217, -0.025533468006879733, 0.031179288236965096, -0.012425567203712079, -0.12445463922615814, 0.1938806843633453, 0.239337297331702, -0.16240981295304271, -0.2782724375726395, -0.01939292465116308, -0.5040581675386557, 0.1401450426708306, 0.16689810889112133, 0.10809452518800734, ... |
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