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 |
|---|---|---|---|---|---|---|
706.1314 | When Did Cosmic Acceleration Start ? | A precise determination, and comparison, of the epoch of the onset of cosmic
acceleration, at redshift z_acc, and of dark energy domination, at z_eq,
provides an interesting measure with which to parameterize dark energy models.
By combining several cosmological datasets we place constraints on the redshift
and age o... | astro-ph gr-qc hep-ph | a precise determination and comparison of the epoch of the onset of cosmic acceleration at redshift z_acc and of dark energy domination at z_eq provides an interesting measure with which to parameterize dark energy models by combining several cosmological datasets we place constraints on the redshift and age of cosmolo... | [['a', 'precise', 'determination', 'and', 'comparison', 'of', 'the', 'epoch', 'of', 'the', 'onset', 'of', 'cosmic', 'acceleration', 'at', 'redshift', 'z_acc', 'and', 'of', 'dark', 'energy', 'domination', 'at', 'z_eq', 'provides', 'an', 'interesting', 'measure', 'with', 'which', 'to', 'parameterize', 'dark', 'energy', '... | [-0.08764898034384136, 0.11816140904464356, -0.11804494870064611, 0.11815069805492054, -0.05668023995293135, -0.12349402892763134, 0.06722993510986933, 0.3364358917217363, -0.19841500668024475, -0.4347867976366119, 0.052470602859234945, -0.23603690986267545, 0.06460615901107138, 0.18369200155773963, 0.03048261851072311... |
706.1315 | The Dirac system on the Anti-de Sitter Universe | We investigate the global solutions of the Dirac equation on the
Anti-de-Sitter Universe. Since this space is not globally hyperbolic, the
Cauchy problem is not, {\it a priori}, well-posed. Nevertheless we can prove
that there exists unitary dynamics, but its uniqueness crucially depends on the
ratio beween the mass ... | math-ph math.AP math.MP | we investigate the global solutions of the dirac equation on the antidesitter universe since this space is not globally hyperbolic the cauchy problem is not it a priori wellposed nevertheless we can prove that there exists unitary dynamics but its uniqueness crucially depends on the ratio beween the mass m of the field... | [['we', 'investigate', 'the', 'global', 'solutions', 'of', 'the', 'dirac', 'equation', 'on', 'the', 'antidesitter', 'universe', 'since', 'this', 'space', 'is', 'not', 'globally', 'hyperbolic', 'the', 'cauchy', 'problem', 'is', 'not', 'it', 'a', 'priori', 'wellposed', 'nevertheless', 'we', 'can', 'prove', 'that', 'there... | [-0.2019515800796124, 0.14643365251905624, -0.1057653877595883, 0.11209135518283657, -0.06799156057818365, -0.13635020562270211, -0.00742387194334278, 0.3052842790881793, -0.24652071952420687, -0.22695651005894418, 0.1229944216093928, -0.26609417861918844, -0.13401380845803826, 0.16590909540675403, -0.02247153987945427... |
706.1316 | Coupling of Optical Lumped Nanocircuit Elements and Effects of
Substrates | We present here a model for the coupling among small nanoparticles excited by
an optical electric field in the framework of our optical lumped nanocircuit
theory [N. Engheta, A. Salandrino, and A. Alu Phys. Rev. Lett. 95, 095504
(2005)]. We derive how this coupling affects the corresponding nanocircuit
model by addin... | cond-mat.mtrl-sci | we present here a model for the coupling among small nanoparticles excited by an optical electric field in the framework of our optical lumped nanocircuit theory n engheta a salandrino and a alu phys rev lett 95 095504 2005 we derive how this coupling affects the corresponding nanocircuit model by adding controlled sou... | [['we', 'present', 'here', 'a', 'model', 'for', 'the', 'coupling', 'among', 'small', 'nanoparticles', 'excited', 'by', 'an', 'optical', 'electric', 'field', 'in', 'the', 'framework', 'of', 'our', 'optical', 'lumped', 'nanocircuit', 'theory', 'n', 'engheta', 'a', 'salandrino', 'and', 'a', 'alu', 'phys', 'rev', 'lett', '... | [-0.10665342995032136, 0.15606039330525942, -0.008314916302749355, -0.0744779676284192, -0.019877134568689923, -0.13712212907349958, 0.09079105229102424, 0.4083804573165253, -0.18420216894134814, -0.3254606704493718, 0.008551198750085729, -0.26511528025730513, -0.197810546688353, 0.20196361116541084, -0.039785346336429... |
706.1317 | A model for learning to segment temporal sequences, utilizing a mixture
of RNN experts together with adaptive variance | This paper proposes a novel learning method for a mixture of recurrent neural
network (RNN) experts model, which can acquire the ability to generate desired
sequences by dynamically switching between experts. Our method is based on
maximum likelihood estimation, using a gradient descent algorithm. This
approach is si... | nlin.AO | this paper proposes a novel learning method for a mixture of recurrent neural network rnn experts model which can acquire the ability to generate desired sequences by dynamically switching between experts our method is based on maximum likelihood estimation using a gradient descent algorithm this approach is similar to... | [['this', 'paper', 'proposes', 'a', 'novel', 'learning', 'method', 'for', 'a', 'mixture', 'of', 'recurrent', 'neural', 'network', 'rnn', 'experts', 'model', 'which', 'can', 'acquire', 'the', 'ability', 'to', 'generate', 'desired', 'sequences', 'by', 'dynamically', 'switching', 'between', 'experts', 'our', 'method', 'is... | [-0.018284802690839336, 0.009443171508610248, -0.11647182848574894, 0.04438220439028115, -0.11345679904784887, -0.1788291748162479, 0.05969597338849018, 0.4170016152724143, -0.2924999794231788, -0.33835250032322123, 0.05205493386564476, -0.19635820453986524, -0.23779327389033092, 0.21998049083406165, -0.122448197025204... |
706.1318 | Constructing a maximum utility slate of on-line advertisements | We present an algorithm for constructing an optimal slate of sponsored search
advertisements which respects the ordering that is the outcome of a generalized
second price auction, but which must also accommodate complicating factors such
as overall budget constraints. The algorithm is easily fast enough to use on
the... | cs.DM cs.DS | we present an algorithm for constructing an optimal slate of sponsored search advertisements which respects the ordering that is the outcome of a generalized second price auction but which must also accommodate complicating factors such as overall budget constraints the algorithm is easily fast enough to use on the fly... | [['we', 'present', 'an', 'algorithm', 'for', 'constructing', 'an', 'optimal', 'slate', 'of', 'sponsored', 'search', 'advertisements', 'which', 'respects', 'the', 'ordering', 'that', 'is', 'the', 'outcome', 'of', 'a', 'generalized', 'second', 'price', 'auction', 'but', 'which', 'must', 'also', 'accommodate', 'complicati... | [-0.07965052640159434, 0.05054909288165002, -0.09248114884981225, 0.10120176949403098, -0.15939386050036597, -0.13963463845392388, 0.11440303572829091, 0.40752446661973674, -0.30625990664045655, -0.3642979626273436, 0.153318430452923, -0.21592015158685465, -0.15840933672077354, 0.19856278123071178, -0.0871547237339039,... |
706.1319 | Dealing with delicate issues in waveforms calculations | We revisit the calculation of gravitational radiation through the use of Weyl
scalars. We point out several possible problems arising from gauge and tetrad
ambiguities and ways to address them. Our analysis indicates how, relatively
simple corrections can be introduced to remove these ambiguities.
| gr-qc | we revisit the calculation of gravitational radiation through the use of weyl scalars we point out several possible problems arising from gauge and tetrad ambiguities and ways to address them our analysis indicates how relatively simple corrections can be introduced to remove these ambiguities | [['we', 'revisit', 'the', 'calculation', 'of', 'gravitational', 'radiation', 'through', 'the', 'use', 'of', 'weyl', 'scalars', 'we', 'point', 'out', 'several', 'possible', 'problems', 'arising', 'from', 'gauge', 'and', 'tetrad', 'ambiguities', 'and', 'ways', 'to', 'address', 'them', 'our', 'analysis', 'indicates', 'how... | [-0.09597396160560576, 0.11082875022177839, -0.1023640452503142, 0.11581968434620649, -0.1764329848387702, -0.11303248291369528, 0.07903307104821909, 0.3594948551194234, -0.2894048248841004, -0.29423399752175267, 0.045194913358004254, -0.2806964546696029, -0.17501747218722646, 0.1560603161342442, -0.07720992108806968, ... |
706.132 | Accretion vs colliding wind models for the gamma-ray binary LS I +61
303: an assessment | LS I +61 303 is a puzzling Be/X-ray binary with variable gamma-ray emission
at up TeV energies. The nature of the compact object and the origin of the
high-energy emission are unclear. One family of models invokes particle
acceleration in shocks from the collision between the B-star wind and a
relativistic pulsar win... | astro-ph | ls i 61 303 is a puzzling bexray binary with variable gammaray emission at up tev energies the nature of the compact object and the origin of the highenergy emission are unclear one family of models invokes particle acceleration in shocks from the collision between the bstar wind and a relativistic pulsar wind while an... | [['ls', 'i', '61', '303', 'is', 'a', 'puzzling', 'bexray', 'binary', 'with', 'variable', 'gammaray', 'emission', 'at', 'up', 'tev', 'energies', 'the', 'nature', 'of', 'the', 'compact', 'object', 'and', 'the', 'origin', 'of', 'the', 'highenergy', 'emission', 'are', 'unclear', 'one', 'family', 'of', 'models', 'invokes', ... | [-0.0913058519271276, 0.09820704813821537, -0.08545866813644659, 0.12689852712402896, -0.0930592215899713, -0.13616821939324986, 0.016488550291162172, 0.3903234618977248, -0.21959701057845096, -0.32467163188078124, 0.0529688381541373, -0.28720768722337037, -0.04895451614833056, 0.23086153235154147, -0.00474962375709693... |
706.1321 | Detailed study of the GRB 030329 radio afterglow deep into the
non-relativistic phase | We explore the physics behind one of the brightest radio afterglows ever, GRB
030329, at late times when the jet is non-relativistic. We determine the
physical parameters of the blast wave and its surroundings, in particular the
index of the electron energy distribution, the energy of the blast wave, and
the density ... | astro-ph | we explore the physics behind one of the brightest radio afterglows ever grb 030329 at late times when the jet is nonrelativistic we determine the physical parameters of the blast wave and its surroundings in particular the index of the electron energy distribution the energy of the blast wave and the density structure... | [['we', 'explore', 'the', 'physics', 'behind', 'one', 'of', 'the', 'brightest', 'radio', 'afterglows', 'ever', 'grb', '030329', 'at', 'late', 'times', 'when', 'the', 'jet', 'is', 'nonrelativistic', 'we', 'determine', 'the', 'physical', 'parameters', 'of', 'the', 'blast', 'wave', 'and', 'its', 'surroundings', 'in', 'par... | [-0.07728674905433097, 0.14695570774660854, -0.06474423441630651, 0.0936118108770814, -0.11651788965923611, -0.06211636047303739, 0.027093875904813033, 0.4697406411046264, -0.1847089973898657, -0.312401057813301, 0.08557487622041754, -0.29805405062689566, -0.03976029857591761, 0.20318698905755192, 0.06613333714384562, ... |
706.1322 | Thermodynamics and the virial expansion for trapped fluids in arbitrary
external potentials | We present the full thermodynamics of a fluid confined by an arbitrary
external potential based on the virial expansion of the grand potential. The
fluid may be classical or quantum and it is assumed that interatomic
interactions are pairwise additive. We indicate how the appropriate
"generalized" volume and pressure... | cond-mat.stat-mech | we present the full thermodynamics of a fluid confined by an arbitrary external potential based on the virial expansion of the grand potential the fluid may be classical or quantum and it is assumed that interatomic interactions are pairwise additive we indicate how the appropriate generalized volume and pressure varia... | [['we', 'present', 'the', 'full', 'thermodynamics', 'of', 'a', 'fluid', 'confined', 'by', 'an', 'arbitrary', 'external', 'potential', 'based', 'on', 'the', 'virial', 'expansion', 'of', 'the', 'grand', 'potential', 'the', 'fluid', 'may', 'be', 'classical', 'or', 'quantum', 'and', 'it', 'is', 'assumed', 'that', 'interato... | [-0.12084122949470115, 0.1310470310424427, -0.12501190556369732, 0.05206548674432661, -0.02001375800889907, -0.08228350029907801, 0.08079266990534961, 0.32143248229097293, -0.2700270838279437, -0.25811957894393833, 0.0848741199262941, -0.2730721173637737, -0.12910214727944744, 0.15463755081372677, -0.019011792616658314... |
706.1323 | GRB 030329: 3 years of radio afterglow monitoring | Radio observations of gamma-ray burst (GRB) afterglows are essential for our
understanding of the physics of relativistic blast waves, as they enable us to
follow the evolution of GRB explosions much longer than the afterglows in any
other wave band. We have performed a three-year monitoring campaign of GRB
030329 wi... | astro-ph | radio observations of gammaray burst grb afterglows are essential for our understanding of the physics of relativistic blast waves as they enable us to follow the evolution of grb explosions much longer than the afterglows in any other wave band we have performed a threeyear monitoring campaign of grb 030329 with the w... | [['radio', 'observations', 'of', 'gammaray', 'burst', 'grb', 'afterglows', 'are', 'essential', 'for', 'our', 'understanding', 'of', 'the', 'physics', 'of', 'relativistic', 'blast', 'waves', 'as', 'they', 'enable', 'us', 'to', 'follow', 'the', 'evolution', 'of', 'grb', 'explosions', 'much', 'longer', 'than', 'the', 'aft... | [-0.06980711375108015, 0.13443406393962007, -0.06735555693660289, 0.15249418477808468, -0.2104376890466944, -0.09408238856440844, 0.026478295056595887, 0.49789734450105116, -0.1260565240765373, -0.31793281363246784, 0.07555720358624518, -0.2816471006076987, -0.02523011432431179, 0.26056779355563425, 0.08632264442882207... |
706.1324 | GRB 030329: three years of radio afterglow monitoring | Radio observations of gamma-ray burst (GRB) afterglows are essential for our
understanding of the physics of relativistic blast waves, as they enable us to
follow the evolution of GRB explosions much longer than the afterglows in any
other wave band. We have performed a three-year monitoring campaign of GRB
030329 wi... | astro-ph | radio observations of gammaray burst grb afterglows are essential for our understanding of the physics of relativistic blast waves as they enable us to follow the evolution of grb explosions much longer than the afterglows in any other wave band we have performed a threeyear monitoring campaign of grb 030329 with the w... | [['radio', 'observations', 'of', 'gammaray', 'burst', 'grb', 'afterglows', 'are', 'essential', 'for', 'our', 'understanding', 'of', 'the', 'physics', 'of', 'relativistic', 'blast', 'waves', 'as', 'they', 'enable', 'us', 'to', 'follow', 'the', 'evolution', 'of', 'grb', 'explosions', 'much', 'longer', 'than', 'the', 'aft... | [-0.07326672201165232, 0.13710296679395853, -0.06644633380683507, 0.15127575167195023, -0.20904909253126758, -0.09655383358817218, 0.030050600449662325, 0.4986876045562783, -0.12682082671925526, -0.3210867624983293, 0.07650134150417154, -0.2767937420297186, -0.021860161500026277, 0.2596363197334212, 0.08319243812477406... |
706.1325 | Possible astronomical references in the planning of the Great Hopewell
Road | The possible existence of astronomical references in the planning of the
so-called Great Hopewell Road, a 90 Kilometres straight road composed of two
parallel earthen embankments which, according to recent surveys, likely
connected the Hopewell ceremonial centres of Newark and Chillicothe, Ohio, are
investigated. It ... | physics.hist-ph | the possible existence of astronomical references in the planning of the socalled great hopewell road a 90 kilometres straight road composed of two parallel earthen embankments which according to recent surveys likely connected the hopewell ceremonial centres of newark and chillicothe ohio are investigated it turns out... | [['the', 'possible', 'existence', 'of', 'astronomical', 'references', 'in', 'the', 'planning', 'of', 'the', 'socalled', 'great', 'hopewell', 'road', 'a', '90', 'kilometres', 'straight', 'road', 'composed', 'of', 'two', 'parallel', 'earthen', 'embankments', 'which', 'according', 'to', 'recent', 'surveys', 'likely', 'con... | [-0.15725822088780342, 0.10051286580379713, -0.073049169674806, 0.032640706310834884, -0.12182529234363661, -0.08966978786924443, 0.09172457392484724, 0.36465959301726386, -0.20394604618346632, -0.3105288463547923, 0.11261953106119793, -0.2619359239761252, -0.1178839396709552, 0.20971600042637922, -0.047112344461795574... |
706.1326 | The oscillation stability problem for the Urysohn sphere: A
combinatorial approach | We study the oscillation stability problem for the Urysohn sphere, an analog
of the distortion problem for $\ell_2$ in the context of the Urysohn space
$\Ur$. In particular, we show that this problem reduces to a purely
combinatorial problem involving a family of countable ultrahomogeneous metric
spaces with finitely... | math.MG math.CO | we study the oscillation stability problem for the urysohn sphere an analog of the distortion problem for ell_2 in the context of the urysohn space ur in particular we show that this problem reduces to a purely combinatorial problem involving a family of countable ultrahomogeneous metric spaces with finitely many dista... | [['we', 'study', 'the', 'oscillation', 'stability', 'problem', 'for', 'the', 'urysohn', 'sphere', 'an', 'analog', 'of', 'the', 'distortion', 'problem', 'for', 'ell_2', 'in', 'the', 'context', 'of', 'the', 'urysohn', 'space', 'ur', 'in', 'particular', 'we', 'show', 'that', 'this', 'problem', 'reduces', 'to', 'a', 'purel... | [-0.13937179489613638, 0.060771577925633584, -0.0663890438336952, 0.11373204996069784, -0.10012996897977941, -0.040325440685538685, 0.03521738057116083, 0.3519413612152943, -0.4058348304208587, -0.2054218072672466, 0.1350212039873369, -0.2956190697081825, -0.18009708445592254, 0.2223524629040256, -0.1660750932699325, 0... |
706.1327 | Hopf Algebras of Heap Ordered Trees and Permutations | It is known that there is a Hopf algebra structure on the vector space with
basis all heap-ordered trees. We give a new bialgebra structure on the space
with basis all permutations and show that there is a direct bialgebra
isomorphism between the Hopf algebra of heap-ordered trees and the bialgebra of
permutations.
| math.RA | it is known that there is a hopf algebra structure on the vector space with basis all heapordered trees we give a new bialgebra structure on the space with basis all permutations and show that there is a direct bialgebra isomorphism between the hopf algebra of heapordered trees and the bialgebra of permutations | [['it', 'is', 'known', 'that', 'there', 'is', 'a', 'hopf', 'algebra', 'structure', 'on', 'the', 'vector', 'space', 'with', 'basis', 'all', 'heapordered', 'trees', 'we', 'give', 'a', 'new', 'bialgebra', 'structure', 'on', 'the', 'space', 'with', 'basis', 'all', 'permutations', 'and', 'show', 'that', 'there', 'is', 'a', ... | [-0.21727465333873933, 0.10819869711643683, -0.033461224639190816, 0.07544316421482572, -0.23179323157682172, -0.08962482980997213, 0.04103146342314639, 0.40258235259438463, -0.40798192457208093, -0.19601208498736597, 0.11305917412007474, -0.19785708775919564, -0.22798823229617105, 0.16712687146972935, -0.0678049002088... |
706.1328 | N = 4 Superfiel Phase Space Coordinates and Hamiltonian Quantization | The N = 4 superfield phase space coordinates are given in the harmonic
superspace. The expressions of the N = 4 classical equations of motion are
determined in terms of the spinorial and harmonic supercharges. Furthermore,
the N = 4 supersymmetric actions are obtained by means of the fermionic and
harmonic functional... | hep-th | the n 4 superfield phase space coordinates are given in the harmonic superspace the expressions of the n 4 classical equations of motion are determined in terms of the spinorial and harmonic supercharges furthermore the n 4 supersymmetric actions are obtained by means of the fermionic and harmonic functionals on the ot... | [['the', 'n', '4', 'superfield', 'phase', 'space', 'coordinates', 'are', 'given', 'in', 'the', 'harmonic', 'superspace', 'the', 'expressions', 'of', 'the', 'n', '4', 'classical', 'equations', 'of', 'motion', 'are', 'determined', 'in', 'terms', 'of', 'the', 'spinorial', 'and', 'harmonic', 'supercharges', 'furthermore', ... | [-0.1793224040216629, 0.20936720741864961, 0.015640338369382497, 0.031773631169926375, -0.008985390337422872, -0.13258725380859313, -0.04986743694648911, 0.3198673195945911, -0.16189518141058776, -0.27947986328329605, 0.0789417341688815, -0.3112306218737593, -0.1731306163695617, 0.13429359060365897, -0.0230408858937712... |
706.1329 | Solidity of viscous liquids. V. Long-wavelength dominance of the
dynamics | This paper is the fifth in a series exploring the physical consequences of
the solidity of glass-forming liquids. Paper IV proposed a model where the
density field is described by a time-dependent Ginzburg-Landau equation of the
nonconserved type with rates in $k$ space of the form $\Gamma_0+Dk^2$. The
model assumes ... | cond-mat.soft | this paper is the fifth in a series exploring the physical consequences of the solidity of glassforming liquids paper iv proposed a model where the density field is described by a timedependent ginzburglandau equation of the nonconserved type with rates in k space of the form gamma_0dk2 the model assumes that dgggamma_... | [['this', 'paper', 'is', 'the', 'fifth', 'in', 'a', 'series', 'exploring', 'the', 'physical', 'consequences', 'of', 'the', 'solidity', 'of', 'glassforming', 'liquids', 'paper', 'iv', 'proposed', 'a', 'model', 'where', 'the', 'density', 'field', 'is', 'described', 'by', 'a', 'timedependent', 'ginzburglandau', 'equation'... | [-0.1345716065649564, 0.17132691676314507, -0.10738606119735374, 0.06106803818164634, -0.03789241892389125, -0.12946363258330773, -0.0021938381289752823, 0.31487934589385985, -0.26315567036055854, -0.2714638164473904, 0.08063841604097333, -0.25919214196813606, -0.15050041171101233, 0.15653391143261816, -7.8240593170954... |
706.133 | Note on: Considering the Case for Biodiversity Cycles: Reexamining the
Evidence for Periodicity in the Fossil Record, by Lieberman and Melott, arXiv
preprint 0704.2896 | Lieberman and Melott built their recent arXiv preprint 0704.2896 on my
published paper and (a preprint of) a subsequent comment by Liebermans
associate Cornette. But had this group waited for the Cornette comment to
actually appear in print together with the expected Reply, they would have
learned that his comment ex... | q-bio.PE astro-ph physics.geo-ph | lieberman and melott built their recent arxiv preprint 07042896 on my published paper and a preprint of a subsequent comment by liebermans associate cornette but had this group waited for the cornette comment to actually appear in print together with the expected reply they would have learned that his comment exposes c... | [['lieberman', 'and', 'melott', 'built', 'their', 'recent', 'arxiv', 'preprint', '07042896', 'on', 'my', 'published', 'paper', 'and', 'a', 'preprint', 'of', 'a', 'subsequent', 'comment', 'by', 'liebermans', 'associate', 'cornette', 'but', 'had', 'this', 'group', 'waited', 'for', 'the', 'cornette', 'comment', 'to', 'act... | [-0.07137909645680338, 0.0794217818444142, -0.14235368127313752, 0.04225600755695875, -0.17598997404954086, -0.1737996596429083, 0.10315505196987133, 0.3393224287136238, -0.1527879953177439, -0.3241734496382479, 0.11178065091242186, -0.29535673084772296, -0.1853214229715781, 0.14966296276284588, -0.23884296437932384, -... |
706.1331 | On a Smale Theorem and Nonhomogeneous Equilibria in Cooperative Systems | A standard result by Smale states that n dimensional strongly cooperative
dynamical systems can have arbitrary dynamics when restricted to unordered
invariant hyperspaces. In this paper this result is extended to the case when
all solutions of the strongly cooperative system are bounded and converge
towards one of on... | math.DS math.AP | a standard result by smale states that n dimensional strongly cooperative dynamical systems can have arbitrary dynamics when restricted to unordered invariant hyperspaces in this paper this result is extended to the case when all solutions of the strongly cooperative system are bounded and converge towards one of only ... | [['a', 'standard', 'result', 'by', 'smale', 'states', 'that', 'n', 'dimensional', 'strongly', 'cooperative', 'dynamical', 'systems', 'can', 'have', 'arbitrary', 'dynamics', 'when', 'restricted', 'to', 'unordered', 'invariant', 'hyperspaces', 'in', 'this', 'paper', 'this', 'result', 'is', 'extended', 'to', 'the', 'case'... | [-0.1785697404274662, 0.14511716188352175, -0.06273266784995155, 0.02130790981212996, 0.00961955831221798, -0.17665685174699106, -0.0067331921936962386, 0.3105460522221584, -0.3010268427395061, -0.22481300983139696, 0.11755756421389021, -0.27097605101252886, -0.1628208717938476, 0.14857005075935056, -0.043761144597007,... |
706.1332 | Constraints on Galaxy Structure and Evolution from the Light of Nearby
Systems | We review knowledge of galaxy structures obtained by their emitted light and
in the local universe where they can be studied in great detail. We discuss the
shapes of, and stellar motions within, galaxies, compositional clues derived
from their spectra, and what luminous matter implies about their dark matter
content... | astro-ph | we review knowledge of galaxy structures obtained by their emitted light and in the local universe where they can be studied in great detail we discuss the shapes of and stellar motions within galaxies compositional clues derived from their spectra and what luminous matter implies about their dark matter content implic... | [['we', 'review', 'knowledge', 'of', 'galaxy', 'structures', 'obtained', 'by', 'their', 'emitted', 'light', 'and', 'in', 'the', 'local', 'universe', 'where', 'they', 'can', 'be', 'studied', 'in', 'great', 'detail', 'we', 'discuss', 'the', 'shapes', 'of', 'and', 'stellar', 'motions', 'within', 'galaxies', 'compositional... | [-0.055494239614879495, 0.11380625561215595, -0.11587849529612748, 0.1747417034267364, -0.11719301412431676, 0.006562210634717199, -0.01886830531007259, 0.4409941788762808, -0.20513297434224456, -0.38387184681706743, 0.03904487339390411, -0.23541599812871608, -0.0918121989205724, 0.1634875420441247, -0.0207089289725132... |
706.1333 | An explicit construction of the Quillen homotopical category of dg Lie
algebras | Let $\g_1$ and $\g_2$ be two dg Lie algebras, then it is well-known that the
$L_\infty$ morphisms from $\g_1$ to $\g_2$ are in 1-1 correspondence to the
solutions of the Maurer-Cartan equation in some dg Lie algebra
$\Bbbk(\g_1,\g_2)$. Then the gauge action by exponents of the zero degree
component $\Bbbk(\g_1,\g_2)^... | math.KT math.QA | let g_1 and g_2 be two dg lie algebras then it is wellknown that the l_infty morphisms from g_1 to g_2 are in 11 correspondence to the solutions of the maurercartan equation in some dg lie algebra bbbkg_1g_2 then the gauge action by exponents of the zero degree component bbbkg_1g_20 on mcsubsetbbbkg_1g_21 gives an expl... | [['let', 'g_1', 'and', 'g_2', 'be', 'two', 'dg', 'lie', 'algebras', 'then', 'it', 'is', 'wellknown', 'that', 'the', 'l_infty', 'morphisms', 'from', 'g_1', 'to', 'g_2', 'are', 'in', '11', 'correspondence', 'to', 'the', 'solutions', 'of', 'the', 'maurercartan', 'equation', 'in', 'some', 'dg', 'lie', 'algebra', 'bbbkg_1g_... | [-0.18093719683459092, 0.053791216651884965, -0.09120618157602589, 0.0965457110384736, -0.14289140736619974, -0.1539045396806865, -0.07469510102949652, 0.413689871142811, -0.42287654759811943, -0.20028365361343684, 0.08910194297345227, -0.23062402203614857, -0.12800432803141404, 0.1409419885804427, -0.2033752826203046,... |
706.1334 | Transients from initial conditions based on Lagrangian perturbation
theory in N-body simulations | We explore the initial conditions for cosmological N-body simulations
suitable for calculating the skewness and kurtosis of the density field. In
general, the initial conditions based on the perturbation theory (PT) provide
incorrect second-order and higher-order growth. These errors implied by the use
of the perturb... | astro-ph | we explore the initial conditions for cosmological nbody simulations suitable for calculating the skewness and kurtosis of the density field in general the initial conditions based on the perturbation theory pt provide incorrect secondorder and higherorder growth these errors implied by the use of the perturbation theo... | [['we', 'explore', 'the', 'initial', 'conditions', 'for', 'cosmological', 'nbody', 'simulations', 'suitable', 'for', 'calculating', 'the', 'skewness', 'and', 'kurtosis', 'of', 'the', 'density', 'field', 'in', 'general', 'the', 'initial', 'conditions', 'based', 'on', 'the', 'perturbation', 'theory', 'pt', 'provide', 'in... | [-0.10705759212995351, 0.11966542834206746, -0.12443817829912047, 0.12088684921330783, -0.01806463900524495, -0.07035613787789526, -0.012885532332741227, 0.3542448149801407, -0.19660968351795266, -0.2942563130342391, 0.14733993700114237, -0.2620667586144939, -0.10219661858354812, 0.21636383336304238, 0.0230088281707466... |
706.1335 | Geometric mesoscopic correlations in quasi-one dimension | We study analytically and numerically field/intensity correlations in wave
transport through volume-disordered waveguide. The obtained channel and spacial
correlations deviate from those found in framework of
Dorokhov-Mello-Pereyra-Kumar (DMPK) formalism, that we relate to
inapplicability of equivalent channel approx... | cond-mat.mes-hall cond-mat.dis-nn | we study analytically and numerically fieldintensity correlations in wave transport through volumedisordered waveguide the obtained channel and spacial correlations deviate from those found in framework of dorokhovmellopereyrakumar dmpk formalism that we relate to inapplicability of equivalent channel approximation in ... | [['we', 'study', 'analytically', 'and', 'numerically', 'fieldintensity', 'correlations', 'in', 'wave', 'transport', 'through', 'volumedisordered', 'waveguide', 'the', 'obtained', 'channel', 'and', 'spacial', 'correlations', 'deviate', 'from', 'those', 'found', 'in', 'framework', 'of', 'dorokhovmellopereyrakumar', 'dmpk... | [-0.1226732041731122, 0.10673076143346927, -0.10654981408179516, 0.0827337926996517, -0.019109881372146663, -0.152852341404096, 0.0008101875716376872, 0.406844744920021, -0.23984982731441656, -0.259442780960706, 0.050483144215485526, -0.284190659946762, -0.17522180344732036, 0.18803790321662311, 0.016978957282290572, 0... |
706.1336 | Can aerosols be trapped in open flows? | The fate of aerosols in open flows is relevant in a variety of physical
contexts. Previous results are consistent with the assumption that such
finite-size particles always escape in open chaotic advection. Here we show
that a different behavior is possible. We analyze the dynamics of aerosols both
in the absence and... | nlin.CD astro-ph physics.flu-dyn | the fate of aerosols in open flows is relevant in a variety of physical contexts previous results are consistent with the assumption that such finitesize particles always escape in open chaotic advection here we show that a different behavior is possible we analyze the dynamics of aerosols both in the absence and prese... | [['the', 'fate', 'of', 'aerosols', 'in', 'open', 'flows', 'is', 'relevant', 'in', 'a', 'variety', 'of', 'physical', 'contexts', 'previous', 'results', 'are', 'consistent', 'with', 'the', 'assumption', 'that', 'such', 'finitesize', 'particles', 'always', 'escape', 'in', 'open', 'chaotic', 'advection', 'here', 'we', 'sho... | [-0.1666411429294385, 0.22847797764380548, -0.06313183638690548, 0.0979134601720778, 0.008482816836542704, -0.09658032336949625, -0.026979464309459383, 0.3218611769378185, -0.24599974029697477, -0.27665317133915696, 0.09429212247487158, -0.2794574227438054, -0.14958635627673092, 0.20218666868115012, -0.0397462772036140... |
706.1337 | A note on Poisson homogeneous spaces | We identify the cotangent bundle Lie algebroid of a Poisson homogeneous space
G/H of a Poisson Lie group G as a quotient of a transformation Lie algebroid
over G. As applications, we describe the modular vector fields of G/H, and we
identify the Poisson cohomology of G/H with coefficients in powers of its
canonical l... | math.DG math.SG | we identify the cotangent bundle lie algebroid of a poisson homogeneous space gh of a poisson lie group g as a quotient of a transformation lie algebroid over g as applications we describe the modular vector fields of gh and we identify the poisson cohomology of gh with coefficients in powers of its canonical line bund... | [['we', 'identify', 'the', 'cotangent', 'bundle', 'lie', 'algebroid', 'of', 'a', 'poisson', 'homogeneous', 'space', 'gh', 'of', 'a', 'poisson', 'lie', 'group', 'g', 'as', 'a', 'quotient', 'of', 'a', 'transformation', 'lie', 'algebroid', 'over', 'g', 'as', 'applications', 'we', 'describe', 'the', 'modular', 'vector', 'f... | [-0.23392459465056595, 0.01648093922995031, -0.07489591158168801, 0.06332379530610169, -0.22600956126984398, -0.08820246804852859, -0.02215964876715157, 0.427553831015603, -0.37783963476323473, -0.18775090262672658, 0.07207034170524991, -0.17205814104842937, -0.19543570770203308, 0.18282555064218023, -0.166615447558273... |
706.1338 | Supersymmetric Hamiltonian Approach to Edge Excitations in $\nu = 5/2$
Fractional Quantum Hall Effect | A supersymmetric Hamiltonian is constructed for the edge excitations of the
Moore-Read (Pfaffian) like state, which is a realization of the N=2
supersymmetric CS model. Fermionic generators and their conjugates are
introduced to deal with the fermion pairing, whose condensation form a BCS like
state. After Bogoliubov... | hep-th cond-mat.mes-hall | a supersymmetric hamiltonian is constructed for the edge excitations of the mooreread pfaffian like state which is a realization of the n2 supersymmetric cs model fermionic generators and their conjugates are introduced to deal with the fermion pairing whose condensation form a bcs like state after bogoliubov transform... | [['a', 'supersymmetric', 'hamiltonian', 'is', 'constructed', 'for', 'the', 'edge', 'excitations', 'of', 'the', 'mooreread', 'pfaffian', 'like', 'state', 'which', 'is', 'a', 'realization', 'of', 'the', 'n2', 'supersymmetric', 'cs', 'model', 'fermionic', 'generators', 'and', 'their', 'conjugates', 'are', 'introduced', 't... | [-0.11344086237243443, 0.22675093465451418, -0.09428649430628866, 0.10812781666131091, -0.04461829559087554, -0.19376335663504765, 0.014021451922807111, 0.28818915606409845, -0.18379797089645372, -0.2726804301367208, 0.03264120626928551, -0.30920809070604655, -0.12811596305774792, 0.09790107604931109, 0.006740605177973... |
706.1339 | Verification theorem and construction of $\epsilon$-optimal controls for
control of abstract evolution equations | We study several aspects of the dynamic programming approach to optimal
control of abstract evolution equations, including a class of semilinear
partial differential equations. We introduce and prove a verification theorem
which provides a sufficient condition for optimality. Moreover we prove sub-
and superoptimalit... | math.OC | we study several aspects of the dynamic programming approach to optimal control of abstract evolution equations including a class of semilinear partial differential equations we introduce and prove a verification theorem which provides a sufficient condition for optimality moreover we prove sub and superoptimality prin... | [['we', 'study', 'several', 'aspects', 'of', 'the', 'dynamic', 'programming', 'approach', 'to', 'optimal', 'control', 'of', 'abstract', 'evolution', 'equations', 'including', 'a', 'class', 'of', 'semilinear', 'partial', 'differential', 'equations', 'we', 'introduce', 'and', 'prove', 'a', 'verification', 'theorem', 'whi... | [-0.18117319546373828, -0.030450427095794503, -0.11924368365933853, 0.10638873082020187, -0.15467495281648422, -0.15740113842600426, 0.04558365249041734, 0.27179811063355636, -0.3300024586330567, -0.3020516783331654, 0.1769196612835263, -0.17548728007490613, -0.19676508238938237, 0.20393062733845518, -0.087825521876636... |
706.134 | Cluster abundances and S-Z power spectra: effects of non-Gaussianity and
early dark energy | In the standard Lambda CDM cosmological model with a Gaussian primordial
density fluctuation field, the relatively low value of the mass variance
parameter (sigma_8=0.74{+0.05}{-0.06}, obtained from the WMAP 3-year data)
results in a reduced likelihood that the measured level of CMB anisotropy on
the scales of cluste... | astro-ph | in the standard lambda cdm cosmological model with a gaussian primordial density fluctuation field the relatively low value of the mass variance parameter sigma_8074005006 obtained from the wmap 3year data results in a reduced likelihood that the measured level of cmb anisotropy on the scales of clusters is due to the ... | [['in', 'the', 'standard', 'lambda', 'cdm', 'cosmological', 'model', 'with', 'a', 'gaussian', 'primordial', 'density', 'fluctuation', 'field', 'the', 'relatively', 'low', 'value', 'of', 'the', 'mass', 'variance', 'parameter', 'sigma_8074005006', 'obtained', 'from', 'the', 'wmap', '3year', 'data', 'results', 'in', 'a', ... | [-0.09604855603977756, 0.09971456913178298, -0.1235026642973037, 0.11739451396967278, -0.05680548469389572, -0.04083587205822363, 0.026938473141705326, 0.31823936940621844, -0.19904658583771884, -0.3573990672059451, 0.029099225707252586, -0.2768045060172583, -0.02527164461958052, 0.1817842873601161, 0.04275063100218210... |
706.1341 | A Study in Depth of f0(1370) | Claims have been made that f0(1370) does not exist. The five primary sets of
data requiring its existence are refitted. Major dispersive effects due to the
opening of the 4pi threshold are included for the first time; the sigma -> 4pi
amplitude plays a strong role. Crystal Barrel data on pbar-p -> 3pizero at rest
req... | hep-ex | claims have been made that f01370 does not exist the five primary sets of data requiring its existence are refitted major dispersive effects due to the opening of the 4pi threshold are included for the first time the sigma 4pi amplitude plays a strong role crystal barrel data on pbarp 3pizero at rest require f01370 sig... | [['claims', 'have', 'been', 'made', 'that', 'f01370', 'does', 'not', 'exist', 'the', 'five', 'primary', 'sets', 'of', 'data', 'requiring', 'its', 'existence', 'are', 'refitted', 'major', 'dispersive', 'effects', 'due', 'to', 'the', 'opening', 'of', 'the', '4pi', 'threshold', 'are', 'included', 'for', 'the', 'first', 't... | [-0.12891002837969953, 0.16542420324055884, -0.041910015972566675, 0.10804336805608467, -0.05774351139502712, -0.12586774827709057, 0.05171635142399062, 0.33970050489658427, -0.1739323998710419, -0.295365835944105, 0.06125576023933017, -0.35936316919523753, 0.004582241811821687, 0.17392803107163515, 0.05871624586937799... |
706.1342 | Low-temperature electron dephasing time in AuPd revisited | Ever since the first discoveries of the quantum-interference transport in
mesoscopic systems, the electron dephasing times, $\tau_\phi$, in the
concentrated AuPd alloys have been extensively measured. The samples were made
from different sources with different compositions, prepared by different
deposition methods, a... | cond-mat.mes-hall cond-mat.dis-nn | ever since the first discoveries of the quantuminterference transport in mesoscopic systems the electron dephasing times tau_phi in the concentrated aupd alloys have been extensively measured the samples were made from different sources with different compositions prepared by different deposition methods and various ge... | [['ever', 'since', 'the', 'first', 'discoveries', 'of', 'the', 'quantuminterference', 'transport', 'in', 'mesoscopic', 'systems', 'the', 'electron', 'dephasing', 'times', 'tau_phi', 'in', 'the', 'concentrated', 'aupd', 'alloys', 'have', 'been', 'extensively', 'measured', 'the', 'samples', 'were', 'made', 'from', 'diffe... | [-0.11221767778915819, 0.21949388787616045, -0.06095125029969495, 0.0376623510645004, 0.01302882738491462, -0.18675636455081984, 0.02245876572560519, 0.38144483740907165, -0.24000444435878307, -0.310036566411145, 0.0540897875551309, -0.334632760938257, -0.07056904862329247, 0.21402402693493058, 0.016634543662075885, 0.... |
706.1343 | Interacting like charges in Landau levels: Planar geometry, symmetries,
and effective quasiparticles | We consider a system of two interacting particles with like but unequal
charges in a magnetic field in the planar geometry. We construct a complete
basis of states compatible with both the axial symmetry and magnetic
translations. The basis is obtained using a canonical transformation that
generates effective quasipa... | cond-mat.mes-hall | we consider a system of two interacting particles with like but unequal charges in a magnetic field in the planar geometry we construct a complete basis of states compatible with both the axial symmetry and magnetic translations the basis is obtained using a canonical transformation that generates effective quasipartic... | [['we', 'consider', 'a', 'system', 'of', 'two', 'interacting', 'particles', 'with', 'like', 'but', 'unequal', 'charges', 'in', 'a', 'magnetic', 'field', 'in', 'the', 'planar', 'geometry', 'we', 'construct', 'a', 'complete', 'basis', 'of', 'states', 'compatible', 'with', 'both', 'the', 'axial', 'symmetry', 'and', 'magne... | [-0.17599427152083874, 0.1699019609443327, -0.05568979789634318, 0.07840520132443693, -0.05010225824403143, -0.12304293726672336, 0.02335427279150722, 0.36969374138677474, -0.21852347969381822, -0.27475785434541133, 0.028244530748677357, -0.2587512659478361, -0.1511794573461434, 0.12249342760642862, 0.0369962978778732,... |
706.1344 | A Class of Partially Solvable Two-Dimensional Quantum Models with
Periodic Potentials | The supersymmetrical approach is used to analyse a class of two-dimensional
quantum systems with periodic potentials. In particular, the method of
SUSY-separation of variables allowed us to find a part of the energy spectra
and the corresponding wave functions (partial solvability) for several models.
These models ar... | hep-th cond-mat.mes-hall math-ph math.MP quant-ph | the supersymmetrical approach is used to analyse a class of twodimensional quantum systems with periodic potentials in particular the method of susyseparation of variables allowed us to find a part of the energy spectra and the corresponding wave functions partial solvability for several models these models are not ame... | [['the', 'supersymmetrical', 'approach', 'is', 'used', 'to', 'analyse', 'a', 'class', 'of', 'twodimensional', 'quantum', 'systems', 'with', 'periodic', 'potentials', 'in', 'particular', 'the', 'method', 'of', 'susyseparation', 'of', 'variables', 'allowed', 'us', 'to', 'find', 'a', 'part', 'of', 'the', 'energy', 'spectr... | [-0.13488255563677978, 0.08472458893590121, -0.06882719471974744, 0.0591988708816327, -0.06801425958426831, -0.14356339301752008, -0.028183607414931706, 0.3349216586262312, -0.2915219978996269, -0.25972513080594817, 0.10808600482794092, -0.28738071163103956, -0.1373996635210579, 0.2111104403966633, 0.000485032202129292... |
706.1345 | Spectroscopy and multiband photometry of the afterglow of intermediate
duration gamma-ray burst 040924 and its host galaxy | We present optical photometry and spectroscopy of the afterglow and host
galaxy of gamma-ray burst 040924. This GRB had a rather short duration of T90
~2.4s, and a well sampled optical afterglow light curve. We aim to use this
dataset to find further evidence that this burst is consistent with a massive
star core-col... | astro-ph | we present optical photometry and spectroscopy of the afterglow and host galaxy of gammaray burst 040924 this grb had a rather short duration of t90 24s and a well sampled optical afterglow light curve we aim to use this dataset to find further evidence that this burst is consistent with a massive star corecollapse pro... | [['we', 'present', 'optical', 'photometry', 'and', 'spectroscopy', 'of', 'the', 'afterglow', 'and', 'host', 'galaxy', 'of', 'gammaray', 'burst', '040924', 'this', 'grb', 'had', 'a', 'rather', 'short', 'duration', 'of', 't90', '24s', 'and', 'a', 'well', 'sampled', 'optical', 'afterglow', 'light', 'curve', 'we', 'aim', '... | [-0.029039196902019112, 0.05156798877987386, -0.08761417178952313, 0.1373893323166177, -0.13234857466329444, -0.10732437748699747, 0.06638570524098232, 0.510448341356947, -0.1624191192919983, -0.3141093985038869, 0.0484563824522527, -0.33568488629336685, -0.007759797827717155, 0.19141718777035305, -0.007583711773870473... |
706.1346 | Southern wide very low-mass stars and brown dwarfs in resolved binary
and multiple systems | The results of the Koenigstuhl survey in the Southern Hemisphere are
presented. I have searched for common-proper motion companions to 173 field
very low-mass stars and brown dwarfs with spectral types > M5.0V and magnitudes
J <= 14.5 mag. I have measured for the first time the common-proper motion of
two new wide sy... | astro-ph | the results of the koenigstuhl survey in the southern hemisphere are presented i have searched for commonproper motion companions to 173 field very lowmass stars and brown dwarfs with spectral types m50v and magnitudes j 145 mag i have measured for the first time the commonproper motion of two new wide systems containi... | [['the', 'results', 'of', 'the', 'koenigstuhl', 'survey', 'in', 'the', 'southern', 'hemisphere', 'are', 'presented', 'i', 'have', 'searched', 'for', 'commonproper', 'motion', 'companions', 'to', '173', 'field', 'very', 'lowmass', 'stars', 'and', 'brown', 'dwarfs', 'with', 'spectral', 'types', 'm50v', 'and', 'magnitudes... | [-0.12493654417722852, 0.13624166350780775, -0.026538359673245797, 0.04949777038426056, -0.07533165850069468, -0.11389631870249876, 0.042324907267230406, 0.40066495469824376, -0.15099105896734738, -0.3907804889250783, 0.05626383624879549, -0.28149743921630366, -0.019395476230714893, 0.19923941607740295, -0.026466082006... |
706.1347 | The Two-State Vector Formalism | The two-state vector formalism (TSVF), the time-symmetric description of the
standard quantum mechanics originated by Aharonov, Bergmann and Lebowitz is
reviewed. The TSVF describes a quantum system at a particular time by two
quantum states: the usual one, evolving forward in time, defined by the results
of a comple... | quant-ph | the twostate vector formalism tsvf the timesymmetric description of the standard quantum mechanics originated by aharonov bergmann and lebowitz is reviewed the tsvf describes a quantum system at a particular time by two quantum states the usual one evolving forward in time defined by the results of a complete measureme... | [['the', 'twostate', 'vector', 'formalism', 'tsvf', 'the', 'timesymmetric', 'description', 'of', 'the', 'standard', 'quantum', 'mechanics', 'originated', 'by', 'aharonov', 'bergmann', 'and', 'lebowitz', 'is', 'reviewed', 'the', 'tsvf', 'describes', 'a', 'quantum', 'system', 'at', 'a', 'particular', 'time', 'by', 'two',... | [-0.13012417171150445, 0.21603723692397275, -0.12738236819083493, 0.045905707511119546, 0.02580189565817515, -0.1503308530834814, 0.04306890801837047, 0.2521462833881378, -0.23131328789517283, -0.26383082032824556, 0.042486306463057795, -0.2405848994354407, -0.08598034419119358, 0.18209326927860578, -0.0176310753573973... |
706.1348 | Weak Value and Weak Measurements | The weak value of a variable O is a description of an effective interaction
with that variable in the limit of weak coupling. It is particularly important
for a pre- and post-selected quantum system.
| quant-ph | the weak value of a variable o is a description of an effective interaction with that variable in the limit of weak coupling it is particularly important for a pre and postselected quantum system | [['the', 'weak', 'value', 'of', 'a', 'variable', 'o', 'is', 'a', 'description', 'of', 'an', 'effective', 'interaction', 'with', 'that', 'variable', 'in', 'the', 'limit', 'of', 'weak', 'coupling', 'it', 'is', 'particularly', 'important', 'for', 'a', 'pre', 'and', 'postselected', 'quantum', 'system']] | [-0.17351990417741678, 0.1489316644596436, -0.08739263446563307, 0.06356728885678903, -0.007899383466471644, -0.18094543341602035, 0.07427323414423667, 0.3308717522989301, -0.22518576031057713, -0.2754276844618075, 0.07710766813868437, -0.2206464069758487, -0.09175409672453123, 0.20045206871102839, 0.002119112444822402... |
706.1349 | Improved quark mass density- dependent model with quark-sigma meson and
quark-omega meson couplings | An improved quark mass density- dependent model with the non-linear scalar
sigma field and the $\omega$-meson field is presented. We show that the present
model can describe saturation properties, the equation of state, the
compressibility and the effective nuclear mass of nuclear matter under mean
field approximatio... | nucl-th | an improved quark mass density dependent model with the nonlinear scalar sigma field and the omegameson field is presented we show that the present model can describe saturation properties the equation of state the compressibility and the effective nuclear mass of nuclear matter under mean field approximation successfu... | [['an', 'improved', 'quark', 'mass', 'density', 'dependent', 'model', 'with', 'the', 'nonlinear', 'scalar', 'sigma', 'field', 'and', 'the', 'omegameson', 'field', 'is', 'presented', 'we', 'show', 'that', 'the', 'present', 'model', 'can', 'describe', 'saturation', 'properties', 'the', 'equation', 'of', 'state', 'the', '... | [-0.08949738389766607, 0.1722926608018184, -0.1216065138502077, 0.09349240882505404, -0.021291071182635964, -0.09149740813452689, -0.024347918726442777, 0.3324669703047295, -0.21661528228919524, -0.319574434157522, 0.026962283548334093, -0.22415815678532006, -0.09025954633767976, 0.09438129421323538, 0.0663173584282764... |
706.135 | The Anisotropic Distribution of Satellite Galaxies | We identify satellites of isolated galaxies in SDSS and examine their angular
distribution. Using mock catalogues generated from cosmological N-body
simulations, we demonstrate that the selection criteria used to select isolated
galaxies and their satellites must be very strict in order to correctly
identify systems ... | astro-ph | we identify satellites of isolated galaxies in sdss and examine their angular distribution using mock catalogues generated from cosmological nbody simulations we demonstrate that the selection criteria used to select isolated galaxies and their satellites must be very strict in order to correctly identify systems in wh... | [['we', 'identify', 'satellites', 'of', 'isolated', 'galaxies', 'in', 'sdss', 'and', 'examine', 'their', 'angular', 'distribution', 'using', 'mock', 'catalogues', 'generated', 'from', 'cosmological', 'nbody', 'simulations', 'we', 'demonstrate', 'that', 'the', 'selection', 'criteria', 'used', 'to', 'select', 'isolated',... | [-0.0940727335671207, 0.08780358080344086, -0.1190742028664365, 0.12774875324981616, -0.10951250900683597, -0.012380935820273022, -0.004343118815951412, 0.4283469962339834, -0.17625449741414437, -0.3654684985182091, 0.06214363870476041, -0.2750485715759772, -0.051810841553945663, 0.18338115069464073, -0.016460350707845... |
706.1351 | Scattering of charge carriers by point defects in bilayer graphene | Theory of scattering of massive chiral fermions in bilayer graphene by radial
symmetric potential is developed. It is shown that in the case when the
electron wavelength is much larger than the radius of the potential the
scattering cross-section is proportional to the electron wavelength. This leads
to the mobility ... | cond-mat.mes-hall cond-mat.mtrl-sci | theory of scattering of massive chiral fermions in bilayer graphene by radial symmetric potential is developed it is shown that in the case when the electron wavelength is much larger than the radius of the potential the scattering crosssection is proportional to the electron wavelength this leads to the mobility indep... | [['theory', 'of', 'scattering', 'of', 'massive', 'chiral', 'fermions', 'in', 'bilayer', 'graphene', 'by', 'radial', 'symmetric', 'potential', 'is', 'developed', 'it', 'is', 'shown', 'that', 'in', 'the', 'case', 'when', 'the', 'electron', 'wavelength', 'is', 'much', 'larger', 'than', 'the', 'radius', 'of', 'the', 'poten... | [-0.11189681316206518, 0.20766412906157664, 0.004060372614707702, 0.01763231722632041, 0.028880215384281024, -0.148716765957383, -0.020618725842676867, 0.358816639185907, -0.1867433495533008, -0.24586163844483402, -0.010266160861087533, -0.33874487640479434, -0.119865174305279, 0.18083889037370682, 0.005714095167767925... |
706.1352 | Hydrodynamic Theory of Granular Solids: Permanent, Transient and
Granular Elasticity | Although fully elastic when static, granular media become transiently elastic
when being slowly sheared -- during which both the elastic energy and stress
relax. Starting from this observation, we cogently derive the framework for
granular hydrodynamics, a set of differential equations consistent with general
princip... | cond-mat.soft | although fully elastic when static granular media become transiently elastic when being slowly sheared during which both the elastic energy and stress relax starting from this observation we cogently derive the framework for granular hydrodynamics a set of differential equations consistent with general principles of ph... | [['although', 'fully', 'elastic', 'when', 'static', 'granular', 'media', 'become', 'transiently', 'elastic', 'when', 'being', 'slowly', 'sheared', 'during', 'which', 'both', 'the', 'elastic', 'energy', 'and', 'stress', 'relax', 'starting', 'from', 'this', 'observation', 'we', 'cogently', 'derive', 'the', 'framework', '... | [-0.08223215264196579, 0.24376798198544958, -0.09400297787327033, 0.035859628953039645, -0.05826406129635871, -0.12996198178913732, -0.011161375368157258, 0.3187455908037149, -0.32417167943472475, -0.2626845365676742, 0.07433936828568291, -0.2847094042226672, -0.14984651606959792, 0.1566207550573521, 0.0276363845771321... |
706.1353 | New 60-cm Radio Survey Telescope with the Sideband-Separating SIS
Receiver for the 200 GHz Band | We have upgraded the 60-cm radio survey telescope located in Nobeyama, Japan.
We developed a new waveguide-type sideband-separating SIS mixer for the
telescope, which enables the simultaneous detection of distinct molecular
emission lines both in the upper and lower sidebands. Over the RF frequency
range of 205-240 G... | astro-ph | we have upgraded the 60cm radio survey telescope located in nobeyama japan we developed a new waveguidetype sidebandseparating sis mixer for the telescope which enables the simultaneous detection of distinct molecular emission lines both in the upper and lower sidebands over the rf frequency range of 205240 ghz the sin... | [['we', 'have', 'upgraded', 'the', '60cm', 'radio', 'survey', 'telescope', 'located', 'in', 'nobeyama', 'japan', 'we', 'developed', 'a', 'new', 'waveguidetype', 'sidebandseparating', 'sis', 'mixer', 'for', 'the', 'telescope', 'which', 'enables', 'the', 'simultaneous', 'detection', 'of', 'distinct', 'molecular', 'emissi... | [-0.10812633093851416, 0.05766259322972586, 0.04303785553202033, -0.025556110256345747, -0.05353173238126943, -0.14591242760558676, 0.057824793766304755, 0.4642214221093133, -0.1438491256525798, -0.30880140710726195, 0.1039091258068274, -0.24446775250372577, -0.05333062185709197, 0.20931377456818492, 0.0379721784287404... |
706.1354 | From Elasticity to Hypoplasticity: Dynamics of Granular Solids | "Granular elasticity," useful for calculating static stress distributions in
granular media, is generalized by including the effects of slowly moving,
deformed grains. The result is a hydrodynamic theory for granular solids that
agrees well with models from soil mechanics.
| cond-mat.soft | granular elasticity useful for calculating static stress distributions in granular media is generalized by including the effects of slowly moving deformed grains the result is a hydrodynamic theory for granular solids that agrees well with models from soil mechanics | [['granular', 'elasticity', 'useful', 'for', 'calculating', 'static', 'stress', 'distributions', 'in', 'granular', 'media', 'is', 'generalized', 'by', 'including', 'the', 'effects', 'of', 'slowly', 'moving', 'deformed', 'grains', 'the', 'result', 'is', 'a', 'hydrodynamic', 'theory', 'for', 'granular', 'solids', 'that',... | [-0.023508281124612458, 0.28733925411525446, -0.1351875475106331, 0.04477367865650031, -0.02084713484136722, -0.11518809250675333, -0.0750661824467198, 0.313672999612605, -0.2644350902678875, -0.2593947617181887, 0.033711025649562285, -0.32530125290250933, -0.17571623884857848, 0.16832445800686494, -0.03796306264419586... |
706.1355 | Water's Hydrogen Bond Strength | Water is necessary both for the evolution of life and its continuance. It
possesses particular properties that cannot be found in other materials and
that are required for life-giving processes. These properties are brought about
by the hydrogen bonded environment particularly evident in liquid water. Each
liquid wat... | cond-mat.soft physics.bio-ph | water is necessary both for the evolution of life and its continuance it possesses particular properties that cannot be found in other materials and that are required for lifegiving processes these properties are brought about by the hydrogen bonded environment particularly evident in liquid water each liquid water mol... | [['water', 'is', 'necessary', 'both', 'for', 'the', 'evolution', 'of', 'life', 'and', 'its', 'continuance', 'it', 'possesses', 'particular', 'properties', 'that', 'can', 'not', 'be', 'found', 'in', 'other', 'materials', 'and', 'that', 'are', 'required', 'for', 'lifegiving', 'processes', 'these', 'properties', 'are', 'b... | [-0.08125657207649929, 0.23739062103978747, -0.04762540578935816, 0.05636593718836136, -0.004303282009718638, -0.1656785814882407, 0.06027342439056817, 0.4074451173330506, -0.2411250690955606, -0.2822411666161188, 0.09770506041842467, -0.29694130124950874, -0.11120808929954161, 0.12676271049087273, 0.029377236905086306... |
706.1356 | A discriminative method to conduct exploratory analyses in networks | This paper, which commented on Newman and Leicht's "Mixture models and
exploratory analysis in networks" (2007, PNAS 104, 9564-9569), has been
withdrawn. The reason for this removal is that we misinterpreted the conceptual
framework that the authors of the original paper use. Specifically, it is
assumed in our paper ... | physics.data-an | this paper which commented on newman and leichts mixture models and exploratory analysis in networks 2007 pnas 104 95649569 has been withdrawn the reason for this removal is that we misinterpreted the conceptual framework that the authors of the original paper use specifically it is assumed in our paper that the variab... | [['this', 'paper', 'which', 'commented', 'on', 'newman', 'and', 'leichts', 'mixture', 'models', 'and', 'exploratory', 'analysis', 'in', 'networks', '2007', 'pnas', '104', '95649569', 'has', 'been', 'withdrawn', 'the', 'reason', 'for', 'this', 'removal', 'is', 'that', 'we', 'misinterpreted', 'the', 'conceptual', 'framew... | [-0.08070350446222299, 0.05119690257620155, -0.11857604940195342, 0.031823243447663345, -0.11767533705947367, -0.15328020489195715, 0.08962952522959493, 0.3661278832770951, -0.21638430855530608, -0.27824154698503883, 0.07971155234646085, -0.30614561258672596, -0.21701270184135651, 0.1001492626251871, -0.133907710254215... |
706.1357 | Self-consistent massive disks in triaxial dark matter halos | Galactic disks in triaxial dark matter halos become deformed by the
elliptical potential in the plane of the disk in such a way as to counteract
the halo ellipticity. We develop a technique to calculate the equilibrium
configuration of such a disk in the combined disk-halo potential, which is
based on the method of J... | astro-ph | galactic disks in triaxial dark matter halos become deformed by the elliptical potential in the plane of the disk in such a way as to counteract the halo ellipticity we develop a technique to calculate the equilibrium configuration of such a disk in the combined diskhalo potential which is based on the method of jog 20... | [['galactic', 'disks', 'in', 'triaxial', 'dark', 'matter', 'halos', 'become', 'deformed', 'by', 'the', 'elliptical', 'potential', 'in', 'the', 'plane', 'of', 'the', 'disk', 'in', 'such', 'a', 'way', 'as', 'to', 'counteract', 'the', 'halo', 'ellipticity', 'we', 'develop', 'a', 'technique', 'to', 'calculate', 'the', 'equ... | [-0.07374578620406932, 0.06168490188262824, -0.13448064744006843, 0.13304082566589517, -0.08815859184001705, -0.03873984230116808, -0.040153983928861894, 0.40347711877631287, -0.16355502067599445, -0.3547172414654467, 0.028439718013396488, -0.22506035829761198, -0.055522905092220756, 0.2148201390435653, -0.036832883747... |
706.1358 | The effects of the little Higgs models on $t\bar{t} h^0$ production via
$\gamma \gamma$ collision at linear colliders | In the frameworks of the littlest Higgs($LH$) model and its extension with
T-parity($LHT$), we studied the associated $t\bar th^0$ production process $e^+
e^- \to \gamma\gamma \to t \bar t h^0$ at the future $e^+e^-$ linear colliders
up to QCD next-to-leading order. We present the regions of $\sqrt{s}-f$
parameter sp... | hep-ph | in the frameworks of the littlest higgslh model and its extension with tparitylht we studied the associated tbar th0 production process e e to gammagamma to t bar t h0 at the future ee linear colliders up to qcd nexttoleading order we present the regions of sqrtsf parameter space in which the lh and lht effects can and... | [['in', 'the', 'frameworks', 'of', 'the', 'littlest', 'higgslh', 'model', 'and', 'its', 'extension', 'with', 'tparitylht', 'we', 'studied', 'the', 'associated', 'tbar', 'th0', 'production', 'process', 'e', 'e', 'to', 'gammagamma', 'to', 't', 'bar', 't', 'h0', 'at', 'the', 'future', 'ee', 'linear', 'colliders', 'up', 't... | [-0.08614735701205142, 0.19728251041429076, -0.0439860175963384, 0.08427712328880621, -0.0810429417936922, -0.15975562159454437, 0.0584564724469745, 0.34327203354282343, -0.2785945044589236, -0.2276102000606253, 0.001660138601437211, -0.31230112758847023, 0.006542282075145476, 0.15316457179770301, 0.051880238411894486,... |
706.1359 | Evidence for high-temperature topological order in an asymmetric quantum
Hall system | Further experiments showed the incorrectness of proposed interpretation.
| cond-mat.mes-hall cond-mat.stat-mech | further experiments showed the incorrectness of proposed interpretation | [['further', 'experiments', 'showed', 'the', 'incorrectness', 'of', 'proposed', 'interpretation']] | [-0.06820531457196921, -0.0802290621213615, -0.16508175432682037, -0.0016127955168485641, -0.06523756403476, -0.0713367322459817, 0.08917792188003659, 0.33685954473912716, -0.14562842552550137, -0.34806436486542225, 0.020998453139327466, -0.22342959186062217, -0.34523723646998405, 0.309881579130888, -0.0628582902718335... |
706.136 | Asymptotic behavior of w in general quintom model | For the quintom models with arbitrary potential $V=V(\phi,\sigma)$, the
asymptotic value of equation of state parameter w is obtained by a new method.
In this method, w of stable attractors are calculated by using the ratio (d ln
V)/(d ln a) in asymptotic region. All the known results, have been obtained by
other met... | gr-qc astro-ph hep-th | for the quintom models with arbitrary potential vvphisigma the asymptotic value of equation of state parameter w is obtained by a new method in this method w of stable attractors are calculated by using the ratio d ln vd ln a in asymptotic region all the known results have been obtained by other methods are reproduced ... | [['for', 'the', 'quintom', 'models', 'with', 'arbitrary', 'potential', 'vvphisigma', 'the', 'asymptotic', 'value', 'of', 'equation', 'of', 'state', 'parameter', 'w', 'is', 'obtained', 'by', 'a', 'new', 'method', 'in', 'this', 'method', 'w', 'of', 'stable', 'attractors', 'are', 'calculated', 'by', 'using', 'the', 'ratio... | [-0.08182238585880545, 0.11286281239332967, -0.0727731111749518, 0.022177882620408276, 0.026466435592499424, -0.1860386657024749, 0.035024279988080755, 0.34339735803545496, -0.21303238933447932, -0.31569178732203657, 0.08074240602904045, -0.27017586635517293, -0.12243101405376783, 0.22897190588419555, -0.00572433965862... |
706.1361 | Domain Wall/Cosmology correspondence in (AdS/dS)_6 x S^4 geometries | We investigate the ten dimensional origin of six dimensional F_4 variant
supergravity with supersymmetric de Sitter background. We address first the
issue of spontaneous compactification, showing that it consists of a warped
compactification on a four sphere of a variant massive type IIA supergravity.
Moreover we ill... | hep-th | we investigate the ten dimensional origin of six dimensional f_4 variant supergravity with supersymmetric de sitter background we address first the issue of spontaneous compactification showing that it consists of a warped compactification on a four sphere of a variant massive type iia supergravity moreover we illustra... | [['we', 'investigate', 'the', 'ten', 'dimensional', 'origin', 'of', 'six', 'dimensional', 'f_4', 'variant', 'supergravity', 'with', 'supersymmetric', 'de', 'sitter', 'background', 'we', 'address', 'first', 'the', 'issue', 'of', 'spontaneous', 'compactification', 'showing', 'that', 'it', 'consists', 'of', 'a', 'warped',... | [-0.15747963391765152, 0.05262285712305256, -0.055987920501940354, 0.13367536078177153, -0.11409952064916011, -0.16950027180475094, 0.0010365007848288582, 0.28659937353504283, -0.15549862952602486, -0.23691817353509606, 0.1469040101203787, -0.2838478109508913, -0.2075212447833951, 0.12081168601489677, -0.12140375011480... |
706.1362 | Particle renormalizations in presence of dissipative environments | We study the Aharonov-Bohm oscillations of a charged particle on a ring of
radius R coupled to a dirty metal environment. With Monte-Carlo methods we
evaluate the curvature of these oscillations which has the form 1/M*R^2, where
M* is an effective mass. We find that at low temperatures T the curvature
approaches at l... | cond-mat.mes-hall | we study the aharonovbohm oscillations of a charged particle on a ring of radius r coupled to a dirty metal environment with montecarlo methods we evaluate the curvature of these oscillations which has the form 1mr2 where m is an effective mass we find that at low temperatures t the curvature approaches at large rl an ... | [['we', 'study', 'the', 'aharonovbohm', 'oscillations', 'of', 'a', 'charged', 'particle', 'on', 'a', 'ring', 'of', 'radius', 'r', 'coupled', 'to', 'a', 'dirty', 'metal', 'environment', 'with', 'montecarlo', 'methods', 'we', 'evaluate', 'the', 'curvature', 'of', 'these', 'oscillations', 'which', 'has', 'the', 'form', '1... | [-0.13187170689141764, 0.20497875603746926, -0.06430148540783932, 0.032419351391761685, 0.0013568563603491772, -0.17189711866909546, 0.021710678901624782, 0.38179073612768166, -0.24390734494248828, -0.2813863190683988, 0.053847825599576134, -0.3155244348183422, -0.06997479828498741, 0.14455347182690212, 0.0050932301835... |
706.1363 | The rational homotopy type of a blow-up in the stable case | Suppose that f:V->W is an embedding of closed oriented manifolds whose normal
bundle has the structure of a complex vector bundle. It is well known in both
complex and symplectic geometry that one can then construct a manifold W' which
is the blow-up of W along V. Assume that dim(W)>2.dim(V)+2 and that H^1(f) is
inje... | math.AT math.SG | suppose that fvw is an embedding of closed oriented manifolds whose normal bundle has the structure of a complex vector bundle it is well known in both complex and symplectic geometry that one can then construct a manifold w which is the blowup of w along v assume that dimw2dimv2 and that h1f is injective we construct ... | [['suppose', 'that', 'fvw', 'is', 'an', 'embedding', 'of', 'closed', 'oriented', 'manifolds', 'whose', 'normal', 'bundle', 'has', 'the', 'structure', 'of', 'a', 'complex', 'vector', 'bundle', 'it', 'is', 'well', 'known', 'in', 'both', 'complex', 'and', 'symplectic', 'geometry', 'that', 'one', 'can', 'then', 'construct'... | [-0.17773296076891218, 0.08124392335162542, -0.06070428120635324, 0.03960370547453857, -0.1329494741729508, -0.1833516883632263, 0.0008454671084202069, 0.34603755510712075, -0.3545696373744789, -0.17835742660592926, 0.07479306658181378, -0.2329269020489646, -0.17715622880496085, 0.17063583640018637, -0.1089661644803265... |
706.1364 | Antiferromagnetism and Superconductivity in a model of Quasi 1D Organic
Conductors | I apply a two-step renormalization group method to the study of the
competition between antiferromagnetism (AFM) and superconductivity in an
anisotropic 2D Hubbard model. I show that this simple model captures the
essentials of the ground-state phases of the quasi 1D organic conductors. As
found experimentally, the g... | cond-mat.str-el cond-mat.supr-con | i apply a twostep renormalization group method to the study of the competition between antiferromagnetism afm and superconductivity in an anisotropic 2d hubbard model i show that this simple model captures the essentials of the groundstate phases of the quasi 1d organic conductors as found experimentally the groundstat... | [['i', 'apply', 'a', 'twostep', 'renormalization', 'group', 'method', 'to', 'the', 'study', 'of', 'the', 'competition', 'between', 'antiferromagnetism', 'afm', 'and', 'superconductivity', 'in', 'an', 'anisotropic', '2d', 'hubbard', 'model', 'i', 'show', 'that', 'this', 'simple', 'model', 'captures', 'the', 'essentials'... | [-0.19061537440678086, 0.24400140530684952, -0.033979729796298826, 0.07221997396742943, 0.013032439470554541, -0.15325626921416682, 0.05554612372964244, 0.3807067173072184, -0.2722743214155086, -0.16366089950550836, -0.026228265038390427, -0.3377792010874008, -0.13170153466570708, 0.11959390902440205, 0.071726986604232... |
706.1365 | Surface-plasmon wave at the planar interface of a metal film and a
structurally chiral medium | The solution of a boundary-value problem formulated for a modified
Kretschmann configuration shows that a surface-plasmon wave can be excited at
the planar interface of a sufficiently thin metal film and a nondissipative
structurally chiral medium, provided the exciting plane wave is p-polarized. An
estimate of the w... | physics.optics physics.class-ph | the solution of a boundaryvalue problem formulated for a modified kretschmann configuration shows that a surfaceplasmon wave can be excited at the planar interface of a sufficiently thin metal film and a nondissipative structurally chiral medium provided the exciting plane wave is ppolarized an estimate of the wavenumb... | [['the', 'solution', 'of', 'a', 'boundaryvalue', 'problem', 'formulated', 'for', 'a', 'modified', 'kretschmann', 'configuration', 'shows', 'that', 'a', 'surfaceplasmon', 'wave', 'can', 'be', 'excited', 'at', 'the', 'planar', 'interface', 'of', 'a', 'sufficiently', 'thin', 'metal', 'film', 'and', 'a', 'nondissipative', ... | [-0.2548363976180553, 0.17506610919874882, -0.09080895985561338, 0.020111115990121935, -0.10517278835177421, -0.1304291747087105, -0.021765253333036194, 0.3392184402793646, -0.26432259141213515, -0.21900204057720574, 0.03624853400344198, -0.27731600993058897, -0.1545852929152633, 0.1919638040052219, 0.10076802168041468... |
706.1366 | On Zermelo'-like problems: a Gauss-Bonnet inequality and a E. Hopf
theorem | The goal of this paper is to describe Zermelo's navigation problem on
Riemannian manifolds as a time-optimal control problem and give an efficient
method in order to evaluate its control curvature. We will show that up to
change the Riemannian metric on the manifold the control curvature of Zermelo's
problem has a si... | math.OC math.DG | the goal of this paper is to describe zermelos navigation problem on riemannian manifolds as a timeoptimal control problem and give an efficient method in order to evaluate its control curvature we will show that up to change the riemannian metric on the manifold the control curvature of zermelos problem has a simple t... | [['the', 'goal', 'of', 'this', 'paper', 'is', 'to', 'describe', 'zermelos', 'navigation', 'problem', 'on', 'riemannian', 'manifolds', 'as', 'a', 'timeoptimal', 'control', 'problem', 'and', 'give', 'an', 'efficient', 'method', 'in', 'order', 'to', 'evaluate', 'its', 'control', 'curvature', 'we', 'will', 'show', 'that', ... | [-0.15364392923580095, -0.007521359761345333, -0.10149773371989255, 0.08229003240646036, -0.17506569099950267, -0.17168566635758667, -0.00492765726061067, 0.3131947729782621, -0.2949777560738417, -0.29349306790710805, 0.10459840042224912, -0.2445125910862871, -0.18061948338380227, 0.23944422190722364, -0.23387326405557... |
706.1367 | Anharmonic behavior in Microwave-driven resistivity oscillations in Hall
bars | We analyzed the magnetoresistivity of a two-dimensional electron system
excited by microwave radiation in a regime of high intensities and low
frequencies. In such a regime, recent experiments show that different features
appear in the magnetoresistivity response which suggest an anharmonic behavior.
These features c... | cond-mat.mes-hall | we analyzed the magnetoresistivity of a twodimensional electron system excited by microwave radiation in a regime of high intensities and low frequencies in such a regime recent experiments show that different features appear in the magnetoresistivity response which suggest an anharmonic behavior these features consist... | [['we', 'analyzed', 'the', 'magnetoresistivity', 'of', 'a', 'twodimensional', 'electron', 'system', 'excited', 'by', 'microwave', 'radiation', 'in', 'a', 'regime', 'of', 'high', 'intensities', 'and', 'low', 'frequencies', 'in', 'such', 'a', 'regime', 'recent', 'experiments', 'show', 'that', 'different', 'features', 'ap... | [-0.17647808469787596, 0.22334164790854197, -0.022775919647843, 0.027304765719842788, -0.026990001879832044, -0.13086580971278072, 0.021634712410602896, 0.3722817584694851, -0.24100759803938368, -0.2586514870857909, 0.01172791064683614, -0.33339718884478015, -0.12348968335538216, 0.2647921541855404, 0.04590188309971597... |
706.1368 | Optical Characterization of Single Mode Components by new
Medianfield-method | In this paper a new method for spotsize-measurement for singlemode optical
components is presented. Based from the classical farfield-method where the
measurements are made circular, the mounting of the used rotary stages and the
long measurement time are great disadvantages. In this paper a new planar
method is desc... | physics.optics | in this paper a new method for spotsizemeasurement for singlemode optical components is presented based from the classical farfieldmethod where the measurements are made circular the mounting of the used rotary stages and the long measurement time are great disadvantages in this paper a new planar method is described w... | [['in', 'this', 'paper', 'a', 'new', 'method', 'for', 'spotsizemeasurement', 'for', 'singlemode', 'optical', 'components', 'is', 'presented', 'based', 'from', 'the', 'classical', 'farfieldmethod', 'where', 'the', 'measurements', 'are', 'made', 'circular', 'the', 'mounting', 'of', 'the', 'used', 'rotary', 'stages', 'and... | [-0.08982211130538158, 0.07604600941496235, -0.0682600321780358, -0.06319734416070527, -0.037713531171903014, -0.136409731162712, -0.0012174138034294758, 0.39982280316097396, -0.23326367206339324, -0.2453888673734452, 0.116189876054081, -0.23482347680255772, -0.1429174077564052, 0.29353107501353537, -0.0984685921376305... |
706.1369 | Visible Wavelength Division Multiplex System for use as a Instructional
Lab System for Higher Education | The demand for high-speed digital communication such as data, video, and the
broadband Internet increases, the required throughput of the modules in
communications systems will also increase. In this paper we present an
instruction system, which works on the basis of a wavelength division multiplex
(WDM) system in th... | physics.optics | the demand for highspeed digital communication such as data video and the broadband internet increases the required throughput of the modules in communications systems will also increase in this paper we present an instruction system which works on the basis of a wavelength division multiplex wdm system in the visible ... | [['the', 'demand', 'for', 'highspeed', 'digital', 'communication', 'such', 'as', 'data', 'video', 'and', 'the', 'broadband', 'internet', 'increases', 'the', 'required', 'throughput', 'of', 'the', 'modules', 'in', 'communications', 'systems', 'will', 'also', 'increase', 'in', 'this', 'paper', 'we', 'present', 'an', 'ins... | [-0.17303901959734502, 0.06764521851800964, -0.05335037902230397, 0.020033009201288223, -0.05422370112501085, -0.14616869719233364, 0.05114986186730675, 0.4220440789288841, -0.24802441283827648, -0.30735160304233433, 0.10724711490911432, -0.26120998412370683, -0.1539317329786718, 0.25597316058352587, -0.127355065424926... |
706.137 | Magnon mode truncation in a rung-dimerized asymmetric spin ladder | An exactly solvable effective model is suggested for an asymmetric spin
ladder with dimerized rungs. Magnon mode truncation originated from magnon
decay (recently observed in the 1D compound ${\rm IPA-CuCl}_3$) is naturally
described within this model. Using Bethe Ansatze we described a one-magnon
sector and obtained... | cond-mat.str-el | an exactly solvable effective model is suggested for an asymmetric spin ladder with dimerized rungs magnon mode truncation originated from magnon decay recently observed in the 1d compound rm ipacucl_3 is naturally described within this model using bethe ansatze we described a onemagnon sector and obtained relations be... | [['an', 'exactly', 'solvable', 'effective', 'model', 'is', 'suggested', 'for', 'an', 'asymmetric', 'spin', 'ladder', 'with', 'dimerized', 'rungs', 'magnon', 'mode', 'truncation', 'originated', 'from', 'magnon', 'decay', 'recently', 'observed', 'in', 'the', '1d', 'compound', 'rm', 'ipacucl_3', 'is', 'naturally', 'descri... | [-0.13034818129586603, 0.19918514125713366, -0.057732646096059506, 0.10088799121680067, -0.055552670425351926, -0.14768489239846957, 0.028140858516973608, 0.36902613441788534, -0.2959033850087401, -0.2397251117755385, 0.023501192982418134, -0.29881196089965456, -0.11513861528707339, 0.13683729902841152, 0.1194420098135... |
706.1371 | Material decomposition mechanisms in femtosecond laser interactions with
metals | A numerical hydrodynamic study of femtosecond laser ablation is presented. A
detailed analysis of material decomposition is performed using a
thermodynamically complete equation of state with separate stable and
metastable phase states and phase boundaries. The lifetime of the metastable
liquid state is estimated bas... | physics.comp-ph | a numerical hydrodynamic study of femtosecond laser ablation is presented a detailed analysis of material decomposition is performed using a thermodynamically complete equation of state with separate stable and metastable phase states and phase boundaries the lifetime of the metastable liquid state is estimated based o... | [['a', 'numerical', 'hydrodynamic', 'study', 'of', 'femtosecond', 'laser', 'ablation', 'is', 'presented', 'a', 'detailed', 'analysis', 'of', 'material', 'decomposition', 'is', 'performed', 'using', 'a', 'thermodynamically', 'complete', 'equation', 'of', 'state', 'with', 'separate', 'stable', 'and', 'metastable', 'phase... | [-0.09668247737863567, 0.20870067285795812, -0.13659216405721963, -0.011849483902551583, 0.0013822280816384591, -0.1177560583819286, 0.08989950041268457, 0.35072688794025453, -0.2494450260492158, -0.26904994183860254, 0.11033206864431122, -0.27629764488665387, -0.058269437178751105, 0.15959902081704058, 0.0281352545550... |
706.1372 | Correlated radio--X-ray variability of Galactic Black Holes: A
radio--X-ray flare in Cygnus X-1 | We report on the first detection of a quasi-simultaneous radio-X-ray flare of
Cygnus X-1. The detection was made on 2005 April 16 with pointed observations
by the Rossi X-ray Timing Explorer and the Ryle telescope, during a phase where
the black hole candidate was close to a transition from the its soft into its
hard... | astro-ph | we report on the first detection of a quasisimultaneous radioxray flare of cygnus x1 the detection was made on 2005 april 16 with pointed observations by the rossi xray timing explorer and the ryle telescope during a phase where the black hole candidate was close to a transition from the its soft into its hard state th... | [['we', 'report', 'on', 'the', 'first', 'detection', 'of', 'a', 'quasisimultaneous', 'radioxray', 'flare', 'of', 'cygnus', 'x1', 'the', 'detection', 'was', 'made', 'on', '2005', 'april', '16', 'with', 'pointed', 'observations', 'by', 'the', 'rossi', 'xray', 'timing', 'explorer', 'and', 'the', 'ryle', 'telescope', 'duri... | [-0.06409554834244773, 0.1657071043198046, -0.044114693185608636, 0.1087162592288989, -0.09711314887298565, -0.08631480289623142, 0.0968686239058642, 0.47611063399205084, -0.16811538489633485, -0.38915920245804286, 0.16271551297119768, -0.3573997085325812, -0.05294129652412314, 0.20390005589119697, -0.01674676633096839... |
706.1373 | Dispersionless limit of the noncommutative potential KP hierarchy and
solutions of the pseudodual chiral model in 2+1 dimensions | The usual dispersionless limit of the KP hierarchy does not work in the case
where the dependent variable has values in a noncommutative (e.g. matrix)
algebra. Passing over to the potential KP hierarchy, there is a corresponding
scaling limit in the noncommutative case, which turns out to be the hierarchy
of a `pseud... | nlin.SI | the usual dispersionless limit of the kp hierarchy does not work in the case where the dependent variable has values in a noncommutative eg matrix algebra passing over to the potential kp hierarchy there is a corresponding scaling limit in the noncommutative case which turns out to be the hierarchy of a pseudodual chir... | [['the', 'usual', 'dispersionless', 'limit', 'of', 'the', 'kp', 'hierarchy', 'does', 'not', 'work', 'in', 'the', 'case', 'where', 'the', 'dependent', 'variable', 'has', 'values', 'in', 'a', 'noncommutative', 'eg', 'matrix', 'algebra', 'passing', 'over', 'to', 'the', 'potential', 'kp', 'hierarchy', 'there', 'is', 'a', '... | [-0.14232558648412427, 0.0715623581022753, -0.07097516866043156, 0.09748459569569948, -0.09033352617457834, -0.15402757586992305, 0.04211220001224834, 0.2609482265441962, -0.306747630842543, -0.26446714907533664, 0.0989831215727305, -0.26772637206359184, -0.1823204510534803, 0.10756912789698961, 0.028810332174095718, 0... |
706.1374 | High Resolution Mapping of Phase Behavior in a Ternary Lipid Mixture: Do
Lipid-Raft Phase Boundaries Depend on Sample-Prep Procedure? | For some time now, we have been using a FRET-based strategy to make
high-resolution studies of phase behavior in ternary lipid-raft membrane
mixtures. Our FRET experiments can be carried out on ordinary, polydisperse
multilamellar vesicle suspensions, so we are able to prepare our samples
according to a procedure tha... | physics.bio-ph | for some time now we have been using a fretbased strategy to make highresolution studies of phase behavior in ternary lipidraft membrane mixtures our fret experiments can be carried out on ordinary polydisperse multilamellar vesicle suspensions so we are able to prepare our samples according to a procedure that was des... | [['for', 'some', 'time', 'now', 'we', 'have', 'been', 'using', 'a', 'fretbased', 'strategy', 'to', 'make', 'highresolution', 'studies', 'of', 'phase', 'behavior', 'in', 'ternary', 'lipidraft', 'membrane', 'mixtures', 'our', 'fret', 'experiments', 'can', 'be', 'carried', 'out', 'on', 'ordinary', 'polydisperse', 'multila... | [-0.06885975177454598, 0.1650822351255235, -0.12123021251275479, 0.018057378998491913, -0.040042012327295894, -0.14361890418427614, 0.09524145621553008, 0.45102121678235774, -0.19161078179582974, -0.33716814915704374, 0.09051788934961866, -0.30597858349039386, -0.142356092151364, 0.17219335574191064, -0.056002137602156... |
706.1375 | Cosmological dynamics of exponential gravity | We present a detailed investigation of the cosmological dynamics based on
$\exp (-R/{\Lambda})$ gravity. We apply the dynamical system approach to both
the vacuum and matter cases and obtain exact solutions and their stability in
the finite and asymptotic regimes. The results show that cosmic histories exist
which ad... | gr-qc astro-ph hep-th | we present a detailed investigation of the cosmological dynamics based on exp rlambda gravity we apply the dynamical system approach to both the vacuum and matter cases and obtain exact solutions and their stability in the finite and asymptotic regimes the results show that cosmic histories exist which admit a double d... | [['we', 'present', 'a', 'detailed', 'investigation', 'of', 'the', 'cosmological', 'dynamics', 'based', 'on', 'exp', 'rlambda', 'gravity', 'we', 'apply', 'the', 'dynamical', 'system', 'approach', 'to', 'both', 'the', 'vacuum', 'and', 'matter', 'cases', 'and', 'obtain', 'exact', 'solutions', 'and', 'their', 'stability', ... | [-0.12832401082568773, 0.0909366009150152, -0.19980813098619832, 0.12113496019843627, -0.04680674875888861, -0.11066044588523889, -0.005227591976466955, 0.3117848594926975, -0.18722704211673277, -0.26166732443468366, 0.12593595589560486, -0.21145241124781244, -0.13862866849045863, 0.20312505209762038, 0.011505688738190... |
706.1376 | Point-contact Andreev reflection spectroscopy of
heavy-fermion-metal/superconductor junctions | Our previous point-contact Andreev reflection studies of the heavy-fermion
superconductor CeCoIn$_5$ using Au tips have shown two clear features: reduced
Andreev signal and asymmetric background conductance [1]. To explore their
physical origins, we have extended our measurements to point-contact junctions
between si... | cond-mat.supr-con cond-mat.str-el | our previous pointcontact andreev reflection studies of the heavyfermion superconductor cecoin_5 using au tips have shown two clear features reduced andreev signal and asymmetric background conductance 1 to explore their physical origins we have extended our measurements to pointcontact junctions between single crystal... | [['our', 'previous', 'pointcontact', 'andreev', 'reflection', 'studies', 'of', 'the', 'heavyfermion', 'superconductor', 'cecoin_5', 'using', 'au', 'tips', 'have', 'shown', 'two', 'clear', 'features', 'reduced', 'andreev', 'signal', 'and', 'asymmetric', 'background', 'conductance', '1', 'to', 'explore', 'their', 'physic... | [-0.15503854604993159, 0.13928529906373185, -0.03592483776693161, -0.04748952545745012, -0.1018673076437643, -0.2379199019418313, 0.13054410017167145, 0.3418015932879196, -0.11232720881928869, -0.37311053860646026, -0.14845962667157156, -0.3982455690033161, -0.11464387328149034, 0.17458057819794004, -0.0412409596476488... |
706.1377 | Bosonic String and String Field Theory: a solution using
Ultradistributions of Exponential Type | In this paper we show that Ultradistributions of Exponential Type (UET) are
appropriate for the description in a consistent way string and string field
theories. A new Lagrangian for the closed string is obtained and shown to be
equivalent to Nambu-Goto's Lagrangian. We also show that the string field is a
linear sup... | hep-th | in this paper we show that ultradistributions of exponential type uet are appropriate for the description in a consistent way string and string field theories a new lagrangian for the closed string is obtained and shown to be equivalent to nambugotos lagrangian we also show that the string field is a linear superpositi... | [['in', 'this', 'paper', 'we', 'show', 'that', 'ultradistributions', 'of', 'exponential', 'type', 'uet', 'are', 'appropriate', 'for', 'the', 'description', 'in', 'a', 'consistent', 'way', 'string', 'and', 'string', 'field', 'theories', 'a', 'new', 'lagrangian', 'for', 'the', 'closed', 'string', 'is', 'obtained', 'and',... | [-0.13938427002112558, 0.1250722740927862, -0.12363653126600627, 0.1566511646646226, -0.07868171299530848, -0.1026281757292816, -0.006579027371166425, 0.3549553621560335, -0.2419342537146263, -0.2061251040258621, 0.06599448561177564, -0.20006889902760047, -0.1652652838179288, 0.1987758149971833, -0.07056253633738772, 0... |
706.1378 | Newton law corrections and instabilities in $f(R)$ gravity with the
effective cosmological constant epoch | We consider class of modified $f(R)$ gravities with the effective
cosmological constant epoch at the early and late universe. Such models pass
most of solar system tests as well they satisfy to cosmological bounds. Despite
their very attractive properties, it is shown that one realistic class of such
models may lead ... | hep-th astro-ph gr-qc | we consider class of modified fr gravities with the effective cosmological constant epoch at the early and late universe such models pass most of solar system tests as well they satisfy to cosmological bounds despite their very attractive properties it is shown that one realistic class of such models may lead to signif... | [['we', 'consider', 'class', 'of', 'modified', 'fr', 'gravities', 'with', 'the', 'effective', 'cosmological', 'constant', 'epoch', 'at', 'the', 'early', 'and', 'late', 'universe', 'such', 'models', 'pass', 'most', 'of', 'solar', 'system', 'tests', 'as', 'well', 'they', 'satisfy', 'to', 'cosmological', 'bounds', 'despit... | [-0.0915100286141611, 0.10436158321521521, -0.1119720188204895, 0.15058398905343243, -0.10873403256902328, -0.2135477510823326, -0.034790765280466894, 0.3119993678979821, -0.23160708935772692, -0.35610443986645274, 0.10806717998399348, -0.24004896526521707, -0.12126652228359419, 0.2192027079770444, -0.03798391244752885... |
706.1379 | On the generalization of the Costas property in the continuum | We extend the definition of the Costas property to functions in the
continuum, namely on intervals of the reals or the rationals, and argue that
such functions can be used in the same applications as discrete Costas arrays.
We construct Costas bijections in the real continuum within the class of
piecewise continuousl... | math.CO | we extend the definition of the costas property to functions in the continuum namely on intervals of the reals or the rationals and argue that such functions can be used in the same applications as discrete costas arrays we construct costas bijections in the real continuum within the class of piecewise continuously dif... | [['we', 'extend', 'the', 'definition', 'of', 'the', 'costas', 'property', 'to', 'functions', 'in', 'the', 'continuum', 'namely', 'on', 'intervals', 'of', 'the', 'reals', 'or', 'the', 'rationals', 'and', 'argue', 'that', 'such', 'functions', 'can', 'be', 'used', 'in', 'the', 'same', 'applications', 'as', 'discrete', 'co... | [-0.12026119174042833, 0.0788004745301805, -0.08227402174088638, 0.09644948003666513, -0.07614818190340884, -0.10375934731273447, 0.0770246441825293, 0.37000953244569246, -0.3212999185547233, -0.21762255325447769, 0.11344438742453349, -0.23071339356756654, -0.18018905651115347, 0.2247249439751613, -0.16399024912825552,... |
706.138 | The Advantages of Four Dimensions for Composite Higgs Models | We examine the relationship between little Higgs and 5d composite models with
identical symmetry structures. By performing an "extreme" deconstruction, one
can reduce any warped composite model to a little Higgs theory on a handful of
sites. This allows us to use 4d intuition and the powerful constraints of
nonlinear... | hep-ph | we examine the relationship between little higgs and 5d composite models with identical symmetry structures by performing an extreme deconstruction one can reduce any warped composite model to a little higgs theory on a handful of sites this allows us to use 4d intuition and the powerful constraints of nonlinear sigma ... | [['we', 'examine', 'the', 'relationship', 'between', 'little', 'higgs', 'and', '5d', 'composite', 'models', 'with', 'identical', 'symmetry', 'structures', 'by', 'performing', 'an', 'extreme', 'deconstruction', 'one', 'can', 'reduce', 'any', 'warped', 'composite', 'model', 'to', 'a', 'little', 'higgs', 'theory', 'on', '... | [-0.08058486134467877, 0.13033463462366096, -0.050125810438034574, 0.13592984571234124, -0.10348346942265288, -0.18484129436743144, 0.02928003179186725, 0.33545589875011295, -0.21448236559988576, -0.32224424546479846, 0.0730428083818092, -0.27266515308496964, -0.1391342028065093, 0.1055925360912185, -0.0672214938227278... |
706.1381 | A geometric invariant theory construction of moduli spaces of stable
maps | We construct the moduli spaces of stable maps, \bar M_g,n(P^r,d), via
geometric invariant theory (GIT). This construction is only valid over Spec C,
but a special case is a GIT presentation of the moduli space of stable curves
of genus g with n marked points, \bar M_g,n; this is valid over Spec Z. Our
method follows ... | math.AG | we construct the moduli spaces of stable maps bar m_gnprd via geometric invariant theory git this construction is only valid over spec c but a special case is a git presentation of the moduli space of stable curves of genus g with n marked points bar m_gn this is valid over spec z our method follows that used in the ca... | [['we', 'construct', 'the', 'moduli', 'spaces', 'of', 'stable', 'maps', 'bar', 'm_gnprd', 'via', 'geometric', 'invariant', 'theory', 'git', 'this', 'construction', 'is', 'only', 'valid', 'over', 'spec', 'c', 'but', 'a', 'special', 'case', 'is', 'a', 'git', 'presentation', 'of', 'the', 'moduli', 'space', 'of', 'stable',... | [-0.19313887419780315, 0.08505641218699232, -0.17076692301072652, 0.0657871750439812, -0.050670276337032076, -0.14275050387258018, 0.032851092645580164, 0.31833067236916174, -0.32256204564171503, -0.15691872176867497, 0.06873647406950735, -0.19930700317932928, -0.12575938875928427, 0.24584551557863155, -0.1736164536633... |
706.1382 | Transversality versus Universality for Additive Quantum Codes | Certain quantum codes allow logic operations to be performed on the encoded
data, such that a multitude of errors introduced by faulty gates can be
corrected. An important class of such operations are {\em transversal}, acting
bitwise between corresponding qubits in each code block, thus allowing error
propagation to... | quant-ph | certain quantum codes allow logic operations to be performed on the encoded data such that a multitude of errors introduced by faulty gates can be corrected an important class of such operations are em transversal acting bitwise between corresponding qubits in each code block thus allowing error propagation to be caref... | [['certain', 'quantum', 'codes', 'allow', 'logic', 'operations', 'to', 'be', 'performed', 'on', 'the', 'encoded', 'data', 'such', 'that', 'a', 'multitude', 'of', 'errors', 'introduced', 'by', 'faulty', 'gates', 'can', 'be', 'corrected', 'an', 'important', 'class', 'of', 'such', 'operations', 'are', 'em', 'transversal',... | [-0.1833315619577964, 0.14898354948543582, -0.04555090198431302, 0.07185917033693166, -0.031412097561621555, -0.2645779864138199, 0.06931410625370013, 0.3886405006878906, -0.30701561753672585, -0.28671970419861653, 0.11973098283719823, -0.1686149561846698, -0.14996863987158845, 0.2896912050054029, -0.1074207286311624, ... |
706.1383 | Fixed point theorem for discontinuous mappings on PN spaces | We present a study on strong t-continuity and measure of discontinuity on PN
spaces. As an application, we prove a fixed point theorem for a self mapping on
PN spaces by means of measure of discontinuity.
| math.FA | we present a study on strong tcontinuity and measure of discontinuity on pn spaces as an application we prove a fixed point theorem for a self mapping on pn spaces by means of measure of discontinuity | [['we', 'present', 'a', 'study', 'on', 'strong', 'tcontinuity', 'and', 'measure', 'of', 'discontinuity', 'on', 'pn', 'spaces', 'as', 'an', 'application', 'we', 'prove', 'a', 'fixed', 'point', 'theorem', 'for', 'a', 'self', 'mapping', 'on', 'pn', 'spaces', 'by', 'means', 'of', 'measure', 'of', 'discontinuity']] | [-0.16700787855328858, -0.04350535668324613, -0.13122115725917474, 0.09054430387914181, 0.0031324348745069334, -0.044842199994517225, 0.11281506506327008, 0.37831364508186066, -0.24386242840971264, -0.2077269627579621, 0.1085583051134433, -0.26182816326618197, -0.17058487183281354, 0.25568561197391576, -0.0692321850253... |
706.1384 | Thermodynamic quantum critical behavior of the Kondo necklace model | We obtain the phase diagram and thermodynamic behavior of the Kondo necklace
model for arbitrary dimensions $d$ using a representation for the localized and
conduction electrons in terms of local Kondo singlet and triplet operators. A
decoupling scheme on the double time Green's functions yields the dispersion
relati... | cond-mat.str-el | we obtain the phase diagram and thermodynamic behavior of the kondo necklace model for arbitrary dimensions d using a representation for the localized and conduction electrons in terms of local kondo singlet and triplet operators a decoupling scheme on the double time greens functions yields the dispersion relation for... | [['we', 'obtain', 'the', 'phase', 'diagram', 'and', 'thermodynamic', 'behavior', 'of', 'the', 'kondo', 'necklace', 'model', 'for', 'arbitrary', 'dimensions', 'd', 'using', 'a', 'representation', 'for', 'the', 'localized', 'and', 'conduction', 'electrons', 'in', 'terms', 'of', 'local', 'kondo', 'singlet', 'and', 'triple... | [-0.17907574368243823, 0.24234055044448202, -0.07167309048570326, 0.051443094257239884, 0.017286296036282726, -0.18391163924854004, 0.10149859379763242, 0.3296695532152541, -0.25819199186459674, -0.22401772149395746, 0.024531618936898317, -0.34440928566793766, -0.07868902258004973, 0.15554188326118218, 0.06506118574163... |
706.1385 | On (g, \phi)-contraction in fuzzy metric spaces | In this paper, we give a generalization of Hicks type contractions and Golet
type contractions on fuzzy metric spaces. We prove some fixed point theorems
for this new type contractions mappings on fuzzy metric spaces.
| math.FA | in this paper we give a generalization of hicks type contractions and golet type contractions on fuzzy metric spaces we prove some fixed point theorems for this new type contractions mappings on fuzzy metric spaces | [['in', 'this', 'paper', 'we', 'give', 'a', 'generalization', 'of', 'hicks', 'type', 'contractions', 'and', 'golet', 'type', 'contractions', 'on', 'fuzzy', 'metric', 'spaces', 'we', 'prove', 'some', 'fixed', 'point', 'theorems', 'for', 'this', 'new', 'type', 'contractions', 'mappings', 'on', 'fuzzy', 'metric', 'spaces'... | [-0.11172144125927896, 0.045555519802934104, -0.02840358648887452, 0.14400416198323535, -0.10352551176294904, -0.11143543602734365, 0.11707107545054682, 0.3312094292658217, -0.2946418731966439, -0.08362792558310662, 0.1818742059986107, -0.3133187755284941, -0.2564546128954081, 0.17747992698979728, -0.2706657986923614, ... |
706.1386 | Interface Width and Bulk Stability: requirements for the simulation of
Deeply Quenched Liquid-Gas Systems | Simulations of liquid-gas systems with extended interfaces are observed to
fail to give accurate results for two reasons: the interface can get ``stuck''
on the lattice or a density overshoot develops around the interface. In the
first case the bulk densities can take a range of values, dependent on the
initial condi... | cond-mat.soft | simulations of liquidgas systems with extended interfaces are observed to fail to give accurate results for two reasons the interface can get stuck on the lattice or a density overshoot develops around the interface in the first case the bulk densities can take a range of values dependent on the initial conditions in t... | [['simulations', 'of', 'liquidgas', 'systems', 'with', 'extended', 'interfaces', 'are', 'observed', 'to', 'fail', 'to', 'give', 'accurate', 'results', 'for', 'two', 'reasons', 'the', 'interface', 'can', 'get', 'stuck', 'on', 'the', 'lattice', 'or', 'a', 'density', 'overshoot', 'develops', 'around', 'the', 'interface', ... | [-0.12584000066597367, 0.12241464884523649, -0.10066472486193691, 0.05946389684361053, -0.03800741747247275, -0.11965861969182025, 0.047851603290916464, 0.3567979818149267, -0.22360481775759122, -0.3298749339460216, 0.06467147553570984, -0.2602449768969987, -0.07816217518382654, 0.18403863697059694, -0.0027159788755711... |
706.1387 | Theory of Neutron Scattering in High-T$_c$ Cuprates: Two Component
Spin-Fermion Model | Recent neutron scattering experiments have revealed that the generic form of
the magnetic excitations in the high-Tc cuprates of wide range of doping has
the so-called "hourglass" shape; it features both upward and downward
excitations at the incommensurate (IC) momenta spanning from the resonance peak
at the commens... | cond-mat.str-el cond-mat.supr-con | recent neutron scattering experiments have revealed that the generic form of the magnetic excitations in the hightc cuprates of wide range of doping has the socalled hourglass shape it features both upward and downward excitations at the incommensurate ic momenta spanning from the resonance peak at the commensurate mom... | [['recent', 'neutron', 'scattering', 'experiments', 'have', 'revealed', 'that', 'the', 'generic', 'form', 'of', 'the', 'magnetic', 'excitations', 'in', 'the', 'hightc', 'cuprates', 'of', 'wide', 'range', 'of', 'doping', 'has', 'the', 'socalled', 'hourglass', 'shape', 'it', 'features', 'both', 'upward', 'and', 'downward... | [-0.17504825432922028, 0.24787688147693568, -0.06610071054811395, 0.061124275856319264, -0.07566850330651731, -0.09775642163387334, 0.05887334311178835, 0.34695509791937335, -0.23033123366920957, -0.2855443926744683, -0.03449571161628376, -0.36025199461583945, -0.08787699859018994, 0.12682949906294486, 0.09611670319857... |
706.1388 | Wall-Crossing Morphisms in Khovanov-Rozansky Homology | We define a wall-crossing morphism for Khovanov-Rozansky homology; that is, a
map between the KR homology of knots related by a crossing change. Using this
map, we extend KR homology to an invariant of singular knots categorifying the
Vasilliev derivative of the HOMFLY polynomial, and of $\mathfrak{sl}_n$ quantum
inv... | math.GT math.QA | we define a wallcrossing morphism for khovanovrozansky homology that is a map between the kr homology of knots related by a crossing change using this map we extend kr homology to an invariant of singular knots categorifying the vasilliev derivative of the homfly polynomial and of mathfraksl_n quantum invariants | [['we', 'define', 'a', 'wallcrossing', 'morphism', 'for', 'khovanovrozansky', 'homology', 'that', 'is', 'a', 'map', 'between', 'the', 'kr', 'homology', 'of', 'knots', 'related', 'by', 'a', 'crossing', 'change', 'using', 'this', 'map', 'we', 'extend', 'kr', 'homology', 'to', 'an', 'invariant', 'of', 'singular', 'knots',... | [-0.27732112508965656, 0.023302472034326154, -0.173325107867034, 0.09911076086185251, -0.06640311633236706, -0.19199864489686055, -0.019499412141158246, 0.2891503115339826, -0.4014358977631976, -0.2246432248405957, 0.011876776329396913, -0.17500572859232003, -0.25173740527437377, 0.12850369743925208, -0.196135283156763... |
706.1389 | Core-shell structures in single flexible-semiflexible block copolymers:
Finding the free energy minimum for the folding transition | We investigate the folding transition of a single diblock copolymer
consisting of a semiflexible and a flexible block. We obtain a {\it
Saturn-shaped} core-shell conformation in the folded state, in which the
flexible block forms a core and the semiflexible block wraps around it. We
demonstrate two distinctive featur... | cond-mat.soft | we investigate the folding transition of a single diblock copolymer consisting of a semiflexible and a flexible block we obtain a it saturnshaped coreshell conformation in the folded state in which the flexible block forms a core and the semiflexible block wraps around it we demonstrate two distinctive features of the ... | [['we', 'investigate', 'the', 'folding', 'transition', 'of', 'a', 'single', 'diblock', 'copolymer', 'consisting', 'of', 'a', 'semiflexible', 'and', 'a', 'flexible', 'block', 'we', 'obtain', 'a', 'it', 'saturnshaped', 'coreshell', 'conformation', 'in', 'the', 'folded', 'state', 'in', 'which', 'the', 'flexible', 'block',... | [-0.14303206833477794, 0.14290173581790133, -0.07501077482544155, 0.0020059019955525914, -0.012660471046433211, -0.2038463122065527, -0.012480154252016401, 0.44637195590928375, -0.26193140972271023, -0.1851814211155456, 0.03618933935509434, -0.23479897347110582, -0.20923959405486842, 0.08008084271148026, 0.054605554991... |
706.139 | Strong atom-field coupling for Bose-Einstein condensates in an optical
cavity on a chip | An optical cavity enhances the interaction between atoms and light, and the
rate of coherent atom-photon coupling can be made larger than all decoherence
rates of the system. For single atoms, this strong coupling regime of cavity
quantum electrodynamics (cQED) has been the subject of spectacular experimental
advance... | quant-ph | an optical cavity enhances the interaction between atoms and light and the rate of coherent atomphoton coupling can be made larger than all decoherence rates of the system for single atoms this strong coupling regime of cavity quantum electrodynamics cqed has been the subject of spectacular experimental advances and gr... | [['an', 'optical', 'cavity', 'enhances', 'the', 'interaction', 'between', 'atoms', 'and', 'light', 'and', 'the', 'rate', 'of', 'coherent', 'atomphoton', 'coupling', 'can', 'be', 'made', 'larger', 'than', 'all', 'decoherence', 'rates', 'of', 'the', 'system', 'for', 'single', 'atoms', 'this', 'strong', 'coupling', 'regim... | [-0.17554332339538656, 0.2040489665635254, -0.004999839015618821, -0.04808822297407681, -0.006483472242791165, -0.20586385948777092, 0.06077285908332836, 0.415226170082166, -0.22338037726245688, -0.28755398540620736, 0.02700919489206005, -0.24712809591432475, -0.057372388696151126, 0.23306789083446386, 0.02262040049254... |
706.1391 | Elastic scattering theory and transport in graphene | Electron properties of graphene are described in terms of Dirac fermions.
Here we thoroughly outline the elastic scattering theory for the
two-dimensional massive Dirac fermions in the presence of an axially symmetric
potential. While the massless limit is relevant for pristine graphene, keeping
finite mass allows fo... | cond-mat.mes-hall cond-mat.mtrl-sci | electron properties of graphene are described in terms of dirac fermions here we thoroughly outline the elastic scattering theory for the twodimensional massive dirac fermions in the presence of an axially symmetric potential while the massless limit is relevant for pristine graphene keeping finite mass allows for gene... | [['electron', 'properties', 'of', 'graphene', 'are', 'described', 'in', 'terms', 'of', 'dirac', 'fermions', 'here', 'we', 'thoroughly', 'outline', 'the', 'elastic', 'scattering', 'theory', 'for', 'the', 'twodimensional', 'massive', 'dirac', 'fermions', 'in', 'the', 'presence', 'of', 'an', 'axially', 'symmetric', 'poten... | [-0.14567449382167397, 0.1924362791676836, -0.04134998757932225, 0.07892211418552049, -0.01917157979191628, -0.15301689752460232, 0.05014047052810443, 0.3634212228893881, -0.24207276961705565, -0.22623591311827038, -0.02455542235395502, -0.3526781182199718, -0.15559136553959557, 0.15530166373045332, 0.04426597632996782... |
706.1392 | Two-dimensional N=(2,2) super Yang-Mills theory on computer | We carry out preliminary numerical study of Sugino's lattice formulation
\cite{Sugino:2004qd,Sugino:2004qdf} of the two-dimensional $\mathcal{N}=(2,2)$
super Yang-Mills theory (2d $\mathcal{N}=(2,2)$ SYM) with the gauge group
$\SU(2)$. The effect of dynamical fermions is included by re-weighting a
quenched ensemble b... | hep-lat hep-th | we carry out preliminary numerical study of suginos lattice formulation citesugino2004qdsugino2004qdf of the twodimensional mathcaln22 super yangmills theory 2d mathcaln22 sym with the gauge group su2 the effect of dynamical fermions is included by reweighting a quenched ensemble by the pfaffian factor it appears that ... | [['we', 'carry', 'out', 'preliminary', 'numerical', 'study', 'of', 'suginos', 'lattice', 'formulation', 'citesugino2004qdsugino2004qdf', 'of', 'the', 'twodimensional', 'mathcaln22', 'super', 'yangmills', 'theory', '2d', 'mathcaln22', 'sym', 'with', 'the', 'gauge', 'group', 'su2', 'the', 'effect', 'of', 'dynamical', 'fe... | [-0.1181118665720643, 0.20466816920265246, -0.07667949896122765, 0.0945563752142271, -0.03911940918460144, -0.12720083946098354, 0.0449152508477352, 0.3706226706332554, -0.19911985439527646, -0.24875101498987612, 0.0875848699879235, -0.29274028616639747, -0.16177803824111991, 0.10954073224434727, 0.009866254756797773, ... |
706.1393 | A universal property of the monoidal 2-category of cospans of finite
linear orders and surjections | We prove that the monoidal 2-category of cospans of finite linear orders and
surjections is the universal monoidal category with an object X with a
semigroup and a cosemigroup structures, where the two structures satisfy a
certain 2-dimensional separable algebra condition.
| math.CT | we prove that the monoidal 2category of cospans of finite linear orders and surjections is the universal monoidal category with an object x with a semigroup and a cosemigroup structures where the two structures satisfy a certain 2dimensional separable algebra condition | [['we', 'prove', 'that', 'the', 'monoidal', '2category', 'of', 'cospans', 'of', 'finite', 'linear', 'orders', 'and', 'surjections', 'is', 'the', 'universal', 'monoidal', 'category', 'with', 'an', 'object', 'x', 'with', 'a', 'semigroup', 'and', 'a', 'cosemigroup', 'structures', 'where', 'the', 'two', 'structures', 'sati... | [-0.19004438510164617, 0.08931192976051534, -0.05344927092955913, 0.07670949969324284, -0.14192581189563497, -0.1379795685992576, -0.04594764618668705, 0.39985590511932967, -0.46123472414910793, -0.1198408137075603, 0.09671565316384659, -0.20616742842830718, -0.10442238880787044, 0.13464676716830581, -0.160599749279208... |
706.1394 | Measurement of the CKM angles alpha and gamma at the BaBar experiment | We present recent measurements of the CKM angles alpha and gamma using data
collected by the BaBar detector at the PEP-II asymmetric-energy e+ e- collider
at the Stanford Linear Accelerator Center. In addition to constraints on alpha
from the decays B0 -> pi+ pi-, B0 -> rho+ pi- and B0 -> rho+ rho-, we also
report th... | hep-ex | we present recent measurements of the ckm angles alpha and gamma using data collected by the babar detector at the pepii asymmetricenergy e e collider at the stanford linear accelerator center in addition to constraints on alpha from the decays b0 pi pi b0 rho pi and b0 rho rho we also report the first measurement of t... | [['we', 'present', 'recent', 'measurements', 'of', 'the', 'ckm', 'angles', 'alpha', 'and', 'gamma', 'using', 'data', 'collected', 'by', 'the', 'babar', 'detector', 'at', 'the', 'pepii', 'asymmetricenergy', 'e', 'e', 'collider', 'at', 'the', 'stanford', 'linear', 'accelerator', 'center', 'in', 'addition', 'to', 'constra... | [-0.14923105129729147, 0.22133174460664715, -0.1440477855908482, -0.014017498563549927, -0.0559158041951773, -0.1870836906246436, 0.1537030244969925, 0.2348061370379899, -0.2469652486641122, -0.1728238917320319, -0.10298002364225281, -0.48519701974810625, 0.03467729759817619, 0.1338113212689717, 0.1604882663966197, 0.1... |
706.1395 | Opportunistic Network Coding for Video Streaming over Wireless | In this paper, we study video streaming over wireless networks with network
coding capabilities. We build upon recent work, which demonstrated that network
coding can increase throughput over a broadcast medium, by mixing packets from
different flows into a single packet, thus increasing the information content
per t... | cs.NI | in this paper we study video streaming over wireless networks with network coding capabilities we build upon recent work which demonstrated that network coding can increase throughput over a broadcast medium by mixing packets from different flows into a single packet thus increasing the information content per transmis... | [['in', 'this', 'paper', 'we', 'study', 'video', 'streaming', 'over', 'wireless', 'networks', 'with', 'network', 'coding', 'capabilities', 'we', 'build', 'upon', 'recent', 'work', 'which', 'demonstrated', 'that', 'network', 'coding', 'can', 'increase', 'throughput', 'over', 'a', 'broadcast', 'medium', 'by', 'mixing', '... | [-0.20088417285129612, 0.03317944437921902, -0.05552578788464431, -0.0038843678928850616, -0.036819314202446426, -0.2169172040751723, 0.10068846671922194, 0.45336442339982164, -0.30573915149329506, -0.2671232699859338, 0.08789385845178554, -0.2558962978044769, -0.19768157705176073, 0.1315819235140702, -0.16541981229131... |
706.1396 | A universal enveloping for L-infinity algebras | For any L-infinity algebra L, we construct an A-infinity structure on the
space of symmetric tensors Sym*(L), which generalizes the classical universal
enveloping for Lie algebras. Our construction is based on an invariant homotopy
on a cobar construction of the symmetric coalgebra, which is obtained through
its rela... | math.RT math.RA | for any linfinity algebra l we construct an ainfinity structure on the space of symmetric tensors syml which generalizes the classical universal enveloping for lie algebras our construction is based on an invariant homotopy on a cobar construction of the symmetric coalgebra which is obtained through its relation with p... | [['for', 'any', 'linfinity', 'algebra', 'l', 'we', 'construct', 'an', 'ainfinity', 'structure', 'on', 'the', 'space', 'of', 'symmetric', 'tensors', 'syml', 'which', 'generalizes', 'the', 'classical', 'universal', 'enveloping', 'for', 'lie', 'algebras', 'our', 'construction', 'is', 'based', 'on', 'an', 'invariant', 'hom... | [-0.13068742579165496, 0.057416066532308796, -0.10741545616666663, 0.0587359600972806, -0.20703996461376828, -0.10243571305401483, -0.0647369600516164, 0.3618624394513526, -0.37024216142149186, -0.17246133493224405, 0.11033207608852535, -0.14695245018756053, -0.18660801392540616, 0.19031926407918054, -0.167958494539390... |
706.1397 | Towards A Realistic Grand Gauge-Higgs Unification | We investigate a 5D SU(6) grand gauge-Higgs unification model compactified on
an orbifold S^1/Z_2. Ordinary quarks and leptons, together with right-handed
neutrinos, are just accommodated into a minimal set of representations of the
gauge group, without introducing any exotic states. The proton decay turns out
to be ... | hep-ph | we investigate a 5d su6 grand gaugehiggs unification model compactified on an orbifold s1z_2 ordinary quarks and leptons together with righthanded neutrinos are just accommodated into a minimal set of representations of the gauge group without introducing any exotic states the proton decay turns out to be forbidden at ... | [['we', 'investigate', 'a', '5d', 'su6', 'grand', 'gaugehiggs', 'unification', 'model', 'compactified', 'on', 'an', 'orbifold', 's1z_2', 'ordinary', 'quarks', 'and', 'leptons', 'together', 'with', 'righthanded', 'neutrinos', 'are', 'just', 'accommodated', 'into', 'a', 'minimal', 'set', 'of', 'representations', 'of', 't... | [-0.143327984759318, 0.3412886264799359, -0.043718757730751456, 0.20640472754043854, -0.11550612854011592, -0.23436265671852516, 0.03981811938771083, 0.3550050386632853, -0.1727086647546717, -0.2761944823039623, 0.03844745611082521, -0.23162238876782842, 0.022841112549090152, -0.006523141108283942, 0.025808454696814736... |
706.1398 | BGG correspondence for toric complete intersections | We generalize the classical Bernstein-Gelfand-Gelfand correspondence to
complete intersections in toric varieties.
| math.RT math.AG | we generalize the classical bernsteingelfandgelfand correspondence to complete intersections in toric varieties | [['we', 'generalize', 'the', 'classical', 'bernsteingelfandgelfand', 'correspondence', 'to', 'complete', 'intersections', 'in', 'toric', 'varieties']] | [-0.19015201747727892, -0.13491592983094355, -0.09044738921026389, 0.22040949078897634, -0.13659654992322126, -0.16852780788516006, -0.049647435545921326, 0.283411483746022, -0.3152996450662613, -0.1196716248523444, 0.019288306434949238, -0.23272394854575396, -0.16686511606288454, 0.11437317046026389, -0.40411360375583... |
706.1399 | Duality and Stability Regions of Multi-rate Broadcast and Multiple
Access Networks | We characterize stability regions of two-user fading Gaussian multiple access
(MAC) and broadcast (BC) networks with centralized scheduling. The data to be
transmitted to the users is encoded into codewords of fixed length. The rates
of the codewords used are restricted to a fixed set of finite cardinality. With
succ... | cs.IT math.IT | we characterize stability regions of twouser fading gaussian multiple access mac and broadcast bc networks with centralized scheduling the data to be transmitted to the users is encoded into codewords of fixed length the rates of the codewords used are restricted to a fixed set of finite cardinality with successive dec... | [['we', 'characterize', 'stability', 'regions', 'of', 'twouser', 'fading', 'gaussian', 'multiple', 'access', 'mac', 'and', 'broadcast', 'bc', 'networks', 'with', 'centralized', 'scheduling', 'the', 'data', 'to', 'be', 'transmitted', 'to', 'the', 'users', 'is', 'encoded', 'into', 'codewords', 'of', 'fixed', 'length', 't... | [-0.26813162632148574, 0.052269788360205925, -0.05089157004668205, 0.01212506448953516, -0.028988801084320854, -0.23300749336334842, 0.12819116353057325, 0.3909780388732475, -0.3341435046383628, -0.20031407347845812, 0.12011124906906237, -0.2337138757523563, -0.10665085922616223, 0.0983696547060929, -0.1051205937252638... |
706.14 | Electronic structure of NaWO$_3$: Role of the impurity potential | We have performed {\it ab-initio} electronic structure calculations to
determine the evolution of the electronic structure of WO$_3$ with Na doping.
Na doping introduces an additional electron when introduced into WO$_3$. The
ensuing electronic structure of Na doped WO$_3$, we find, is very similar to
the electronic ... | cond-mat.mtrl-sci | we have performed it abinitio electronic structure calculations to determine the evolution of the electronic structure of wo_3 with na doping na doping introduces an additional electron when introduced into wo_3 the ensuing electronic structure of na doped wo_3 we find is very similar to the electronic structure of an ... | [['we', 'have', 'performed', 'it', 'abinitio', 'electronic', 'structure', 'calculations', 'to', 'determine', 'the', 'evolution', 'of', 'the', 'electronic', 'structure', 'of', 'wo_3', 'with', 'na', 'doping', 'na', 'doping', 'introduces', 'an', 'additional', 'electron', 'when', 'introduced', 'into', 'wo_3', 'the', 'ensui... | [-0.07185313684028496, 0.1360194794943133, -0.04093701456921226, 0.060742441027579024, -0.028659912069763885, -0.16471790449710888, 0.07502563362684819, 0.3887013186179443, -0.2912045067919572, -0.30466908433500234, -0.040572627188014125, -0.28549431306494233, -0.1454563332566593, 0.12351599288463525, 0.018353975728290... |
706.1401 | Controlling for individual heterogeneity in longitudinal models, with
applications to student achievement | Longitudinal data tracking repeated measurements on individuals are highly
valued for research because they offer controls for unmeasured individual
heterogeneity that might otherwise bias results. Random effects or mixed models
approaches, which treat individual heterogeneity as part of the model error
term and use ... | stat.AP | longitudinal data tracking repeated measurements on individuals are highly valued for research because they offer controls for unmeasured individual heterogeneity that might otherwise bias results random effects or mixed models approaches which treat individual heterogeneity as part of the model error term and use gene... | [['longitudinal', 'data', 'tracking', 'repeated', 'measurements', 'on', 'individuals', 'are', 'highly', 'valued', 'for', 'research', 'because', 'they', 'offer', 'controls', 'for', 'unmeasured', 'individual', 'heterogeneity', 'that', 'might', 'otherwise', 'bias', 'results', 'random', 'effects', 'or', 'mixed', 'models', ... | [-0.055874247404406906, 0.11398734299655189, -0.09430636731259576, 0.11649170621436693, -0.10415050219524198, -0.19340796180295985, 0.07166329421090416, 0.38678063130056534, -0.26803695415524215, -0.34561658551211694, 0.08665170264980956, -0.2963434612516918, -0.16267050345580886, 0.15829766405482046, -0.08119064318393... |
706.1402 | Analyzing Design Process and Experiments on the AnITA Generic Tutoring
System | In the field of tutoring systems, investigations have shown that there are
many tutoring systems specific to a specific domain that, because of their
static architecture, cannot be adapted to other domains. As consequence, often
neither methods nor knowledge can be reused. In addition, the knowledge
engineer must hav... | cs.CY cs.HC | in the field of tutoring systems investigations have shown that there are many tutoring systems specific to a specific domain that because of their static architecture cannot be adapted to other domains as consequence often neither methods nor knowledge can be reused in addition the knowledge engineer must have program... | [['in', 'the', 'field', 'of', 'tutoring', 'systems', 'investigations', 'have', 'shown', 'that', 'there', 'are', 'many', 'tutoring', 'systems', 'specific', 'to', 'a', 'specific', 'domain', 'that', 'because', 'of', 'their', 'static', 'architecture', 'can', 'not', 'be', 'adapted', 'to', 'other', 'domains', 'as', 'conseque... | [-0.09228645671858915, 0.03752079904692883, -0.08648383075477344, 0.04418881692990527, -0.14578764617978457, -0.1571099187225148, -0.0005802543831063423, 0.4062899032016536, -0.23305763099286816, -0.33705532704730945, 0.17316311961290856, -0.23107303491888379, -0.20205247610483965, 0.22142804640032976, -0.1036019981141... |
706.1403 | Spin Coulomb drag beyond the random phase approximation | We study the spin Coulomb drag in a quasi-two-dimensional electron gas beyond
the random phase approximation (RPA). We find that the finite transverse width
of the electron gas causes a significant reduction of the spin Coulomb drag.
This reduction, however, is largely compensated by the enhancement coming from
the i... | cond-mat.mes-hall | we study the spin coulomb drag in a quasitwodimensional electron gas beyond the random phase approximation rpa we find that the finite transverse width of the electron gas causes a significant reduction of the spin coulomb drag this reduction however is largely compensated by the enhancement coming from the inclusion o... | [['we', 'study', 'the', 'spin', 'coulomb', 'drag', 'in', 'a', 'quasitwodimensional', 'electron', 'gas', 'beyond', 'the', 'random', 'phase', 'approximation', 'rpa', 'we', 'find', 'that', 'the', 'finite', 'transverse', 'width', 'of', 'the', 'electron', 'gas', 'causes', 'a', 'significant', 'reduction', 'of', 'the', 'spin'... | [-0.125170539302441, 0.20264826349914075, -0.05244163863360882, 0.04973169849254191, 0.00030650014678637187, -0.09230393342673779, 0.0865398620814085, 0.30408734815816085, -0.2213159732396404, -0.30434537678956985, -0.06515578397704909, -0.314582686573267, -0.10863702733069658, 0.14823450333128374, 0.001020045230786005... |
706.1404 | Rate of Convergence of Space Time Approximations for stochastic
evolution equations | Stochastic evolution equations in Banach spaces with unbounded nonlinear
drift and diffusion operators driven by a finite dimensional Brownian motion
are considered. Under some regularity condition assumed for the solution, the
rate of convergence of various numerical approximations are estimated under
strong monoton... | math.PR | stochastic evolution equations in banach spaces with unbounded nonlinear drift and diffusion operators driven by a finite dimensional brownian motion are considered under some regularity condition assumed for the solution the rate of convergence of various numerical approximations are estimated under strong monotonicit... | [['stochastic', 'evolution', 'equations', 'in', 'banach', 'spaces', 'with', 'unbounded', 'nonlinear', 'drift', 'and', 'diffusion', 'operators', 'driven', 'by', 'a', 'finite', 'dimensional', 'brownian', 'motion', 'are', 'considered', 'under', 'some', 'regularity', 'condition', 'assumed', 'for', 'the', 'solution', 'the',... | [-0.12699666268317333, 0.09117016663302237, -0.03181521570893811, 0.10581701982300729, -0.11226831356744602, -0.15795217302919767, -0.05920792105538187, 0.34160291236727985, -0.35808779057393325, -0.16823430118887728, 0.19808032957371324, -0.20915608227586568, -0.11372760606846258, 0.2070549835603851, -0.11358637321017... |
706.1405 | The absolute order on the symmetric group, constructible partially
ordered sets and Cohen-Macaulay complexes | The absolute order is a natural partial order on a Coxeter group W. It can be
viewed as an analogue of the weak order on W in which the role of the
generating set of simple reflections in W is played by the set of all
reflections in W. By use of a notion of constructibility for partially ordered
sets, it is proved th... | math.CO | the absolute order is a natural partial order on a coxeter group w it can be viewed as an analogue of the weak order on w in which the role of the generating set of simple reflections in w is played by the set of all reflections in w by use of a notion of constructibility for partially ordered sets it is proved that th... | [['the', 'absolute', 'order', 'is', 'a', 'natural', 'partial', 'order', 'on', 'a', 'coxeter', 'group', 'w', 'it', 'can', 'be', 'viewed', 'as', 'an', 'analogue', 'of', 'the', 'weak', 'order', 'on', 'w', 'in', 'which', 'the', 'role', 'of', 'the', 'generating', 'set', 'of', 'simple', 'reflections', 'in', 'w', 'is', 'playe... | [-0.15878893656825477, 0.10779005999965276, -0.05950989902696826, 0.03895724582993849, -0.08946348562074656, -0.025406669435853308, 0.028756580891256982, 0.3352107276632027, -0.3192065277560191, -0.2702589118726213, 0.12100309115749869, -0.2522014782996848, -0.11816871072250333, 0.1786327301693911, -0.08983091835609891... |
706.1406 | Jordan structures and non-associative geometry | In this survey paper we give an overview over constructions of geometries
associated to Jordan structures (algebras, triple systems and pairs), featuring
analogs of these constructions with the Lie functor on the one hand and with
the approach of non-commutative geometry on the other hand.
| math.RA | in this survey paper we give an overview over constructions of geometries associated to jordan structures algebras triple systems and pairs featuring analogs of these constructions with the lie functor on the one hand and with the approach of noncommutative geometry on the other hand | [['in', 'this', 'survey', 'paper', 'we', 'give', 'an', 'overview', 'over', 'constructions', 'of', 'geometries', 'associated', 'to', 'jordan', 'structures', 'algebras', 'triple', 'systems', 'and', 'pairs', 'featuring', 'analogs', 'of', 'these', 'constructions', 'with', 'the', 'lie', 'functor', 'on', 'the', 'one', 'hand'... | [-0.14842350207683114, -0.0021597748696674697, -0.07731601192305486, 0.02119439167436212, -0.10283949772516886, -0.14116384004139237, -0.04867691919983675, 0.3604568872186873, -0.2767790553884374, -0.2790286812517378, 0.13695991225281937, -0.2687846726543891, -0.19103726351426709, 0.27368439762956565, -0.12430269258717... |
706.1407 | Absolute continuity of the measures of the Dunkl intetwining operator
and its dualand applications | In this paper we consider the representing measures $\mu_{x},x\in
\QTR{Bbb}{R}^{d}$, and $\nu_{y},y\in \QTR{Bbb}{R}^{d}$, of the Dunkl
intertwining operator and of its dual. When the multiplicity function is
positive, we prove that for all $x\in \QTR{Bbb}{R}_{\QTO{mbox}{reg}}^{d}$ we
have $d\mu_{x}(y)=\QTR{cal}{K}(x,... | math.FA math.CA | in this paper we consider the representing measures mu_xxin qtrbbbrd and nu_yyin qtrbbbrd of the dunkl intertwining operator and of its dual when the multiplicity function is positive we prove that for all xin qtrbbbr_qtomboxregd we have dmu_xyqtrcalkxydy and for almost all yin qtrbbbrd we have dnu_yxqtrcalkxyomega_kxd... | [['in', 'this', 'paper', 'we', 'consider', 'the', 'representing', 'measures', 'mu_xxin', 'qtrbbbrd', 'and', 'nu_yyin', 'qtrbbbrd', 'of', 'the', 'dunkl', 'intertwining', 'operator', 'and', 'of', 'its', 'dual', 'when', 'the', 'multiplicity', 'function', 'is', 'positive', 'we', 'prove', 'that', 'for', 'all', 'xin', 'qtrbb... | [-0.13083781804677777, 0.10553345418619839, -0.007002307737076824, 0.019437345365242272, -0.0037755648637275126, -0.13745159470603208, -0.025732473662091335, 0.41093203852969135, -0.24723289265636017, -0.13357616501492553, 0.11599428198877088, -0.38345692882483656, -0.15694798996926032, 0.17060341974932022, -0.08519812... |
706.1408 | Sensitivity of principal Hessian direction analysis | We provide sensitivity comparisons for two competing versions of the
dimension reduction method principal Hessian directions (pHd). These
comparisons consider the effects of small perturbations on the estimation of
the dimension reduction subspace via the influence function. We show that the
two versions of pHd can b... | stat.ME | we provide sensitivity comparisons for two competing versions of the dimension reduction method principal hessian directions phd these comparisons consider the effects of small perturbations on the estimation of the dimension reduction subspace via the influence function we show that the two versions of phd can behave ... | [['we', 'provide', 'sensitivity', 'comparisons', 'for', 'two', 'competing', 'versions', 'of', 'the', 'dimension', 'reduction', 'method', 'principal', 'hessian', 'directions', 'phd', 'these', 'comparisons', 'consider', 'the', 'effects', 'of', 'small', 'perturbations', 'on', 'the', 'estimation', 'of', 'the', 'dimension',... | [-0.10830510650010942, 0.08226198020834223, -0.07585815293262306, 0.10756248217957655, -0.06529111171466778, -0.11449926515625229, 0.02484019012054772, 0.35264774607223215, -0.2195930678388375, -0.30748698104498456, 0.13371008170601342, -0.2910885644118184, -0.1842824066062322, 0.17098348365092958, -0.08341647664455751... |
706.1409 | A Proof of a Recursion for Bessel Moments | We provide a proof of a conjecture in (Bailey, Borwein, Borwein, Crandall
2007) on the existence and form of linear recursions for moments of powers of
the Bessel function $K_0$.
| cs.SC math.CA | we provide a proof of a conjecture in bailey borwein borwein crandall 2007 on the existence and form of linear recursions for moments of powers of the bessel function k_0 | [['we', 'provide', 'a', 'proof', 'of', 'a', 'conjecture', 'in', 'bailey', 'borwein', 'borwein', 'crandall', '2007', 'on', 'the', 'existence', 'and', 'form', 'of', 'linear', 'recursions', 'for', 'moments', 'of', 'powers', 'of', 'the', 'bessel', 'function', 'k_0']] | [-0.19123739162459968, 0.0097417121908317, -0.15630868915468454, 0.051437080713609855, -0.10076795431474844, -0.07006311997150381, 0.057804685365408656, 0.2458363105232517, -0.23029714748263358, -0.22645513011763493, 0.0712303336050051, -0.264790919663695, -0.16929713133722543, 0.21728354170918465, -0.04680641548087199... |
706.141 | Evolutionary Mesh Numbering: Preliminary Results | Mesh numbering is a critical issue in Finite Element Methods, as the
computational cost of one analysis is highly dependent on the order of the
nodes of the mesh. This paper presents some preliminary investigations on the
problem of mesh numbering using Evolutionary Algorithms. Three conclusions can
be drawn from the... | cs.NA cs.NE math.NA math.OC | mesh numbering is a critical issue in finite element methods as the computational cost of one analysis is highly dependent on the order of the nodes of the mesh this paper presents some preliminary investigations on the problem of mesh numbering using evolutionary algorithms three conclusions can be drawn from these ex... | [['mesh', 'numbering', 'is', 'a', 'critical', 'issue', 'in', 'finite', 'element', 'methods', 'as', 'the', 'computational', 'cost', 'of', 'one', 'analysis', 'is', 'highly', 'dependent', 'on', 'the', 'order', 'of', 'the', 'nodes', 'of', 'the', 'mesh', 'this', 'paper', 'presents', 'some', 'preliminary', 'investigations', ... | [-0.05730400752265029, 0.04078954189235392, -0.10392575401500492, 0.07388034369029707, -0.10394796130002036, -0.15706181790244705, 0.07806884095945513, 0.3983549190752074, -0.24362015556320996, -0.3402620082732268, 0.12192621360976294, -0.2549992900127914, -0.14524364418456118, 0.19689315740955982, -0.06378263073208641... |
706.1411 | Finite size effects and 2-string deviations in the spin-1 XXZ chains | In an earlier work [1] J. Suzuki proposed a set of nonlinear integral
equations (NLIE) to describe the excited state spectrum of the integrable
spin-1 XXZ chain in its repulsive regime. In this paper we extend his equations
for the attractive regime of the model, and calculate analytically the
conformal spectrum of t... | hep-th | in an earlier work 1 j suzuki proposed a set of nonlinear integral equations nlie to describe the excited state spectrum of the integrable spin1 xxz chain in its repulsive regime in this paper we extend his equations for the attractive regime of the model and calculate analytically the conformal spectrum of the spin ch... | [['in', 'an', 'earlier', 'work', '1', 'j', 'suzuki', 'proposed', 'a', 'set', 'of', 'nonlinear', 'integral', 'equations', 'nlie', 'to', 'describe', 'the', 'excited', 'state', 'spectrum', 'of', 'the', 'integrable', 'spin1', 'xxz', 'chain', 'in', 'its', 'repulsive', 'regime', 'in', 'this', 'paper', 'we', 'extend', 'his', ... | [-0.1492151218967942, 0.1308520887020507, -0.02208056234099626, 0.08321935790693286, -0.045803979182472594, -0.13865990403548376, -0.005385235738735851, 0.2988545075672996, -0.24639084079087928, -0.21489019342954016, 0.09088319918693422, -0.2903754322848457, -0.12328940214445958, 0.1385091550924539, 0.00388506685823693... |
706.1412 | The Alignments of the Galaxy Spins with the Real-Space Tidal Field
Reconstructed from the Two Mass Redshift Survey | We report a direct observational evidence for the existence of the galaxy
spin alignments with the real space tidal field. We calculate the real space
tidal field from the real space density field reconstructed recently from the
Two Mass Redshift Survey (2MRS) by Erdogdu et al. in 2006. Using a total of
12122 nearby ... | astro-ph | we report a direct observational evidence for the existence of the galaxy spin alignments with the real space tidal field we calculate the real space tidal field from the real space density field reconstructed recently from the two mass redshift survey 2mrs by erdogdu et al in 2006 using a total of 12122 nearby spiral ... | [['we', 'report', 'a', 'direct', 'observational', 'evidence', 'for', 'the', 'existence', 'of', 'the', 'galaxy', 'spin', 'alignments', 'with', 'the', 'real', 'space', 'tidal', 'field', 'we', 'calculate', 'the', 'real', 'space', 'tidal', 'field', 'from', 'the', 'real', 'space', 'density', 'field', 'reconstructed', 'recen... | [-0.13190169511944988, 0.07951377047924325, -0.10337781743262894, 0.12917644574306905, -0.10765243268571795, -0.00357151348143816, -0.0005139157903613523, 0.3795199345424771, -0.19093005963528412, -0.3328012704756111, 0.015148415721487254, -0.27796612089499834, -0.08783976426813751, 0.17756550868041812, 0.0274735139636... |
706.1413 | Evolutionary stability in quantum games | In evolutionary game theory an Evolutionarily Stable Strategy (ESS) is a
refinement of the Nash equilibrium concept that is sometimes also recognized as
evolutionary stability. It is a game-theoretic model, well known to
mathematical biologists, that was found quite useful in the understanding of
evolutionary dynamic... | quant-ph | in evolutionary game theory an evolutionarily stable strategy ess is a refinement of the nash equilibrium concept that is sometimes also recognized as evolutionary stability it is a gametheoretic model well known to mathematical biologists that was found quite useful in the understanding of evolutionary dynamics of a p... | [['in', 'evolutionary', 'game', 'theory', 'an', 'evolutionarily', 'stable', 'strategy', 'ess', 'is', 'a', 'refinement', 'of', 'the', 'nash', 'equilibrium', 'concept', 'that', 'is', 'sometimes', 'also', 'recognized', 'as', 'evolutionary', 'stability', 'it', 'is', 'a', 'gametheoretic', 'model', 'well', 'known', 'to', 'ma... | [-0.10280008160771104, 0.07178368339782537, -0.25187068979721516, 0.16084289297941723, -0.025033178520970978, -0.15356437907757936, 0.04541662105657451, 0.34292286516574677, -0.3009028034284711, -0.3211768443288747, 0.09173616945372487, -0.1525817060319241, -0.24273257941240445, 0.09358889222130529, -0.1329425881995121... |
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