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 |
|---|---|---|---|---|---|---|
708.3149 | Convexity of Hypersurfaces in Spherical Spaces | A spherical set is called convex if for every pair of its points there is at
least one minimal geodesic segment that joins these points and lies in the set.
We prove that for n >= 3 a complete locally-convex (topological) immersion of a
connected (n-1)-manifold into the n-sphere is a surjection onto the boundary of
a... | math.MG math.DG | a spherical set is called convex if for every pair of its points there is at least one minimal geodesic segment that joins these points and lies in the set we prove that for n 3 a complete locallyconvex topological immersion of a connected n1manifold into the nsphere is a surjection onto the boundary of a convex set | [['a', 'spherical', 'set', 'is', 'called', 'convex', 'if', 'for', 'every', 'pair', 'of', 'its', 'points', 'there', 'is', 'at', 'least', 'one', 'minimal', 'geodesic', 'segment', 'that', 'joins', 'these', 'points', 'and', 'lies', 'in', 'the', 'set', 'we', 'prove', 'that', 'for', 'n', '3', 'a', 'complete', 'locallyconvex'... | [-0.19960232042097326, 0.0903114745762713, -0.08162062224161265, 0.010306483341364896, -0.06259091133010927, -0.15218127926747346, 0.05121364582586905, 0.35315502015070926, -0.30078193646502394, -0.13456814964141312, 0.12866790177388887, -0.36821392846518547, -0.10714009130004279, 0.1786516826631951, -0.098593776155431... |
708.315 | Unrecognized Backscattering in Low Energy Beta Spectroscopy | We present studies on electron backscattering from the surface of plastic
scintillator beta detectors. By using a setup of two detectors coaxial with a
strong external magnetic field - one detector serving as primary detector, the
other as veto-detector to detect backscattering - we investigate amount and
spectrum of... | physics.ins-det | we present studies on electron backscattering from the surface of plastic scintillator beta detectors by using a setup of two detectors coaxial with a strong external magnetic field one detector serving as primary detector the other as vetodetector to detect backscattering we investigate amount and spectrum of unrecogn... | [['we', 'present', 'studies', 'on', 'electron', 'backscattering', 'from', 'the', 'surface', 'of', 'plastic', 'scintillator', 'beta', 'detectors', 'by', 'using', 'a', 'setup', 'of', 'two', 'detectors', 'coaxial', 'with', 'a', 'strong', 'external', 'magnetic', 'field', 'one', 'detector', 'serving', 'as', 'primary', 'dete... | [-0.11876983319876565, 0.1902816043687327, -0.027793200330480057, 0.07010714302989929, -0.01438872576074894, -0.21530472767292796, -0.02624203759478405, 0.35483335216036616, -0.1891915240626344, -0.39525760633542256, 0.0837181295021711, -0.39483400639694405, -0.0808720343390151, 0.2197825193648254, 0.028853704524568886... |
708.3151 | Natural Frobenius Submanifolds | I.A.B. Strachan introduced the notion of a natural Frobenius submanifold of a
Frobenius manifold and gave a sufficient but not necessary condition for a
submanifold to be a natural Frobenius submanifold. This paper will give a
necessary and sufficient condition and classify the natural Frobenius
hypersurfaces.
| math.SG math.DG | iab strachan introduced the notion of a natural frobenius submanifold of a frobenius manifold and gave a sufficient but not necessary condition for a submanifold to be a natural frobenius submanifold this paper will give a necessary and sufficient condition and classify the natural frobenius hypersurfaces | [['iab', 'strachan', 'introduced', 'the', 'notion', 'of', 'a', 'natural', 'frobenius', 'submanifold', 'of', 'a', 'frobenius', 'manifold', 'and', 'gave', 'a', 'sufficient', 'but', 'not', 'necessary', 'condition', 'for', 'a', 'submanifold', 'to', 'be', 'a', 'natural', 'frobenius', 'submanifold', 'this', 'paper', 'will', ... | [-0.23112680549915557, -0.00013246456965925577, -0.09537382654683746, 0.1595968237911027, -0.162635520586501, -0.1984802964143455, -0.04144709792909334, 0.2581484559113565, -0.2685825112073318, -0.22853760729017464, 0.11355199231563703, -0.09822668337627598, -0.1928188636413087, 0.09124766016864906, -0.2794952955825821... |
708.3152 | An asymptotically stable scheme for diffusive coagulation-fragmentation
models | This paper is devoted to the analysis of a numerical scheme for the
coagulation and fragmentation equation with diffusion in space. A finite volume
scheme is developed, based on a conservative formulation of the space
nonhomogeneous coagulation-fragmentation model, it is shown that the scheme
preserves positivity, to... | math.NA | this paper is devoted to the analysis of a numerical scheme for the coagulation and fragmentation equation with diffusion in space a finite volume scheme is developed based on a conservative formulation of the space nonhomogeneous coagulationfragmentation model it is shown that the scheme preserves positivity total vol... | [['this', 'paper', 'is', 'devoted', 'to', 'the', 'analysis', 'of', 'a', 'numerical', 'scheme', 'for', 'the', 'coagulation', 'and', 'fragmentation', 'equation', 'with', 'diffusion', 'in', 'space', 'a', 'finite', 'volume', 'scheme', 'is', 'developed', 'based', 'on', 'a', 'conservative', 'formulation', 'of', 'the', 'space... | [-0.13250711391186482, 0.04271386869585336, -0.13458618389637167, 0.046487231599862004, -0.026909970247478626, -0.05871850257016607, 0.015494823485348762, 0.34148917953247454, -0.26902844701240314, -0.23469335179942757, 0.1456168679322408, -0.22477143071591854, -0.1339469608753475, 0.1770998369728618, -0.00905726482021... |
708.3153 | Symmetries and conservation laws in Lagrangian gauge theories with
applications to the mechanics of black holes and to gravity in three
dimensions | The treatment of exact conservation laws in Lagrangian gauge theories
constitutes the main axis of the first part of the thesis. The formalism is
developed as a self-consistent theory but is inspired by earlier works, mainly
by cohomological results, covariant phase space methods and by the Hamiltonian
formalism. The... | hep-th | the treatment of exact conservation laws in lagrangian gauge theories constitutes the main axis of the first part of the thesis the formalism is developed as a selfconsistent theory but is inspired by earlier works mainly by cohomological results covariant phase space methods and by the hamiltonian formalism the thermo... | [['the', 'treatment', 'of', 'exact', 'conservation', 'laws', 'in', 'lagrangian', 'gauge', 'theories', 'constitutes', 'the', 'main', 'axis', 'of', 'the', 'first', 'part', 'of', 'the', 'thesis', 'the', 'formalism', 'is', 'developed', 'as', 'a', 'selfconsistent', 'theory', 'but', 'is', 'inspired', 'by', 'earlier', 'works'... | [-0.16532096508645983, 0.12224178030850232, -0.098292273633923, 0.11267635247152999, -0.07380085387164263, -0.1076623064643338, -0.04680692082083172, 0.29223700644170547, -0.1815468843676438, -0.2575513537438041, 0.08248794525128517, -0.26821573476888527, -0.16566818564337837, 0.15757572772856082, -0.0734407038772633, ... |
708.3154 | Two-way classical communication remarkably improves local
distinguishability | We analyze the difference in the local distinguishability among the following
three restrictions; (i) Local operations and only one-way classical
communications (one-way LOCC) are permitted. (ii) Local operations and two-way
classical communications (two-way LOCC) are permitted. (iii) All separable
operations are per... | quant-ph | we analyze the difference in the local distinguishability among the following three restrictions i local operations and only oneway classical communications oneway locc are permitted ii local operations and twoway classical communications twoway locc are permitted iii all separable operations are permitted we obtain tw... | [['we', 'analyze', 'the', 'difference', 'in', 'the', 'local', 'distinguishability', 'among', 'the', 'following', 'three', 'restrictions', 'i', 'local', 'operations', 'and', 'only', 'oneway', 'classical', 'communications', 'oneway', 'locc', 'are', 'permitted', 'ii', 'local', 'operations', 'and', 'twoway', 'classical', '... | [-0.16188248651574405, 0.14297645958468422, -0.046858503463560006, 0.06569569918218816, 0.0030131633360673425, -0.288112275354879, 0.11035963172801364, 0.34089748466282455, -0.280376450307864, -0.2718923893973599, 0.09664067058105835, -0.23131334076924118, -0.10275097412194951, 0.1786600901551781, -0.08336761316963354,... |
708.3155 | Sfermion masses in the supersymmetric economical 3-3-1 model | Sfermion masses and eigenstates in the supersymmetric economical 3-3-1 model
are studied. By lepton number conservation, the exotic squarks and
superpartners of ordinary quarks are decoupled. Due to the fact that in the
3-3-1 models, one generation of quarks behaves differently from other two, by
R-parity conservatio... | hep-ph | sfermion masses and eigenstates in the supersymmetric economical 331 model are studied by lepton number conservation the exotic squarks and superpartners of ordinary quarks are decoupled due to the fact that in the 331 models one generation of quarks behaves differently from other two by rparity conservation the mass m... | [['sfermion', 'masses', 'and', 'eigenstates', 'in', 'the', 'supersymmetric', 'economical', '331', 'model', 'are', 'studied', 'by', 'lepton', 'number', 'conservation', 'the', 'exotic', 'squarks', 'and', 'superpartners', 'of', 'ordinary', 'quarks', 'are', 'decoupled', 'due', 'to', 'the', 'fact', 'that', 'in', 'the', '331... | [-0.11250620877310152, 0.3179935977433718, 0.039555821536229024, 0.20226431863247266, -0.0415009337657642, -0.18431221208565177, 0.009487957091327952, 0.32196640481932026, -0.18036993582763017, -0.3290138931884881, 0.012047316459187817, -0.3156565451844325, 0.027004905447604196, 0.09101051912763186, -0.0023553906722114... |
708.3156 | Infrared point source variability between the Spitzer and MSX surveys of
the Galactic mid-plane | We present a list of 552 sources with suspected variability, based on a
comparison of mid-infrared photometry from the GLIMPSE I and MSX surveys, which
were carried out nearly a decade apart. We were careful to address issues such
as the difference in resolution and sensitivity between the two surveys, as
well as the... | astro-ph | we present a list of 552 sources with suspected variability based on a comparison of midinfrared photometry from the glimpse i and msx surveys which were carried out nearly a decade apart we were careful to address issues such as the difference in resolution and sensitivity between the two surveys as well as the differ... | [['we', 'present', 'a', 'list', 'of', '552', 'sources', 'with', 'suspected', 'variability', 'based', 'on', 'a', 'comparison', 'of', 'midinfrared', 'photometry', 'from', 'the', 'glimpse', 'i', 'and', 'msx', 'surveys', 'which', 'were', 'carried', 'out', 'nearly', 'a', 'decade', 'apart', 'we', 'were', 'careful', 'to', 'ad... | [-0.0302253658662383, 0.038865799059231695, -0.07485921510423606, 0.07417195435338773, -0.07748979373524587, -0.05440695961483587, 0.11226431021275811, 0.44586221205118376, -0.16798203275807633, -0.36254313255015475, 0.13614620893584709, -0.394059506087349, -0.0468392787874342, 0.17968439243924925, -0.06560562584214867... |
708.3157 | The Maslov cocycle, smooth structures and real-analytic complete
integrability | This paper studies smooth obstructions to integrability and proves two main
results. First, it is shown that if a smooth topological n-torus admits a
real-analytically completely integrable convex hamiltonian on its cotangent
bundle, then the torus is diffeomorphic to the standard n-torus. This is the
first known res... | math.SG math.DS | this paper studies smooth obstructions to integrability and proves two main results first it is shown that if a smooth topological ntorus admits a realanalytically completely integrable convex hamiltonian on its cotangent bundle then the torus is diffeomorphic to the standard ntorus this is the first known result where... | [['this', 'paper', 'studies', 'smooth', 'obstructions', 'to', 'integrability', 'and', 'proves', 'two', 'main', 'results', 'first', 'it', 'is', 'shown', 'that', 'if', 'a', 'smooth', 'topological', 'ntorus', 'admits', 'a', 'realanalytically', 'completely', 'integrable', 'convex', 'hamiltonian', 'on', 'its', 'cotangent', ... | [-0.22493127674406924, 0.04862319939094809, -0.0909435088583909, 0.07522252176080856, -0.16494200745204446, -0.1792381104389462, -0.0890069594841724, 0.3567133738548247, -0.2937784252363607, -0.11579298199722629, 0.15302766064062304, -0.24602291160134956, -0.2338957956334183, 0.1786132612769757, -0.1715987384097155, 0.... |
708.3158 | An expression for stationary distribution in nonequilibrium steady state | We study the nonequilibrium steady state realized in a general stochastic
system attached to multiple heat baths and/or driven by an external force.
Starting from the detailed fluctuation theorem we derive concise and suggestive
expressions for the corresponding stationary distribution which are correct up
to the sec... | cond-mat.stat-mech | we study the nonequilibrium steady state realized in a general stochastic system attached to multiple heat baths andor driven by an external force starting from the detailed fluctuation theorem we derive concise and suggestive expressions for the corresponding stationary distribution which are correct up to the second ... | [['we', 'study', 'the', 'nonequilibrium', 'steady', 'state', 'realized', 'in', 'a', 'general', 'stochastic', 'system', 'attached', 'to', 'multiple', 'heat', 'baths', 'andor', 'driven', 'by', 'an', 'external', 'force', 'starting', 'from', 'the', 'detailed', 'fluctuation', 'theorem', 'we', 'derive', 'concise', 'and', 'su... | [-0.13242219338654845, 0.1868557445880376, -0.10192690367558013, 0.07202798721302196, -0.006832699465487048, -0.13024153600438176, 0.06391652426399534, 0.32217247644004143, -0.2807926376476431, -0.2653531820260894, 0.0481331110061538, -0.3261964524808888, -0.09079602183164837, 0.2150376269389292, -0.0158404681709743, 0... |
708.3159 | Four-dimensional double singular oscillator | The Schr\"odinger equation for the four-dimensional double singular
oscillator is separable in Eulerian, doble polar and spheroidal coordinates in
${\rm I R}^4$. It is shown that the coefficients for the expansion of double
polar basis in terms of the Eulerian basis can be expressed through the
Clebsch-Gordan coeffic... | quant-ph | the schrodinger equation for the fourdimensional double singular oscillator is separable in eulerian doble polar and spheroidal coordinates in rm i r4 it is shown that the coefficients for the expansion of double polar basis in terms of the eulerian basis can be expressed through the clebschgordan coefficients of the g... | [['the', 'schrodinger', 'equation', 'for', 'the', 'fourdimensional', 'double', 'singular', 'oscillator', 'is', 'separable', 'in', 'eulerian', 'doble', 'polar', 'and', 'spheroidal', 'coordinates', 'in', 'rm', 'i', 'r4', 'it', 'is', 'shown', 'that', 'the', 'coefficients', 'for', 'the', 'expansion', 'of', 'double', 'polar... | [-0.18720463971424448, 0.09845617175146583, -0.10166293715814217, 0.06467850793740668, -0.10211518165167599, -0.05323073123803451, -0.04798949645122602, 0.3185004150672328, -0.2782522672343822, -0.16687649367598906, 0.07152045135652381, -0.22832962121520678, -0.1891960423173649, 0.21199410251297413, 0.00297980646913250... |
708.316 | Graphene-like massless Dirac fermions in Harper systems | It is shown that systems described by Harper's equation exhibit a Dirac point
at the center of the spectrum whenever the field parameter is a fraction of
even denominator. The Dirac point is formed by the touching of two subbands,
and the physics around such point is characterized by the relative field only,
as if th... | cond-mat.mes-hall | it is shown that systems described by harpers equation exhibit a dirac point at the center of the spectrum whenever the field parameter is a fraction of even denominator the dirac point is formed by the touching of two subbands and the physics around such point is characterized by the relative field only as if the latt... | [['it', 'is', 'shown', 'that', 'systems', 'described', 'by', 'harpers', 'equation', 'exhibit', 'a', 'dirac', 'point', 'at', 'the', 'center', 'of', 'the', 'spectrum', 'whenever', 'the', 'field', 'parameter', 'is', 'a', 'fraction', 'of', 'even', 'denominator', 'the', 'dirac', 'point', 'is', 'formed', 'by', 'the', 'touchi... | [-0.1542459244119181, 0.16047248018994217, -0.09074315921447816, 0.06014938458379003, -0.04707476262535368, -0.15715770944952964, 0.04189844459428319, 0.3166139398923232, -0.2821345711038226, -0.30445224078859956, 0.07735776545457719, -0.2964398968610026, -0.11579539272047225, 0.16869186370943984, 0.013770585431761686,... |
708.3161 | Ground State Properties of an Asymmetric Hubbard Model for Unbalanced
Ultracold Fermionic Quantum Gases | In order to describe unbalanced ultracold fermionic quantum gases on optical
lattices in a harmonic trap, we investigate an attractive ($U<0$) asymmetric
($t_\uparrow\neq t_\downarrow$) Hubbard model with a Zeeman-like magnetic
field. In view of the model's spatial inhomogeneity, we focus in this paper on
the solutio... | cond-mat.str-el | in order to describe unbalanced ultracold fermionic quantum gases on optical lattices in a harmonic trap we investigate an attractive u0 asymmetric t_uparrowneq t_downarrow hubbard model with a zeemanlike magnetic field in view of the models spatial inhomogeneity we focus in this paper on the solution at hartreefock le... | [['in', 'order', 'to', 'describe', 'unbalanced', 'ultracold', 'fermionic', 'quantum', 'gases', 'on', 'optical', 'lattices', 'in', 'a', 'harmonic', 'trap', 'we', 'investigate', 'an', 'attractive', 'u0', 'asymmetric', 't_uparrowneq', 't_downarrow', 'hubbard', 'model', 'with', 'a', 'zeemanlike', 'magnetic', 'field', 'in',... | [-0.18430284440058142, 0.18541244825769665, -0.02151558411703126, 0.0777690873819416, 0.013006143386743656, -0.13675952511393044, 0.058558290281288373, 0.34868545798355177, -0.2069096800565005, -0.23396245002657276, 0.0076840901747345924, -0.2819636448721835, -0.10972687744293107, 0.12260689082306694, 0.052631366399933... |
708.3162 | Frustrated minority spins in GeNi2O4 | Recently, two consecutive phase transitions were observed, upon cooling, in
an antiferromagnetic spinel GeNi$_2$O$_4$ at $T_{N1}=12.1$ K and $T_{N2}=11.4$
K, respectively \cite{matsuno, crawford}. Using unpolarized and polarized
elastic neutron scattering we show that the two transitions are due to the
existence of f... | cond-mat.str-el | recently two consecutive phase transitions were observed upon cooling in an antiferromagnetic spinel geni_2o_4 at t_n1121 k and t_n2114 k respectively citematsuno crawford using unpolarized and polarized elastic neutron scattering we show that the two transitions are due to the existence of frustrated minority spins in... | [['recently', 'two', 'consecutive', 'phase', 'transitions', 'were', 'observed', 'upon', 'cooling', 'in', 'an', 'antiferromagnetic', 'spinel', 'geni_2o_4', 'at', 't_n1121', 'k', 'and', 't_n2114', 'k', 'respectively', 'citematsuno', 'crawford', 'using', 'unpolarized', 'and', 'polarized', 'elastic', 'neutron', 'scattering... | [-0.20968659645525597, 0.2832935830636171, 0.033002744426367754, 0.008545233235604466, -0.013704643342174402, -0.11001959164086886, 0.09586673752529969, 0.4365322457923859, -0.24064267572297268, -0.26518014104676846, 0.025394759410914004, -0.39171294047802435, -0.053308339053843204, 0.11445788880555789, 0.1408875921208... |
708.3163 | Jeans type analysis of chemotactic collapse | We perform a linear dynamical stability analysis of a general hydrodynamic
model of chemotactic aggregation [Chavanis & Sire, Physica A, in press (2007)].
Specifically, we study the stability of an infinite and homogeneous
distribution of cells against "chemotactic collapse". We discuss the analogy
between the chemot... | physics.bio-ph | we perform a linear dynamical stability analysis of a general hydrodynamic model of chemotactic aggregation chavanis sire physica a in press 2007 specifically we study the stability of an infinite and homogeneous distribution of cells against chemotactic collapse we discuss the analogy between the chemotactic collapse ... | [['we', 'perform', 'a', 'linear', 'dynamical', 'stability', 'analysis', 'of', 'a', 'general', 'hydrodynamic', 'model', 'of', 'chemotactic', 'aggregation', 'chavanis', 'sire', 'physica', 'a', 'in', 'press', '2007', 'specifically', 'we', 'study', 'the', 'stability', 'of', 'an', 'infinite', 'and', 'homogeneous', 'distribu... | [-0.16185805446618948, 0.14670009540460147, -0.10995740409136988, 0.06424953546192425, -0.03845977837986806, -0.10109540099762016, 0.008959690129439183, 0.25019235579004767, -0.24331781556281973, -0.24421910143767794, 0.05311736303322273, -0.23981314361935444, -0.15379547381079664, 0.14883607989131456, 0.00385968282216... |
708.3164 | Algebraic systems of matrices and Grobner basis | One studies a particular algebraic system where the unknowns are matrices. We
solve this system according to the parameters values thanks to the theory of
Grobner basis.
| math.RA | one studies a particular algebraic system where the unknowns are matrices we solve this system according to the parameters values thanks to the theory of grobner basis | [['one', 'studies', 'a', 'particular', 'algebraic', 'system', 'where', 'the', 'unknowns', 'are', 'matrices', 'we', 'solve', 'this', 'system', 'according', 'to', 'the', 'parameters', 'values', 'thanks', 'to', 'the', 'theory', 'of', 'grobner', 'basis']] | [-0.13225159788918164, 0.030236572717074996, -0.07038055194748773, 0.004293915069731021, -0.09820821720899807, -0.1137316207125507, 0.04332426853943616, 0.2404413981432164, -0.33688865457144046, -0.27091842719043296, 0.17119235867910362, -0.25887809611029095, -0.16210547551788665, 0.16459285274699884, -0.06169984296516... |
708.3165 | Sharp Magnetic Field Dependence of the 2D Hall Coefficient Induced by
Classical Memory Effects | We show that a sharp dependence of the Hall coefficient $R$ on the magnetic
field $B$ arises in two-dimensional electron systems with randomly located
strong scatterers. The phenomenon is due to classical memory effects. We
calculate analytically the dependence $R(B)$ for the case of scattering by hard
disks of radiu... | cond-mat.dis-nn cond-mat.mes-hall | we show that a sharp dependence of the hall coefficient r on the magnetic field b arises in twodimensional electron systems with randomly located strong scatterers the phenomenon is due to classical memory effects we calculate analytically the dependence rb for the case of scattering by hard disks of radius a randomly ... | [['we', 'show', 'that', 'a', 'sharp', 'dependence', 'of', 'the', 'hall', 'coefficient', 'r', 'on', 'the', 'magnetic', 'field', 'b', 'arises', 'in', 'twodimensional', 'electron', 'systems', 'with', 'randomly', 'located', 'strong', 'scatterers', 'the', 'phenomenon', 'is', 'due', 'to', 'classical', 'memory', 'effects', 'w... | [-0.18737836943265446, 0.17533686030201795, -0.023446444138066798, 0.010245492368580668, -0.021393526716506094, -0.15510348611836874, 0.0348273853116434, 0.3453227176474846, -0.29970931935283107, -0.2847944770417199, 0.03903661457522643, -0.30307387591934026, -0.09168161892491143, 0.1701576318591833, -0.003260637720577... |
708.3166 | Web Server Benchmark Application WiiBench using Erlang/OTP R11 and
Fedora-Core Linux 5.0 | As the web grows and the amount of traffics on the web server increase,
problems related to performance begin to appear. Some of the problems, such as
the number of users that can access the server simultaneously, the number of
requests that can be handled by the server per second (requests per second) to
bandwidth c... | cs.NI | as the web grows and the amount of traffics on the web server increase problems related to performance begin to appear some of the problems such as the number of users that can access the server simultaneously the number of requests that can be handled by the server per second requests per second to bandwidth consumpti... | [['as', 'the', 'web', 'grows', 'and', 'the', 'amount', 'of', 'traffics', 'on', 'the', 'web', 'server', 'increase', 'problems', 'related', 'to', 'performance', 'begin', 'to', 'appear', 'some', 'of', 'the', 'problems', 'such', 'as', 'the', 'number', 'of', 'users', 'that', 'can', 'access', 'the', 'server', 'simultaneously... | [-0.14947618743831134, 0.00553109214255908, -0.055802957482082416, 0.02704240545131599, -0.11749751345594844, -0.2260553210442624, 0.13541035981845095, 0.35081291280501714, -0.2806983626013749, -0.3948486696322819, 0.130007888774395, -0.3042028780099019, -0.05694650091585258, 0.22292663956651965, -0.09628248447271805, ... |
708.3167 | Asymmetric Fermi superfluid with different atomic species in a harmonic
trap | We study the dilute fermion gas with pairing between two species and unequal
concentrations in a harmonic trap using the mean field theory and the local
density approximation. We found that the system can exhibit a superfluid shell
structure sandwiched by the normal fermions. This superfluid shell structure
occurs if... | cond-mat.supr-con cond-mat.other | we study the dilute fermion gas with pairing between two species and unequal concentrations in a harmonic trap using the mean field theory and the local density approximation we found that the system can exhibit a superfluid shell structure sandwiched by the normal fermions this superfluid shell structure occurs if the... | [['we', 'study', 'the', 'dilute', 'fermion', 'gas', 'with', 'pairing', 'between', 'two', 'species', 'and', 'unequal', 'concentrations', 'in', 'a', 'harmonic', 'trap', 'using', 'the', 'mean', 'field', 'theory', 'and', 'the', 'local', 'density', 'approximation', 'we', 'found', 'that', 'the', 'system', 'can', 'exhibit', '... | [-0.13704755275019645, 0.3164142044460667, -0.05578975422041757, 0.09970358458563819, -0.006263639804508005, -0.18484734307775008, 0.03738467670794177, 0.34741881637434874, -0.21742101994210056, -0.26101797629131135, 0.006237863085698336, -0.3167901442785348, -0.027249982241275054, 0.11643597398485456, 0.04641687639169... |
708.3168 | A Generic Approach to Searching for Jacobians | We consider the problem of finding cryptographically suitable Jacobians. By
applying a probabilistic generic algorithm to compute the zeta functions of low
genus curves drawn from an arbitrary family, we can search for Jacobians
containing a large subgroup of prime order. For a suitable distribution of
curves, the co... | math.NT math.AG | we consider the problem of finding cryptographically suitable jacobians by applying a probabilistic generic algorithm to compute the zeta functions of low genus curves drawn from an arbitrary family we can search for jacobians containing a large subgroup of prime order for a suitable distribution of curves the complexi... | [['we', 'consider', 'the', 'problem', 'of', 'finding', 'cryptographically', 'suitable', 'jacobians', 'by', 'applying', 'a', 'probabilistic', 'generic', 'algorithm', 'to', 'compute', 'the', 'zeta', 'functions', 'of', 'low', 'genus', 'curves', 'drawn', 'from', 'an', 'arbitrary', 'family', 'we', 'can', 'search', 'for', 'j... | [-0.18647913647884573, 0.09943422997150467, -0.08696158154419174, 0.031894401371203085, -0.0443248581348194, -0.1317245844406662, 0.04933687885878263, 0.35835953358284856, -0.2643921230264284, -0.34240989807165334, 0.08157193569587198, -0.2520568666117335, -0.08353272828583916, 0.2836339572246221, -0.11452728368997298,... |
708.3169 | Using Josephson junctions to determine the pairing state of
superconductors without crystal inversion symmetry | Theoretical studies of a planar tunnel junction between two superconductors
with antisymmetric spin-orbit coupling are presented. The half-space Green's
function for such a superconductor is determined. This is then used to derive
expressions for the dissipative current and the Josephson current of the
junction. Nume... | cond-mat.supr-con | theoretical studies of a planar tunnel junction between two superconductors with antisymmetric spinorbit coupling are presented the halfspace greens function for such a superconductor is determined this is then used to derive expressions for the dissipative current and the josephson current of the junction numerical re... | [['theoretical', 'studies', 'of', 'a', 'planar', 'tunnel', 'junction', 'between', 'two', 'superconductors', 'with', 'antisymmetric', 'spinorbit', 'coupling', 'are', 'presented', 'the', 'halfspace', 'greens', 'function', 'for', 'such', 'a', 'superconductor', 'is', 'determined', 'this', 'is', 'then', 'used', 'to', 'deriv... | [-0.270608752656906, 0.142506641513721, -0.0019444955107793818, 0.043376912307032056, -0.09431733569599748, -0.1837491138717084, 0.032824440298950285, 0.39577341709679703, -0.22287698150839566, -0.2580956349270494, -0.04844142884920859, -0.27671648009218336, -0.10966828498966628, 0.20921552703125265, 0.0641937064256791... |
708.317 | Holographic QCD with Isospin Chemical Potential | We consider configurations of D4-D8-\bar D8 branes which correspond to large
N QCD with non-vanishing temperature and chemical potential for baryon number
and isospin. We study the holographic dual of this model and find a rich phase
structure. The phases, distinguished by the values of quark condensates, are
separat... | hep-th hep-ph | we consider configurations of d4d8bar d8 branes which correspond to large n qcd with nonvanishing temperature and chemical potential for baryon number and isospin we study the holographic dual of this model and find a rich phase structure the phases distinguished by the values of quark condensates are separated by the ... | [['we', 'consider', 'configurations', 'of', 'd4d8bar', 'd8', 'branes', 'which', 'correspond', 'to', 'large', 'n', 'qcd', 'with', 'nonvanishing', 'temperature', 'and', 'chemical', 'potential', 'for', 'baryon', 'number', 'and', 'isospin', 'we', 'study', 'the', 'holographic', 'dual', 'of', 'this', 'model', 'and', 'find', ... | [-0.15832558751257286, 0.24206787200543928, -0.09178023318118239, 0.04479129265087682, -0.015039289747742383, -0.0855876451698006, 0.06595467929602475, 0.3071324612844635, -0.18129657465662505, -0.27033521291623647, 0.03824218120614721, -0.28702881262713187, -0.09782418948786988, 0.048571919012386854, 0.038675484509440... |
708.3171 | The p53-MDM2 network: from oscillations to apoptosis | The p53 protein is well-known for its tumour suppressor function. The
p53-MDM2 negative feedback loop constitutes the core module of a network of
regulatory interactions activated under cellular stress. In normal cells, the
level of p53 proteins is kept low by MDM2, i.e. MDM2 negatively regulates the
activity of p53.... | q-bio.MN | the p53 protein is wellknown for its tumour suppressor function the p53mdm2 negative feedback loop constitutes the core module of a network of regulatory interactions activated under cellular stress in normal cells the level of p53 proteins is kept low by mdm2 ie mdm2 negatively regulates the activity of p53 in the cas... | [['the', 'p53', 'protein', 'is', 'wellknown', 'for', 'its', 'tumour', 'suppressor', 'function', 'the', 'p53mdm2', 'negative', 'feedback', 'loop', 'constitutes', 'the', 'core', 'module', 'of', 'a', 'network', 'of', 'regulatory', 'interactions', 'activated', 'under', 'cellular', 'stress', 'in', 'normal', 'cells', 'the', ... | [-0.14562850390554077, 0.17741285336834314, 0.04871295545351185, 0.05776905062221511, -0.010862413346972865, -0.17581082879812182, 0.1234939898003016, 0.31748043985092356, -0.26774150369387556, -0.1991357280571452, 0.06701679069245824, -0.2490401516928721, -0.2920529930064838, 0.16392960066236006, -0.12893870432419455,... |
708.3172 | Fostering Consensus in Multidimensional Continuous Opinion Dynamics
under Bounded Confidence | Social consensus is important for society. Sometimes the success of society
depends on a consensus (e.g. the decision to pay taxes or to commit to the
constitution). Examples for continuous opinion dynamics are discussions about
tax rates or budget plan proposals for governments investments. Another example
is a comm... | physics.soc-ph | social consensus is important for society sometimes the success of society depends on a consensus eg the decision to pay taxes or to commit to the constitution examples for continuous opinion dynamics are discussions about tax rates or budget plan proposals for governments investments another example is a commission of... | [['social', 'consensus', 'is', 'important', 'for', 'society', 'sometimes', 'the', 'success', 'of', 'society', 'depends', 'on', 'a', 'consensus', 'eg', 'the', 'decision', 'to', 'pay', 'taxes', 'or', 'to', 'commit', 'to', 'the', 'constitution', 'examples', 'for', 'continuous', 'opinion', 'dynamics', 'are', 'discussions',... | [-0.09085945932252798, 0.08137391083058901, -0.08748172636842355, 0.08360917762067402, -0.146061683857115, -0.18437831934541463, 0.15124376748281065, 0.4033893158566207, -0.2067956295562908, -0.30951832337770613, 0.15038428532658143, -0.31091823981609196, -0.11999586010613711, 0.15541388734272915, -0.1192514481395483, ... |
708.3173 | Electro-Magnetic Waves within a Model for Charged Solitons | We analyze the model of topological fermions (MTF), where charged fermions
are treated as soliton solutions of the field equations. In the region far from
the sources we find plane waves solutions with the properties of
electro-magnetic waves.
| hep-th | we analyze the model of topological fermions mtf where charged fermions are treated as soliton solutions of the field equations in the region far from the sources we find plane waves solutions with the properties of electromagnetic waves | [['we', 'analyze', 'the', 'model', 'of', 'topological', 'fermions', 'mtf', 'where', 'charged', 'fermions', 'are', 'treated', 'as', 'soliton', 'solutions', 'of', 'the', 'field', 'equations', 'in', 'the', 'region', 'far', 'from', 'the', 'sources', 'we', 'find', 'plane', 'waves', 'solutions', 'with', 'the', 'properties', ... | [-0.19623498392511943, 0.17237416669530303, -0.03373277626049362, 0.08870856689387246, -0.05535140061309855, -0.08169436788088397, 0.0012370474930656584, 0.31759706502290147, -0.20764876245275923, -0.2520437597444183, 0.05873636061656534, -0.3960785531487904, -0.13174416926248292, 0.1476648311608618, 0.0949430038446352... |
708.3174 | On the topology of surface singularities {z^n=f(x,y)}, for f irreducible | The splice quotients are an interesting class of normal surface singularities
with rational homology sphere links, defined by W. Neumann and J. Wahl. If
Gamma is a tree of rational curves that satisfies certain combinatorial
conditions, then there exist splice quotients with resolution graph Gamma.
Suppose the equati... | math.AG | the splice quotients are an interesting class of normal surface singularities with rational homology sphere links defined by w neumann and j wahl if gamma is a tree of rational curves that satisfies certain combinatorial conditions then there exist splice quotients with resolution graph gamma suppose the equation znfxy... | [['the', 'splice', 'quotients', 'are', 'an', 'interesting', 'class', 'of', 'normal', 'surface', 'singularities', 'with', 'rational', 'homology', 'sphere', 'links', 'defined', 'by', 'w', 'neumann', 'and', 'j', 'wahl', 'if', 'gamma', 'is', 'a', 'tree', 'of', 'rational', 'curves', 'that', 'satisfies', 'certain', 'combinat... | [-0.19525294502103782, 0.08205182774463142, -0.1055453604006249, 0.06264876959511362, -0.09495790543682549, -0.194773657457984, 0.0006202191256148659, 0.3600257793461661, -0.3459244240399288, -0.1941692362660947, 0.08146740714816944, -0.2692216414340731, -0.14634960190514507, 0.16617594144873968, -0.12463251433294753, ... |
708.3175 | Fractional charge perspective on the band-gap in density-functional
theory | The calculation of the band-gap by density-functional theory (DFT) methods is
examined by considering the behavior of the energy as a function of number of
electrons. It is found that the incorrect band-gap prediction with most
approximate functionals originates mainly from errors in describing systems
with fractiona... | cond-mat.mtrl-sci | the calculation of the bandgap by densityfunctional theory dft methods is examined by considering the behavior of the energy as a function of number of electrons it is found that the incorrect bandgap prediction with most approximate functionals originates mainly from errors in describing systems with fractional charge... | [['the', 'calculation', 'of', 'the', 'bandgap', 'by', 'densityfunctional', 'theory', 'dft', 'methods', 'is', 'examined', 'by', 'considering', 'the', 'behavior', 'of', 'the', 'energy', 'as', 'a', 'function', 'of', 'number', 'of', 'electrons', 'it', 'is', 'found', 'that', 'the', 'incorrect', 'bandgap', 'prediction', 'wit... | [-0.08862421298707443, 0.08390212086633556, -0.0892609877084682, 0.08587818601541991, -0.0047293779986702705, -0.09071031062717526, 0.0782554409974678, 0.3658805972904213, -0.23222072000426724, -0.3601870421644431, 0.02233589402292201, -0.3231058678443521, -0.14250612128833848, 0.18021799234119207, -0.00487690022701593... |
708.3176 | Integrating out the Dirac sea: Effective field theory approach to
exactly solvable four-fermion models | We use 1+1 dimensional large N Gross-Neveu models as a laboratory to derive
microscopically effective Lagrangians for positive energy fermions only. When
applied to baryons, the Euler-Lagrange equation for these effective theories
assumes the form of a non-linear Dirac equation. Its solution reproduces the
full semi-... | hep-th hep-ph nucl-th | we use 11 dimensional large n grossneveu models as a laboratory to derive microscopically effective lagrangians for positive energy fermions only when applied to baryons the eulerlagrange equation for these effective theories assumes the form of a nonlinear dirac equation its solution reproduces the full semiclassical ... | [['we', 'use', '11', 'dimensional', 'large', 'n', 'grossneveu', 'models', 'as', 'a', 'laboratory', 'to', 'derive', 'microscopically', 'effective', 'lagrangians', 'for', 'positive', 'energy', 'fermions', 'only', 'when', 'applied', 'to', 'baryons', 'the', 'eulerlagrange', 'equation', 'for', 'these', 'effective', 'theorie... | [-0.1188492716393537, 0.19261786739548875, -0.053631850484008384, 0.1483105608391472, -0.09083403491725524, -0.1636090276672298, -0.016894952329393063, 0.2927668928686116, -0.1929356780084264, -0.2889465466969543, 0.014366912793937243, -0.32661170228901837, -0.14193967232842827, 0.09932280006145852, 0.05009101182351717... |
708.3177 | Convergence of products of stochastic matrices with positive diagonals
and the opinion dynamics background | We present a convergence result for infinite products of stochastic matrices
with positive diagonals. We regard infinity of the product to the left. Such a
product converges partly to a fixed matrix if the minimal positive entry of
each matrix does not converge too fast to zero and if either zero-entries are
symmetri... | math.OC math.DS | we present a convergence result for infinite products of stochastic matrices with positive diagonals we regard infinity of the product to the left such a product converges partly to a fixed matrix if the minimal positive entry of each matrix does not converge too fast to zero and if either zeroentries are symmetric in ... | [['we', 'present', 'a', 'convergence', 'result', 'for', 'infinite', 'products', 'of', 'stochastic', 'matrices', 'with', 'positive', 'diagonals', 'we', 'regard', 'infinity', 'of', 'the', 'product', 'to', 'the', 'left', 'such', 'a', 'product', 'converges', 'partly', 'to', 'a', 'fixed', 'matrix', 'if', 'the', 'minimal', '... | [-0.1113787742266268, 0.15421238684467153, -0.04053226462156888, 0.037038839116831423, -0.06515279099990598, -0.15104566375610598, 0.05285095805792432, 0.3627102530781964, -0.2978109348352933, -0.19857024323407627, 0.1850577205554337, -0.27712280991928356, -0.13445066439045036, 0.09112309268471507, -0.09263249842874836... |
708.3178 | Phase diagram of a Bose-Fermi mixture in a one-dimensional optical
lattice in terms of fidelity and entanglement | We study the ground-state phase diagram of a Bose-Fermi mixture loaded in a
one-dimensional optical lattice by computing the ground-state fidelity and
quantum entanglement. We find that the fidelity is able to signal quantum phase
transitions between the Luttinger liquid phase, the density-wave phase, and the
phase s... | cond-mat.str-el | we study the groundstate phase diagram of a bosefermi mixture loaded in a onedimensional optical lattice by computing the groundstate fidelity and quantum entanglement we find that the fidelity is able to signal quantum phase transitions between the luttinger liquid phase the densitywave phase and the phase separation ... | [['we', 'study', 'the', 'groundstate', 'phase', 'diagram', 'of', 'a', 'bosefermi', 'mixture', 'loaded', 'in', 'a', 'onedimensional', 'optical', 'lattice', 'by', 'computing', 'the', 'groundstate', 'fidelity', 'and', 'quantum', 'entanglement', 'we', 'find', 'that', 'the', 'fidelity', 'is', 'able', 'to', 'signal', 'quantu... | [-0.1946489882988057, 0.2711479585351689, -0.11216922298605952, 0.018244013996861343, 0.04171249233186245, -0.17263137263112835, 0.14299558076475347, 0.3801801931645189, -0.23492635693401098, -0.22798171914847834, 0.05958856589526736, -0.2802365017788751, -0.14167535430086511, 0.08494062228128314, 0.0751441778482071, 0... |
708.3179 | A physical basis for MOND | MOND is a phenomenological theory with no apparent physical justification
which seems to undermine some of the basic principles that underpin established
theoretical physics. It is nevertheless remarkably successful over its sphere
of application and this suggests MOND may have some physical basis. It is shown
here t... | physics.gen-ph | mond is a phenomenological theory with no apparent physical justification which seems to undermine some of the basic principles that underpin established theoretical physics it is nevertheless remarkably successful over its sphere of application and this suggests mond may have some physical basis it is shown here that ... | [['mond', 'is', 'a', 'phenomenological', 'theory', 'with', 'no', 'apparent', 'physical', 'justification', 'which', 'seems', 'to', 'undermine', 'some', 'of', 'the', 'basic', 'principles', 'that', 'underpin', 'established', 'theoretical', 'physics', 'it', 'is', 'nevertheless', 'remarkably', 'successful', 'over', 'its', '... | [-0.08377797511477386, 0.08776867958335464, -0.2074636361018444, 0.17376521350363167, -0.1620771075605363, -0.19345087908570552, -0.010171226492578475, 0.33860389451082384, -0.2386734934342611, -0.2908821251346833, 0.06106157232716214, -0.17518633305897108, -0.20017149746905083, 0.2257524978162514, -0.11364710338077405... |
708.318 | Curved Casimir Operators and the BGG Machinery | We prove that the Casimir operator acting on sections of a homogeneous vector
bundle over a generalized flag manifold naturally extends to an invariant
differential operator on arbitrary parabolic geometries. We study some
properties of the resulting invariant operators and compute their action on
various special typ... | math.DG math.RT | we prove that the casimir operator acting on sections of a homogeneous vector bundle over a generalized flag manifold naturally extends to an invariant differential operator on arbitrary parabolic geometries we study some properties of the resulting invariant operators and compute their action on various special types ... | [['we', 'prove', 'that', 'the', 'casimir', 'operator', 'acting', 'on', 'sections', 'of', 'a', 'homogeneous', 'vector', 'bundle', 'over', 'a', 'generalized', 'flag', 'manifold', 'naturally', 'extends', 'to', 'an', 'invariant', 'differential', 'operator', 'on', 'arbitrary', 'parabolic', 'geometries', 'we', 'study', 'some... | [-0.15583698814460897, 0.05375549155974686, -0.09898330855472874, 0.0846987541759105, -0.12050181288201706, -0.09407016445595004, -0.051027385563933984, 0.36034925638291077, -0.2945628395507566, -0.18550299396034048, 0.0938058671866301, -0.21306159610453085, -0.1897049900418257, 0.21923388516483436, -0.1265295880275363... |
708.3181 | Point Mutations Effects on Charge Transport Properties of the
Tumor-Suppressor Gene p53 | We report on a theoretical study of point mutations effects on charge
transfer properties in the DNA sequence of the tumor-suppressor p53 gene. On
the basis of effective single-strand or double-strand tight-binding models
which simulate hole propagation along the DNA, a statistical analysis of charge
transmission mod... | q-bio.GN cond-mat.soft q-bio.QM | we report on a theoretical study of point mutations effects on charge transfer properties in the dna sequence of the tumorsuppressor p53 gene on the basis of effective singlestrand or doublestrand tightbinding models which simulate hole propagation along the dna a statistical analysis of charge transmission modulations... | [['we', 'report', 'on', 'a', 'theoretical', 'study', 'of', 'point', 'mutations', 'effects', 'on', 'charge', 'transfer', 'properties', 'in', 'the', 'dna', 'sequence', 'of', 'the', 'tumorsuppressor', 'p53', 'gene', 'on', 'the', 'basis', 'of', 'effective', 'singlestrand', 'or', 'doublestrand', 'tightbinding', 'models', 'w... | [-0.15845803423324245, 0.11312992188796987, -0.05191281464034587, 0.10243751407925332, -0.0018737171881235718, -0.13032793496955145, 0.1325864778201127, 0.39210748207870494, -0.24373978541724467, -0.22164483334911003, 0.008187792563465622, -0.2803037483872992, -0.22970350633971812, 0.15200785170518533, -0.0634047129201... |
708.3182 | Topology of Smectic Order on Compact Substrates | Smectic orders on curved substrates can be described by differential forms of
rank one (1-forms), whose geometric meaning is the differential of the local
phase field of density modulation. The exterior derivative of 1-form is the
local dislocation density. Elastic deformations are described by superposition
of exact... | cond-mat.soft cond-mat.stat-mech | smectic orders on curved substrates can be described by differential forms of rank one 1forms whose geometric meaning is the differential of the local phase field of density modulation the exterior derivative of 1form is the local dislocation density elastic deformations are described by superposition of exact differen... | [['smectic', 'orders', 'on', 'curved', 'substrates', 'can', 'be', 'described', 'by', 'differential', 'forms', 'of', 'rank', 'one', '1forms', 'whose', 'geometric', 'meaning', 'is', 'the', 'differential', 'of', 'the', 'local', 'phase', 'field', 'of', 'density', 'modulation', 'the', 'exterior', 'derivative', 'of', '1form'... | [-0.2086773265032022, 0.19328661597659433, -0.06419430157014479, 0.053391126822112354, -0.06236766200944236, -0.10050939303270079, -0.03075000665404236, 0.33608233186651054, -0.2927665351094996, -0.32316307910543873, 0.09970431850193356, -0.2610987615620157, -0.1820634834210926, 0.14420951774146984, -0.0249529666185939... |
708.3183 | Pseudo-periodicity and 1/f noise from the sum of similar intermittent
signals | The usual interpretation of noise is represented by a sum of many independent
two-level elementary random signals with a distribution of relaxation times. In
this paper it is demonstrated that also the superposition of many similar
single-sided two-level signals, with the same relaxation time, produces noise.
This is... | physics.data-an physics.gen-ph | the usual interpretation of noise is represented by a sum of many independent twolevel elementary random signals with a distribution of relaxation times in this paper it is demonstrated that also the superposition of many similar singlesided twolevel signals with the same relaxation time produces noise this is possible... | [['the', 'usual', 'interpretation', 'of', 'noise', 'is', 'represented', 'by', 'a', 'sum', 'of', 'many', 'independent', 'twolevel', 'elementary', 'random', 'signals', 'with', 'a', 'distribution', 'of', 'relaxation', 'times', 'in', 'this', 'paper', 'it', 'is', 'demonstrated', 'that', 'also', 'the', 'superposition', 'of',... | [-0.12623863246129907, 0.14879780020656536, -0.0784092021336698, 0.04729442066920218, -0.025478278651185658, -0.14513043546036858, 0.015103439118399325, 0.3725101827826027, -0.3191163393506861, -0.29624505582994415, 0.07075504998236125, -0.2590635895334265, -0.15484432442399734, 0.20639941934243086, -0.0411540314140122... |
708.3184 | Unitarity in the Brout-Englert-Higgs Mechanism for Gravity | Just like the vector bosons in Abelian and non-Abelian gauge theories,
gravitons can attain mass by spontaneous local symmetry breaking. The question
is whether this can happen in a Lorentz-invariant way. We consider the use of
four scalar fields that break coordinate reparametrization invariance, by
playing the role... | hep-th gr-qc | just like the vector bosons in abelian and nonabelian gauge theories gravitons can attain mass by spontaneous local symmetry breaking the question is whether this can happen in a lorentzinvariant way we consider the use of four scalar fields that break coordinate reparametrization invariance by playing the role of pref... | [['just', 'like', 'the', 'vector', 'bosons', 'in', 'abelian', 'and', 'nonabelian', 'gauge', 'theories', 'gravitons', 'can', 'attain', 'mass', 'by', 'spontaneous', 'local', 'symmetry', 'breaking', 'the', 'question', 'is', 'whether', 'this', 'can', 'happen', 'in', 'a', 'lorentzinvariant', 'way', 'we', 'consider', 'the', ... | [-0.14098531736100942, 0.2617005975344679, -0.09103454017156819, 0.13340483397530364, -0.10352048175687444, -0.195842592837984, 0.010837793767229835, 0.3202691071227179, -0.22796172399417872, -0.2859111181664482, 0.05509555488242768, -0.26052601624683325, -0.11905764243669752, 0.08865673710816234, -0.021278706155091857... |
708.3185 | Nucleosynthesis from massive stars 50 years after B2FH | We review some important observed properties of massive stars. Then we
discuss how mass loss and rotation affect their evolution and help in giving
better fits to observational constraints. Consequences for nucleosynthesis at
different metallicities are discussed. Mass loss appear to be the key feature
at high metall... | astro-ph | we review some important observed properties of massive stars then we discuss how mass loss and rotation affect their evolution and help in giving better fits to observational constraints consequences for nucleosynthesis at different metallicities are discussed mass loss appear to be the key feature at high metallicity... | [['we', 'review', 'some', 'important', 'observed', 'properties', 'of', 'massive', 'stars', 'then', 'we', 'discuss', 'how', 'mass', 'loss', 'and', 'rotation', 'affect', 'their', 'evolution', 'and', 'help', 'in', 'giving', 'better', 'fits', 'to', 'observational', 'constraints', 'consequences', 'for', 'nucleosynthesis', '... | [-0.07274197103993539, 0.2005585188140724, -0.08878743133562453, 0.1830477543495207, -0.09881631101924866, -0.08837485616219873, 0.09110693193792818, 0.43230038483871175, -0.1751321804495578, -0.36096540458480464, 0.04158993551126597, -0.2701161607532179, -0.04080213587930336, 0.17211369600864176, -0.09110713411212207,... |
708.3186 | Pinch Points and Kasteleyn Transitions: How Spin Ice Changes its Entropy | Complex disordered states - from liquids and glasses to exotic quantum matter
- are ubiquitous in nature. Their key properties include finite entropy,
power-law correlations and emergent organising principles. In spin ice, spin
correlations are determined by an ice rules organising principle that
stabilises a magneti... | cond-mat.other | complex disordered states from liquids and glasses to exotic quantum matter are ubiquitous in nature their key properties include finite entropy powerlaw correlations and emergent organising principles in spin ice spin correlations are determined by an ice rules organising principle that stabilises a magnetic state wit... | [['complex', 'disordered', 'states', 'from', 'liquids', 'and', 'glasses', 'to', 'exotic', 'quantum', 'matter', 'are', 'ubiquitous', 'in', 'nature', 'their', 'key', 'properties', 'include', 'finite', 'entropy', 'powerlaw', 'correlations', 'and', 'emergent', 'organising', 'principles', 'in', 'spin', 'ice', 'spin', 'corre... | [-0.13441778011746755, 0.2660654092567488, -0.08848891899838639, 0.07007435742618363, -0.059153052137176296, -0.168270674359915, 0.026314513186043522, 0.36059940862310985, -0.30432939435653134, -0.2564095787729333, 0.058514328332155384, -0.2947322625989969, -0.15194881221178133, 0.12875950407493403, 0.04725788366944421... |
708.3187 | Dynamical properties and structure of Julia sets of postcritically
bounded polynomial semigroups | We discuss the dynamic and structural properties of polynomial semigroups, a
natural extension of iteration theory to random (walk) dynamics, where the
semigroup $G$ of complex polynomials (under the operation of composition of
functions) is such that there exists a bounded set in the plane which contains
any finite ... | math.DS math.CV | we discuss the dynamic and structural properties of polynomial semigroups a natural extension of iteration theory to random walk dynamics where the semigroup g of complex polynomials under the operation of composition of functions is such that there exists a bounded set in the plane which contains any finite critical v... | [['we', 'discuss', 'the', 'dynamic', 'and', 'structural', 'properties', 'of', 'polynomial', 'semigroups', 'a', 'natural', 'extension', 'of', 'iteration', 'theory', 'to', 'random', 'walk', 'dynamics', 'where', 'the', 'semigroup', 'g', 'of', 'complex', 'polynomials', 'under', 'the', 'operation', 'of', 'composition', 'of'... | [-0.18788697491083, 0.13223527461084347, -0.07177623958541422, 0.018496719895403697, -0.08638379967366759, -0.08415554637450198, 0.01482370307032721, 0.36476436985354305, -0.33848893667780916, -0.20036072166501276, 0.12727767202322962, -0.30414874826592064, -0.14278657203515827, 0.2096920170204431, -0.07363958917655714... |
708.3188 | Strong wavefront lemma and counting lattice points in sectors | We compute the asymptotics of the number of integral quadratic forms with
prescribed orthogonal decompositions and, more generally, the asymptotics of
the number of lattice points lying in sectors of affine symmetric spaces. A new
key ingredient in this article is the strong wavefront lemma, which shows that
the gene... | math.NT math.GR | we compute the asymptotics of the number of integral quadratic forms with prescribed orthogonal decompositions and more generally the asymptotics of the number of lattice points lying in sectors of affine symmetric spaces a new key ingredient in this article is the strong wavefront lemma which shows that the generalize... | [['we', 'compute', 'the', 'asymptotics', 'of', 'the', 'number', 'of', 'integral', 'quadratic', 'forms', 'with', 'prescribed', 'orthogonal', 'decompositions', 'and', 'more', 'generally', 'the', 'asymptotics', 'of', 'the', 'number', 'of', 'lattice', 'points', 'lying', 'in', 'sectors', 'of', 'affine', 'symmetric', 'spaces... | [-0.19016487904785512, 0.10498527612847587, -0.10398772866853202, 0.045286708210672565, -0.11512778652831912, -0.08739096469556291, -0.009392073067526022, 0.3069050974833469, -0.2995657178107649, -0.17722295575464767, 0.1263385041888493, -0.22446876734417553, -0.17681785778452952, 0.17120720529928804, -0.09448426539699... |
708.3189 | Beauty in the Standard Model and Beyond | The study of CP violation in the B system allows us to perform quantitative
tests of the CP symmetry in the Standard Model. Many precise measurements of
the sides and angles of the Unitarity Triangle used to test the theory are made
possible by the abundant experimental data accumulated at the B factories and
the Tev... | hep-ex | the study of cp violation in the b system allows us to perform quantitative tests of the cp symmetry in the standard model many precise measurements of the sides and angles of the unitarity triangle used to test the theory are made possible by the abundant experimental data accumulated at the b factories and the tevatr... | [['the', 'study', 'of', 'cp', 'violation', 'in', 'the', 'b', 'system', 'allows', 'us', 'to', 'perform', 'quantitative', 'tests', 'of', 'the', 'cp', 'symmetry', 'in', 'the', 'standard', 'model', 'many', 'precise', 'measurements', 'of', 'the', 'sides', 'and', 'angles', 'of', 'the', 'unitarity', 'triangle', 'used', 'to', ... | [-0.08167214845363276, 0.09970967016598008, -0.07042272058483887, 0.07171060860785375, -0.09511163020618708, -0.19478445942794165, 0.13050286020629154, 0.23500802630491285, -0.2546914172280266, -0.3300988627485482, 0.08512944868114967, -0.29562958599512146, -0.03066819005208202, 0.1773049357594047, 0.0458815646279289, ... |
708.319 | Detecting Infinitely Many Semisimple Representations in a Fixed Finite
Dimension | Let $n$ be a positive integer, and let $k$ be a field (of arbitrary
characteristic) accessible to symbolic computation. We describe an algorithmic
test for determining whether or not a finitely presented $k$-algebra $R$ has
infinitely many equivalence classes of semisimple representations $R \to
M_n(k')$, where $k'$ ... | math.RA math.AC | let n be a positive integer and let k be a field of arbitrary characteristic accessible to symbolic computation we describe an algorithmic test for determining whether or not a finitely presented kalgebra r has infinitely many equivalence classes of semisimple representations r to m_nk where k is the algebraic closure ... | [['let', 'n', 'be', 'a', 'positive', 'integer', 'and', 'let', 'k', 'be', 'a', 'field', 'of', 'arbitrary', 'characteristic', 'accessible', 'to', 'symbolic', 'computation', 'we', 'describe', 'an', 'algorithmic', 'test', 'for', 'determining', 'whether', 'or', 'not', 'a', 'finitely', 'presented', 'kalgebra', 'r', 'has', 'i... | [-0.1875338910669997, 0.08788972257273754, -0.0869414248935333, 0.011211070780097166, -0.10900938748836336, -0.25722938703895526, -0.03998805369568489, 0.29843048401540373, -0.34438416529901145, -0.27073793035432153, 0.0871235634393354, -0.2405890141011829, -0.08222793359820527, 0.2361616151515258, -0.07089563635733012... |
708.3191 | Cohomology and Support Varieties for Lie Superalgebras II | In \cite{BKN} the authors initiated a study of the representation theory of
classical Lie superalgebras via a cohomological approach. Detecting subalgebras
were constructed and a theory of support varieties was developed. The dimension
of a detecting subalgebra coincides with the defect of the Lie superalgebra and
th... | math.RT | in citebkn the authors initiated a study of the representation theory of classical lie superalgebras via a cohomological approach detecting subalgebras were constructed and a theory of support varieties was developed the dimension of a detecting subalgebra coincides with the defect of the lie superalgebra and the dimen... | [['in', 'citebkn', 'the', 'authors', 'initiated', 'a', 'study', 'of', 'the', 'representation', 'theory', 'of', 'classical', 'lie', 'superalgebras', 'via', 'a', 'cohomological', 'approach', 'detecting', 'subalgebras', 'were', 'constructed', 'and', 'a', 'theory', 'of', 'support', 'varieties', 'was', 'developed', 'the', '... | [-0.13588806831726938, 0.021881003055854567, -0.06525387302307147, 0.05608669419639877, -0.11994091898335942, -0.15101850083031293, 0.004151223947493625, 0.3152788800054363, -0.24169940432600145, -0.21659700827939168, 0.10826224106879506, -0.20798049740593083, -0.19274278124794364, 0.20012160206679255, -0.1141460299841... |
708.3192 | Uniformly perfect analytic and conformal attractor sets | Conditions are given which imply that analytic iterated function systems
(IFS's) in the complex plane have uniformly perfect attractor sets. In
particular, it is shown that the attractor set of a finitely generated
conformal IFS is uniformly perfect when it contains two or more points. Also,
an example of a finitely ... | math.DS math.CV | conditions are given which imply that analytic iterated function systems ifss in the complex plane have uniformly perfect attractor sets in particular it is shown that the attractor set of a finitely generated conformal ifs is uniformly perfect when it contains two or more points also an example of a finitely generated... | [['conditions', 'are', 'given', 'which', 'imply', 'that', 'analytic', 'iterated', 'function', 'systems', 'ifss', 'in', 'the', 'complex', 'plane', 'have', 'uniformly', 'perfect', 'attractor', 'sets', 'in', 'particular', 'it', 'is', 'shown', 'that', 'the', 'attractor', 'set', 'of', 'a', 'finitely', 'generated', 'conforma... | [-0.17129080702603283, 0.13508981770968193, -0.12043852283949813, 0.043683723794416554, -0.05620743261815439, -0.14392341644458112, -0.06623782839385732, 0.37225473515929713, -0.2869761243702904, -0.1450299625660503, 0.13138560206824612, -0.3070545308291912, -0.18999897452792333, 0.256605907670042, -0.0700738897787467,... |
708.3193 | Discrete rearranging disordered patterns, part I: Robust statistical
tools in two or three dimensions | Discrete rearranging patterns include cellular patterns, for instance liquid
foams, biological tissues, grains in polycrystals; assemblies of particles such
as beads, granular materials, colloids, molecules, atoms; and interconnected
networks. Such a pattern can be described as a list of links between
neighbouring si... | cond-mat.soft | discrete rearranging patterns include cellular patterns for instance liquid foams biological tissues grains in polycrystals assemblies of particles such as beads granular materials colloids molecules atoms and interconnected networks such a pattern can be described as a list of links between neighbouring sites performi... | [['discrete', 'rearranging', 'patterns', 'include', 'cellular', 'patterns', 'for', 'instance', 'liquid', 'foams', 'biological', 'tissues', 'grains', 'in', 'polycrystals', 'assemblies', 'of', 'particles', 'such', 'as', 'beads', 'granular', 'materials', 'colloids', 'molecules', 'atoms', 'and', 'interconnected', 'networks... | [-0.10058114101411775, 0.1387579464632644, -0.07868408251109474, 0.08364139932342335, -0.057949043880857594, -0.12875223500278155, 0.03785465192904166, 0.38488824508759545, -0.27375311437361965, -0.3026313299672046, 0.08611831390469787, -0.2792731012503933, -0.1917309817391311, 0.17992889822071947, -0.03978474707547746... |
708.3194 | Comment on Experiments Related to the Aharonov-Bohm Phase Shift | Recent experiments undertaken by Caprez, Barwick, and Batelaan should clarify
the connections between classical and quantum theories in connection with the
Aharonov-Bohm phase shift. It is pointed out that resistive aspects for the
solenoid current carriers play a role in the classical but not the quantum
analysis fo... | physics.class-ph physics.gen-ph | recent experiments undertaken by caprez barwick and batelaan should clarify the connections between classical and quantum theories in connection with the aharonovbohm phase shift it is pointed out that resistive aspects for the solenoid current carriers play a role in the classical but not the quantum analysis for the ... | [['recent', 'experiments', 'undertaken', 'by', 'caprez', 'barwick', 'and', 'batelaan', 'should', 'clarify', 'the', 'connections', 'between', 'classical', 'and', 'quantum', 'theories', 'in', 'connection', 'with', 'the', 'aharonovbohm', 'phase', 'shift', 'it', 'is', 'pointed', 'out', 'that', 'resistive', 'aspects', 'for'... | [-0.16717773850120785, 0.17871558628078685, -0.1257087345493127, 0.10149768257165799, -0.07363888812083078, -0.12873619630461536, 0.1063672547475491, 0.34436830707702293, -0.21637613328555264, -0.2755256568990558, 0.05466258960792862, -0.25744410994720746, -0.17120738910982408, 0.21414243985326534, -0.01962520193353474... |
708.3195 | Ignition latitude and the shape of Type I X-ray bursts | The shape of the lightcurve during the rising phase of Type I X-ray bursts is
determined by many factors including the ignition latitude, the accretion rate,
and the rotation rate of the star. We develop a phenomenological model of the
burst rise process and show that simple measures of the burst morphology can be
ro... | astro-ph | the shape of the lightcurve during the rising phase of type i xray bursts is determined by many factors including the ignition latitude the accretion rate and the rotation rate of the star we develop a phenomenological model of the burst rise process and show that simple measures of the burst morphology can be robust d... | [['the', 'shape', 'of', 'the', 'lightcurve', 'during', 'the', 'rising', 'phase', 'of', 'type', 'i', 'xray', 'bursts', 'is', 'determined', 'by', 'many', 'factors', 'including', 'the', 'ignition', 'latitude', 'the', 'accretion', 'rate', 'and', 'the', 'rotation', 'rate', 'of', 'the', 'star', 'we', 'develop', 'a', 'phenome... | [-0.055501600457490356, 0.17976187850159686, -0.042089422715935805, 0.12912571536716036, -0.059125173922992595, -0.09180818975268715, 0.10062804896438467, 0.42123199696990027, -0.21908476932541185, -0.3062504652813347, 0.11138882727844748, -0.28313341651759716, -0.08203748676359006, 0.26929568915384944, -0.058629169179... |
708.3196 | New Global Fit to the Total Photon-Proton Cross-Section sigma L+T and to
the Structure Function F2 | A fit to world data on the photon-proton cross section sigma L+T and the
unpolarised structure function F2 is presented. The 23-parameter ALLM model
based on Reggeon and Pomeron exchange is used. Cross section data were
reconstructed to avoid inconsistencies with respect to R of the published F2
data base. Parameter ... | hep-ph | a fit to world data on the photonproton cross section sigma lt and the unpolarised structure function f2 is presented the 23parameter allm model based on reggeon and pomeron exchange is used cross section data were reconstructed to avoid inconsistencies with respect to r of the published f2 data base parameter uncertai... | [['a', 'fit', 'to', 'world', 'data', 'on', 'the', 'photonproton', 'cross', 'section', 'sigma', 'lt', 'and', 'the', 'unpolarised', 'structure', 'function', 'f2', 'is', 'presented', 'the', '23parameter', 'allm', 'model', 'based', 'on', 'reggeon', 'and', 'pomeron', 'exchange', 'is', 'used', 'cross', 'section', 'data', 'we... | [-0.08780068201436238, 0.03536539371548728, -0.08952509493313053, 0.1640372561333193, -0.0821699886498126, -0.10859668643467806, 0.020377028733491898, 0.37505379021167756, -0.21303120528093794, -0.3163535914098082, -0.014275137419727716, -0.391171513565562, 0.006176668202335184, 0.1612867079886862, 0.03562003650109876,... |
708.3197 | From Microscales to Macroscales in 3D: Selfconsistent Equation of State
for Supernova and Neutron Star Models | First results from a fully self-consistent, temperature-dependent equation of
state that spans the whole density range of neutron stars and supernova cores
are presented. The equation of state (EoS) is calculated using a mean-field
Hartree-Fock method in three dimensions (3D). The nuclear interaction is
represented b... | astro-ph nucl-th | first results from a fully selfconsistent temperaturedependent equation of state that spans the whole density range of neutron stars and supernova cores are presented the equation of state eos is calculated using a meanfield hartreefock method in three dimensions 3d the nuclear interaction is represented by the phenome... | [['first', 'results', 'from', 'a', 'fully', 'selfconsistent', 'temperaturedependent', 'equation', 'of', 'state', 'that', 'spans', 'the', 'whole', 'density', 'range', 'of', 'neutron', 'stars', 'and', 'supernova', 'cores', 'are', 'presented', 'the', 'equation', 'of', 'state', 'eos', 'is', 'calculated', 'using', 'a', 'mea... | [-0.04435707995149541, 0.16420520163090124, -0.10765539341251955, 0.09027710927584626, -0.028049746906796208, -0.08423128505551651, 0.0572110241631823, 0.3494412927885477, -0.21235555512944887, -0.3424430285677588, -0.012095704633296907, -0.26137755511400357, -0.023104812592793643, 0.17268958312824964, 0.06558093117218... |
708.3198 | Universal price impact functions of individual trades in an order-driven
market | The trade size $\omega$ has direct impact on the price formation of the stock
traded. Econophysical analyses of transaction data for the US and Australian
stock markets have uncovered market-specific scaling laws, where a master curve
of price impact can be obtained in each market when stock capitalization $C$ is
inc... | q-fin.TR physics.soc-ph | the trade size omega has direct impact on the price formation of the stock traded econophysical analyses of transaction data for the us and australian stock markets have uncovered marketspecific scaling laws where a master curve of price impact can be obtained in each market when stock capitalization c is included as a... | [['the', 'trade', 'size', 'omega', 'has', 'direct', 'impact', 'on', 'the', 'price', 'formation', 'of', 'the', 'stock', 'traded', 'econophysical', 'analyses', 'of', 'transaction', 'data', 'for', 'the', 'us', 'and', 'australian', 'stock', 'markets', 'have', 'uncovered', 'marketspecific', 'scaling', 'laws', 'where', 'a', ... | [-0.10286098114929551, 0.13213891762583832, -0.11740565731487863, 0.1221242451755956, -0.06662174288973548, -0.12980400725099883, 0.11868610750830381, 0.39255396402526843, -0.26439564896854345, -0.28227849011872436, 0.14270111513715314, -0.35921387780137115, -0.12852152106810177, 0.18111842053562602, -0.082456979770824... |
708.3199 | Phases of Thermal N=2 Quiver Gauge Theories | We consider large N U(N)^M thermal N=2 quiver gauge theories on S^1 x S^3. We
obtain a phase diagram of the theory with R-symmetry chemical potentials,
separating a low-temperature/high-chemical potential region from a
high-temperature/low-chemical potential region. In close analogy with the N=4
SYM case, the free en... | hep-th | we consider large n unm thermal n2 quiver gauge theories on s1 x s3 we obtain a phase diagram of the theory with rsymmetry chemical potentials separating a lowtemperaturehighchemical potential region from a hightemperaturelowchemical potential region in close analogy with the n4 sym case the free energy is of order o1 ... | [['we', 'consider', 'large', 'n', 'unm', 'thermal', 'n2', 'quiver', 'gauge', 'theories', 'on', 's1', 'x', 's3', 'we', 'obtain', 'a', 'phase', 'diagram', 'of', 'the', 'theory', 'with', 'rsymmetry', 'chemical', 'potentials', 'separating', 'a', 'lowtemperaturehighchemical', 'potential', 'region', 'from', 'a', 'hightempera... | [-0.17847740931614042, 0.2317402252733747, -0.06459709763714142, 0.04526864804781148, -0.0005745552864271341, -0.10590439322692602, 0.04823922752654756, 0.3420716952244492, -0.20262660193689092, -0.23914045187135793, 0.06822823515682741, -0.3007399786849381, -0.10554249259372021, 0.06729288173949864, 0.0044939605268342... |
708.32 | First-principles study of the effects of gold adsorption on the Al(001)
surface properties | In this work, we have studied theoretically the effects of gold adsorption on
the Al(001) surface, using {\it ab initio} pseudo-potential method in the
framework of the density functional theory. Having found the hollow sites at
the Al(001) surface as the most preferred adsorption sites, we have
investigated the effe... | cond-mat.mtrl-sci | in this work we have studied theoretically the effects of gold adsorption on the al001 surface using it ab initio pseudopotential method in the framework of the density functional theory having found the hollow sites at the al001 surface as the most preferred adsorption sites we have investigated the effects of the au ... | [['in', 'this', 'work', 'we', 'have', 'studied', 'theoretically', 'the', 'effects', 'of', 'gold', 'adsorption', 'on', 'the', 'al001', 'surface', 'using', 'it', 'ab', 'initio', 'pseudopotential', 'method', 'in', 'the', 'framework', 'of', 'the', 'density', 'functional', 'theory', 'having', 'found', 'the', 'hollow', 'site... | [-0.06419952762934966, 0.1275288193349355, -0.039590083501393224, 0.010438170159542449, 0.060250567938497215, -0.1117999438261021, 0.0859686339050639, 0.43195793826154544, -0.24511528326362653, -0.34669973410536786, -0.016508260237812093, -0.34202571303685964, -0.0974684097303476, 0.1291829880133185, 0.0291235288120590... |
708.3201 | Recent developments of the DDVV Conjecture | In this paper, we give a survey of the recent develpoments of the DDVV
conjecture.
| math.DG | in this paper we give a survey of the recent develpoments of the ddvv conjecture | [['in', 'this', 'paper', 'we', 'give', 'a', 'survey', 'of', 'the', 'recent', 'develpoments', 'of', 'the', 'ddvv', 'conjecture']] | [-0.202962256302791, 0.001564604030655963, -0.15387744350092752, -0.029642436561906443, -0.04851424893630402, 0.009577653271013073, 0.04744752184654187, 0.2450045936607889, -0.2129384907228606, -0.2854689129495195, 0.1054791192041843, -0.23730230915160583, -0.2317558065322893, 0.1708816694361823, -0.16266474280772464, ... |
708.3202 | Stochastic solution of nonlinear and nonhomogeneous evolution problems
by a differential Kolmogorov equation | A large class of physically important nonlinear and nonhomogeneous evolution
problems, characterized by advection-like and diffusion-like processes, can be
usefully studied by a time-differential form of Kolmogorov's solution of the
backward-time Fokker-Planck equation. The differential solution embodies an
integral ... | physics.data-an physics.flu-dyn | a large class of physically important nonlinear and nonhomogeneous evolution problems characterized by advectionlike and diffusionlike processes can be usefully studied by a timedifferential form of kolmogorovs solution of the backwardtime fokkerplanck equation the differential solution embodies an integral representat... | [['a', 'large', 'class', 'of', 'physically', 'important', 'nonlinear', 'and', 'nonhomogeneous', 'evolution', 'problems', 'characterized', 'by', 'advectionlike', 'and', 'diffusionlike', 'processes', 'can', 'be', 'usefully', 'studied', 'by', 'a', 'timedifferential', 'form', 'of', 'kolmogorovs', 'solution', 'of', 'the', '... | [-0.09035443204807163, 0.028114203860669974, -0.11798612406946779, 0.10091993869263376, -0.15719756776868268, -0.18702254319805803, -0.04703593395586027, 0.23430835386753324, -0.34332083974306177, -0.25105331760899324, 0.10752224969882064, -0.2542685302168678, -0.18175723491713586, 0.21023868263426532, -0.0326135070782... |
708.3203 | Scalar-tensor black holes coupled to Euler-Heisenberg nonlinear
electrodynamics | The no-scalar-hair conjecture rules out the existence of asymptotically flat
black holes with a scalar dressing for a large class of theories.
No-scalar-hair theorems have been proved for the cases of neutral black holes
and for charged black holes in the Maxwell electrodynamics. These theorems,
however, do not apply... | gr-qc | the noscalarhair conjecture rules out the existence of asymptotically flat black holes with a scalar dressing for a large class of theories noscalarhair theorems have been proved for the cases of neutral black holes and for charged black holes in the maxwell electrodynamics these theorems however do not apply in the ca... | [['the', 'noscalarhair', 'conjecture', 'rules', 'out', 'the', 'existence', 'of', 'asymptotically', 'flat', 'black', 'holes', 'with', 'a', 'scalar', 'dressing', 'for', 'a', 'large', 'class', 'of', 'theories', 'noscalarhair', 'theorems', 'have', 'been', 'proved', 'for', 'the', 'cases', 'of', 'neutral', 'black', 'holes', ... | [-0.15991335577387927, 0.06923408721570123, -0.04636356803574458, 0.13379583081008273, -0.09222387106538835, -0.1965205077977964, -0.0527045729915809, 0.2637489246536103, -0.11291689999041299, -0.27820265668384364, 0.06013120212204134, -0.3088897706880799, -0.1252962690919186, 0.1814150980851881, -0.0317875866656488, 0... |
708.3204 | Main effects of the Earth's rotation on the stationary states of
ultra-cold neutrons | The relativistic corrections in the Hamiltonian for a particle in a uniformly
rotating frame are discussed. They are shown to be negligible in the case of
ultra-cold neutrons (UCN) in the Earth's gravity. The effect, on the energy
levels of UCN, of the main term due to the Earth's rotation, i.e. the
angular-momentum ... | quant-ph gr-qc | the relativistic corrections in the hamiltonian for a particle in a uniformly rotating frame are discussed they are shown to be negligible in the case of ultracold neutrons ucn in the earths gravity the effect on the energy levels of ucn of the main term due to the earths rotation ie the angularmomentum term is calcula... | [['the', 'relativistic', 'corrections', 'in', 'the', 'hamiltonian', 'for', 'a', 'particle', 'in', 'a', 'uniformly', 'rotating', 'frame', 'are', 'discussed', 'they', 'are', 'shown', 'to', 'be', 'negligible', 'in', 'the', 'case', 'of', 'ultracold', 'neutrons', 'ucn', 'in', 'the', 'earths', 'gravity', 'the', 'effect', 'on... | [-0.12880638594662688, 0.24718025154364642, -0.05521858945999767, 0.12193956108826365, 0.009206881093333907, -0.047430687722986316, -0.013805210367957158, 0.2965972394640766, -0.24322879682781537, -0.2895793600925314, 0.004767793043057865, -0.3107347657292414, 0.0054438281526316456, 0.18832079741804958, -0.069023925225... |
708.3205 | Human breath analysis via cavity-enhanced optical frequency comb
spectroscopy | To date, researchers have identified over 1000 different compounds contained
in human breath. These molecules have both endogenous and exogenous origins and
provide information about physiological processes occurring in the body as well
as environment-related ingestion or absorption of contaminants1,2. While the
pres... | physics.optics physics.atom-ph physics.chem-ph physics.ins-det | to date researchers have identified over 1000 different compounds contained in human breath these molecules have both endogenous and exogenous origins and provide information about physiological processes occurring in the body as well as environmentrelated ingestion or absorption of contaminants12 while the presence an... | [['to', 'date', 'researchers', 'have', 'identified', 'over', '1000', 'different', 'compounds', 'contained', 'in', 'human', 'breath', 'these', 'molecules', 'have', 'both', 'endogenous', 'and', 'exogenous', 'origins', 'and', 'provide', 'information', 'about', 'physiological', 'processes', 'occurring', 'in', 'the', 'body'... | [-0.0626391965226026, 0.11103471989631768, 0.013310598900358453, 0.03278769861303697, 0.008402188770381397, -0.11933827248295067, 0.0541079573821826, 0.40858363897967165, -0.2135864843263245, -0.3553168128443057, 0.1051556053784513, -0.3051645796888513, -0.10578212081683708, 0.18446888662003175, -0.039538774097368855, ... |
708.3206 | Photonic crystal laser-driven accelerator structures | Laser-driven acceleration holds great promise for significantly improving
accelerating gradient. However, scaling the conventional process of
structure-based acceleration in vacuum down to optical wavelengths requires a
substantially different kind of structure. We require an optical waveguide that
(1) is constructed... | physics.acc-ph physics.optics | laserdriven acceleration holds great promise for significantly improving accelerating gradient however scaling the conventional process of structurebased acceleration in vacuum down to optical wavelengths requires a substantially different kind of structure we require an optical waveguide that 1 is constructed out of d... | [['laserdriven', 'acceleration', 'holds', 'great', 'promise', 'for', 'significantly', 'improving', 'accelerating', 'gradient', 'however', 'scaling', 'the', 'conventional', 'process', 'of', 'structurebased', 'acceleration', 'in', 'vacuum', 'down', 'to', 'optical', 'wavelengths', 'requires', 'a', 'substantially', 'differ... | [-0.11380182291707686, 0.16110188844274417, -0.045957236199847186, -0.0019095920721604572, -0.05868632301811782, -0.12439036542126, 0.026549515441850146, 0.49138985527458634, -0.25132545920627375, -0.290893117972248, 0.07441781532301864, -0.22498611101474594, -0.11898755477697222, 0.23055921782468008, -0.01005598716437... |
708.3207 | Potential confinement property in the Parabolic Anderson Model | We consider the parabolic Anderson model, the Cauchy problem for the heat
equation with random potential in $Z^d$. We use i.i.d. potentials $\xi: Z^d \to
\R$ in the third universality class, namely the class of almost bounded
potentials, in the classification of van der Hofstad, Konig and Morters
[HKM06]. This class ... | math.PR | we consider the parabolic anderson model the cauchy problem for the heat equation with random potential in zd we use iid potentials xi zd to r in the third universality class namely the class of almost bounded potentials in the classification of van der hofstad konig and morters hkm06 this class consists of potentials ... | [['we', 'consider', 'the', 'parabolic', 'anderson', 'model', 'the', 'cauchy', 'problem', 'for', 'the', 'heat', 'equation', 'with', 'random', 'potential', 'in', 'zd', 'we', 'use', 'iid', 'potentials', 'xi', 'zd', 'to', 'r', 'in', 'the', 'third', 'universality', 'class', 'namely', 'the', 'class', 'of', 'almost', 'bounded... | [-0.10906632760054787, 0.09291349951725107, -0.05469381256554379, 0.04823372038693369, -0.04584997853974706, -0.14685036232406945, 0.0337210625227656, 0.34260524340338777, -0.2867445314360648, -0.24254433002284506, 0.07012222617049702, -0.2946039327305079, -0.13164190801530212, 0.16055780607479692, -0.08319441505141326... |
708.3208 | Mermin inequalities for perfect correlations | Any n-qubit state with n independent perfect correlations is equivalent to a
graph state. We present the optimal Bell inequalities for perfect correlations
and maximal violation for all classes of graph states with n < 7 qubits. Twelve
of them were previously unknown and four give the same violation as the
Greenberge... | quant-ph | any nqubit state with n independent perfect correlations is equivalent to a graph state we present the optimal bell inequalities for perfect correlations and maximal violation for all classes of graph states with n 7 qubits twelve of them were previously unknown and four give the same violation as the greenbergerhornez... | [['any', 'nqubit', 'state', 'with', 'n', 'independent', 'perfect', 'correlations', 'is', 'equivalent', 'to', 'a', 'graph', 'state', 'we', 'present', 'the', 'optimal', 'bell', 'inequalities', 'for', 'perfect', 'correlations', 'and', 'maximal', 'violation', 'for', 'all', 'classes', 'of', 'graph', 'states', 'with', 'n', '... | [-0.15410781737806306, 0.2139476327069073, -0.024886484563228537, 0.09212092208088238, -0.019205106162756194, -0.25388110777912815, 0.05518480710547845, 0.32611173470733595, -0.1833444027659306, -0.33890375752215746, 0.08028177797153103, -0.3455803700890697, -0.019381756985895945, 0.12570451859567985, 0.006798264631604... |
708.3209 | Relativistic Aberration for Accelerating Observers | We investigate the effects of the aberration of light for a uniformly
accelerating observer. The observer we consider is initially at rest with
respect to a luminous spherical object--a star, say--and then starts to move
away with constant acceleration. The main results we derive are the following:
(i) The observer a... | physics.class-ph gr-qc | we investigate the effects of the aberration of light for a uniformly accelerating observer the observer we consider is initially at rest with respect to a luminous spherical objecta star sayand then starts to move away with constant acceleration the main results we derive are the following i the observer always sees a... | [['we', 'investigate', 'the', 'effects', 'of', 'the', 'aberration', 'of', 'light', 'for', 'a', 'uniformly', 'accelerating', 'observer', 'the', 'observer', 'we', 'consider', 'is', 'initially', 'at', 'rest', 'with', 'respect', 'to', 'a', 'luminous', 'spherical', 'objecta', 'star', 'sayand', 'then', 'starts', 'to', 'move'... | [-0.1108590417063125, 0.1641787221754096, -0.08502934661852878, 0.0401768497547714, -0.08066936308041034, -0.14442917766197153, -0.00805274840790733, 0.38440010527421425, -0.23622697007291518, -0.27093722382113167, 0.116009130808468, -0.30012179137116707, -0.08379423969408224, 0.16119722985832796, -0.09377651608431223,... |
708.321 | Effects of fluctuation on alpha-omega dynamo models | We analyse the role of a fluctuating alpha-effect in alpha-omega dynamo
models, and show that there is a mechanism for magnetic field generation, valid
at large scale separation, deriving from the interaction of mean shear and a
fluctuating alpha-effect. It is shown that this effect can act as a dynamo even
in the ab... | astro-ph | we analyse the role of a fluctuating alphaeffect in alphaomega dynamo models and show that there is a mechanism for magnetic field generation valid at large scale separation deriving from the interaction of mean shear and a fluctuating alphaeffect it is shown that this effect can act as a dynamo even in the absence of ... | [['we', 'analyse', 'the', 'role', 'of', 'a', 'fluctuating', 'alphaeffect', 'in', 'alphaomega', 'dynamo', 'models', 'and', 'show', 'that', 'there', 'is', 'a', 'mechanism', 'for', 'magnetic', 'field', 'generation', 'valid', 'at', 'large', 'scale', 'separation', 'deriving', 'from', 'the', 'interaction', 'of', 'mean', 'she... | [-0.21807852716421172, 0.2436091092427912, -0.07615310608804839, 0.1425585959980596, -0.04318425426744435, -0.029782471077975957, -0.02345325430370357, 0.29644345691146917, -0.27084946675761923, -0.3119837781541968, 0.08833886747095376, -0.1907927658510943, -0.17298138249435857, 0.21298860457457908, 0.00042953542497468... |
708.3211 | Monte Carlo study of Bose Laughlin wave function for filling factors
1/2, 1/4 and 1/6 | Strongly correlated two-dimensional electronic systems subject to a
perpendicular magnetic field at lowest Landau level (LLL) filling factors: 1/2,
1/4 and 1/6 are believed to be composite fermion (CF) Fermi liquid phases. Even
though a Bose Laughlin wave function cannot describe these filling factors we
investigate ... | cond-mat.str-el cond-mat.mes-hall | strongly correlated twodimensional electronic systems subject to a perpendicular magnetic field at lowest landau level lll filling factors 12 14 and 16 are believed to be composite fermion cf fermi liquid phases even though a bose laughlin wave function cannot describe these filling factors we investigate whether such ... | [['strongly', 'correlated', 'twodimensional', 'electronic', 'systems', 'subject', 'to', 'a', 'perpendicular', 'magnetic', 'field', 'at', 'lowest', 'landau', 'level', 'lll', 'filling', 'factors', '12', '14', 'and', '16', 'are', 'believed', 'to', 'be', 'composite', 'fermion', 'cf', 'fermi', 'liquid', 'phases', 'even', 't... | [-0.14364843462100066, 0.2515459562825264, -0.06208318729116113, 0.14567686480645015, 0.026729737930374857, -0.18021432442228066, 0.11249838185484128, 0.3170540828707834, -0.18744726257161207, -0.3254757308269907, 0.00894998990533711, -0.29799042894636224, -0.06124682101302299, 0.13799920483123537, 0.07461415974098264,... |
708.3212 | A New Study of the Transition to Uniform Nuclear Matter in Neutron Stars
and Supernovae | A comprehensive microscopic study of the properties of bulk matter at
densities just below nuclear saturation $\rho_s = 2.5 \sim 10^{14}$ g
cm$^{-3}$, zero and finite temperature and high neutron fraction, is outlined,
and preliminary results presented. Such matter is expected to exist in the
inner crust of neutron s... | astro-ph nucl-th | a comprehensive microscopic study of the properties of bulk matter at densities just below nuclear saturation rho_s 25 sim 1014 g cm3 zero and finite temperature and high neutron fraction is outlined and preliminary results presented such matter is expected to exist in the inner crust of neutron stars and during the co... | [['a', 'comprehensive', 'microscopic', 'study', 'of', 'the', 'properties', 'of', 'bulk', 'matter', 'at', 'densities', 'just', 'below', 'nuclear', 'saturation', 'rho_s', '25', 'sim', '1014', 'g', 'cm3', 'zero', 'and', 'finite', 'temperature', 'and', 'high', 'neutron', 'fraction', 'is', 'outlined', 'and', 'preliminary', ... | [-0.08601939448033322, 0.311702880153402, -0.03033726147116452, 0.07989916877561538, -0.06385743637859333, -0.00951229458766394, 0.07997169606692967, 0.29704919231475374, -0.1363714528804431, -0.3860367395472331, 0.053262665629249493, -0.3242927306469102, 0.05828550978197304, 0.1597962265215875, 0.025439110187599895, -... |
708.3213 | Continuous Time Random Walks in periodic systems: fluid limit and
fractional differential equations on the circle | In this article, the continuous time random walk on the circle is studied. We
derive the corresponding generalized master equation and discuss the effects of
topology, especially important when Levy flights are allowed. Then, we work out
the fluid limit equation, formulated in terms of the periodic version of the
fra... | cond-mat.stat-mech | in this article the continuous time random walk on the circle is studied we derive the corresponding generalized master equation and discuss the effects of topology especially important when levy flights are allowed then we work out the fluid limit equation formulated in terms of the periodic version of the fractional ... | [['in', 'this', 'article', 'the', 'continuous', 'time', 'random', 'walk', 'on', 'the', 'circle', 'is', 'studied', 'we', 'derive', 'the', 'corresponding', 'generalized', 'master', 'equation', 'and', 'discuss', 'the', 'effects', 'of', 'topology', 'especially', 'important', 'when', 'levy', 'flights', 'are', 'allowed', 'th... | [-0.1330765701501685, 0.126481076761368, -0.07773821671383783, 0.10140438400866354, -0.05793416473795386, -0.13265384292120444, 0.03176700226852999, 0.33605725070571196, -0.25124067337361766, -0.21919831562349024, 0.1527240244890837, -0.2468975446515662, -0.22870170390781233, 0.20077031405149576, -0.06052155400188092, ... |
708.3214 | 3D N = 1 SYM Chern-Simons theory on the Lattice | We present a method to implement 3-dimensional N = 1 SUSY Yang-Mills theory
(a theory with two real supercharges containing gauge fields and an adjoint
Majorana fermion) on the lattice, including a way to implement the Chern-Simons
term present in this theory. At nonzero Chern-Simons number our implementation
suffers... | hep-lat hep-th | we present a method to implement 3dimensional n 1 susy yangmills theory a theory with two real supercharges containing gauge fields and an adjoint majorana fermion on the lattice including a way to implement the chernsimons term present in this theory at nonzero chernsimons number our implementation suffers from a sign... | [['we', 'present', 'a', 'method', 'to', 'implement', '3dimensional', 'n', '1', 'susy', 'yangmills', 'theory', 'a', 'theory', 'with', 'two', 'real', 'supercharges', 'containing', 'gauge', 'fields', 'and', 'an', 'adjoint', 'majorana', 'fermion', 'on', 'the', 'lattice', 'including', 'a', 'way', 'to', 'implement', 'the', '... | [-0.18504999287402893, 0.20864882884724684, -0.060890737573227174, 0.02496896023402297, -0.09728684825999544, -0.17010888035845342, -0.0027051848842750623, 0.31708245274103897, -0.19630253788885438, -0.29620372791644894, 0.06863915662522888, -0.2945792792435688, -0.2295239598702498, 0.08899870286754603, -0.028849251308... |
708.3215 | Cumulative hard X-ray spectrum of local AGN: a link to the cosmic X-ray
background | We determine the cumulative spectral energy distribution (SED) of local AGN
in the 3-300 keV band and compare it with the spectrum of the cosmic X-ray
background (CXB) in order to test the widely accepted paradigm that the CXB is
a superposition of AGN and to place constraints on AGN evolution. We performed
a stackin... | astro-ph | we determine the cumulative spectral energy distribution sed of local agn in the 3300 kev band and compare it with the spectrum of the cosmic xray background cxb in order to test the widely accepted paradigm that the cxb is a superposition of agn and to place constraints on agn evolution we performed a stacking analysi... | [['we', 'determine', 'the', 'cumulative', 'spectral', 'energy', 'distribution', 'sed', 'of', 'local', 'agn', 'in', 'the', '3300', 'kev', 'band', 'and', 'compare', 'it', 'with', 'the', 'spectrum', 'of', 'the', 'cosmic', 'xray', 'background', 'cxb', 'in', 'order', 'to', 'test', 'the', 'widely', 'accepted', 'paradigm', 't... | [-0.014328984912742483, 0.10881623501578967, -0.08478460612653999, 0.16724553584461332, -0.09096883237031651, -0.056178647289977325, 0.045001121185033036, 0.4879789385227949, -0.15757006334127688, -0.3675390549601842, 0.03993972387793969, -0.3417658614959066, 0.03448993280564653, 0.2093392091431379, 0.01559392431196063... |
708.3216 | Robust creation of arbitrary-sized Dicke states using a single laser
pulse | We propose a novel technique for the creation of maximally entangled
symmetric Dicke states in an ion trap using adiabatic passage, which requires
only a pair of chirped pulses from a single laser and is applicable to any
number of ions and excitations. By utilising a particular factorisation of the
Hilbert space for... | quant-ph | we propose a novel technique for the creation of maximally entangled symmetric dicke states in an ion trap using adiabatic passage which requires only a pair of chirped pulses from a single laser and is applicable to any number of ions and excitations by utilising a particular factorisation of the hilbert space for mul... | [['we', 'propose', 'a', 'novel', 'technique', 'for', 'the', 'creation', 'of', 'maximally', 'entangled', 'symmetric', 'dicke', 'states', 'in', 'an', 'ion', 'trap', 'using', 'adiabatic', 'passage', 'which', 'requires', 'only', 'a', 'pair', 'of', 'chirped', 'pulses', 'from', 'a', 'single', 'laser', 'and', 'is', 'applicabl... | [-0.11988469220252823, 0.19724952372368446, -0.04791387519181038, 0.054064606511100004, 0.01777512523081912, -0.16574830515722258, 0.061701598369096104, 0.4303100478270841, -0.2316163883841209, -0.2675786170885956, 0.048215620126987324, -0.22358165836719945, -0.07102311857969838, 0.2311799508989253, -0.0506309938402764... |
708.3217 | Dijet Cross Sections and Parton Densities in Diffractive DIS at HERA | Differential dijet cross sections in diffractive deep-inelastic scattering
are measured with the H1 detector at HERA using an integrated luminosity of
51.5 pb-1. The selected events are of the type ep --> eXY, where the system X
contains at least two jets and is well separated in rapidity from the low mass
proton dis... | hep-ex | differential dijet cross sections in diffractive deepinelastic scattering are measured with the h1 detector at hera using an integrated luminosity of 515 pb1 the selected events are of the type ep exy where the system x contains at least two jets and is well separated in rapidity from the low mass proton dissociation s... | [['differential', 'dijet', 'cross', 'sections', 'in', 'diffractive', 'deepinelastic', 'scattering', 'are', 'measured', 'with', 'the', 'h1', 'detector', 'at', 'hera', 'using', 'an', 'integrated', 'luminosity', 'of', '515', 'pb1', 'the', 'selected', 'events', 'are', 'of', 'the', 'type', 'ep', 'exy', 'where', 'the', 'syst... | [-0.018309105581279784, 0.18497709338644902, -0.1557480675433325, 0.1550947791319186, 0.0016848663545409165, -0.012049136140823714, -0.015193506464290109, 0.3783164505965143, -0.1823551275983494, -0.24459966401780509, -0.030233622584086767, -0.3859595203765273, 0.0883320637422907, 0.14025481073738935, 0.087264920811256... |
708.3218 | Fictitious Play in 3x3 Games: the transition between periodic and
chaotic behaviour | In the 60's Shapley provided an example of a two player fictitious game with
periodic behaviour. In this game, player $A$ aims to copy $B$'s behaviour and
player $B$ aims to play one ahead of player $A$. In this paper we generalize
Shapley's example by introducing an external parameter. We show that the
periodic beha... | math.DS | in the 60s shapley provided an example of a two player fictitious game with periodic behaviour in this game player a aims to copy bs behaviour and player b aims to play one ahead of player a in this paper we generalize shapleys example by introducing an external parameter we show that the periodic behaviour in shapleys... | [['in', 'the', '60s', 'shapley', 'provided', 'an', 'example', 'of', 'a', 'two', 'player', 'fictitious', 'game', 'with', 'periodic', 'behaviour', 'in', 'this', 'game', 'player', 'a', 'aims', 'to', 'copy', 'bs', 'behaviour', 'and', 'player', 'b', 'aims', 'to', 'play', 'one', 'ahead', 'of', 'player', 'a', 'in', 'this', 'p... | [-0.16651909423131517, 0.1143650765878309, -0.13327181074572236, 0.05955887584584869, -0.03700117565887539, -0.18030785030769783, 0.08555757410944118, 0.3520899875612374, -0.26076910275508436, -0.258976557008835, 0.09876610002104651, -0.27658877259376324, -0.22765466646013552, 0.12389472943365748, -0.10600761757967503,... |
708.3219 | Doppler Boosting, Superluminal Motion, and the Kinematics of AGN Jets | We discuss results from a decade long program to study the fine-scale
structure and the kinematics of relativistic AGN jets with the aim of better
understanding the acceleration and collimation of the relativistic plasma
forming AGN jets. From the observed distribution of brightness temperature,
apparent velocity, fl... | astro-ph | we discuss results from a decade long program to study the finescale structure and the kinematics of relativistic agn jets with the aim of better understanding the acceleration and collimation of the relativistic plasma forming agn jets from the observed distribution of brightness temperature apparent velocity flux den... | [['we', 'discuss', 'results', 'from', 'a', 'decade', 'long', 'program', 'to', 'study', 'the', 'finescale', 'structure', 'and', 'the', 'kinematics', 'of', 'relativistic', 'agn', 'jets', 'with', 'the', 'aim', 'of', 'better', 'understanding', 'the', 'acceleration', 'and', 'collimation', 'of', 'the', 'relativistic', 'plasm... | [-0.05893625562506107, 0.14866706330365942, -0.08160930077888463, 0.14055254407688617, -0.11171594263654888, -0.09282183559742152, -0.014153281203266886, 0.46817163100237386, -0.18764635323181242, -0.36387995881306234, 0.036315546348576616, -0.2677849482023974, 0.02528366403196726, 0.20488603613512965, -0.0131920012211... |
708.322 | Optimal strategies in the average consensus problem | We prove that for a set of communicating agents to compute the average of
their initial positions (average consensus problem), the optimal topology of
communication is given by a de Bruijn's graph. Consensus is then reached in a
finitely many steps. A more general family of strategies, constructed by block
Kronecker ... | cs.MA cs.NI math.OC | we prove that for a set of communicating agents to compute the average of their initial positions average consensus problem the optimal topology of communication is given by a de bruijns graph consensus is then reached in a finitely many steps a more general family of strategies constructed by block kronecker products ... | [['we', 'prove', 'that', 'for', 'a', 'set', 'of', 'communicating', 'agents', 'to', 'compute', 'the', 'average', 'of', 'their', 'initial', 'positions', 'average', 'consensus', 'problem', 'the', 'optimal', 'topology', 'of', 'communication', 'is', 'given', 'by', 'a', 'de', 'bruijns', 'graph', 'consensus', 'is', 'then', 'r... | [-0.19242730290605292, 0.08062165893488012, -0.08594277138048309, 0.057658049903446966, -0.043879055137888104, -0.1585394241610321, 0.08934488451755526, 0.4052225411317106, -0.3038037382697655, -0.2676366251435573, 0.1283095406301288, -0.2350614943494231, -0.1310468059392267, 0.14849862910144157, -0.11825067598088565, ... |
708.3221 | Transient and Highly Polarized Double-Peaked H-alpha Emission in the
Seyfert 2 Nucleus of NGC 2110 | We have discovered an extremely broad, double-peaked H-alpha emission line in
the polarized flux spectrum of NGC 2110, establishing that this well-studied
Seyfert 2 galaxy contains a disk-like hidden broad-line region (BLR). Several
properties of NGC 2110 suggest that it is an obscured twin of Arp 102B, the
prototypi... | astro-ph | we have discovered an extremely broad doublepeaked halpha emission line in the polarized flux spectrum of ngc 2110 establishing that this wellstudied seyfert 2 galaxy contains a disklike hidden broadline region blr several properties of ngc 2110 suggest that it is an obscured twin of arp 102b the prototypical doublepea... | [['we', 'have', 'discovered', 'an', 'extremely', 'broad', 'doublepeaked', 'halpha', 'emission', 'line', 'in', 'the', 'polarized', 'flux', 'spectrum', 'of', 'ngc', '2110', 'establishing', 'that', 'this', 'wellstudied', 'seyfert', '2', 'galaxy', 'contains', 'a', 'disklike', 'hidden', 'broadline', 'region', 'blr', 'severa... | [-0.023579418760283972, -0.044881875886872424, -0.06270985830531911, 0.14799579682889893, -0.122905843541055, -0.16485290507634365, -0.0151320615812212, 0.569369626484176, -0.05702092481213947, -0.2660385523949815, -0.011750087330601532, -0.27961900612238305, -0.026439119744035164, 0.20046978457578163, -0.0197249271876... |
708.3222 | On the consistency of coset space dimensional reduction | In this letter we consider higher-dimensional Yang-Mills theories and examine
their consistent coset space dimensional reduction. Utilizing a suitable ansatz
and imposing a simple set of constraints we determine the four-dimensional
gauge theory obtained from the reduction of both the higher-dimensional
Lagrangian an... | hep-th | in this letter we consider higherdimensional yangmills theories and examine their consistent coset space dimensional reduction utilizing a suitable ansatz and imposing a simple set of constraints we determine the fourdimensional gauge theory obtained from the reduction of both the higherdimensional lagrangian and the c... | [['in', 'this', 'letter', 'we', 'consider', 'higherdimensional', 'yangmills', 'theories', 'and', 'examine', 'their', 'consistent', 'coset', 'space', 'dimensional', 'reduction', 'utilizing', 'a', 'suitable', 'ansatz', 'and', 'imposing', 'a', 'simple', 'set', 'of', 'constraints', 'we', 'determine', 'the', 'fourdimensiona... | [-0.12301823740563123, 0.11254585927986227, -0.07664314094290603, 0.09221830638671236, -0.06122346268239198, -0.11170587331434945, 0.026906035009233165, 0.291882644087309, -0.20156119429157116, -0.26663527705386514, 0.11755134865052241, -0.22553244572191034, -0.16487076782505028, 0.15947044134372845, -0.068080890618148... |
708.3223 | Real Zeros and Normal Distribution for statistics on Stirling
permutations defined by Gessel and Stanley | We study Stirling permutations defined by Gessel and Stanley.
We prove that their generating function according to the number of descents
has real roots only. We use that fact to prove that the distribution of these
descents, and other, equidistributed statistics on these objects converge to a
normal distribution.
| math.CO math.PR | we study stirling permutations defined by gessel and stanley we prove that their generating function according to the number of descents has real roots only we use that fact to prove that the distribution of these descents and other equidistributed statistics on these objects converge to a normal distribution | [['we', 'study', 'stirling', 'permutations', 'defined', 'by', 'gessel', 'and', 'stanley', 'we', 'prove', 'that', 'their', 'generating', 'function', 'according', 'to', 'the', 'number', 'of', 'descents', 'has', 'real', 'roots', 'only', 'we', 'use', 'that', 'fact', 'to', 'prove', 'that', 'the', 'distribution', 'of', 'thes... | [-0.13661669732584636, 0.12635422368742982, -0.12679881823002076, 0.10695524373072751, -0.10524231288106922, -0.06343830220059168, 0.07307471319728968, 0.3615320573503874, -0.3053651912403958, -0.28755740045892947, 0.036233776809685696, -0.3030615318946692, -0.19985948159473435, 0.17754730178347353, -0.1511812714897856... |
708.3224 | The Frobenius Problem in a Free Monoid | The classical Frobenius problem is to compute the largest number g not
representable as a non-negative integer linear combination of non-negative
integers x_1, x_2, ..., x_k, where gcd(x_1, x_2, ..., x_k) = 1. In this paper
we consider generalizations of the Frobenius problem to the noncommutative
setting of a free m... | cs.DM math.CO | the classical frobenius problem is to compute the largest number g not representable as a nonnegative integer linear combination of nonnegative integers x_1 x_2 x_k where gcdx_1 x_2 x_k 1 in this paper we consider generalizations of the frobenius problem to the noncommutative setting of a free monoid unlike the commuta... | [['the', 'classical', 'frobenius', 'problem', 'is', 'to', 'compute', 'the', 'largest', 'number', 'g', 'not', 'representable', 'as', 'a', 'nonnegative', 'integer', 'linear', 'combination', 'of', 'nonnegative', 'integers', 'x_1', 'x_2', 'x_k', 'where', 'gcdx_1', 'x_2', 'x_k', '1', 'in', 'this', 'paper', 'we', 'consider',... | [-0.186609937828064, 0.09132325340779528, -0.04236634166982885, 0.0474815659227972, -0.11555621783750561, -0.17610005111409685, -0.04351491974039863, 0.3175753453650918, -0.38808785708477866, -0.19650141816013134, 0.07475030339824465, -0.29231103491455984, -0.13828975131484464, 0.1625212441311958, -0.14075225865086302,... |
708.3225 | Phase diagram of randomly pinned vortex matter in layered
superconductors: dependence on the details of the point pinning | We study the thermodynamic and structural properties of the superconducting
vortex system in high temperature layered superconductors, with magnetic field
normal to the layers, in the presence of a small concentration of strong random
point pinning defects via numerical minimization of a model free energy
functional ... | cond-mat.supr-con | we study the thermodynamic and structural properties of the superconducting vortex system in high temperature layered superconductors with magnetic field normal to the layers in the presence of a small concentration of strong random point pinning defects via numerical minimization of a model free energy functional in t... | [['we', 'study', 'the', 'thermodynamic', 'and', 'structural', 'properties', 'of', 'the', 'superconducting', 'vortex', 'system', 'in', 'high', 'temperature', 'layered', 'superconductors', 'with', 'magnetic', 'field', 'normal', 'to', 'the', 'layers', 'in', 'the', 'presence', 'of', 'a', 'small', 'concentration', 'of', 'st... | [-0.1493433311793592, 0.21650096130863167, -0.06337589283174933, 0.004916617209821551, -0.018441648306776838, -0.1070354765023925, 0.09318443583958755, 0.3661422808237596, -0.27589029882019805, -0.28503628533138936, 0.06825399805779513, -0.3007505986441636, -0.10037575116721607, 0.10911605259622517, 0.01373061811492375... |
708.3226 | A Dichotomy Theorem for General Minimum Cost Homomorphism Problem | In the constraint satisfaction problem ($CSP$), the aim is to find an
assignment of values to a set of variables subject to specified constraints. In
the minimum cost homomorphism problem ($MinHom$), one is additionally given
weights $c_{va}$ for every variable $v$ and value $a$, and the aim is to find
an assignment ... | cs.LG cs.CC | in the constraint satisfaction problem csp the aim is to find an assignment of values to a set of variables subject to specified constraints in the minimum cost homomorphism problem minhom one is additionally given weights c_va for every variable v and value a and the aim is to find an assignment f to the variables tha... | [['in', 'the', 'constraint', 'satisfaction', 'problem', 'csp', 'the', 'aim', 'is', 'to', 'find', 'an', 'assignment', 'of', 'values', 'to', 'a', 'set', 'of', 'variables', 'subject', 'to', 'specified', 'constraints', 'in', 'the', 'minimum', 'cost', 'homomorphism', 'problem', 'minhom', 'one', 'is', 'additionally', 'given'... | [-0.12253495026379824, 0.03798606902982544, -0.04992757584505643, 0.07158692750649956, -0.13366127304004458, -0.16364338035540035, 0.08227552089673014, 0.329418959243832, -0.3447771301636329, -0.3511114193795201, 0.09693961678660856, -0.2500492929591415, -0.10292841988699272, 0.1943055171842645, -0.15759460263264677, 0... |
708.3227 | Network formation and relaxation dynamics in a new model for colloidal
gelation | We investigate the gel formation from the equilibrium sol phase in a simple
model that has the characteristics of (colloidal) gel-forming systems at a
finite temperature. At low volume fraction and low temperatures, particles are
linked by long-living bonds and form an open percolating network. By means of
molecular ... | cond-mat.soft cond-mat.dis-nn | we investigate the gel formation from the equilibrium sol phase in a simple model that has the characteristics of colloidal gelforming systems at a finite temperature at low volume fraction and low temperatures particles are linked by longliving bonds and form an open percolating network by means of molecular dynamics ... | [['we', 'investigate', 'the', 'gel', 'formation', 'from', 'the', 'equilibrium', 'sol', 'phase', 'in', 'a', 'simple', 'model', 'that', 'has', 'the', 'characteristics', 'of', 'colloidal', 'gelforming', 'systems', 'at', 'a', 'finite', 'temperature', 'at', 'low', 'volume', 'fraction', 'and', 'low', 'temperatures', 'particl... | [-0.14638039888232016, 0.21575710555713157, -0.06943065974861383, 0.009314032544692357, 0.05264843016862869, -0.08513528733203808, 0.07668178617954254, 0.36788238150378066, -0.29404410723596813, -0.2637797844906648, 0.06346955272989968, -0.2930474925537904, -0.1415909531371047, 0.08476594021854301, 0.04468347133447727,... |
708.3228 | Coxeter multiarrangements with quasi-constant multiplicities | We study structures of derivation modules of Coxeter multiarrangements with
quasi-constant multiplicities by using the primitive derivation. As an
application, we show that the characteristic polynomial of a Coxeter
multiarrangement with quasi-constant multiplicity is combinatorially
computable.
| math.CO math.AC | we study structures of derivation modules of coxeter multiarrangements with quasiconstant multiplicities by using the primitive derivation as an application we show that the characteristic polynomial of a coxeter multiarrangement with quasiconstant multiplicity is combinatorially computable | [['we', 'study', 'structures', 'of', 'derivation', 'modules', 'of', 'coxeter', 'multiarrangements', 'with', 'quasiconstant', 'multiplicities', 'by', 'using', 'the', 'primitive', 'derivation', 'as', 'an', 'application', 'we', 'show', 'that', 'the', 'characteristic', 'polynomial', 'of', 'a', 'coxeter', 'multiarrangement'... | [-0.18782971426844597, 0.11273260242928194, -0.1281026749768191, 0.01851268015970062, -0.1062603173777461, -0.10700526334241861, -0.08040469996760496, 0.32730042230751777, -0.3542789285485115, -0.2125578113288308, 0.03772908591458367, -0.2142470246180892, -0.18613863964047697, 0.2193742930119495, -0.12106476837976111, ... |
708.3229 | Ballistic vs Diffusive Transport in Current-Induced Magnetization
Switching | We test whether current-induced magnetization switching due to
spin-transfer-torque in ferromagnetic/non-magnetic/ferromagnetic (F/N/F)
trilayers changes significantly when scattering within the N-metal layers is
changed from ballistic to diffusive. Here ballistic corresponds to a ratio r =
lambda/t greater than or e... | cond-mat.mtrl-sci | we test whether currentinduced magnetization switching due to spintransfertorque in ferromagneticnonmagneticferromagnetic fnf trilayers changes significantly when scattering within the nmetal layers is changed from ballistic to diffusive here ballistic corresponds to a ratio r lambdat greater than or equal to 3 for a c... | [['we', 'test', 'whether', 'currentinduced', 'magnetization', 'switching', 'due', 'to', 'spintransfertorque', 'in', 'ferromagneticnonmagneticferromagnetic', 'fnf', 'trilayers', 'changes', 'significantly', 'when', 'scattering', 'within', 'the', 'nmetal', 'layers', 'is', 'changed', 'from', 'ballistic', 'to', 'diffusive',... | [-0.11874476129365764, 0.20882391454330806, 0.05314122581581489, 0.00689844497487527, -0.04897245351056536, -0.22620102820982194, 0.09903155193575819, 0.40503312685880166, -0.2729246620217274, -0.29205079834330183, -0.00972605990306153, -0.33976960270505013, -0.04644430657358969, 0.1816579578625006, 0.03058532368720926... |
708.323 | Can Alice and Bob be random: a study on human playing zero knowledge
protocols | The research described in this abstract was initiated by discussions between
the author and Giovanni Di Crescenzo in Barcelona in early 2004. It was during
Advanced Course on Contemporary Cryptology that Di Crescenzo gave a course on
zero knowledge protocols (ZKP), see [1]. After that course we started to play
with u... | cs.CR cs.CY | the research described in this abstract was initiated by discussions between the author and giovanni di crescenzo in barcelona in early 2004 it was during advanced course on contemporary cryptology that di crescenzo gave a course on zero knowledge protocols zkp see 1 after that course we started to play with unorthodox... | [['the', 'research', 'described', 'in', 'this', 'abstract', 'was', 'initiated', 'by', 'discussions', 'between', 'the', 'author', 'and', 'giovanni', 'di', 'crescenzo', 'in', 'barcelona', 'in', 'early', '2004', 'it', 'was', 'during', 'advanced', 'course', 'on', 'contemporary', 'cryptology', 'that', 'di', 'crescenzo', 'ga... | [-0.06061016855070765, 0.08863650730109951, -0.12124332995227541, 0.07746088384451826, -0.07903506092235363, -0.16706470238421572, 0.021779471537454076, 0.34757515241841924, -0.15366698143836321, -0.34539698159552357, 0.14421329761494286, -0.25533183498747564, -0.16437330205788772, 0.2004025262938106, -0.12972658552920... |
708.3231 | Current-induced torques due to compensated antiferromagnets | We analyse the influence of current induced torques on the magnetization
configuration of a ferromagnet in a circuit containing a compensated
antiferromagnet. We argue that these torques are generically non-zero and
support this conclusion with a microscopic NEGF calculation for a circuit
containing antiferromagnetic... | cond-mat.mes-hall | we analyse the influence of current induced torques on the magnetization configuration of a ferromagnet in a circuit containing a compensated antiferromagnet we argue that these torques are generically nonzero and support this conclusion with a microscopic negf calculation for a circuit containing antiferromagnetic nim... | [['we', 'analyse', 'the', 'influence', 'of', 'current', 'induced', 'torques', 'on', 'the', 'magnetization', 'configuration', 'of', 'a', 'ferromagnet', 'in', 'a', 'circuit', 'containing', 'a', 'compensated', 'antiferromagnet', 'we', 'argue', 'that', 'these', 'torques', 'are', 'generically', 'nonzero', 'and', 'support', ... | [-0.23401725707538767, 0.15368099542470967, -0.026044528193135814, 0.018914518666328727, -0.10021980643476837, -0.07152184325542937, 0.07129389761447362, 0.38200792956461266, -0.24177258317472367, -0.2801102871847589, -0.004175898630353735, -0.30419008120349267, -0.13928206701104234, 0.18236905240976228, 0.071969362202... |
708.3232 | Complexity results for CR mappings between spheres | Using elementary number theory, we prove several results about the complexity
of CR mappings between spheres. It is known that CR mappings between spheres,
invariant under finite groups, lead to sharp bounds for degree estimates on
real polynomials constant on a hyperplane. We show here that there are
infinitely many... | math.CV math.NT | using elementary number theory we prove several results about the complexity of cr mappings between spheres it is known that cr mappings between spheres invariant under finite groups lead to sharp bounds for degree estimates on real polynomials constant on a hyperplane we show here that there are infinitely many degree... | [['using', 'elementary', 'number', 'theory', 'we', 'prove', 'several', 'results', 'about', 'the', 'complexity', 'of', 'cr', 'mappings', 'between', 'spheres', 'it', 'is', 'known', 'that', 'cr', 'mappings', 'between', 'spheres', 'invariant', 'under', 'finite', 'groups', 'lead', 'to', 'sharp', 'bounds', 'for', 'degree', '... | [-0.15170957800932228, 0.0738146972109098, -0.08305609511211515, 0.12732028551166877, -0.08190558608155697, -0.14809021255467086, 0.05334394131670706, 0.3618510918971151, -0.28608449656516316, -0.26232653206214307, 0.08040034185629338, -0.2838713499577716, -0.196885568863363, 0.24777762373909354, -0.09523965341504663, ... |
708.3233 | Sakai-Sugimoto model, Tachyon Condensation and Chiral symmetry Breaking | We modify the Sakai-Sugimoto model of chiral symmetry breaking to take into
account the open string tachyon which stretches between the flavour D8-branes
and anti D8-branes. There are several reasons of consistency for doing this:
(i) Even if it might be reasonable to ignore the tachyon in the ultraviolet
where the f... | hep-th | we modify the sakaisugimoto model of chiral symmetry breaking to take into account the open string tachyon which stretches between the flavour d8branes and anti d8branes there are several reasons of consistency for doing this i even if it might be reasonable to ignore the tachyon in the ultraviolet where the flavour br... | [['we', 'modify', 'the', 'sakaisugimoto', 'model', 'of', 'chiral', 'symmetry', 'breaking', 'to', 'take', 'into', 'account', 'the', 'open', 'string', 'tachyon', 'which', 'stretches', 'between', 'the', 'flavour', 'd8branes', 'and', 'anti', 'd8branes', 'there', 'are', 'several', 'reasons', 'of', 'consistency', 'for', 'doi... | [-0.13501381308716887, 0.22898134834009826, -0.0824717084548491, 0.12758123128442095, -0.1091143803397084, -0.1732836121474119, 0.024413537094369532, 0.3184210094390437, -0.19864982931929476, -0.2434582664631307, 0.05325630053412169, -0.2788935992962626, -0.0780322008245789, 0.0278947759012226, -0.014082933069371126, 0... |
708.3234 | The Repetition Property for Sequences on Tori Generated by Polynomials
or Skew-Shifts | The repetition property of a sequence in a metric space, a notion introduced
by us in an earlier paper, is of importance in the spectral analysis of ergodic
Schr\"odinger operators. It may be used to exclude eigenvalues for such
operators. In this paper we study the question of when a sequence on a torus
that is gene... | math.DS math.CA | the repetition property of a sequence in a metric space a notion introduced by us in an earlier paper is of importance in the spectral analysis of ergodic schrodinger operators it may be used to exclude eigenvalues for such operators in this paper we study the question of when a sequence on a torus that is generated by... | [['the', 'repetition', 'property', 'of', 'a', 'sequence', 'in', 'a', 'metric', 'space', 'a', 'notion', 'introduced', 'by', 'us', 'in', 'an', 'earlier', 'paper', 'is', 'of', 'importance', 'in', 'the', 'spectral', 'analysis', 'of', 'ergodic', 'schrodinger', 'operators', 'it', 'may', 'be', 'used', 'to', 'exclude', 'eigenv... | [-0.13903686837450172, 0.11612986159406921, -0.1168993359766482, 0.06034554099517592, -0.052964504753249916, -0.09552246613134996, 0.028240401742540385, 0.38508109532798945, -0.23338643409144344, -0.20855648783715755, 0.12169907133231002, -0.2630536029314141, -0.16870686982423486, 0.20715425291956727, -0.11230228599056... |
708.3235 | Does Planck mass run on the cosmological horizon scale? | Einstein's theory of general relativity, which contains a universal value of
the Planck mass, has been so far successfully invoked to explain gravitational
dynamics from sub-millimeter scales to the scale of the cosmological horizon.
However, one may envisage that in alternative theories of gravity, the
effective val... | astro-ph gr-qc hep-th | einsteins theory of general relativity which contains a universal value of the planck mass has been so far successfully invoked to explain gravitational dynamics from submillimeter scales to the scale of the cosmological horizon however one may envisage that in alternative theories of gravity the effective value of the... | [['einsteins', 'theory', 'of', 'general', 'relativity', 'which', 'contains', 'a', 'universal', 'value', 'of', 'the', 'planck', 'mass', 'has', 'been', 'so', 'far', 'successfully', 'invoked', 'to', 'explain', 'gravitational', 'dynamics', 'from', 'submillimeter', 'scales', 'to', 'the', 'scale', 'of', 'the', 'cosmological'... | [-0.12051866689903869, 0.13565359548449998, -0.12441394518095034, 0.12704850846504862, -0.14950587003043406, -0.10269553952815907, -0.05419473674717463, 0.26062855138788343, -0.2461482776466895, -0.3398178875791254, 0.11554905419082691, -0.245688930853201, -0.08404132689832261, 0.18495418627151392, -0.03295616635759534... |
708.3236 | Flux locking a superfluid interferometer | We demonstrate a flux locking technique using injected heat current to
linearize the output of a superfluid helium-4 interferometer. A rotation flux
through the interferometer loop produces a shift in the phase of the superfluid
order parameter. This shift is nullified via negative feedback by a phase-shift
caused by... | cond-mat.other | we demonstrate a flux locking technique using injected heat current to linearize the output of a superfluid helium4 interferometer a rotation flux through the interferometer loop produces a shift in the phase of the superfluid order parameter this shift is nullified via negative feedback by a phaseshift caused by the i... | [['we', 'demonstrate', 'a', 'flux', 'locking', 'technique', 'using', 'injected', 'heat', 'current', 'to', 'linearize', 'the', 'output', 'of', 'a', 'superfluid', 'helium4', 'interferometer', 'a', 'rotation', 'flux', 'through', 'the', 'interferometer', 'loop', 'produces', 'a', 'shift', 'in', 'the', 'phase', 'of', 'the', ... | [-0.21458124864147976, 0.23287959619483445, -0.07889676885679364, 0.01608562593719398, -0.0818611634458648, -0.09847498578892555, 0.12309911864576861, 0.33344914217013866, -0.28840881562791765, -0.28701837685366627, 0.052077673562962445, -0.24461748043540865, -0.08310114993946627, 0.23454673402011395, -0.01343732670648... |
708.3237 | Braneworld dynamics in Einstein-Gauss-Bonnet gravity | We discuss the cosmological evolution of a braneworld in five dimensional
Gauss-Bonnet gravity. Our discussion allows the fifth (bulk) dimension to be
space-like as well as time-like. The resulting equations of motion have the
form of a cubic equation in the (H^2,(\rho+\sigma)^2) plane, where \sigma is
the brane tens... | gr-qc astro-ph hep-ph | we discuss the cosmological evolution of a braneworld in five dimensional gaussbonnet gravity our discussion allows the fifth bulk dimension to be spacelike as well as timelike the resulting equations of motion have the form of a cubic equation in the h2rhosigma2 plane where sigma is the brane tension and rho is the ma... | [['we', 'discuss', 'the', 'cosmological', 'evolution', 'of', 'a', 'braneworld', 'in', 'five', 'dimensional', 'gaussbonnet', 'gravity', 'our', 'discussion', 'allows', 'the', 'fifth', 'bulk', 'dimension', 'to', 'be', 'spacelike', 'as', 'well', 'as', 'timelike', 'the', 'resulting', 'equations', 'of', 'motion', 'have', 'th... | [-0.15330976998205664, 0.11655582140095988, -0.14624845510241474, 0.09418995081021604, -0.14201533654034673, -0.14328215351301454, -0.04744244112445564, 0.2668995550438333, -0.19565494856822285, -0.2471271609190664, 0.08193277185632036, -0.2598047267426586, -0.06689281856453569, 0.13461165312382814, -0.0243899029021724... |
708.3238 | How well do we know the Unitarity Triangle? An experimental review | In the past 10 years our knowledge of the parameters rho and eta of the
Cabibbo-Kobayashi-Maskawa matrix has improved substantially. This article
reviews the measurements that contributed to this advance, and discusses their
implication in terms of understanding CP violation in the Standard Model and
beyond.
| hep-ex | in the past 10 years our knowledge of the parameters rho and eta of the cabibbokobayashimaskawa matrix has improved substantially this article reviews the measurements that contributed to this advance and discusses their implication in terms of understanding cp violation in the standard model and beyond | [['in', 'the', 'past', '10', 'years', 'our', 'knowledge', 'of', 'the', 'parameters', 'rho', 'and', 'eta', 'of', 'the', 'cabibbokobayashimaskawa', 'matrix', 'has', 'improved', 'substantially', 'this', 'article', 'reviews', 'the', 'measurements', 'that', 'contributed', 'to', 'this', 'advance', 'and', 'discusses', 'their'... | [-0.07114327082450947, 0.1014492538575407, -0.03522563282825539, -0.006658265028027413, -0.052320844574790935, -0.04720631638622802, 0.10349967816601628, 0.26010643075341766, -0.25054092510886816, -0.34349071323547675, 0.08607829595237727, -0.2868410050970219, -0.13637653216415935, 0.17257919619568501, -0.0597951650902... |
708.3239 | Electron-Electron Interactions in Graphene | We discuss the validity (or not) of the ring-diagram approximation (i.e. RPA)
in the calculation of graphene self-energy in the weak-coupling ($r_s \ll 1$)
limit, showing that RPA is a controlled and valid approximation for
\textit{extrinsic} graphene where the Fermi level is away from the Dirac point.
| cond-mat.mtrl-sci cond-mat.mes-hall | we discuss the validity or not of the ringdiagram approximation ie rpa in the calculation of graphene selfenergy in the weakcoupling r_s ll 1 limit showing that rpa is a controlled and valid approximation for textitextrinsic graphene where the fermi level is away from the dirac point | [['we', 'discuss', 'the', 'validity', 'or', 'not', 'of', 'the', 'ringdiagram', 'approximation', 'ie', 'rpa', 'in', 'the', 'calculation', 'of', 'graphene', 'selfenergy', 'in', 'the', 'weakcoupling', 'r_s', 'll', '1', 'limit', 'showing', 'that', 'rpa', 'is', 'a', 'controlled', 'and', 'valid', 'approximation', 'for', 'tex... | [-0.13032557713323395, 0.12784308630406208, -0.07526108581046372, 0.08957747881725917, 0.039931180937539626, -0.12181953833762395, 0.1644500316242161, 0.3153011567850152, -0.21972278861895853, -0.19589340836619554, -0.026256809896870476, -0.34855089018769236, -0.09525164654579661, 0.1549329864539449, 0.0614298689103199... |
708.324 | The growth of luminous red galaxies by merging | We study the role of major and minor mergers in the mass growth of luminous
red galaxies. We present small-scale ($0.01<r<8\,\hMpc$) projected
cross-correlation functions of $23043$ luminous early-type galaxies from the
Sloan Digital Sky Survey (SDSS) Luminous Red Galaxy (LRG) sample
($0.16<z<0.30$, $\MMi\approx -22.... | astro-ph | we study the role of major and minor mergers in the mass growth of luminous red galaxies we present smallscale 001r8hmpc projected crosscorrelation functions of 23043 luminous earlytype galaxies from the sloan digital sky survey sdss luminous red galaxy lrg sample 016z030 mmiapprox 2275mag with all their companions in ... | [['we', 'study', 'the', 'role', 'of', 'major', 'and', 'minor', 'mergers', 'in', 'the', 'mass', 'growth', 'of', 'luminous', 'red', 'galaxies', 'we', 'present', 'smallscale', '001r8hmpc', 'projected', 'crosscorrelation', 'functions', 'of', '23043', 'luminous', 'earlytype', 'galaxies', 'from', 'the', 'sloan', 'digital', '... | [-0.05032711725646361, 0.08644270385372471, -0.08642398532236682, 0.12117814102686254, -0.11539601568480837, -0.029119644384319382, 0.02918843668413575, 0.4473423780484056, -0.11410841999587557, -0.31363567258525005, 0.028905289525036106, -0.3784081941095694, -0.04779951591049909, 0.22406079543712246, -0.00383433939150... |
708.3241 | Supersolid Bose-Fermi Mixtures in Optical Lattices | We study a mixture of strongly interacting bosons and spinless fermions with
on-site repulsion in a three-dimensional optical lattice. For this purpose we
develop and apply a generalized DMFT scheme, which is exact in infinite
dimensions and reliably describes the full range from weak to strong coupling.
We restrict ... | cond-mat.other | we study a mixture of strongly interacting bosons and spinless fermions with onsite repulsion in a threedimensional optical lattice for this purpose we develop and apply a generalized dmft scheme which is exact in infinite dimensions and reliably describes the full range from weak to strong coupling we restrict ourselv... | [['we', 'study', 'a', 'mixture', 'of', 'strongly', 'interacting', 'bosons', 'and', 'spinless', 'fermions', 'with', 'onsite', 'repulsion', 'in', 'a', 'threedimensional', 'optical', 'lattice', 'for', 'this', 'purpose', 'we', 'develop', 'and', 'apply', 'a', 'generalized', 'dmft', 'scheme', 'which', 'is', 'exact', 'in', 'i... | [-0.219058121026484, 0.2688946064427188, -0.011445416886474668, 0.14207252221225194, -0.015282176012538144, -0.20981191684367115, 0.07602456033220227, 0.3418159669783619, -0.19633859112263494, -0.17587085456596976, -0.010545741837500528, -0.3189796134301452, -0.09139429946842882, 0.05707819233696485, 0.1280141560379991... |
708.3242 | Multi-Dimensional Simulations for Early Phase Spectra of Aspherical
Hypernovae: SN 1998bw and Off-Axis Hypernovae | Early phase optical spectra of aspherical jet-like supernovae (SNe) are
presented. We focus on energetic core-collapse SNe, or hypernovae. Based on
hydrodynamic and nucleosynthetic models, radiative transfer in SN atmosphere is
solved with a multi-dimensional Monte-Carlo radiative transfer code, SAMURAI.
Since the lu... | astro-ph | early phase optical spectra of aspherical jetlike supernovae sne are presented we focus on energetic corecollapse sne or hypernovae based on hydrodynamic and nucleosynthetic models radiative transfer in sn atmosphere is solved with a multidimensional montecarlo radiative transfer code samurai since the luminosity is bo... | [['early', 'phase', 'optical', 'spectra', 'of', 'aspherical', 'jetlike', 'supernovae', 'sne', 'are', 'presented', 'we', 'focus', 'on', 'energetic', 'corecollapse', 'sne', 'or', 'hypernovae', 'based', 'on', 'hydrodynamic', 'and', 'nucleosynthetic', 'models', 'radiative', 'transfer', 'in', 'sn', 'atmosphere', 'is', 'solv... | [-0.051744665069889055, 0.14610096566423583, -0.022518507643219304, 0.14060958193080939, -0.0929264284321107, -0.14616914386587107, -0.021847493629491725, 0.49784957711201383, -0.1999403152450481, -0.2976716781168601, 0.02217601690961815, -0.31804800769862007, 0.02528040289248833, 0.20711709307506682, 0.013465720662968... |
708.3243 | Large-Scale Gravitational Instability and Star Formation in the Large
Magellanic Cloud | Large-scale star formation in disk galaxies is hypothesized to be driven by
global gravitational instability. The observed gas surface density is commonly
used to compute the strength of gravitational instability, but according to
this criterion star formation often appears to occur in gravitationally stable
regions.... | astro-ph | largescale star formation in disk galaxies is hypothesized to be driven by global gravitational instability the observed gas surface density is commonly used to compute the strength of gravitational instability but according to this criterion star formation often appears to occur in gravitationally stable regions one p... | [['largescale', 'star', 'formation', 'in', 'disk', 'galaxies', 'is', 'hypothesized', 'to', 'be', 'driven', 'by', 'global', 'gravitational', 'instability', 'the', 'observed', 'gas', 'surface', 'density', 'is', 'commonly', 'used', 'to', 'compute', 'the', 'strength', 'of', 'gravitational', 'instability', 'but', 'according... | [-0.1252288749220959, 0.12573309019488754, -0.07254427016230684, 0.12422000326905938, -0.08720287717598017, -0.025194309724391854, 0.023449232986655518, 0.33138738778518073, -0.1999036236689543, -0.32155382120279813, 0.06439047757110292, -0.24153731537874013, -0.07557891586318088, 0.16245615041005101, -0.01140921790826... |
708.3244 | About the Power to Enforce and Prevent Consensus by Manipulating
Communication Rules | We explore the possibilities of enforcing and preventing consensus in
continuous opinion dynamics that result from modifications in the communication
rules. We refer to the model of Weisbuch and Deffuant, where $n$ agents adjust
their continuous opinions as a result of random pairwise encounters whenever
their opinio... | physics.soc-ph | we explore the possibilities of enforcing and preventing consensus in continuous opinion dynamics that result from modifications in the communication rules we refer to the model of weisbuch and deffuant where n agents adjust their continuous opinions as a result of random pairwise encounters whenever their opinions dif... | [['we', 'explore', 'the', 'possibilities', 'of', 'enforcing', 'and', 'preventing', 'consensus', 'in', 'continuous', 'opinion', 'dynamics', 'that', 'result', 'from', 'modifications', 'in', 'the', 'communication', 'rules', 'we', 'refer', 'to', 'the', 'model', 'of', 'weisbuch', 'and', 'deffuant', 'where', 'n', 'agents', '... | [-0.13794555302910172, 0.1376349829706712, -0.08967968339036479, 0.08268273527230803, -0.10465865429287767, -0.18279567600108718, 0.13875118146459595, 0.40621083017473963, -0.26732821962950637, -0.3194829506084535, 0.09277807412364507, -0.2441764677636396, -0.1585451146130896, 0.11895650921177596, -0.11052164947393381,... |
708.3245 | Surface modes and breathers in finite arrays of nonlinear waveguides | We present the complete set of symmetric and antisymmetric (edge and corner)
surface modes in finite one-- and two--dimensional arrays of waveguides. We
provide classification of the modes based on the anti-continuum limit, study
their stability and bifurcations, and discuss relation between surface and bulk
modes. W... | cond-mat.other nlin.PS | we present the complete set of symmetric and antisymmetric edge and corner surface modes in finite one and twodimensional arrays of waveguides we provide classification of the modes based on the anticontinuum limit study their stability and bifurcations and discuss relation between surface and bulk modes we put forward... | [['we', 'present', 'the', 'complete', 'set', 'of', 'symmetric', 'and', 'antisymmetric', 'edge', 'and', 'corner', 'surface', 'modes', 'in', 'finite', 'one', 'and', 'twodimensional', 'arrays', 'of', 'waveguides', 'we', 'provide', 'classification', 'of', 'the', 'modes', 'based', 'on', 'the', 'anticontinuum', 'limit', 'stu... | [-0.2174806349700497, 0.13814326580764064, -0.06261578329928941, 0.02184812225882084, -0.07882822864508678, -0.12728697198232816, 0.07968612528601361, 0.3673454486734925, -0.19635016239819028, -0.21353782473071928, 0.14114954372710217, -0.30923378411980884, -0.16649031224885896, 0.1526814317330718, 0.042461391181624945... |
708.3246 | Transversity quark distributions in a covariant quark-diquark model | Transversity quark light-cone momentum distributions are calculated for the
nucleon. We utilize a modified Nambu--Jona-Lasinio model in which confinement
is simulated by eliminating unphysical thresholds for nucleon decay into
quarks. The nucleon bound state is obtained by solving the relativistic Faddeev
equation in... | hep-ph | transversity quark lightcone momentum distributions are calculated for the nucleon we utilize a modified nambujonalasinio model in which confinement is simulated by eliminating unphysical thresholds for nucleon decay into quarks the nucleon bound state is obtained by solving the relativistic faddeev equation in the qua... | [['transversity', 'quark', 'lightcone', 'momentum', 'distributions', 'are', 'calculated', 'for', 'the', 'nucleon', 'we', 'utilize', 'a', 'modified', 'nambujonalasinio', 'model', 'in', 'which', 'confinement', 'is', 'simulated', 'by', 'eliminating', 'unphysical', 'thresholds', 'for', 'nucleon', 'decay', 'into', 'quarks',... | [-0.025522862954877636, 0.24340260720395662, -0.12892370812713783, 0.15456263950228336, -0.08411317633246963, -0.0900501508731395, 0.04133157546760792, 0.37094237828785753, -0.088109023477684, -0.23202161368061888, -0.12001720384788758, -0.3006976668901266, -0.027561580356051947, 0.07735587692908705, 0.0803981068980028... |
708.3247 | A new integrable generalization of the Korteweg - de Vries equation | A new integrable sixth-order nonlinear wave equation is discovered by means
of the Painleve analysis, which is equivalent to the Korteweg - de Vries
equation with a source. A Lax representation and a Backlund self-transformation
are found of the new equation, and its travelling wave solutions and
generalized symmetri... | nlin.SI math-ph math.AP math.MP nlin.PS | a new integrable sixthorder nonlinear wave equation is discovered by means of the painleve analysis which is equivalent to the korteweg de vries equation with a source a lax representation and a backlund selftransformation are found of the new equation and its travelling wave solutions and generalized symmetries are st... | [['a', 'new', 'integrable', 'sixthorder', 'nonlinear', 'wave', 'equation', 'is', 'discovered', 'by', 'means', 'of', 'the', 'painleve', 'analysis', 'which', 'is', 'equivalent', 'to', 'the', 'korteweg', 'de', 'vries', 'equation', 'with', 'a', 'source', 'a', 'lax', 'representation', 'and', 'a', 'backlund', 'selftransforma... | [-0.19106373730488596, 0.033793315177365224, -0.1041583025409859, 0.10664375051285843, -0.20843785704702747, -0.20451208434960977, -0.11791439354419708, 0.2135743831797522, -0.3017789580840237, -0.1967811404385281, 0.13071971199456223, -0.34476488807751815, -0.21028739031480284, 0.15962446087553184, 0.04689457647654475... |
708.3248 | Electroweak Symmetry Breaking in the E6SSM | The Exceptional Supersymmetric Standard Model (E6SSM) is an E6 inspired model
with an extra gauged U(1) symmetry, which solves the mu-problem in a similar
way to the NMSSM but without the accompanying problems of singlet tadpoles or
domain walls. It predicts new exotic particles at the TeV scale. We investigate
the R... | hep-ph | the exceptional supersymmetric standard model e6ssm is an e6 inspired model with an extra gauged u1 symmetry which solves the muproblem in a similar way to the nmssm but without the accompanying problems of singlet tadpoles or domain walls it predicts new exotic particles at the tev scale we investigate the renormalisa... | [['the', 'exceptional', 'supersymmetric', 'standard', 'model', 'e6ssm', 'is', 'an', 'e6', 'inspired', 'model', 'with', 'an', 'extra', 'gauged', 'u1', 'symmetry', 'which', 'solves', 'the', 'muproblem', 'in', 'a', 'similar', 'way', 'to', 'the', 'nmssm', 'but', 'without', 'the', 'accompanying', 'problems', 'of', 'singlet'... | [-0.10142301844061467, 0.21481081092333829, -0.07410893536413486, 0.18395086732206425, -0.1294776245721438, -0.21408381751539668, -0.018341864404279026, 0.33128370060009904, -0.22368063095412896, -0.3494297234404288, 0.0737453137349149, -0.24103574750924042, -0.04794483352714124, 0.06680647043767647, 0.0098311929764707... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.