id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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710.0053 | High-sensitivity imaging with multi-mode twin beams | Twin entangled beams produced by single-pass parametric down-conversion (PDC)
offer the opportunity to detect weak amount of absorption with an improved
sensitivity with respect to standard techniques which make use of classical
light sources. We propose a differential measurement scheme which exploits the
spatial qu... | quant-ph | twin entangled beams produced by singlepass parametric downconversion pdc offer the opportunity to detect weak amount of absorption with an improved sensitivity with respect to standard techniques which make use of classical light sources we propose a differential measurement scheme which exploits the spatial quantum c... | [['twin', 'entangled', 'beams', 'produced', 'by', 'singlepass', 'parametric', 'downconversion', 'pdc', 'offer', 'the', 'opportunity', 'to', 'detect', 'weak', 'amount', 'of', 'absorption', 'with', 'an', 'improved', 'sensitivity', 'with', 'respect', 'to', 'standard', 'techniques', 'which', 'make', 'use', 'of', 'classical... | [-0.058830030877994544, 0.11257453748123171, -0.08213383665502962, 0.05816000697390635, -0.09516323058963266, -0.19358699906394997, 0.09691085161140828, 0.39651577574993246, -0.2956769340185087, -0.31662265122120975, 0.041586713519628477, -0.2485123478404399, -0.0321122666459475, 0.22642996326200107, -0.063822441227011... |
710.0054 | Coupled nanopillar waveguides: optical properties and applications | In this paper we review basic properties of coupled periodic and aperiodic
nanopillar waveguides. A coupled nanopillar waveguide consists of several rows
of periodically or aperiodically placed dielectric rods (pillars). In such a
waveguide, light confinement is due to the total internal reflection, while
guided mode... | physics.optics cond-mat.mes-hall | in this paper we review basic properties of coupled periodic and aperiodic nanopillar waveguides a coupled nanopillar waveguide consists of several rows of periodically or aperiodically placed dielectric rods pillars in such a waveguide light confinement is due to the total internal reflection while guided modes disper... | [['in', 'this', 'paper', 'we', 'review', 'basic', 'properties', 'of', 'coupled', 'periodic', 'and', 'aperiodic', 'nanopillar', 'waveguides', 'a', 'coupled', 'nanopillar', 'waveguide', 'consists', 'of', 'several', 'rows', 'of', 'periodically', 'or', 'aperiodically', 'placed', 'dielectric', 'rods', 'pillars', 'in', 'such... | [-0.20373951497798165, 0.18343306673069795, 0.024950481913983823, -0.0963208613715445, -0.08734188660979271, -0.16051839511220653, -0.0024711435521021486, 0.5146570011352499, -0.2615944715340932, -0.2557602558284998, 0.07838303168304264, -0.30975123138477406, -0.17602543078052502, 0.1819830957520753, -0.012938617536177... |
710.0055 | Periodic solutions for a class of singulary perturbated systems | In this paper we provide conditions to ensure the existence, for $e>0$
sufficiently small, of periodic solutions of given period $T>0$ in a prescribed
domain $U$ for a class of singularly perturbed first order differential
systems. Here $e>0$ is the perturbation parameter. Our approach, based on the
topological degre... | math.CA | in this paper we provide conditions to ensure the existence for e0 sufficiently small of periodic solutions of given period t0 in a prescribed domain u for a class of singularly perturbed first order differential systems here e0 is the perturbation parameter our approach based on the topological degree theory and the a... | [['in', 'this', 'paper', 'we', 'provide', 'conditions', 'to', 'ensure', 'the', 'existence', 'for', 'e0', 'sufficiently', 'small', 'of', 'periodic', 'solutions', 'of', 'given', 'period', 't0', 'in', 'a', 'prescribed', 'domain', 'u', 'for', 'a', 'class', 'of', 'singularly', 'perturbed', 'first', 'order', 'differential', ... | [-0.1918816827135263, 0.06769680291424496, -0.10280491742254286, 0.010141360830607732, -0.047009024231766276, -0.13018469355877613, 0.004350235326225859, 0.265251255563491, -0.26797367988543197, -0.26774877571797634, 0.13145355667066913, -0.25814804377975864, -0.15689297255824555, 0.17053737145449435, -0.11281733744480... |
710.0056 | Small parameter perturbations of nonlinear periodic systems | In this paper we consider a class of nonlinear periodic differential systems
perturbed by two nonlinear periodic terms with multiplicative different powers
of a small parameter $e>0$. For such a class of systems we provide conditions
which guarantee the existence of periodic solutions of given period $T>0$.
These con... | math.CA | in this paper we consider a class of nonlinear periodic differential systems perturbed by two nonlinear periodic terms with multiplicative different powers of a small parameter e0 for such a class of systems we provide conditions which guarantee the existence of periodic solutions of given period t0 these conditions ar... | [['in', 'this', 'paper', 'we', 'consider', 'a', 'class', 'of', 'nonlinear', 'periodic', 'differential', 'systems', 'perturbed', 'by', 'two', 'nonlinear', 'periodic', 'terms', 'with', 'multiplicative', 'different', 'powers', 'of', 'a', 'small', 'parameter', 'e0', 'for', 'such', 'a', 'class', 'of', 'systems', 'we', 'prov... | [-0.24252728539674231, 0.07271972269545249, -0.02360948042392179, 0.0071553099712926066, -0.044930378376092345, -0.09853439556900412, -0.022034768627404614, 0.27391271194857025, -0.29586274311360383, -0.2132154382523839, 0.12645709629631946, -0.25762029854511775, -0.1841333219953985, 0.236387701653358, -0.0470821005938... |
710.0057 | A new approach in the theory of ordinary differential equations with
small parameter | A topological degree based averaging principle has been proposed by J. Mawhin
in his PhD thesis [J. Mawhin, Le Probleme des Solutions Periodiques en
Mecanique non Lineaire, These de doctorat en sciences, Universite de Liege,
1969]. In the present paper we extend this result for the case when the
unperturbed system is... | math.CA | a topological degree based averaging principle has been proposed by j mawhin in his phd thesis j mawhin le probleme des solutions periodiques en mecanique non lineaire these de doctorat en sciences universite de liege 1969 in the present paper we extend this result for the case when the unperturbed system is nonlinear ... | [['a', 'topological', 'degree', 'based', 'averaging', 'principle', 'has', 'been', 'proposed', 'by', 'j', 'mawhin', 'in', 'his', 'phd', 'thesis', 'j', 'mawhin', 'le', 'probleme', 'des', 'solutions', 'periodiques', 'en', 'mecanique', 'non', 'lineaire', 'these', 'de', 'doctorat', 'en', 'sciences', 'universite', 'de', 'lie... | [-0.16749959616988366, 0.0492602842294478, -0.16289650176851345, -0.0034400447621010244, -0.08786605830370847, -0.13616727560625544, -0.07663116946683399, 0.1783428125748677, -0.18121666810974213, -0.2741254393809608, 0.1118584986676329, -0.2925329207575747, -0.15625936269227947, 0.1569834801734292, -0.1630498601522828... |
710.0058 | Non-Minimal Inflation after WMAP3 | The Wilkinson Microwave Anisotropy Probe (WMAP) three year results are used
to constraint non-minimal inflation models. Two different non-minimally coupled
scalar field potentials are considered to calculate corresponding slow-roll
parameters of non-minimal inflation. The results of numerical analysis of
parameter sp... | astro-ph | the wilkinson microwave anisotropy probe wmap three year results are used to constraint nonminimal inflation models two different nonminimally coupled scalar field potentials are considered to calculate corresponding slowroll parameters of nonminimal inflation the results of numerical analysis of parameter space are co... | [['the', 'wilkinson', 'microwave', 'anisotropy', 'probe', 'wmap', 'three', 'year', 'results', 'are', 'used', 'to', 'constraint', 'nonminimal', 'inflation', 'models', 'two', 'different', 'nonminimally', 'coupled', 'scalar', 'field', 'potentials', 'are', 'considered', 'to', 'calculate', 'corresponding', 'slowroll', 'para... | [-0.17030063001080775, 0.13350377115868747, -0.03359917092184799, 0.0900003048710716, -0.1628798544824792, -0.19179351861254337, -0.07210662986378735, 0.3031419042665034, -0.14157144156977153, -0.37908207572614533, 0.03226689461809702, -0.2967597888902021, -0.06580584600137976, 0.22236268155169314, 0.04843835896836259,... |
710.0059 | Motif-based communities in complex networks | Community definitions usually focus on edges, inside and between the
communities. However, the high density of edges within a community determines
correlations between nodes going beyond nearest-neighbours, and which are
indicated by the presence of motifs. We show how motifs can be used to define
general classes of ... | physics.comp-ph physics.data-an physics.soc-ph | community definitions usually focus on edges inside and between the communities however the high density of edges within a community determines correlations between nodes going beyond nearestneighbours and which are indicated by the presence of motifs we show how motifs can be used to define general classes of nodes in... | [['community', 'definitions', 'usually', 'focus', 'on', 'edges', 'inside', 'and', 'between', 'the', 'communities', 'however', 'the', 'high', 'density', 'of', 'edges', 'within', 'a', 'community', 'determines', 'correlations', 'between', 'nodes', 'going', 'beyond', 'nearestneighbours', 'and', 'which', 'are', 'indicated',... | [-0.09552067145705223, 0.08418382141688788, -0.04143779829295503, 0.10782740932159326, -0.07534019070098529, -0.11365559404028416, 0.08114578183488669, 0.36319696914555655, -0.26846817929952127, -0.3518525847372272, 0.04206095652252033, -0.282826904792691, -0.25778324245097667, 0.11365714042472679, -0.03065897547954542... |
710.006 | Methods of topological degree theory in Malkin I. G. - Melnikov V. K.'s
problems for periodically perturbed systems | A topological degree based averaging principle has been proposed by J. Mawhin
in his PhD thesis [J. Mawhin, Le Probleme des Solutions Periodiques en
Mecanique non Lineaire, These de doctorat en sciences, Universite de Liege,
1969]. In his thesis the author gives analogous topological degree versions of
classical bifu... | math.CA | a topological degree based averaging principle has been proposed by j mawhin in his phd thesis j mawhin le probleme des solutions periodiques en mecanique non lineaire these de doctorat en sciences universite de liege 1969 in his thesis the author gives analogous topological degree versions of classical bifurcation res... | [['a', 'topological', 'degree', 'based', 'averaging', 'principle', 'has', 'been', 'proposed', 'by', 'j', 'mawhin', 'in', 'his', 'phd', 'thesis', 'j', 'mawhin', 'le', 'probleme', 'des', 'solutions', 'periodiques', 'en', 'mecanique', 'non', 'lineaire', 'these', 'de', 'doctorat', 'en', 'sciences', 'universite', 'de', 'lie... | [-0.20708123365572342, 0.05153571088837149, -0.1501921551709529, 0.04340654956661941, -0.07579835496338395, -0.13552757655270398, -0.04262284553648594, 0.1807619130316501, -0.2289710874814773, -0.22684807317952316, 0.10377703849808313, -0.3005912732488165, -0.1985288488853257, 0.16098538255124975, -0.15014648092134544,... |
710.0061 | Higher Order Normalizations in the Generalized Photogravitational
Restricted Three Body Problem with Poynting-Robertson Drag | Higher order normalizations are performed in the generalized
photogravitational restricted three body problem with Poynting-Robertson drag.
In this problem we have taken bigger primary as a source of radiation and
smaller primary as an oblate spheroid. Whittaker method is used to transform
the second order part of th... | math.DS | higher order normalizations are performed in the generalized photogravitational restricted three body problem with poyntingrobertson drag in this problem we have taken bigger primary as a source of radiation and smaller primary as an oblate spheroid whittaker method is used to transform the second order part of the ham... | [['higher', 'order', 'normalizations', 'are', 'performed', 'in', 'the', 'generalized', 'photogravitational', 'restricted', 'three', 'body', 'problem', 'with', 'poyntingrobertson', 'drag', 'in', 'this', 'problem', 'we', 'have', 'taken', 'bigger', 'primary', 'as', 'a', 'source', 'of', 'radiation', 'and', 'smaller', 'prim... | [-0.1275831131858687, 0.09833125955265132, -0.0980849433208591, 0.04949335433875917, -0.06064001296582664, -0.06815355298298026, -0.04551516898811377, 0.3217945889055986, -0.27007151189549217, -0.2934890969592179, 0.07455647920342644, -0.28922957809770417, -0.12365278225103073, 0.17940839590376306, -0.0340299993163328,... |
710.0062 | Domain of attraction of asymptotically stable periodic solutions
obtained via averaging principle | In this paper we propose an approach to evaluate the domain of attraction of
asymptotically stable periodic solutions obtained via averaging principle
(second Bogolubov's theorem or Mel'nikov's method). We discuss also how this
result is extended in the case when the right hand part is nonsmooth.
| math.CA | in this paper we propose an approach to evaluate the domain of attraction of asymptotically stable periodic solutions obtained via averaging principle second bogolubovs theorem or melnikovs method we discuss also how this result is extended in the case when the right hand part is nonsmooth | [['in', 'this', 'paper', 'we', 'propose', 'an', 'approach', 'to', 'evaluate', 'the', 'domain', 'of', 'attraction', 'of', 'asymptotically', 'stable', 'periodic', 'solutions', 'obtained', 'via', 'averaging', 'principle', 'second', 'bogolubovs', 'theorem', 'or', 'melnikovs', 'method', 'we', 'discuss', 'also', 'how', 'this... | [-0.09677982751442038, 0.040987045213430814, -0.11887506818722772, 0.07513484912519545, -0.07645944971591234, -0.119941220132877, 0.03785651070622565, 0.3466784916818142, -0.2937780032136842, -0.19965005564786817, 0.15626216211619423, -0.2152952897038473, -0.21673569794359576, 0.17716133394582279, -0.12816151563564074,... |
710.0063 | The Lorentz force effect on the On-Off dynamo intermittency | An investigation of the dynamo instability close to the threshold produced by
an ABC forced flow is presented. We focus on the on-off intermittency behavior
of the dynamo and the counter-effect of the Lorentz force in the non-linear
stage of the dynamo. The Lorentz force drastically alters the statistics of the
turbu... | physics.flu-dyn astro-ph nlin.CD | an investigation of the dynamo instability close to the threshold produced by an abc forced flow is presented we focus on the onoff intermittency behavior of the dynamo and the countereffect of the lorentz force in the nonlinear stage of the dynamo the lorentz force drastically alters the statistics of the turbulent fl... | [['an', 'investigation', 'of', 'the', 'dynamo', 'instability', 'close', 'to', 'the', 'threshold', 'produced', 'by', 'an', 'abc', 'forced', 'flow', 'is', 'presented', 'we', 'focus', 'on', 'the', 'onoff', 'intermittency', 'behavior', 'of', 'the', 'dynamo', 'and', 'the', 'countereffect', 'of', 'the', 'lorentz', 'force', '... | [-0.2182797266206905, 0.2325746209067338, -0.09929398327968479, 0.08001063534612554, -0.040525414512243146, -0.05747174667924935, 0.030886374938977407, 0.25224892140687233, -0.25864375708929077, -0.288236188677937, 0.08298481104049368, -0.23247783214121667, -0.12332284307332551, 0.2510843038242432, -0.02240867816289168... |
710.0064 | A sufficient condition for the linear stability of magnetohydrodynamic
equilibria with field aligned incompressible flows | A sufficient condition for the linear stability of three dimensional
equilibria with incompressible flows parallel to the magnetic field is derived.
The condition involves physically interpretable terms related to the magnetic
shear and the flow shear.
| physics.plasm-ph | a sufficient condition for the linear stability of three dimensional equilibria with incompressible flows parallel to the magnetic field is derived the condition involves physically interpretable terms related to the magnetic shear and the flow shear | [['a', 'sufficient', 'condition', 'for', 'the', 'linear', 'stability', 'of', 'three', 'dimensional', 'equilibria', 'with', 'incompressible', 'flows', 'parallel', 'to', 'the', 'magnetic', 'field', 'is', 'derived', 'the', 'condition', 'involves', 'physically', 'interpretable', 'terms', 'related', 'to', 'the', 'magnetic',... | [-0.24414231234954464, 0.16321619589709574, -0.05251968326047063, 0.02979043132897156, -0.08323970364613666, -0.11764359470301618, -0.08387693942576233, 0.2751101789375146, -0.3035290625412017, -0.2597955656755302, 0.12011134133596595, -0.13882622686732146, -0.1050372782887684, 0.19409501816456518, -0.01857146975170407... |
710.0065 | Commutativity and ideals in algebraic crossed products | We investigate properties of commutative subrings and ideals in
non-commutative algebraic crossed products for actions by arbitrary groups. A
description of the commutant of the base coefficient subring in the crossed
product ring is given. Conditions for commutativity and maximal commutativity
of the commutant of th... | math.RA | we investigate properties of commutative subrings and ideals in noncommutative algebraic crossed products for actions by arbitrary groups a description of the commutant of the base coefficient subring in the crossed product ring is given conditions for commutativity and maximal commutativity of the commutant of the bas... | [['we', 'investigate', 'properties', 'of', 'commutative', 'subrings', 'and', 'ideals', 'in', 'noncommutative', 'algebraic', 'crossed', 'products', 'for', 'actions', 'by', 'arbitrary', 'groups', 'a', 'description', 'of', 'the', 'commutant', 'of', 'the', 'base', 'coefficient', 'subring', 'in', 'the', 'crossed', 'product'... | [-0.25607101719166775, 0.041869798180414364, -0.010434268595417961, -0.0009293038007551028, -0.03810192582265396, -0.0800751804151029, -0.046927911307041846, 0.2979958920623176, -0.36985362505947705, -0.16598668929267055, 0.12421402732312951, -0.2326816167042125, -0.059038350421663686, 0.17294545193241598, -0.120682633... |
710.0066 | HMC algorithm for two-flavour lattice QCD: Schwarz-preconditioning with
a one-dimensional domain decomposition | We study a variant of the Schwarz-preconditioned HMC algorithm. In contrast
to the original proposal of L\"uscher, we apply the domain decomposition in one
lattice direction only. This is sufficient to reduce the condition number of
the fermion matrix restricted to the domains compared with the full fermion
matrix. F... | hep-lat | we study a variant of the schwarzpreconditioned hmc algorithm in contrast to the original proposal of luscher we apply the domain decomposition in one lattice direction only this is sufficient to reduce the condition number of the fermion matrix restricted to the domains compared with the full fermion matrix for the sa... | [['we', 'study', 'a', 'variant', 'of', 'the', 'schwarzpreconditioned', 'hmc', 'algorithm', 'in', 'contrast', 'to', 'the', 'original', 'proposal', 'of', 'luscher', 'we', 'apply', 'the', 'domain', 'decomposition', 'in', 'one', 'lattice', 'direction', 'only', 'this', 'is', 'sufficient', 'to', 'reduce', 'the', 'condition',... | [-0.11070168206298893, 0.0900852643715387, -0.06501888460056349, 0.04787543883060359, -0.09428013861179352, -0.1180864951361648, 0.04215422050434758, 0.3702648137780753, -0.21741542947393927, -0.26369309452870354, 0.1412184597649188, -0.2649385372600095, -0.10713610687631775, 0.16536279854110697, -0.04875674538780004, ... |
710.0067 | Invariant measures of Hamiltonian systems with prescribed asymptotic
Maslov index | We study the properties of the asymptotic Maslov index of invariant measures
for time-periodic Hamiltonian systems on the cotangent bundle of a compact
manifold M. We show that if M has finite fundamental group and the Hamiltonian
satisfies some general growth assumptions on the momenta, the asymptotic Maslov
indices... | math.DS math.SG | we study the properties of the asymptotic maslov index of invariant measures for timeperiodic hamiltonian systems on the cotangent bundle of a compact manifold m we show that if m has finite fundamental group and the hamiltonian satisfies some general growth assumptions on the momenta the asymptotic maslov indices of p... | [['we', 'study', 'the', 'properties', 'of', 'the', 'asymptotic', 'maslov', 'index', 'of', 'invariant', 'measures', 'for', 'timeperiodic', 'hamiltonian', 'systems', 'on', 'the', 'cotangent', 'bundle', 'of', 'a', 'compact', 'manifold', 'm', 'we', 'show', 'that', 'if', 'm', 'has', 'finite', 'fundamental', 'group', 'and', ... | [-0.259361779450795, 0.12700831042863736, -0.1508554757490535, 0.08252614027964335, -0.04097249215085279, -0.11438506293822737, -0.005656896357643692, 0.31865149098688134, -0.22557177180972168, -0.23115429616368868, 0.09608405717795797, -0.2630398689344635, -0.18400707456064136, 0.14683961057059658, -0.1222366213983418... |
710.0068 | Wheeler's Gravitomagnetism Revisited I: A Purely Lorentz-Compton
Approach to Vector Gravitational Waves and Trio-Holes | A theory of vector gravitational waves is presented on the basis of an
additional gravitational field, recovering ideas that go back to H. A. Lorentz,
field that A. Wheeler called ``gravitomagnetism''. The theory is independent of
Einstein's General Relativity Theory, but is consistent with the
Einstein-Lorentz frame... | physics.gen-ph | a theory of vector gravitational waves is presented on the basis of an additional gravitational field recovering ideas that go back to h a lorentz field that a wheeler called gravitomagnetism the theory is independent of einsteins general relativity theory but is consistent with the einsteinlorentz framework of special... | [['a', 'theory', 'of', 'vector', 'gravitational', 'waves', 'is', 'presented', 'on', 'the', 'basis', 'of', 'an', 'additional', 'gravitational', 'field', 'recovering', 'ideas', 'that', 'go', 'back', 'to', 'h', 'a', 'lorentz', 'field', 'that', 'a', 'wheeler', 'called', 'gravitomagnetism', 'the', 'theory', 'is', 'independe... | [-0.1350949046787836, 0.13576431198546948, -0.11778184883697058, 0.07339545528739891, -0.12583669006664266, -0.13949424829033594, -0.015598968446244716, 0.2842685491527601, -0.2225590346140727, -0.2522249134177322, 0.05869987667087586, -0.2277516887337971, -0.13271791775340355, 0.199464359935323, -0.03876906265855156, ... |
710.0069 | High-order accurate implicit methods for the pricing of barrier options | This paper deals with a high-order accurate implicit finite-difference
approach to the pricing of barrier options. In this way various types of
barrier options are priced, including barrier options paying rebates, and
options on dividend-paying-stocks. Moreover, the barriers may be monitored
either continuously or di... | q-fin.PR math.NA math.PR | this paper deals with a highorder accurate implicit finitedifference approach to the pricing of barrier options in this way various types of barrier options are priced including barrier options paying rebates and options on dividendpayingstocks moreover the barriers may be monitored either continuously or discretely in... | [['this', 'paper', 'deals', 'with', 'a', 'highorder', 'accurate', 'implicit', 'finitedifference', 'approach', 'to', 'the', 'pricing', 'of', 'barrier', 'options', 'in', 'this', 'way', 'various', 'types', 'of', 'barrier', 'options', 'are', 'priced', 'including', 'barrier', 'options', 'paying', 'rebates', 'and', 'options'... | [-0.08333821973160337, -0.005339429916081126, -0.09805901143814391, 0.07701794120013622, -0.09232624929558608, -0.16641441592946649, 0.0975127582186375, 0.44291091328639476, -0.2788926926212477, -0.28604127209419844, 0.10898032711272998, -0.221649300982626, -0.06819092316675138, 0.2554220506238186, -0.08553114663580524... |
710.007 | Casimir operators of Lie algebras with a nilpotent radical | We show that a Lie algebra having a nilpotent radical has a fundamental set
of invariants consisting of Casimir operators. We give a different proof of
this fact in the special and well-known case where the radical is abelian.
| math.OC math.GR | we show that a lie algebra having a nilpotent radical has a fundamental set of invariants consisting of casimir operators we give a different proof of this fact in the special and wellknown case where the radical is abelian | [['we', 'show', 'that', 'a', 'lie', 'algebra', 'having', 'a', 'nilpotent', 'radical', 'has', 'a', 'fundamental', 'set', 'of', 'invariants', 'consisting', 'of', 'casimir', 'operators', 'we', 'give', 'a', 'different', 'proof', 'of', 'this', 'fact', 'in', 'the', 'special', 'and', 'wellknown', 'case', 'where', 'the', 'radi... | [-0.20355991584559283, 0.07860026501405698, -0.08611312885888112, -0.010940090872538395, -0.10804058763628396, -0.12947783891398174, -0.025418593763158873, 0.30184501419082665, -0.2781195522118837, -0.1699492286126583, 0.09010574323996806, -0.23974362656306952, -0.16578833820919195, 0.18735726717381906, -0.113643805281... |
710.0071 | Symmetry properties of a nonlinear acoustics model | We give a classification into conjugacy classes of subalgebras of the
symmetry algebra generated by the Zabolotskaya-Khokhlov equation, and obtain
all similarity reductions of this equation into $(1+1)$-dimensional equations.
We thus show that Lie classical reduction approach may also give rise to more
general reduce... | math.OC math-ph math.MP | we give a classification into conjugacy classes of subalgebras of the symmetry algebra generated by the zabolotskayakhokhlov equation and obtain all similarity reductions of this equation into 11dimensional equations we thus show that lie classical reduction approach may also give rise to more general reduced equations... | [['we', 'give', 'a', 'classification', 'into', 'conjugacy', 'classes', 'of', 'subalgebras', 'of', 'the', 'symmetry', 'algebra', 'generated', 'by', 'the', 'zabolotskayakhokhlov', 'equation', 'and', 'obtain', 'all', 'similarity', 'reductions', 'of', 'this', 'equation', 'into', '11dimensional', 'equations', 'we', 'thus', ... | [-0.11598414150605312, 0.057439093954110544, -0.07405783215523767, 0.0673486567058934, -0.08439342828759396, -0.13302800372423632, -0.004675410034607595, 0.2930934574566226, -0.29945710027562594, -0.327726690084743, 0.10529401569641125, -0.2766776679417313, -0.13585009190615321, 0.22940290945151182, -0.0249580642305759... |
710.0072 | The vector and axial vector current in Wilson ChPT | We construct the vector and axial vector currents in Wilson Chiral
Perturbation Theory (WChPT), the low-energy effective theory for lattice QCD
with Wilson fermions.
Our construction is slightly different compared to ChPT in continuum QCD,
where the currents are essentially the (partially) conserved currents
associ... | hep-lat | we construct the vector and axial vector currents in wilson chiral perturbation theory wchpt the lowenergy effective theory for lattice qcd with wilson fermions our construction is slightly different compared to chpt in continuum qcd where the currents are essentially the partially conserved currents associated with th... | [['we', 'construct', 'the', 'vector', 'and', 'axial', 'vector', 'currents', 'in', 'wilson', 'chiral', 'perturbation', 'theory', 'wchpt', 'the', 'lowenergy', 'effective', 'theory', 'for', 'lattice', 'qcd', 'with', 'wilson', 'fermions', 'our', 'construction', 'is', 'slightly', 'different', 'compared', 'to', 'chpt', 'in',... | [-0.133777969688203, 0.2446939496481314, -0.06105927582636165, 0.08689861982646915, -0.04786429732080756, -0.09892191012558113, 0.03607498058004745, 0.3701406808880468, -0.18767009410334545, -0.2105631571288945, 0.08066031268066985, -0.2828328267884596, -0.11146440455276105, 0.07240408947190088, 0.015291142051056441, 0... |
710.0073 | Strongly coupled large N spectrum of two matrices coupled via a
Yang-Mills interaction | We consider the large N spectrum of the quantum mechanical hamiltonian of two
hermitean matrices coupled via a Yang-Mills interaction. In a framework where
one of the matrices is treated exactly and the other is treated as a creation
operator impurity, the difference equation associated with the Yang-Mills
interactio... | hep-th | we consider the large n spectrum of the quantum mechanical hamiltonian of two hermitean matrices coupled via a yangmills interaction in a framework where one of the matrices is treated exactly and the other is treated as a creation operator impurity the difference equation associated with the yangmills interaction is d... | [['we', 'consider', 'the', 'large', 'n', 'spectrum', 'of', 'the', 'quantum', 'mechanical', 'hamiltonian', 'of', 'two', 'hermitean', 'matrices', 'coupled', 'via', 'a', 'yangmills', 'interaction', 'in', 'a', 'framework', 'where', 'one', 'of', 'the', 'matrices', 'is', 'treated', 'exactly', 'and', 'the', 'other', 'is', 'tr... | [-0.16783144435670116, 0.19820174241051225, -0.03718298763073612, 0.08894508659590662, -0.005858234938990214, -0.16285861631173013, -0.023244123843655286, 0.30906048377441003, -0.2263268821937318, -0.2799284229755844, 0.05730807029476186, -0.33006643584127177, -0.10212896532139344, 0.13731437203667984, 0.04143588344501... |
710.0074 | Localized reversible nanoscale phase separation in Pr_0.63Ca_0.37MnO_3
single crystal using a scanning tunneling microscope tip | We report the destabilization of the charge ordered insulating (COI) state in
a localized region of Pr_0.63Ca_0.37MnO_3 single crystal by current injection
using a scanning tunneling microscope tip. This leads to controlled phase
separation and formation of localized metallic nanoislands in the COI matrix
which have ... | cond-mat.mtrl-sci cond-mat.str-el | we report the destabilization of the charge ordered insulating coi state in a localized region of pr_063ca_037mno_3 single crystal by current injection using a scanning tunneling microscope tip this leads to controlled phase separation and formation of localized metallic nanoislands in the coi matrix which have been de... | [['we', 'report', 'the', 'destabilization', 'of', 'the', 'charge', 'ordered', 'insulating', 'coi', 'state', 'in', 'a', 'localized', 'region', 'of', 'pr_063ca_037mno_3', 'single', 'crystal', 'by', 'current', 'injection', 'using', 'a', 'scanning', 'tunneling', 'microscope', 'tip', 'this', 'leads', 'to', 'controlled', 'ph... | [-0.15697623540345057, 0.2254388054901491, -0.05244931993238105, -0.013529765612666347, -0.00609441116664624, -0.17486048047430813, 0.1023129229321504, 0.38187472261141236, -0.2821057423410055, -0.3300294089049362, 0.03135050511449216, -0.2625864355645159, -0.06505743972140185, 0.13017445482444345, -0.01102048186651684... |
710.0075 | Elliptic functions and efficient control of Ising spin chains with
unequal couplings | In this article, we study optimal control of dynamics in a linear chain of
three spin 1/2, weakly coupled with unequal Ising couplings. We address the
problem of time-optimal synthesis of multiple spin quantum coherences. We
derive time-optimal pulse sequence for creating a desired spin order by
computing geodesics o... | quant-ph | in this article we study optimal control of dynamics in a linear chain of three spin 12 weakly coupled with unequal ising couplings we address the problem of timeoptimal synthesis of multiple spin quantum coherences we derive timeoptimal pulse sequence for creating a desired spin order by computing geodesics on a spher... | [['in', 'this', 'article', 'we', 'study', 'optimal', 'control', 'of', 'dynamics', 'in', 'a', 'linear', 'chain', 'of', 'three', 'spin', '12', 'weakly', 'coupled', 'with', 'unequal', 'ising', 'couplings', 'we', 'address', 'the', 'problem', 'of', 'timeoptimal', 'synthesis', 'of', 'multiple', 'spin', 'quantum', 'coherences... | [-0.22033021214883775, 0.17157480557118385, -0.01891115479072771, 0.056645523373915166, -0.06568259714493671, -0.17066128817924225, -0.03480985404838485, 0.3769851532348324, -0.2901115779509732, -0.2738059373357548, 0.08175926163004568, -0.2621295776737567, -0.10740403259674516, 0.20319016322789069, 0.00391107767175596... |
710.0076 | A note on quantum 3-manifold invariants and hyperbolic volume | We investigate the conjectural relations between the
Reshetikhin-Turaev-Witten quantum SU(2) invariants and the volume of hyperbolic
3-manifolds. Given a finite set of sufficiently large positive integers, say J,
we construct examples of closed hyperbolic 3-manifolds with the same invariants
at all levels in J and di... | math.GT math.QA | we investigate the conjectural relations between the reshetikhinturaevwitten quantum su2 invariants and the volume of hyperbolic 3manifolds given a finite set of sufficiently large positive integers say j we construct examples of closed hyperbolic 3manifolds with the same invariants at all levels in j and different vol... | [['we', 'investigate', 'the', 'conjectural', 'relations', 'between', 'the', 'reshetikhinturaevwitten', 'quantum', 'su2', 'invariants', 'and', 'the', 'volume', 'of', 'hyperbolic', '3manifolds', 'given', 'a', 'finite', 'set', 'of', 'sufficiently', 'large', 'positive', 'integers', 'say', 'j', 'we', 'construct', 'examples'... | [-0.23966926587943702, 0.19370061028352442, -0.02970399312239061, 0.09824007327490031, -0.050355527500443635, -0.15781325665599805, 0.017481475270927905, 0.25314524008872663, -0.24211139176437196, -0.2843942353520493, 0.03030036908742833, -0.3136654574661813, -0.1182717071261574, 0.16824450222973494, -0.105246995337941... |
710.0077 | 2-loop Quantum Yang-Mills Condensate as Dark Energy | In seeking a model solving the coincidence problem, the effective Yang-Mills
condensate (YMC) is an alternative candidate for dark energy. A study is made
for the model up to the 2-loop order of quantum corrections. It is found that,
like in the 1-loop model, for generic initial conditions during the radiation
era, t... | astro-ph | in seeking a model solving the coincidence problem the effective yangmills condensate ymc is an alternative candidate for dark energy a study is made for the model up to the 2loop order of quantum corrections it is found that like in the 1loop model for generic initial conditions during the radiation era there is alway... | [['in', 'seeking', 'a', 'model', 'solving', 'the', 'coincidence', 'problem', 'the', 'effective', 'yangmills', 'condensate', 'ymc', 'is', 'an', 'alternative', 'candidate', 'for', 'dark', 'energy', 'a', 'study', 'is', 'made', 'for', 'the', 'model', 'up', 'to', 'the', '2loop', 'order', 'of', 'quantum', 'corrections', 'it'... | [-0.10891542003449539, 0.1546478892040044, -0.10981149491044166, 0.10604411556446196, -0.047442051377552356, -0.15725441676483531, 0.01627097478359128, 0.2809914901386946, -0.22908565024035457, -0.32929391396110474, 0.08081952217844841, -0.31939939164920994, -0.03841949144135351, 0.14698635189915482, 0.0396541105077156... |
710.0078 | The Method of the Description of Dynamics Nonequilibrium Systems within
the Frames of the Classical Mechanics | Within the frames of the analytical mechanics the method of the description
of dynamics of nonequilibrium systems of potentially interacting elements is
develops. The method is based on an opportunity of representation of
nonequilibrium system by set of interacting equilibrium subsystems. The
equation of motion of in... | physics.gen-ph | within the frames of the analytical mechanics the method of the description of dynamics of nonequilibrium systems of potentially interacting elements is develops the method is based on an opportunity of representation of nonequilibrium system by set of interacting equilibrium subsystems the equation of motion of intera... | [['within', 'the', 'frames', 'of', 'the', 'analytical', 'mechanics', 'the', 'method', 'of', 'the', 'description', 'of', 'dynamics', 'of', 'nonequilibrium', 'systems', 'of', 'potentially', 'interacting', 'elements', 'is', 'develops', 'the', 'method', 'is', 'based', 'on', 'an', 'opportunity', 'of', 'representation', 'of'... | [-0.17281416939980307, 0.0960617159783629, -0.17832319352905765, 0.005904184184632762, 0.0247615052408777, -0.110093071964721, -0.007374524940238442, 0.2516909756069613, -0.2564429079214934, -0.28044749455266565, 0.02786079698328882, -0.30894940474265536, -0.131005194073348, 0.19607993919229091, -0.015556338337943131, ... |
710.0079 | Scattering of Noncommutative Waves and Solitons in a Supersymmetric
Chiral Model in 2+1 Dimensions | Interactions of noncommutative waves and solitons in 2+1 dimensions can be
analyzed exactly for a supersymmetric and integrable U(n) chiral model
extending the Ward model. Using the Moyal-deformed dressing method in an
antichiral superspace, we construct explicit time-dependent solutions of its
noncommutative field e... | hep-th | interactions of noncommutative waves and solitons in 21 dimensions can be analyzed exactly for a supersymmetric and integrable un chiral model extending the ward model using the moyaldeformed dressing method in an antichiral superspace we construct explicit timedependent solutions of its noncommutative field equations ... | [['interactions', 'of', 'noncommutative', 'waves', 'and', 'solitons', 'in', '21', 'dimensions', 'can', 'be', 'analyzed', 'exactly', 'for', 'a', 'supersymmetric', 'and', 'integrable', 'un', 'chiral', 'model', 'extending', 'the', 'ward', 'model', 'using', 'the', 'moyaldeformed', 'dressing', 'method', 'in', 'an', 'antichi... | [-0.1490815795492381, 0.1726017891503943, -0.04901677147790906, 0.10735340874089161, -0.07361492752097547, -0.1886397917114664, -0.09815463849809021, 0.2934444220853038, -0.20840291914064438, -0.2446884809061885, 0.11507961775059812, -0.2797585591499228, -0.18237749985419213, 0.14338514429982752, 0.00883370079100132, 0... |
710.008 | Equivalent metrics and compactifications | Let (X,d) be a metric space and m\in X. Suppose that \phi:X\times
X\to\mathbold{R} is a nonnegative symmetric function. We define a metric
d^{\phi,m} on X which is equivalent to d. If d^{\phi,m} is totally bounded, its
completion is a compactification of (X,d). As examples, we construct two
compactifications of (\mat... | math.GT math.GN | let xd be a metric space and min x suppose that phixtimes xtomathboldr is a nonnegative symmetric function we define a metric dphim on x which is equivalent to d if dphim is totally bounded its completion is a compactification of xd as examples we construct two compactifications of mathhboldrsd_e where d_e is the eucli... | [['let', 'xd', 'be', 'a', 'metric', 'space', 'and', 'min', 'x', 'suppose', 'that', 'phixtimes', 'xtomathboldr', 'is', 'a', 'nonnegative', 'symmetric', 'function', 'we', 'define', 'a', 'metric', 'dphim', 'on', 'x', 'which', 'is', 'equivalent', 'to', 'd', 'if', 'dphim', 'is', 'totally', 'bounded', 'its', 'completion', 'i... | [-0.17204695222123215, 0.1410828224874826, -0.0841608348612984, 0.07831598630528552, -0.08194577675830159, -0.21714014783329158, -0.03846379738576986, 0.3813400722488209, -0.2958702050425388, -0.12126516356322638, 0.1397400474417265, -0.3521874103936608, -0.15965241302425662, 0.12953917425194825, -0.1319324769148672, -... |
710.0081 | Skeleton expansions for directed polymers in disordered media | Partial summations of perturbation expansions of the directed polymer in
disordered media (DPRM) enables one to represent the latter as skeleton
expansions in powers of the effective coupling constant $\Delta (t)$, which
corresponds to the binding state between two replicas in the replica field
theory of DPRM, and is... | cond-mat.stat-mech cond-mat.dis-nn | partial summations of perturbation expansions of the directed polymer in disordered media dprm enables one to represent the latter as skeleton expansions in powers of the effective coupling constant delta t which corresponds to the binding state between two replicas in the replica field theory of dprm and is equivalent... | [['partial', 'summations', 'of', 'perturbation', 'expansions', 'of', 'the', 'directed', 'polymer', 'in', 'disordered', 'media', 'dprm', 'enables', 'one', 'to', 'represent', 'the', 'latter', 'as', 'skeleton', 'expansions', 'in', 'powers', 'of', 'the', 'effective', 'coupling', 'constant', 'delta', 't', 'which', 'correspo... | [-0.18287624382136441, 0.1939656955003818, -0.05014658681346639, 0.034301346669464744, -0.015233679177009896, -0.10221227073136156, 0.04709090473216461, 0.3193141923936671, -0.27415455180883713, -0.2622830105773237, 0.015896183519132998, -0.31936160476291425, -0.08882231712708097, 0.09518737725001339, 0.051606378415982... |
710.0082 | Permutative categories, multicategories, and algebraic K-theory | We show that the $K$-theory construction of arXiv:math/0403403, which
preserves multiplicative structure, extends to a symmetric monoidal closed
bicomplete source category, with the multiplicative structure still preserved.
The source category of arXiv:math/0403403, whose objects are permutative
categories, maps full... | math.KT math.AT | we show that the ktheory construction of arxivmath0403403 which preserves multiplicative structure extends to a symmetric monoidal closed bicomplete source category with the multiplicative structure still preserved the source category of arxivmath0403403 whose objects are permutative categories maps fully and faithfull... | [['we', 'show', 'that', 'the', 'ktheory', 'construction', 'of', 'arxivmath0403403', 'which', 'preserves', 'multiplicative', 'structure', 'extends', 'to', 'a', 'symmetric', 'monoidal', 'closed', 'bicomplete', 'source', 'category', 'with', 'the', 'multiplicative', 'structure', 'still', 'preserved', 'the', 'source', 'cate... | [-0.11320674582859691, 0.016093114486002192, -0.05441015236535851, 0.1070457359357756, -0.16017685948433924, -0.14346786712923523, -0.05818033702576495, 0.44851827446599396, -0.4683971845982026, -0.209178938416346, 0.08948431178281198, -0.17290409683007557, -0.13295567954643345, 0.15471056806949937, -0.2058588171909962... |
710.0083 | Sorting and Selection with Random Costs | There is a growing body of work on sorting and selection in models other than
the unit-cost comparison model. This work is the first treatment of a natural
stochastic variant of the problem where the cost of comparing two elements is a
random variable. Each cost is chosen independently and is known to the
algorithm. ... | cs.DS | there is a growing body of work on sorting and selection in models other than the unitcost comparison model this work is the first treatment of a natural stochastic variant of the problem where the cost of comparing two elements is a random variable each cost is chosen independently and is known to the algorithm in par... | [['there', 'is', 'a', 'growing', 'body', 'of', 'work', 'on', 'sorting', 'and', 'selection', 'in', 'models', 'other', 'than', 'the', 'unitcost', 'comparison', 'model', 'this', 'work', 'is', 'the', 'first', 'treatment', 'of', 'a', 'natural', 'stochastic', 'variant', 'of', 'the', 'problem', 'where', 'the', 'cost', 'of', '... | [-0.10025014656404142, 0.12175100133069516, -0.04031156508512247, 0.03311336491691798, -0.03984266070662724, -0.16411873615716638, 0.08842572938609759, 0.38425068423876996, -0.25876577026707204, -0.30593630032586483, 0.14672670753498096, -0.28939514298348085, -0.11945176672580761, 0.18358913744176628, -0.08081810485215... |
710.0084 | Special relativity in complex vector algebra | Many different mathematical languages have been invented to describe the
ideas of Einstein's special relativity. One of the most powerful languages is
the Minkowski space-time algebra of D. Hestenes. We discuss the ideas of
special relativity in a complex 4-dimensional algebra of observables, which is
algebraically i... | math-ph math.MP | many different mathematical languages have been invented to describe the ideas of einsteins special relativity one of the most powerful languages is the minkowski spacetime algebra of d hestenes we discuss the ideas of special relativity in a complex 4dimensional algebra of observables which is algebraically isomorphic... | [['many', 'different', 'mathematical', 'languages', 'have', 'been', 'invented', 'to', 'describe', 'the', 'ideas', 'of', 'einsteins', 'special', 'relativity', 'one', 'of', 'the', 'most', 'powerful', 'languages', 'is', 'the', 'minkowski', 'spacetime', 'algebra', 'of', 'd', 'hestenes', 'we', 'discuss', 'the', 'ideas', 'of... | [-0.1575837590816346, 0.06023701668124307, -0.11931657540527257, 0.1395172255462967, -0.21146954816173424, -0.21358316468752242, -0.1340983006764542, 0.279520937258547, -0.29529095274523237, -0.207492386888374, 0.09982425502543761, -0.22110060777684504, -0.1416768005625768, 0.19037859141191638, -0.14603509880941024, -0... |
710.0085 | On inverse scattering at high energies for the multidimensional Newton
equation in electromagnetic field | We consider the multidimensional (nonrelativistic) Newton equation in a
static electromagnetic field $$\ddot x = F(x,\dot x), F(x,\dot x)=-\nabla
V(x)+B(x)\dot x, \dot x={dx\over dt}, x\in C^2(\R,\R^n),\eqno{(*)}$$ where $V
\in C^2(\R^n,\R),$ $B(x)$ is the $n\times n$ real antisymmetric matrix with
elements $B_{i,k}(... | math-ph math.MP | we consider the multidimensional nonrelativistic newton equation in a static electromagnetic field ddot x fxdot x fxdot xnabla vxbxdot x dot xdxover dt xin c2rrneqno where v in c2rnr bx is the ntimes n real antisymmetric matrix with elements b_ikx b_ikin c1rnr and b satisfies the closure condition and paj_1_xvx paj_2_x... | [['we', 'consider', 'the', 'multidimensional', 'nonrelativistic', 'newton', 'equation', 'in', 'a', 'static', 'electromagnetic', 'field', 'ddot', 'x', 'fxdot', 'x', 'fxdot', 'xnabla', 'vxbxdot', 'x', 'dot', 'xdxover', 'dt', 'xin', 'c2rrneqno', 'where', 'v', 'in', 'c2rnr', 'bx', 'is', 'the', 'ntimes', 'n', 'real', 'antis... | [-0.1301215452581851, 0.09930153290642246, -0.037927534689919815, 0.05359606630561218, -0.037665313056937454, -0.1487819508097514, -0.0018711658216219534, 0.3559230304941863, -0.2866640516526618, -0.22214778501829305, 0.07850055658760809, -0.3547913051486291, -0.09888096780761974, 0.18668145726163252, 0.025331866504900... |
710.0086 | An Optical Lattice Clock with Spin-polarized 87Sr Atoms | We present a new evaluation of an 87Sr optical lattice clock using spin
polarized atoms. The frequency of the 1S0-3P0 clock transition is found to be
429 228 004 229 873.6 Hz with a fractional accuracy of 2.6 10^{-15}, a value
that is comparable to the frequency difference between the various primary
standards throug... | physics.atom-ph | we present a new evaluation of an 87sr optical lattice clock using spin polarized atoms the frequency of the 1s03p0 clock transition is found to be 429 228 004 229 8736 hz with a fractional accuracy of 26 1015 a value that is comparable to the frequency difference between the various primary standards throughout the wo... | [['we', 'present', 'a', 'new', 'evaluation', 'of', 'an', '87sr', 'optical', 'lattice', 'clock', 'using', 'spin', 'polarized', 'atoms', 'the', 'frequency', 'of', 'the', '1s03p0', 'clock', 'transition', 'is', 'found', 'to', 'be', '429', '228', '004', '229', '8736', 'hz', 'with', 'a', 'fractional', 'accuracy', 'of', '26',... | [-0.12501984222463386, 0.1496537450432644, -0.011851086842772715, -0.03428526429171838, -0.006392110974582679, -0.08617760874467957, 0.12158258291824228, 0.42992323582224984, -0.17155046457671286, -0.3446198862648624, 0.07681174752788673, -0.3046194249490166, -0.01122865075355067, 0.23394101945792928, -0.04583065802067... |
710.0087 | Boson-assisted tunneling in layered metals | A theory for boson-assisted tunneling via randomly distributed resonant
states in a layered metals is developed. As particular examples, we consider
the electron-phonon interaction and the interaction between localized and
conduction electrons. The theory is applied to explain a non-monotonic
variation of the out-pla... | cond-mat.str-el cond-mat.mes-hall | a theory for bosonassisted tunneling via randomly distributed resonant states in a layered metals is developed as particular examples we consider the electronphonon interaction and the interaction between localized and conduction electrons the theory is applied to explain a nonmonotonic variation of the outplane resist... | [['a', 'theory', 'for', 'bosonassisted', 'tunneling', 'via', 'randomly', 'distributed', 'resonant', 'states', 'in', 'a', 'layered', 'metals', 'is', 'developed', 'as', 'particular', 'examples', 'we', 'consider', 'the', 'electronphonon', 'interaction', 'and', 'the', 'interaction', 'between', 'localized', 'and', 'conducti... | [-0.1574448883789135, 0.2316731544868911, -0.013500831071652617, 0.07719002301147317, 0.002021088155315203, -0.18428856259504078, 0.07439799951480738, 0.3592808092487793, -0.29030871866088287, -0.250684087968194, -0.06466693176851407, -0.360253426081994, -0.15832994620808782, 0.15805665224644483, 0.06113651192144436, -... |
710.0088 | Lagrangian curves on spectral curves of monopoles | We study Lagrangian points on smooth holomorphic curves in T${\mathbb P}^1$
equipped with a natural neutral K\"ahler structure, and prove that they must
form real curves. By virtue of the identification of T${\mathbb P}^1$ with the
space ${\mathbb L}({\mathbb E}^3)$ of oriented affine lines in Euclidean
3-space ${\ma... | math.DG hep-th | we study lagrangian points on smooth holomorphic curves in tmathbb p1 equipped with a natural neutral kahler structure and prove that they must form real curves by virtue of the identification of tmathbb p1 with the space mathbb lmathbb e3 of oriented affine lines in euclidean 3space mathbb e3 these lagrangian curves g... | [['we', 'study', 'lagrangian', 'points', 'on', 'smooth', 'holomorphic', 'curves', 'in', 'tmathbb', 'p1', 'equipped', 'with', 'a', 'natural', 'neutral', 'kahler', 'structure', 'and', 'prove', 'that', 'they', 'must', 'form', 'real', 'curves', 'by', 'virtue', 'of', 'the', 'identification', 'of', 'tmathbb', 'p1', 'with', '... | [-0.20403839278170058, 0.0721178619019244, -0.07201570133047719, 0.05561857663785979, -0.08083063823982112, -0.1597083685258704, 0.0013615017696734398, 0.3856889049612707, -0.26459712055061135, -0.1891404922240444, 0.07983146459615278, -0.2835288965774159, -0.16994034485110351, 0.21301277050928724, -0.12124535324983299... |
710.0089 | Blazar Observations with VERITAS | The Very Energetic Radiation Imaging Telescope Array System (VERITAS) is an
array of four 12m diameter Imaging Atmospheric Cherenkov Technique (IACT)
telescopes operated at the base of Mt. Hopkins in southern Arizona. The
four-telescope experiment started operation in April, 2007. GeV and TeV
gamma-ray observations o... | astro-ph | the very energetic radiation imaging telescope array system veritas is an array of four 12m diameter imaging atmospheric cherenkov technique iact telescopes operated at the base of mt hopkins in southern arizona the fourtelescope experiment started operation in april 2007 gev and tev gammaray observations of blazars ca... | [['the', 'very', 'energetic', 'radiation', 'imaging', 'telescope', 'array', 'system', 'veritas', 'is', 'an', 'array', 'of', 'four', '12m', 'diameter', 'imaging', 'atmospheric', 'cherenkov', 'technique', 'iact', 'telescopes', 'operated', 'at', 'the', 'base', 'of', 'mt', 'hopkins', 'in', 'southern', 'arizona', 'the', 'fo... | [-0.09103900689802978, 0.20367181684501368, -0.05932719395870621, 0.1275791158864874, -0.13269885199080253, -0.09285708660816495, -0.03177665040196701, 0.42833654188561715, -0.13236645258021082, -0.45949672671013525, 0.10252589906228642, -0.3303890819982465, -0.05206379507422105, 0.26248248770362004, -0.002677055279156... |
710.009 | The Diverse Stellar Populations of the W3 Star Forming Complex | An 800 sq-arcmin mosaic image of the W3 star forming complex obtained with
the Chandra X-ray Observatory gives a valuable new view of the spatial
structure of its young stellar populations. The Chandra image reveals about
1300 faint X-ray sources, most of which are PMS stars in the cloud. Some, but
not all, of the hi... | astro-ph | an 800 sqarcmin mosaic image of the w3 star forming complex obtained with the chandra xray observatory gives a valuable new view of the spatial structure of its young stellar populations the chandra image reveals about 1300 faint xray sources most of which are pms stars in the cloud some but not all of the highmass sta... | [['an', '800', 'sqarcmin', 'mosaic', 'image', 'of', 'the', 'w3', 'star', 'forming', 'complex', 'obtained', 'with', 'the', 'chandra', 'xray', 'observatory', 'gives', 'a', 'valuable', 'new', 'view', 'of', 'the', 'spatial', 'structure', 'of', 'its', 'young', 'stellar', 'populations', 'the', 'chandra', 'image', 'reveals', ... | [-0.053273449339996615, 0.12818718811892957, -0.04211897008219915, 0.1311380838407657, -0.1250837804312793, -0.01806906651524184, 0.04671596126544363, 0.4566576030781179, -0.11333048107788643, -0.3522446981993858, 0.03304680737520494, -0.2527779200339929, 0.012633373594092848, 0.14241701334846757, -0.055409592092377176... |
710.0091 | On rational blow-downs in Heegaard-Floer homology | Motivated by a result of L.P. Roberts on rational blow-downs in
Heegaard-Floer homology, we study such operations along 3-manifolds that arise
as branched double covers of $S^{3}$ along several non-alternating, slice
knots.
| math.GT | motivated by a result of lp roberts on rational blowdowns in heegaardfloer homology we study such operations along 3manifolds that arise as branched double covers of s3 along several nonalternating slice knots | [['motivated', 'by', 'a', 'result', 'of', 'lp', 'roberts', 'on', 'rational', 'blowdowns', 'in', 'heegaardfloer', 'homology', 'we', 'study', 'such', 'operations', 'along', '3manifolds', 'that', 'arise', 'as', 'branched', 'double', 'covers', 'of', 's3', 'along', 'several', 'nonalternating', 'slice', 'knots']] | [-0.3194563865545206, 0.04732412047451362, -0.0758704362087883, 0.15032303420593962, -0.08636055565148126, -0.16011084026831668, 0.01825140068103792, 0.3932384439976886, -0.35004522936651483, -0.25905744545161724, 0.14911232911617844, -0.22569134204240981, -0.2106907084780687, 0.2683295172464568, -0.20864098561287392, ... |
710.0092 | Geometry of moving planes | The concept of number and its generalization has played a central role in the
development of mathematics over many centuries and many civilizations.
Noteworthy milestones in this long and arduous process were the developments of
the real and complex numbers which have achieved universal acceptance. Serious
attempts h... | math-ph math.MP | the concept of number and its generalization has played a central role in the development of mathematics over many centuries and many civilizations noteworthy milestones in this long and arduous process were the developments of the real and complex numbers which have achieved universal acceptance serious attempts have ... | [['the', 'concept', 'of', 'number', 'and', 'its', 'generalization', 'has', 'played', 'a', 'central', 'role', 'in', 'the', 'development', 'of', 'mathematics', 'over', 'many', 'centuries', 'and', 'many', 'civilizations', 'noteworthy', 'milestones', 'in', 'this', 'long', 'and', 'arduous', 'process', 'were', 'the', 'develo... | [-0.07219934708231854, 0.08252769973542955, -0.11753108366392553, 0.07077806079058872, -0.1235653771708409, -0.08831717529230648, -0.03279749481945247, 0.3595258288551122, -0.3053788783132202, -0.33878592304471467, 0.14930904118551147, -0.21360245521387292, -0.18727482952591445, 0.2363877937404646, -0.14243249400363614... |
710.0093 | Generalized Dolbeault sequences in parabolic geometry | In this paper, we show the existence of a sequence of invariant differential
operators on a particular homogeneous model $G/P$ of a Cartan geometry. The
first operator in this sequence can be locally identified with the Dirac
operator in $k$ Clifford variables, $D=(D_1,..., D_k)$, where $D_i=\sum_j
e_j\cdot \partial_... | math.DG | in this paper we show the existence of a sequence of invariant differential operators on a particular homogeneous model gp of a cartan geometry the first operator in this sequence can be locally identified with the dirac operator in k clifford variables dd_1 d_k where d_isum_j e_jcdot partial_ij cinftyrnksto cinftyrnks... | [['in', 'this', 'paper', 'we', 'show', 'the', 'existence', 'of', 'a', 'sequence', 'of', 'invariant', 'differential', 'operators', 'on', 'a', 'particular', 'homogeneous', 'model', 'gp', 'of', 'a', 'cartan', 'geometry', 'the', 'first', 'operator', 'in', 'this', 'sequence', 'can', 'be', 'locally', 'identified', 'with', 't... | [-0.17884280218277127, 0.13626431872641356, -0.07786202618929867, 0.048388432870221244, -0.06557807177887298, -0.1134477928862907, -0.033220795270608505, 0.35156214006322745, -0.33089607507766533, -0.24159690029349198, 0.09592373679333832, -0.26641847465846996, -0.19240716369677102, 0.15613430954545038, -0.087181501740... |
710.0094 | The Destiny of Universes After the Big Trip | The big trip can be describe with the help of the Wheeler-DeWitt wave
equation ${\hat H}\psi(w,a)=0$. The probability to find the universe after big
trip in the state with $w=w_0$ will be maximal if $\partial\psi(w,a)/\partial
w|_{w=w_0}=0$ for any values of the scale factor $a$. It is shown that this
will be the cas... | astro-ph | the big trip can be describe with the help of the wheelerdewitt wave equation hat hpsiwa0 the probability to find the universe after big trip in the state with ww_0 will be maximal if partialpsiwapartial w_ww_00 for any values of the scale factor a it is shown that this will be the case if and only if w_013 this fact a... | [['the', 'big', 'trip', 'can', 'be', 'describe', 'with', 'the', 'help', 'of', 'the', 'wheelerdewitt', 'wave', 'equation', 'hat', 'hpsiwa0', 'the', 'probability', 'to', 'find', 'the', 'universe', 'after', 'big', 'trip', 'in', 'the', 'state', 'with', 'ww_0', 'will', 'be', 'maximal', 'if', 'partialpsiwapartial', 'w_ww_00'... | [-0.06860062277624629, 0.16942499815731457, -0.14054294879009066, 0.05615644682333559, -0.08634145214761559, -0.10675940611460981, 0.019142616209328958, 0.3385637037664358, -0.2988630555030939, -0.24756027668665506, 0.133880989273549, -0.2659414429250127, -0.09794690055576594, 0.18498029996101795, -0.0975987762702923, ... |
710.0095 | Quantum communication complexity of block-composed functions | A major open problem in communication complexity is whether or not quantum
protocols can be exponentially more efficient than classical protocols on
_total_ Boolean functions in the two-party interactive model. The answer
appears to be ``No''. In 2002, Razborov proved this conjecture for so far the
most general class... | quant-ph | a major open problem in communication complexity is whether or not quantum protocols can be exponentially more efficient than classical protocols on _total_ boolean functions in the twoparty interactive model the answer appears to be no in 2002 razborov proved this conjecture for so far the most general class of functi... | [['a', 'major', 'open', 'problem', 'in', 'communication', 'complexity', 'is', 'whether', 'or', 'not', 'quantum', 'protocols', 'can', 'be', 'exponentially', 'more', 'efficient', 'than', 'classical', 'protocols', 'on', '_total_', 'boolean', 'functions', 'in', 'the', 'twoparty', 'interactive', 'model', 'the', 'answer', 'a... | [-0.18277782335155449, 0.12416508814484808, -0.05303674776834913, 0.04749565151179632, -0.03481399227215463, -0.24925978351267009, 0.04554064049455924, 0.3633768830385779, -0.3056950868643476, -0.22113854590678164, 0.06302106799508891, -0.28786617831107886, -0.12523793191903373, 0.18368188563162977, -0.0979347224210334... |
710.0096 | The opacity of grains in protoplanetary atmospheres | We have computed the size distribution of silicate grains in the outer
radiative region of the envelope of a protoplanet evolving according to the
scenario of Pollack et al. (1996). Our computation includes grain growth due to
Brownian motion and overtake of smaller grains by larger ones. We also include
the input of... | astro-ph | we have computed the size distribution of silicate grains in the outer radiative region of the envelope of a protoplanet evolving according to the scenario of pollack et al 1996 our computation includes grain growth due to brownian motion and overtake of smaller grains by larger ones we also include the input of new gr... | [['we', 'have', 'computed', 'the', 'size', 'distribution', 'of', 'silicate', 'grains', 'in', 'the', 'outer', 'radiative', 'region', 'of', 'the', 'envelope', 'of', 'a', 'protoplanet', 'evolving', 'according', 'to', 'the', 'scenario', 'of', 'pollack', 'et', 'al', '1996', 'our', 'computation', 'includes', 'grain', 'growth... | [-0.04971425915122649, 0.12454840437469124, -0.07068039228899713, 0.027799256176664924, -0.04214270462773374, -0.01746246790616242, 0.0567211463984582, 0.35494756335506866, -0.21906800556462258, -0.3789230768505964, 0.07023385128412007, -0.23826489209183535, -0.05709287038457186, 0.1629029213325149, -0.0766365717513703... |
710.0097 | Pseudo-scalar meson form factors with maximally twisted Wilson fermions
at Nf = 2 | We present preliminary results for various electroweak form factors of
pseudo-scalar mesons using the tree-level improved Symanzik gauge action and
the maximally twisted mass fermionic action with Nf = 2 dynamical flavors. Our
results, obtained for both light and heavy quark masses at a single lattice
spacing (a ~ 0.... | hep-lat hep-ph | we present preliminary results for various electroweak form factors of pseudoscalar mesons using the treelevel improved symanzik gauge action and the maximally twisted mass fermionic action with nf 2 dynamical flavors our results obtained for both light and heavy quark masses at a single lattice spacing a 009 fm and at... | [['we', 'present', 'preliminary', 'results', 'for', 'various', 'electroweak', 'form', 'factors', 'of', 'pseudoscalar', 'mesons', 'using', 'the', 'treelevel', 'improved', 'symanzik', 'gauge', 'action', 'and', 'the', 'maximally', 'twisted', 'mass', 'fermionic', 'action', 'with', 'nf', '2', 'dynamical', 'flavors', 'our', ... | [-0.10340269819188108, 0.26941491212099306, -0.09598656830962236, 0.08852711545449554, -0.014411230218517625, -0.1266309554236667, 0.11482945356740208, 0.36895273048795907, -0.1545304979022297, -0.268281344234566, 0.021440361339592807, -0.28918230837953635, -0.05234180735971998, 0.12943613464073614, 0.03487703869472337... |
710.0098 | A survey of large N continuum phase transitions | The main focus of this talk is the physics of large N QCD on a continuum
torus. A cascade of phase transitions associated with the breaking of U(1)
symmetries will be discussed. The continuum Wilson loop as a function of its
area will be discussed along with its universality properties and the
associated double scali... | hep-lat hep-th | the main focus of this talk is the physics of large n qcd on a continuum torus a cascade of phase transitions associated with the breaking of u1 symmetries will be discussed the continuum wilson loop as a function of its area will be discussed along with its universality properties and the associated double scaling lim... | [['the', 'main', 'focus', 'of', 'this', 'talk', 'is', 'the', 'physics', 'of', 'large', 'n', 'qcd', 'on', 'a', 'continuum', 'torus', 'a', 'cascade', 'of', 'phase', 'transitions', 'associated', 'with', 'the', 'breaking', 'of', 'u1', 'symmetries', 'will', 'be', 'discussed', 'the', 'continuum', 'wilson', 'loop', 'as', 'a',... | [-0.17920504671529727, 0.252810230453919, -0.03607966827611909, 0.09170871755145325, -0.042509520039028297, -0.14839957723295136, -0.010301833227482847, 0.3520486984006335, -0.19909064827767092, -0.24559268313336424, 0.12597832384424498, -0.2707712609625825, -0.16394232059375638, 0.11140776705821004, -0.033139395348282... |
710.0099 | Elastic-like Collision of Gap Solitons in Bragg Gap Regions within
Nonlocal Nonlinear Photonic Crystals | We analyze the existence, stability, and mobility of gap solitons in a
periodic photonic structure with nonlocal nonlinearity. Within the Bragg region
of band gaps, gap solitons exhibit better stability and higher mobility due to
the combinations of non-locality effect and the oscillation nature of Bloch
waves. Using... | physics.optics | we analyze the existence stability and mobility of gap solitons in a periodic photonic structure with nonlocal nonlinearity within the bragg region of band gaps gap solitons exhibit better stability and higher mobility due to the combinations of nonlocality effect and the oscillation nature of bloch waves using linear ... | [['we', 'analyze', 'the', 'existence', 'stability', 'and', 'mobility', 'of', 'gap', 'solitons', 'in', 'a', 'periodic', 'photonic', 'structure', 'with', 'nonlocal', 'nonlinearity', 'within', 'the', 'bragg', 'region', 'of', 'band', 'gaps', 'gap', 'solitons', 'exhibit', 'better', 'stability', 'and', 'higher', 'mobility', ... | [-0.2347150481382043, 0.10472936128095096, -0.09006969329463888, 0.08758694432647329, -0.07523508512472012, -0.159501626954547, 0.025975289471846606, 0.39651539362967014, -0.27335007865057914, -0.2787070625594684, 0.07679449987825843, -0.28845589379875025, -0.1872689713514885, 0.16379376735576257, 0.01749996506467661, ... |
710.01 | Design Considerations for the Next Generation of Atmospheric Imaging
Cherenkov Telescopes | We estimate the limiting angular resolution and detection area for an array
of 3 large-aperture Imaging Atmospheric Cherenkov Telescopes. We consider an
idealized IACT system in order to understand the limitations imposed by the
intrinsic nature of the atmospheric showers and geometry of the detector
configuration. T... | astro-ph | we estimate the limiting angular resolution and detection area for an array of 3 largeaperture imaging atmospheric cherenkov telescopes we consider an idealized iact system in order to understand the limitations imposed by the intrinsic nature of the atmospheric showers and geometry of the detector configuration the id... | [['we', 'estimate', 'the', 'limiting', 'angular', 'resolution', 'and', 'detection', 'area', 'for', 'an', 'array', 'of', '3', 'largeaperture', 'imaging', 'atmospheric', 'cherenkov', 'telescopes', 'we', 'consider', 'an', 'idealized', 'iact', 'system', 'in', 'order', 'to', 'understand', 'the', 'limitations', 'imposed', 'b... | [-0.13423918303521862, 0.09428749943313901, -0.01929536079578511, 0.04851052113028325, -0.06196360484246615, -0.06417461029755381, 0.015194303700239858, 0.39979929835177386, -0.22004519603573358, -0.4013728935675757, 0.14168986930015529, -0.275301256462686, -0.07259748423642193, 0.19442817446095154, -0.0438966537099126... |
710.0101 | Counting Nodal Lines Which Touch the Boundary of an Analytic Domain | We consider the zeros on the boundary $\partial \Omega$ of a Neumann
eigenfunction $\phi_{\lambda}$ of a real analytic plane domain $\Omega$. We
prove that the number of its boundary zeros is $O (\lambda)$ where $-\Delta
\phi_{\lambda} = \lambda^2 \phi_{\lambda}$. We also prove that the number of
boundary critical po... | math.SP math.AP | we consider the zeros on the boundary partial omega of a neumann eigenfunction phi_lambda of a real analytic plane domain omega we prove that the number of its boundary zeros is o lambda where delta phi_lambda lambda2 phi_lambda we also prove that the number of boundary critical points of either a neumann or dirichlet ... | [['we', 'consider', 'the', 'zeros', 'on', 'the', 'boundary', 'partial', 'omega', 'of', 'a', 'neumann', 'eigenfunction', 'phi_lambda', 'of', 'a', 'real', 'analytic', 'plane', 'domain', 'omega', 'we', 'prove', 'that', 'the', 'number', 'of', 'its', 'boundary', 'zeros', 'is', 'o', 'lambda', 'where', 'delta', 'phi_lambda', ... | [-0.2624828879775051, 0.0964008139054631, -0.025834384429756375, 0.016779251843838702, -0.13021591745893515, -0.103127522261015, 0.043332731292124775, 0.2812892776795678, -0.2469088299761689, -0.188875594324181, 0.13965169902029817, -0.33893197316617246, -0.09049791261176801, 0.18272375720109613, -0.016850303821561354,... |
710.0102 | Representing Dehn twists with branched coverings | We show that any homologically non-trivial Dehn twist of a compact surface F
with boundary is the lifting of a half-twist in the braid group B_n, with
respect to a suitable branched covering p : F -> B^2. In particular, we allow
the surface to have disconnected boundary. As a consequence, any allowable
Lefschetz fibr... | math.GT | we show that any homologically nontrivial dehn twist of a compact surface f with boundary is the lifting of a halftwist in the braid group b_n with respect to a suitable branched covering p f b2 in particular we allow the surface to have disconnected boundary as a consequence any allowable lefschetz fibration on b2 is ... | [['we', 'show', 'that', 'any', 'homologically', 'nontrivial', 'dehn', 'twist', 'of', 'a', 'compact', 'surface', 'f', 'with', 'boundary', 'is', 'the', 'lifting', 'of', 'a', 'halftwist', 'in', 'the', 'braid', 'group', 'b_n', 'with', 'respect', 'to', 'a', 'suitable', 'branched', 'covering', 'p', 'f', 'b2', 'in', 'particul... | [-0.2832683367979905, 0.0986191349839496, -0.10739555600143615, 0.01067795912321243, -0.13134458443770805, -0.17055853576739394, 0.040145961153838366, 0.39319046639970373, -0.29498020089453175, -0.2077983037378299, 0.09281619611225786, -0.22562736166375025, -0.1144730406739409, 0.182508799055266, -0.12294488056033429, ... |
710.0103 | Transport Control of Eyring-Fluids along a Transversely-Corrugated
Nanoannulus | The volume flow rates of Eyring-fluids inside the wavy-rough nanoannulus were
obtained analytically (up to the second order) by using the verified model and
boundary perturbation method. Our results show that the wavy-roughness could
enhance the flow rate especially for smaller forcing due to the larger
surface-to-vo... | cond-mat.soft cond-mat.other | the volume flow rates of eyringfluids inside the wavyrough nanoannulus were obtained analytically up to the second order by using the verified model and boundary perturbation method our results show that the wavyroughness could enhance the flow rate especially for smaller forcing due to the larger surfacetovolume ratio... | [['the', 'volume', 'flow', 'rates', 'of', 'eyringfluids', 'inside', 'the', 'wavyrough', 'nanoannulus', 'were', 'obtained', 'analytically', 'up', 'to', 'the', 'second', 'order', 'by', 'using', 'the', 'verified', 'model', 'and', 'boundary', 'perturbation', 'method', 'our', 'results', 'show', 'that', 'the', 'wavyroughness... | [-0.09144628645627054, 0.14791802544617555, -0.0753451923809045, 0.032144592716716804, -0.04310665754754874, -0.09278555172956088, 0.03847267107198854, 0.3317985193762969, -0.3054815154563595, -0.31176421810760274, 0.15400854354227925, -0.2419534390063056, -0.09818295544719549, 0.23962871535363925, -0.0341942204408102,... |
710.0104 | Regular reflection in self-similar potential flow and the sonic
criterion | Reflection of a shock from a solid wedge is a classical problem in gas
dynamics. Depending on the parameters either a regular or a irregular
(Mach-type) reflection results. We construct regular reflection as an exact
self-similar solution for potential flow. For some upstream Mach numbers and
isentropic coefficients,... | math-ph math.MP | reflection of a shock from a solid wedge is a classical problem in gas dynamics depending on the parameters either a regular or a irregular machtype reflection results we construct regular reflection as an exact selfsimilar solution for potential flow for some upstream mach numbers and isentropic coefficients a solutio... | [['reflection', 'of', 'a', 'shock', 'from', 'a', 'solid', 'wedge', 'is', 'a', 'classical', 'problem', 'in', 'gas', 'dynamics', 'depending', 'on', 'the', 'parameters', 'either', 'a', 'regular', 'or', 'a', 'irregular', 'machtype', 'reflection', 'results', 'we', 'construct', 'regular', 'reflection', 'as', 'an', 'exact', '... | [-0.17123162912725498, 0.10275264599335464, -0.09940029202779341, 0.057103702319889434, -0.09772258785152291, -0.17658453586045653, 0.041337466798722744, 0.3470487671179904, -0.2728140568619387, -0.20604817494232622, 0.14222301264655673, -0.25552539985316497, -0.10270731899719168, 0.23912265809809063, -0.01740609214175... |
710.0105 | Zipf's Law and Avoidance of Excessive Synonymy | Zipf's law states that if words of language are ranked in the order of
decreasing frequency in texts, the frequency of a word is inversely
proportional to its rank. It is very robust as an experimental observation, but
to date it escaped satisfactory theoretical explanation. We suggest that Zipf's
law may arise from ... | cs.CL physics.soc-ph | zipfs law states that if words of language are ranked in the order of decreasing frequency in texts the frequency of a word is inversely proportional to its rank it is very robust as an experimental observation but to date it escaped satisfactory theoretical explanation we suggest that zipfs law may arise from the evol... | [['zipfs', 'law', 'states', 'that', 'if', 'words', 'of', 'language', 'are', 'ranked', 'in', 'the', 'order', 'of', 'decreasing', 'frequency', 'in', 'texts', 'the', 'frequency', 'of', 'a', 'word', 'is', 'inversely', 'proportional', 'to', 'its', 'rank', 'it', 'is', 'very', 'robust', 'as', 'an', 'experimental', 'observatio... | [-0.08462957917615327, 0.16399524239462682, -0.11193208769919462, 0.12821989052289567, -0.17019743485543043, -0.1330291981558635, 0.11325622113671766, 0.3807404361554046, -0.3256728992338723, -0.287032382583607, 0.030066856617497195, -0.34805585507915093, -0.14697332405693717, 0.18006674217063684, -0.10133077213957684,... |
710.0106 | Fuzzy almost quadratic functions | We approximate a fuzzy almost quadratic function by a quadratic function in a
fuzzy sense. More precisely, we establish a fuzzy Hyers--Ulam--Rassias
stability of the quadratic functional equation $f(x+y)+f(x-y)=2f(x)+2f(y)$. Our
result can be regarded as a generalization of the stability phenomenon in the
framework o... | math.FA | we approximate a fuzzy almost quadratic function by a quadratic function in a fuzzy sense more precisely we establish a fuzzy hyersulamrassias stability of the quadratic functional equation fxyfxy2fx2fy our result can be regarded as a generalization of the stability phenomenon in the framework of normed spaces we also ... | [['we', 'approximate', 'a', 'fuzzy', 'almost', 'quadratic', 'function', 'by', 'a', 'quadratic', 'function', 'in', 'a', 'fuzzy', 'sense', 'more', 'precisely', 'we', 'establish', 'a', 'fuzzy', 'hyersulamrassias', 'stability', 'of', 'the', 'quadratic', 'functional', 'equation', 'fxyfxy2fx2fy', 'our', 'result', 'can', 'be'... | [-0.14615447726673217, 0.010604996371586791, -0.1668432467601827, 0.1686737437534039, -0.07904279812193307, -0.07611688376083726, 0.0633098622325991, 0.25846105520842505, -0.34656194756265546, -0.2150604458922734, 0.09937658880409769, -0.2405706788947592, -0.2705560313751463, 0.16558954580763324, -0.10605561064525706, ... |
710.0107 | A Mazur--Ulam theorem in non-Archimedean normed spaces | The classical Mazur--Ulam theorem which states that every surjective isometry
between real normed spaces is affine is not valid for non-Archimedean normed
spaces. In this paper, we establish a Mazur--Ulam theorem in the
non-Archimedean strictly convex normed spaces.
| math.FA math.CA | the classical mazurulam theorem which states that every surjective isometry between real normed spaces is affine is not valid for nonarchimedean normed spaces in this paper we establish a mazurulam theorem in the nonarchimedean strictly convex normed spaces | [['the', 'classical', 'mazurulam', 'theorem', 'which', 'states', 'that', 'every', 'surjective', 'isometry', 'between', 'real', 'normed', 'spaces', 'is', 'affine', 'is', 'not', 'valid', 'for', 'nonarchimedean', 'normed', 'spaces', 'in', 'this', 'paper', 'we', 'establish', 'a', 'mazurulam', 'theorem', 'in', 'the', 'nonar... | [-0.17470521227407612, 0.07506466389780767, -0.13646893154241538, 0.1995595126615004, -0.1110344955109452, -0.1393617414011571, -0.019625898325007017, 0.3737533022894671, -0.4188299545724141, 0.018485907269151586, 0.08401201817047733, -0.22500185041051163, -0.15790012421846195, 0.24231812534363648, -0.28980887585662696... |
710.0108 | Symmetry based Structure Entropy of Complex Networks | Precisely quantifying the heterogeneity or disorder of a network system is
very important and desired in studies of behavior and function of the network
system. Although many degree-based entropies have been proposed to measure the
heterogeneity of real networks, heterogeneity implicated in the structure of
networks ... | physics.soc-ph | precisely quantifying the heterogeneity or disorder of a network system is very important and desired in studies of behavior and function of the network system although many degreebased entropies have been proposed to measure the heterogeneity of real networks heterogeneity implicated in the structure of networks can n... | [['precisely', 'quantifying', 'the', 'heterogeneity', 'or', 'disorder', 'of', 'a', 'network', 'system', 'is', 'very', 'important', 'and', 'desired', 'in', 'studies', 'of', 'behavior', 'and', 'function', 'of', 'the', 'network', 'system', 'although', 'many', 'degreebased', 'entropies', 'have', 'been', 'proposed', 'to', '... | [-0.14105693003997052, 0.09014377429816199, -0.10041884351651081, 0.1052917476966589, -0.03664775358629413, -0.14510448057747757, 0.017024148350982513, 0.40349944499838686, -0.26564943296640803, -0.283737250073399, 0.07896007289673435, -0.2826442617741931, -0.2718937512981938, 0.14166020074723443, -0.08262867767027476,... |
710.0109 | Simultaneous cooling of an artificial atom and its neighboring quantum
system | We propose an approach for cooling both an artificial atom (e.g., a flux
qubit) and its neighboring quantum system, the latter modeled by either a
quantum two-level system or a quantum resonator. The flux qubit is cooled by
manipulating its states, following an inverse process of state population
inversion, and then ... | cond-mat.supr-con cond-mat.mes-hall quant-ph | we propose an approach for cooling both an artificial atom eg a flux qubit and its neighboring quantum system the latter modeled by either a quantum twolevel system or a quantum resonator the flux qubit is cooled by manipulating its states following an inverse process of state population inversion and then the qubit is... | [['we', 'propose', 'an', 'approach', 'for', 'cooling', 'both', 'an', 'artificial', 'atom', 'eg', 'a', 'flux', 'qubit', 'and', 'its', 'neighboring', 'quantum', 'system', 'the', 'latter', 'modeled', 'by', 'either', 'a', 'quantum', 'twolevel', 'system', 'or', 'a', 'quantum', 'resonator', 'the', 'flux', 'qubit', 'is', 'coo... | [-0.14348973610291355, 0.2515989982613399, -0.0002670241078655971, -0.014299540103341937, 0.024966706727680407, -0.24507056206562802, 0.0812995518092066, 0.3999295164781966, -0.2923531840702421, -0.2792703843528503, 0.05994819661259259, -0.28470223487207763, -0.06888460233734038, 0.21152942411748593, -0.025176842423695... |
710.011 | Storage of spin squeezing in a two-component Bose-Einstein condensate | Efficient control of spin squeezing in a two-component Bose-Einstein
Condensate is studied by rapidly turning-off the external field at a time that
maximal spin squeezing appears. We show that strong reduction of spin
fluctuation can be maintained in a nearly fixed direction for a long time. We
explain the underlying... | quant-ph cond-mat.other | efficient control of spin squeezing in a twocomponent boseeinstein condensate is studied by rapidly turningoff the external field at a time that maximal spin squeezing appears we show that strong reduction of spin fluctuation can be maintained in a nearly fixed direction for a long time we explain the underlying physic... | [['efficient', 'control', 'of', 'spin', 'squeezing', 'in', 'a', 'twocomponent', 'boseeinstein', 'condensate', 'is', 'studied', 'by', 'rapidly', 'turningoff', 'the', 'external', 'field', 'at', 'a', 'time', 'that', 'maximal', 'spin', 'squeezing', 'appears', 'we', 'show', 'that', 'strong', 'reduction', 'of', 'spin', 'fluc... | [-0.2193715325711916, 0.23873150531823437, -0.10148478760772074, 0.08614310677512549, -0.007874655603275944, -0.13273486488809189, 0.030873137755164256, 0.3816754622384906, -0.2506451165303588, -0.25574340593690675, 0.07079178010656809, -0.1817651487964516, -0.07279904695848624, 0.20353501486436773, 0.03404844434310992... |
710.0111 | Enhancement of flux pinning and high critical current density in
graphite doped MgB2 superconductor | We report the synthesis and characterization of graphite (C) doped MgB2-xCx
(x = 0.0, 0.1, 0.2 and 0.3) samples. The crystal structure and microstructural
characterization have been investigated by x-ray diffractometer and
transmission electron microscopic (TEM) analysis. The superconducting
properties especially Jc ... | cond-mat.supr-con cond-mat.str-el | we report the synthesis and characterization of graphite c doped mgb2xcx x 00 01 02 and 03 samples the crystal structure and microstructural characterization have been investigated by xray diffractometer and transmission electron microscopic tem analysis the superconducting properties especially jc and hc2 have been me... | [['we', 'report', 'the', 'synthesis', 'and', 'characterization', 'of', 'graphite', 'c', 'doped', 'mgb2xcx', 'x', '00', '01', '02', 'and', '03', 'samples', 'the', 'crystal', 'structure', 'and', 'microstructural', 'characterization', 'have', 'been', 'investigated', 'by', 'xray', 'diffractometer', 'and', 'transmission', '... | [-0.11599553139793159, 0.2135575867846216, -0.018429035503330114, -0.03546426335774493, 0.0350112728107372, -0.14509352365214573, 0.10755902785693475, 0.44663579702616957, -0.17648000844716155, -0.35796415992081165, 0.036161427343896, -0.35169265652347725, -0.04085783077654434, 0.1975033166164761, 0.015176998688948302,... |
710.0112 | Improvement of conversion efficiency of atom-molecule Bose-Einstein
condensate | We investigate the stimulated Raman adiabatic passage in two-color
photoassociation for a atom-molecule Bose-Einstein condensate. By applying two
time-varying Guassian laser pulses that fulfill generalized two-photon
resonance condition, we obtain highly efficient atom-molecule conversion. The
efficiency depends on t... | quant-ph | we investigate the stimulated raman adiabatic passage in twocolor photoassociation for a atommolecule boseeinstein condensate by applying two timevarying guassian laser pulses that fulfill generalized twophoton resonance condition we obtain highly efficient atommolecule conversion the efficiency depends on the freeboun... | [['we', 'investigate', 'the', 'stimulated', 'raman', 'adiabatic', 'passage', 'in', 'twocolor', 'photoassociation', 'for', 'a', 'atommolecule', 'boseeinstein', 'condensate', 'by', 'applying', 'two', 'timevarying', 'guassian', 'laser', 'pulses', 'that', 'fulfill', 'generalized', 'twophoton', 'resonance', 'condition', 'we... | [-0.14663999058874483, 0.25476033491540256, -0.04453304136898053, 0.04535400659493092, 0.010992647030280304, -0.14488230430189583, 0.14537408867440485, 0.5095409781877267, -0.22108564251181434, -0.2627215738392482, -0.04856372938957065, -0.1879718948818617, -0.05835470303072263, 0.23421086258081308, 0.02868699450519378... |
710.0113 | Stability of nodal quasi-particles in superconductors with coexisting
orders | We establish a condition for the perturbative stability of zero energy nodal
points in the quasi-particle spectrum of superconductors in the presence of
coexisting \textit{commensurate} orders. The nodes are found to be stable if
the Hamiltonian is invariant under time reversal followed by a lattice
translation. The ... | cond-mat.supr-con cond-mat.str-el | we establish a condition for the perturbative stability of zero energy nodal points in the quasiparticle spectrum of superconductors in the presence of coexisting textitcommensurate orders the nodes are found to be stable if the hamiltonian is invariant under time reversal followed by a lattice translation the principl... | [['we', 'establish', 'a', 'condition', 'for', 'the', 'perturbative', 'stability', 'of', 'zero', 'energy', 'nodal', 'points', 'in', 'the', 'quasiparticle', 'spectrum', 'of', 'superconductors', 'in', 'the', 'presence', 'of', 'coexisting', 'textitcommensurate', 'orders', 'the', 'nodes', 'are', 'found', 'to', 'be', 'stable... | [-0.23905581006990143, 0.18572139450099687, -0.053293837358991444, 0.07250330333834068, -0.024517845598534798, -0.11622449364119643, 0.06948001861152514, 0.32833732778213026, -0.25233013371766455, -0.2471044333717248, 0.08130377434804038, -0.28391388256732425, -0.09859360023204919, 0.18356375997020324, -0.0121234121247... |
710.0114 | Reinforcement learning in market games | Financial markets investors are involved in many games -- they must interact
with other agents to achieve their goals. Among them are those directly
connected with their activity on markets but one cannot neglect other aspects
that influence human decisions and their performance as investors.
Distinguishing all subga... | q-fin.TR physics.data-an physics.soc-ph | financial markets investors are involved in many games they must interact with other agents to achieve their goals among them are those directly connected with their activity on markets but one cannot neglect other aspects that influence human decisions and their performance as investors distinguishing all subgames is ... | [['financial', 'markets', 'investors', 'are', 'involved', 'in', 'many', 'games', 'they', 'must', 'interact', 'with', 'other', 'agents', 'to', 'achieve', 'their', 'goals', 'among', 'them', 'are', 'those', 'directly', 'connected', 'with', 'their', 'activity', 'on', 'markets', 'but', 'one', 'can', 'not', 'neglect', 'other... | [-0.08360409971183716, 0.07916440463635478, -0.096628857462995, 0.10985461691834851, -0.14356877647647212, -0.19508414308604022, 0.08384357289337045, 0.46909162757748907, -0.28051736660894344, -0.3012187856551133, 0.11698962023166876, -0.30764888384146616, -0.16337215876212047, 0.15087420160522347, -0.1374652610340325,... |
710.0115 | Null Energy Condition and Dark Energy Models | Null Energy Condition (NEC) requires the equation of state (EoS) of the
universe $w_u$ satisfy $w_u\geq-1$, which implies, for instance in a universe
with matter and dark energy dominating
$w_u=w_m\Omega_m+w_{de}\Omega_{de}=w_{de}\Omega_{de}\geq-1$. In this paper we
study constraints on the dark energy models from th... | gr-qc astro-ph hep-ph hep-th | null energy condition nec requires the equation of state eos of the universe w_u satisfy w_ugeq1 which implies for instance in a universe with matter and dark energy dominating w_uw_momega_mw_deomega_dew_deomega_degeq1 in this paper we study constraints on the dark energy models from the requirement of the nec we will ... | [['null', 'energy', 'condition', 'nec', 'requires', 'the', 'equation', 'of', 'state', 'eos', 'of', 'the', 'universe', 'w_u', 'satisfy', 'w_ugeq1', 'which', 'implies', 'for', 'instance', 'in', 'a', 'universe', 'with', 'matter', 'and', 'dark', 'energy', 'dominating', 'w_uw_momega_mw_deomega_dew_deomega_degeq1', 'in', 'th... | [-0.1522364839267864, 0.16259641885545437, -0.13737352968882618, 0.11838450268709774, -0.10454865663342662, -0.18082432179689045, -0.011795267915141171, 0.265790004389194, -0.2052070102919408, -0.34623754640844295, 0.042903030541066714, -0.2315130128347262, -0.058871004702187354, 0.12562448516056487, -0.013212082672833... |
710.0116 | Distributed MIMO receiver - Achievable rates and upper bounds | In this paper we investigate the achievable rate of a system that includes a
nomadic transmitter with several antennas, which is received by multiple
agents, exhibiting independent channel gains and additive circular-symmetric
complex Gaussian noise. In the nomadic regime, we assume that the agents do not
have any de... | cs.IT math.IT | in this paper we investigate the achievable rate of a system that includes a nomadic transmitter with several antennas which is received by multiple agents exhibiting independent channel gains and additive circularsymmetric complex gaussian noise in the nomadic regime we assume that the agents do not have any decoding ... | [['in', 'this', 'paper', 'we', 'investigate', 'the', 'achievable', 'rate', 'of', 'a', 'system', 'that', 'includes', 'a', 'nomadic', 'transmitter', 'with', 'several', 'antennas', 'which', 'is', 'received', 'by', 'multiple', 'agents', 'exhibiting', 'independent', 'channel', 'gains', 'and', 'additive', 'circularsymmetric'... | [-0.19345248758817854, 0.0734694195458339, -0.050911196164958095, 0.04909110411187065, -0.06789312527650589, -0.2541509211256072, 0.1188719700763209, 0.4085907477642841, -0.27297297866579673, -0.23687809893426082, 0.12127772079721821, -0.22215047969984184, -0.1660265371794866, 0.18303377525408135, -0.10911617772760747,... |
710.0117 | The clustering coefficient and community structure of bipartite networks | Many real-world networks display a natural bipartite structure. It is
necessary and important to study the bipartite networks by using the bipartite
structure of the data. Here we propose a modification of the clustering
coefficient given by the fraction of cycles with size four in bipartite
networks. Then we compare... | physics.soc-ph | many realworld networks display a natural bipartite structure it is necessary and important to study the bipartite networks by using the bipartite structure of the data here we propose a modification of the clustering coefficient given by the fraction of cycles with size four in bipartite networks then we compare the t... | [['many', 'realworld', 'networks', 'display', 'a', 'natural', 'bipartite', 'structure', 'it', 'is', 'necessary', 'and', 'important', 'to', 'study', 'the', 'bipartite', 'networks', 'by', 'using', 'the', 'bipartite', 'structure', 'of', 'the', 'data', 'here', 'we', 'propose', 'a', 'modification', 'of', 'the', 'clustering'... | [-0.13755642764292794, 0.05127571378728713, -0.06113656735132364, 0.06426790428337302, -0.04946521187031811, -0.12366238960318944, 0.003943699377652427, 0.4044002862647176, -0.28254709528317273, -0.29431546719702467, 0.08788035680481698, -0.2835561415545685, -0.25890634111552074, 0.12183285355356267, -0.034907345396938... |
710.0118 | Pion and kaon production in central Pb+Pb collisions at 20A and 30A GeV:
Evidence for the onset of deconfinement | Results on charged pion and kaon production in central Pb+Pb collisions at
20A and 30A GeV are presented and compared to data at lower and higher
energies. A rapid change of the energy dependence is observed around 30A GeV
for the yields of pions and kaons as well as for the shape of the transverse
mass spectra. The ... | nucl-ex | results on charged pion and kaon production in central pbpb collisions at 20a and 30a gev are presented and compared to data at lower and higher energies a rapid change of the energy dependence is observed around 30a gev for the yields of pions and kaons as well as for the shape of the transverse mass spectra the chang... | [['results', 'on', 'charged', 'pion', 'and', 'kaon', 'production', 'in', 'central', 'pbpb', 'collisions', 'at', '20a', 'and', '30a', 'gev', 'are', 'presented', 'and', 'compared', 'to', 'data', 'at', 'lower', 'and', 'higher', 'energies', 'a', 'rapid', 'change', 'of', 'the', 'energy', 'dependence', 'is', 'observed', 'aro... | [-0.028561793513786557, 0.2647957929452373, -0.12022247599088587, 0.14246755014888055, 0.05281721923330968, -0.09181376050268723, -0.024472239638932726, 0.34228818072006106, -0.12503875308373774, -0.3405307367105376, -0.012787240574570287, -0.38113663204818626, 0.1416181134250523, 0.1794352121968669, 0.0636580014093355... |
710.0119 | Precise measurements of electron and hole g-factors of single quantum
dots by using nuclear field | We demonstrated the cancellation of the external magnetic field by the
nuclear field at one edge of the nuclear polarization bistability in single
InAlAs quantum dots. The cancellation for the electron Zeeman splitting gives
the precise value of the hole g-factor. By combining with the exciton g-factor
that is obtain... | cond-mat.mtrl-sci cond-mat.other | we demonstrated the cancellation of the external magnetic field by the nuclear field at one edge of the nuclear polarization bistability in single inalas quantum dots the cancellation for the electron zeeman splitting gives the precise value of the hole gfactor by combining with the exciton gfactor that is obtained fro... | [['we', 'demonstrated', 'the', 'cancellation', 'of', 'the', 'external', 'magnetic', 'field', 'by', 'the', 'nuclear', 'field', 'at', 'one', 'edge', 'of', 'the', 'nuclear', 'polarization', 'bistability', 'in', 'single', 'inalas', 'quantum', 'dots', 'the', 'cancellation', 'for', 'the', 'electron', 'zeeman', 'splitting', '... | [-0.18916221229812583, 0.19747680919622448, 0.008001564253071273, 0.03997478770828378, 0.01180207187536399, -0.12964743390880726, -0.0011047802116671526, 0.4003474059879679, -0.23878392125983294, -0.3320702379128921, -0.019485798233339714, -0.24999577091453043, -0.010503737029392977, 0.23329460671221888, 0.082905454318... |
710.012 | Magnetic Strings in Einstein-Born-Infeld-Dilaton Gravity | A class of spinning magnetic string in 4-dimensional Einstein-dilaton gravity
with Liouville type potential which produces a longitudinal nonlinear
electromagnetic field is presented. These solutions have no curvature
singularity and no horizon, but have a conic geometry. In these spacetimes,
when the rotation parame... | hep-th | a class of spinning magnetic string in 4dimensional einsteindilaton gravity with liouville type potential which produces a longitudinal nonlinear electromagnetic field is presented these solutions have no curvature singularity and no horizon but have a conic geometry in these spacetimes when the rotation parameter does... | [['a', 'class', 'of', 'spinning', 'magnetic', 'string', 'in', '4dimensional', 'einsteindilaton', 'gravity', 'with', 'liouville', 'type', 'potential', 'which', 'produces', 'a', 'longitudinal', 'nonlinear', 'electromagnetic', 'field', 'is', 'presented', 'these', 'solutions', 'have', 'no', 'curvature', 'singularity', 'and... | [-0.19085338994821843, 0.14793819029691804, -0.0680246658079947, 0.07476684631546959, -0.12065127715468407, -0.15825272294071813, -0.047235773286471765, 0.3286259218274305, -0.17902578711509703, -0.256536618397998, 0.1066472647439999, -0.293812309888502, -0.12745643489373226, 0.1557770168563972, -0.05691747411619872, 0... |
710.0121 | On Isomorphism Classes and Invariants of Low Dimensional Complex
Filiform Leibniz Algebras (PART 1) | The paper aims to investigate the classification problem of low dimensional
complex none Lie filiform Leibniz algebras. There are two sources to get
classification of filiform Leibniz algebras. The first of them is the naturally
graded none Lie filiform Leibniz algebras and the another one is the naturally
graded fil... | math.RA math.AG | the paper aims to investigate the classification problem of low dimensional complex none lie filiform leibniz algebras there are two sources to get classification of filiform leibniz algebras the first of them is the naturally graded none lie filiform leibniz algebras and the another one is the naturally graded filifor... | [['the', 'paper', 'aims', 'to', 'investigate', 'the', 'classification', 'problem', 'of', 'low', 'dimensional', 'complex', 'none', 'lie', 'filiform', 'leibniz', 'algebras', 'there', 'are', 'two', 'sources', 'to', 'get', 'classification', 'of', 'filiform', 'leibniz', 'algebras', 'the', 'first', 'of', 'them', 'is', 'the',... | [-0.1418245449343598, 0.029802423309248344, 0.016881768012688935, 0.07665006768289268, -0.17599215764417558, -0.1562003044956854, -0.060589259853402744, 0.40271239141829457, -0.3585713963448621, -0.24232590093130343, 0.14233119874782124, -0.2154216643631164, -0.16281158744210475, 0.18338458756012474, -0.169695554376199... |
710.0122 | A canonical bundle formular of projective Lagrangian fibrations | We classify singular fibres of a projective Lagrangian fibration over
codimension one points. As an application, we obtain a canonical bundle formula
for a projective Lagrangian fibration over a smooth manifold.
| math.AG | we classify singular fibres of a projective lagrangian fibration over codimension one points as an application we obtain a canonical bundle formula for a projective lagrangian fibration over a smooth manifold | [['we', 'classify', 'singular', 'fibres', 'of', 'a', 'projective', 'lagrangian', 'fibration', 'over', 'codimension', 'one', 'points', 'as', 'an', 'application', 'we', 'obtain', 'a', 'canonical', 'bundle', 'formula', 'for', 'a', 'projective', 'lagrangian', 'fibration', 'over', 'a', 'smooth', 'manifold']] | [-0.2969615710598807, -0.11373315350060546, -0.13541664820044272, 0.07072901034787778, -0.12318608891819754, -0.19819940308169012, -0.04451482208265412, 0.3314800328545032, -0.30396005583386265, -0.08516468077657684, 0.05761507688270461, -0.2261705507314013, -0.15510939025590498, 0.2278377959024041, -0.23113648776686, ... |
710.0123 | Bottom Baryons | Recently CDF and D0 collaborations observed several bottom baryons. In this
work we perform a systematic study of the masses of bottom baryons up to
$1/m_Q$ in the framework of heavy quark effective field theory (HQET) using the
QCD sum rule approach. The extracted chromo-magnetic splitting between the
bottom baryon ... | hep-ph hep-ex nucl-ex nucl-th | recently cdf and d0 collaborations observed several bottom baryons in this work we perform a systematic study of the masses of bottom baryons up to 1m_q in the framework of heavy quark effective field theory hqet using the qcd sum rule approach the extracted chromomagnetic splitting between the bottom baryon heavy doub... | [['recently', 'cdf', 'and', 'd0', 'collaborations', 'observed', 'several', 'bottom', 'baryons', 'in', 'this', 'work', 'we', 'perform', 'a', 'systematic', 'study', 'of', 'the', 'masses', 'of', 'bottom', 'baryons', 'up', 'to', '1m_q', 'in', 'the', 'framework', 'of', 'heavy', 'quark', 'effective', 'field', 'theory', 'hqet... | [-0.043327806421138086, 0.2277614633103126, -0.08779170356112821, 0.1543776574524537, -0.06107935071762266, -0.07247018061803076, 0.13470791997026715, 0.30166991893202066, -0.16918884294011213, -0.31649100700200633, -0.07421645619866342, -0.34685905130002004, 0.02466802759866776, 0.043442487267070805, 0.102522918553059... |
710.0124 | Modeling Lepton-Nucleon Inelastic Scattering from High to Low Momentum
Transfer | We present a model for inclusive charged lepton-nucleon and
(anti)neutrino-nucleon cross sections at momentum transfer squared, $Q^2$,
$\sim1 {\rm GeV}^2$. We quantify the impact of existing low-Q charged-lepton
deep-inelastic scattering (DIS) data on effects due to high-twist operators and
on the extraction of parto... | hep-ph | we present a model for inclusive charged leptonnucleon and antineutrinonucleon cross sections at momentum transfer squared q2 sim1 rm gev2 we quantify the impact of existing lowq chargedlepton deepinelastic scattering dis data on effects due to hightwist operators and on the extraction of parton distribution functions ... | [['we', 'present', 'a', 'model', 'for', 'inclusive', 'charged', 'leptonnucleon', 'and', 'antineutrinonucleon', 'cross', 'sections', 'at', 'momentum', 'transfer', 'squared', 'q2', 'sim1', 'rm', 'gev2', 'we', 'quantify', 'the', 'impact', 'of', 'existing', 'lowq', 'chargedlepton', 'deepinelastic', 'scattering', 'dis', 'da... | [-0.053755017261054104, 0.15437258181056157, -0.09259819478195692, 0.18558753076441853, -0.010733502685824143, -0.02323687602433243, 0.03641183737033446, 0.3766688128135034, -0.188906029635109, -0.22713426761329175, -0.013167107316465781, -0.370389069670013, 0.04932551269885153, 0.1511736676878562, 0.048819023003722706... |
710.0125 | On regular configurations and disjoint cycles in shift graphs | Configurations are necklaces with prescribed numbers of red and black beads.
Among all possible configurations, the regular one plays an important role in
many applications. In this paper, several aspects of regular configurations are
discussed, including construction, uniqueness, symmetry group and the link with
bal... | math.CO | configurations are necklaces with prescribed numbers of red and black beads among all possible configurations the regular one plays an important role in many applications in this paper several aspects of regular configurations are discussed including construction uniqueness symmetry group and the link with balanced wor... | [['configurations', 'are', 'necklaces', 'with', 'prescribed', 'numbers', 'of', 'red', 'and', 'black', 'beads', 'among', 'all', 'possible', 'configurations', 'the', 'regular', 'one', 'plays', 'an', 'important', 'role', 'in', 'many', 'applications', 'in', 'this', 'paper', 'several', 'aspects', 'of', 'regular', 'configura... | [-0.22509495942638472, 0.1780318024398434, -0.0037269246493271744, 0.07431466274403527, -0.0460671622582435, -0.11324698133087092, 0.006255751200644606, 0.37050890936874425, -0.22950395849625488, -0.3198733731725632, 0.10831605554123379, -0.2727040871056718, -0.15351135502722893, 0.1976986654380408, -0.0653330612477365... |
710.0126 | Reduced Weyl asymptotics for pseudodifferential operators on bounded
domains II. The compact group case | Let $G\subset \O(n)$ be a compact group of isometries acting on
$n$-dimensional Euclidean space $\R^n$, and ${\bf{X}}$ a bounded domain in
$\R^n$ which is transformed into itself under the action of $G$. Consider a
symmetric, classical pseudodifferential operator $A_0$ in $\L^2(\R^n)$ that
commutes with the regular r... | math.AP math.SP | let gsubset on be a compact group of isometries acting on ndimensional euclidean space rn and bfx a bounded domain in rn which is transformed into itself under the action of g consider a symmetric classical pseudodifferential operator a_0 in l2rn that commutes with the regular representation of g and assume that it is ... | [['let', 'gsubset', 'on', 'be', 'a', 'compact', 'group', 'of', 'isometries', 'acting', 'on', 'ndimensional', 'euclidean', 'space', 'rn', 'and', 'bfx', 'a', 'bounded', 'domain', 'in', 'rn', 'which', 'is', 'transformed', 'into', 'itself', 'under', 'the', 'action', 'of', 'g', 'consider', 'a', 'symmetric', 'classical', 'ps... | [-0.14771193044171446, 0.10263815462253877, -0.09165080489359517, 0.02356236013995648, -0.10681866792341073, -0.11227282470561006, -0.008851009345024216, 0.3379757709319697, -0.28952868536057674, -0.1585111815108582, 0.1472568052074853, -0.3081042194726313, -0.11965036981613977, 0.19358776876588865, -0.0830472782428446... |
710.0127 | Difficulty in the Fermi-Liquid-Based Theory for the In-Plane Magnetic
Anisotropy in Untwinned High-T_c Superconductor | Recently, Eremin and Manske [1] presented a oneband Fermi-liquid theory for
the in-plane magnetic anisotropy in untwinned high-Tc superconductor
YBa2Cu3O6:85 (YBCO). They claimed that they found good agreement with inelastic
neutron scattering (INS) spectra. In this Comment, we point out that their
conclusion on this... | cond-mat.supr-con cond-mat.str-el | recently eremin and manske 1 presented a oneband fermiliquid theory for the inplane magnetic anisotropy in untwinned hightc superconductor yba2cu3o685 ybco they claimed that they found good agreement with inelastic neutron scattering ins spectra in this comment we point out that their conclusion on this important probl... | [['recently', 'eremin', 'and', 'manske', '1', 'presented', 'a', 'oneband', 'fermiliquid', 'theory', 'for', 'the', 'inplane', 'magnetic', 'anisotropy', 'in', 'untwinned', 'hightc', 'superconductor', 'yba2cu3o685', 'ybco', 'they', 'claimed', 'that', 'they', 'found', 'good', 'agreement', 'with', 'inelastic', 'neutron', 's... | [-0.127516924651994, 0.13115471387234343, -0.09729267886422317, 0.09093951061669063, -0.07359373656197868, -0.15270723978956713, 0.11081747686117084, 0.41836198369554917, -0.2149000859112832, -0.3084659356110055, 0.00037536541389397764, -0.3782894066695509, -0.08256978142990506, 0.19947118451668286, -0.0533677977670369... |
710.0128 | Investigation of the Faraday Rotation Measure and Magnetic Field
Structures of Several AGN Jets on Sub-Parsec to Parsec Scales | Preliminary VLBA polarisation results on 6 ``blazars'' from 6.5-cm to 7-mm
are presented here. Observing at several different wavelengths, separated by
short and long intervals, enabled reliable information about the magnetic (B)
field structure to be obtained and for the effect of Faraday Rotation to be
determined a... | astro-ph | preliminary vlba polarisation results on 6 blazars from 65cm to 7mm are presented here observing at several different wavelengths separated by short and long intervals enabled reliable information about the magnetic b field structure to be obtained and for the effect of faraday rotation to be determined and corrected f... | [['preliminary', 'vlba', 'polarisation', 'results', 'on', '6', 'blazars', 'from', '65cm', 'to', '7mm', 'are', 'presented', 'here', 'observing', 'at', 'several', 'different', 'wavelengths', 'separated', 'by', 'short', 'and', 'long', 'intervals', 'enabled', 'reliable', 'information', 'about', 'the', 'magnetic', 'b', 'fie... | [-0.1339452370118938, 0.14007024295824522, -0.04327066249128333, 0.09260559262704766, -0.08167496447659735, -0.09775210438161402, 0.002502445825436888, 0.4511279036339961, -0.204162200174515, -0.33835945813916624, 0.07364697595307677, -0.21881325970599919, 0.03691021198602883, 0.24463448507441699, 0.000669787905759509,... |
710.0129 | Existence and mutiplicity of solutions to elliptic equations of fourth
order on compact manifolds | This paper deals with a fourth order elliptic equation on compact Riemannian
manifolds.We establish the existence of solutions to the equation with critical
Sobolev growth which is the subject of the first theorem. In the second one, we
prove the multiplicity of solutions in the subcritical case.
| math.AP | this paper deals with a fourth order elliptic equation on compact riemannian manifoldswe establish the existence of solutions to the equation with critical sobolev growth which is the subject of the first theorem in the second one we prove the multiplicity of solutions in the subcritical case | [['this', 'paper', 'deals', 'with', 'a', 'fourth', 'order', 'elliptic', 'equation', 'on', 'compact', 'riemannian', 'manifoldswe', 'establish', 'the', 'existence', 'of', 'solutions', 'to', 'the', 'equation', 'with', 'critical', 'sobolev', 'growth', 'which', 'is', 'the', 'subject', 'of', 'the', 'first', 'theorem', 'in', ... | [-0.19098058164767598, 0.01740117704131357, -0.08025732701239378, 0.038555169882981674, -0.07921382667415816, -0.0755530831343292, -0.05802552066692759, 0.19959915754304308, -0.26024083886295557, -0.21466784604379666, 0.16451270105418467, -0.32752021843486506, -0.0951446119857871, 0.1806592770507964, -0.077632139214193... |
710.013 | Tests \`a la Hurewicz dans le plan | We give, for some Borel sets of a product of two Polish spaces, including the
Borel sets with countable sections, a Hurewicz-like characterization of those
which cannot become a transfinite difference of open sets by changing the two
Polish topologies.
| math.LO math.GN | we give for some borel sets of a product of two polish spaces including the borel sets with countable sections a hurewiczlike characterization of those which cannot become a transfinite difference of open sets by changing the two polish topologies | [['we', 'give', 'for', 'some', 'borel', 'sets', 'of', 'a', 'product', 'of', 'two', 'polish', 'spaces', 'including', 'the', 'borel', 'sets', 'with', 'countable', 'sections', 'a', 'hurewiczlike', 'characterization', 'of', 'those', 'which', 'can', 'not', 'become', 'a', 'transfinite', 'difference', 'of', 'open', 'sets', 'b... | [-0.15052906632218965, 0.18972976506892136, -0.085806169842438, 0.15672335130866707, -0.05851722449609419, -0.03872947721378651, 0.1003682447551954, 0.3766339167770816, -0.2707343887446857, -0.1805023423895785, 0.14211454059610643, -0.29264277092567303, -0.019081684579027862, 0.30254087348542424, -0.09637755557622124, ... |
710.0131 | Uniformisations partielles et crit\`eres \`a la Hurewicz dans le plan | We give characterizations of the Borel sets potentially in some Wadge class,
among the Borel sets with countable vertical sections of a product of two
Polish spaces. To do this, we use some partial uniformization results.
| math.LO math.GN | we give characterizations of the borel sets potentially in some wadge class among the borel sets with countable vertical sections of a product of two polish spaces to do this we use some partial uniformization results | [['we', 'give', 'characterizations', 'of', 'the', 'borel', 'sets', 'potentially', 'in', 'some', 'wadge', 'class', 'among', 'the', 'borel', 'sets', 'with', 'countable', 'vertical', 'sections', 'of', 'a', 'product', 'of', 'two', 'polish', 'spaces', 'to', 'do', 'this', 'we', 'use', 'some', 'partial', 'uniformization', 're... | [-0.15279947965690452, 0.09461258829105645, -0.05715369813454648, 0.13869602836914258, -0.12561523650462428, -0.024128616101936333, 0.09444942247743408, 0.4050355082533012, -0.29068120708689094, -0.14190086409346098, 0.08692072311532684, -0.30952671118494535, -0.0580138528926505, 0.25888599565789466, -0.143683278027714... |
710.0132 | Classes de Wadge potentielles des bor\'eliens \`a coupes d\'enombrables | We give, for each non self-dual Wadge class C contained in the class of the
Gdelta sets, a characterization of Borel sets which are not potentially in C,
among Borel sets with countable vertical sections; to do this, we use results
of partial uniformization.
| math.LO math.GN | we give for each non selfdual wadge class c contained in the class of the gdelta sets a characterization of borel sets which are not potentially in c among borel sets with countable vertical sections to do this we use results of partial uniformization | [['we', 'give', 'for', 'each', 'non', 'selfdual', 'wadge', 'class', 'c', 'contained', 'in', 'the', 'class', 'of', 'the', 'gdelta', 'sets', 'a', 'characterization', 'of', 'borel', 'sets', 'which', 'are', 'not', 'potentially', 'in', 'c', 'among', 'borel', 'sets', 'with', 'countable', 'vertical', 'sections', 'to', 'do', '... | [-0.15525804366387258, 0.06731907056051899, -0.01760164493779567, 0.06413112134958449, -0.10025081389837644, -0.08824457798618823, 0.08116122610359029, 0.3617098626723005, -0.2819320263171738, -0.15967256564181298, 0.055435451239728456, -0.29341946982524614, -0.04378122713586146, 0.23415528517613315, -0.108672138959677... |
710.0133 | Classes de Wadge potentielles et th\'eor\`emes d'uniformisation
partielle | We want to give a construction as simple as possible of a Borel subset of a
product of two Polish spaces. This introduces the notion of potential Wadge
class. Among other things, we study the non-potentially closed sets, by proving
Hurewicz-like results. This leads to partial uniformization theorems, on big
sets, in ... | math.LO math.GN | we want to give a construction as simple as possible of a borel subset of a product of two polish spaces this introduces the notion of potential wadge class among other things we study the nonpotentially closed sets by proving hurewiczlike results this leads to partial uniformization theorems on big sets in the sense o... | [['we', 'want', 'to', 'give', 'a', 'construction', 'as', 'simple', 'as', 'possible', 'of', 'a', 'borel', 'subset', 'of', 'a', 'product', 'of', 'two', 'polish', 'spaces', 'this', 'introduces', 'the', 'notion', 'of', 'potential', 'wadge', 'class', 'among', 'other', 'things', 'we', 'study', 'the', 'nonpotentially', 'close... | [-0.15713559038210975, 0.04784448305934162, -0.058005071339844644, 0.11578265935482489, -0.12468956032041777, -0.0898277868864016, 0.11331985841339486, 0.3133028877693844, -0.31655046226993455, -0.19308259098206537, 0.07124351509807283, -0.2755032709278798, -0.11867310372339088, 0.2130222363452727, -0.1910173987843475,... |
710.0134 | Complexit\'e des bor\'eliens \`a coupes d\'enombrables | We give, for each level of complexity L, a Hurewicz-like characterization of
the Borel subsets with countable sections of a product of two Polish spaces
that cannot become in L by changing the two Polish topologies.
| math.LO math.GN | we give for each level of complexity l a hurewiczlike characterization of the borel subsets with countable sections of a product of two polish spaces that cannot become in l by changing the two polish topologies | [['we', 'give', 'for', 'each', 'level', 'of', 'complexity', 'l', 'a', 'hurewiczlike', 'characterization', 'of', 'the', 'borel', 'subsets', 'with', 'countable', 'sections', 'of', 'a', 'product', 'of', 'two', 'polish', 'spaces', 'that', 'can', 'not', 'become', 'in', 'l', 'by', 'changing', 'the', 'two', 'polish', 'topolog... | [-0.1738725146970938, 0.19424408932241635, -0.06813158734223328, 0.10129540073811202, -0.056894147617591394, -0.08629862738244638, 0.09625683896042206, 0.385648455974218, -0.24100157991051674, -0.19917432052662243, 0.09471120664887633, -0.252534615228305, -0.03101150824914913, 0.24936620925232214, -0.08110848240352966,... |
710.0135 | Neutralino Annihilations and the Gas Temperature in the Dark Ages | Assuming the dark matter is made entirely from neutralinos, we re-visit the
role of their annihilation on the temperature of diffuse gas in the high
redshift universe. We consider neutralinos of particle mass 36 GeV and 100 GeV,
respectively. The former is able to produce ~7 electron/positron particles per
annihilati... | astro-ph | assuming the dark matter is made entirely from neutralinos we revisit the role of their annihilation on the temperature of diffuse gas in the high redshift universe we consider neutralinos of particle mass 36 gev and 100 gev respectively the former is able to produce 7 electronpositron particles per annihilation throug... | [['assuming', 'the', 'dark', 'matter', 'is', 'made', 'entirely', 'from', 'neutralinos', 'we', 'revisit', 'the', 'role', 'of', 'their', 'annihilation', 'on', 'the', 'temperature', 'of', 'diffuse', 'gas', 'in', 'the', 'high', 'redshift', 'universe', 'we', 'consider', 'neutralinos', 'of', 'particle', 'mass', '36', 'gev', ... | [-0.0978982318560218, 0.27647226319452983, -0.05872001551817787, 0.13018725607256998, -0.006713994278501467, -0.06706018596335109, 0.024015938140988603, 0.357955427937036, -0.21075763358237318, -0.34230144778108695, -0.006675731789042494, -0.3121388587919143, 0.10108993532949016, 0.18039130021682823, 0.0819583603899168... |
710.0136 | A Simple Model for Cavity Enhanced Slow Lights in Vertical Cavity
Surface Emission Lasers | We develop a simple model for the slow lights in Vertical Cavity Surface
Emission Lasers (VCSELs), with the combination of cavity and population
pulsation effects. The dependences of probe signal power, injection bias
current and wavelength detuning for the group delays are demonstrated
numerically and experimentally... | physics.optics | we develop a simple model for the slow lights in vertical cavity surface emission lasers vcsels with the combination of cavity and population pulsation effects the dependences of probe signal power injection bias current and wavelength detuning for the group delays are demonstrated numerically and experimentally up to ... | [['we', 'develop', 'a', 'simple', 'model', 'for', 'the', 'slow', 'lights', 'in', 'vertical', 'cavity', 'surface', 'emission', 'lasers', 'vcsels', 'with', 'the', 'combination', 'of', 'cavity', 'and', 'population', 'pulsation', 'effects', 'the', 'dependences', 'of', 'probe', 'signal', 'power', 'injection', 'bias', 'curre... | [-0.15677048265594445, 0.17382151450340946, -0.041397505071169384, -0.01763751867110841, -0.03405456265900284, -0.16731068288208917, 0.06749668971557791, 0.4799749377804498, -0.25449648119683843, -0.31958958942753574, 0.06392652069722923, -0.23226365180065234, -0.061265632793462525, 0.27922477769316173, -0.007506414446... |
710.0137 | The B and Be Star Population of NGC 3766 | We present multiple epochs of H-alpha spectroscopy for 47 members of the open
cluster NGC 3766 to investigate the long term variability of its Be stars.
Sixteen of the stars in this sample are Be stars, including one new discovery.
Of these, we observe an unprecedented 11 Be stars that undergo disk appearances
and/or... | astro-ph | we present multiple epochs of halpha spectroscopy for 47 members of the open cluster ngc 3766 to investigate the long term variability of its be stars sixteen of the stars in this sample are be stars including one new discovery of these we observe an unprecedented 11 be stars that undergo disk appearances andor near di... | [['we', 'present', 'multiple', 'epochs', 'of', 'halpha', 'spectroscopy', 'for', '47', 'members', 'of', 'the', 'open', 'cluster', 'ngc', '3766', 'to', 'investigate', 'the', 'long', 'term', 'variability', 'of', 'its', 'be', 'stars', 'sixteen', 'of', 'the', 'stars', 'in', 'this', 'sample', 'are', 'be', 'stars', 'including... | [-0.060565040960057596, 0.13810619011878178, -0.10671211605000755, 0.07478250758924886, -0.11754460058822903, -0.07351482604508815, 0.07660911344801602, 0.43435383129702965, -0.1972624380946281, -0.3476903348715733, 0.0800690235964873, -0.2832361200986349, -0.040332638068408096, 0.1997118700336179, -0.08449650920887032... |
710.0138 | K-matrix and Dalitz plot analysis from FOCUS | Dalitz analysis is a powerful tool for physics studies within and beyond the
Standard Model. In the last decade it has helped to investigate the Heavy
Flavor hadronic decay dynamics and is now being applied to extract angles of
the CKM Unitarity triangle. To perform such sophisticate analyses we need to
model the str... | hep-ex | dalitz analysis is a powerful tool for physics studies within and beyond the standard model in the last decade it has helped to investigate the heavy flavor hadronic decay dynamics and is now being applied to extract angles of the ckm unitarity triangle to perform such sophisticate analyses we need to model the strong ... | [['dalitz', 'analysis', 'is', 'a', 'powerful', 'tool', 'for', 'physics', 'studies', 'within', 'and', 'beyond', 'the', 'standard', 'model', 'in', 'the', 'last', 'decade', 'it', 'has', 'helped', 'to', 'investigate', 'the', 'heavy', 'flavor', 'hadronic', 'decay', 'dynamics', 'and', 'is', 'now', 'being', 'applied', 'to', '... | [-0.016593476995191675, 0.14233773158605587, -0.14824274100085838, 0.13869126829903256, -0.11052984058698441, -0.16502313163785381, 0.04058715112586605, 0.3570216820634743, -0.227890608614271, -0.27246949118760194, 0.07896297840163746, -0.32629351582913163, -0.07870891054490324, 0.17930397196633227, 0.05950315404891413... |
710.0139 | Getting a kick out of the stellar disk(s) in the galactic center | Recent observations of the Galactic center revealed a nuclear disk of young
OB stars, in addition to many similar outlying stars with higher eccentricities
and/or high inclinations relative to the disk (some of them possibly belonging
to a second disk). Binaries in such nuclear disks, if they exist in
non-negligible ... | astro-ph | recent observations of the galactic center revealed a nuclear disk of young ob stars in addition to many similar outlying stars with higher eccentricities andor high inclinations relative to the disk some of them possibly belonging to a second disk binaries in such nuclear disks if they exist in nonnegligible fractions... | [['recent', 'observations', 'of', 'the', 'galactic', 'center', 'revealed', 'a', 'nuclear', 'disk', 'of', 'young', 'ob', 'stars', 'in', 'addition', 'to', 'many', 'similar', 'outlying', 'stars', 'with', 'higher', 'eccentricities', 'andor', 'high', 'inclinations', 'relative', 'to', 'the', 'disk', 'some', 'of', 'them', 'po... | [-0.0912963180243969, 0.1636469665840268, -0.06565164473373443, 0.1182432419611141, -0.10114898698963225, -0.013380916610360146, 0.055083318188786506, 0.4127355565801263, -0.19359011525288225, -0.3345079580396414, 0.03819993904326111, -0.268777191221714, -0.03468709472753108, 0.2042723520938307, -0.08640329365991056, -... |
710.014 | High density effective theory on the lattice | Long-range interactions in finite density QCD necessitate a non-perturbative
approach in order to reliably map out the key features and spectrum of the QCD
phase diagram. However, the complex nature of the fermion determinant in this
sector prohibits the use of established Monte Carlo techniques that utilize
importan... | hep-lat | longrange interactions in finite density qcd necessitate a nonperturbative approach in order to reliably map out the key features and spectrum of the qcd phase diagram however the complex nature of the fermion determinant in this sector prohibits the use of established monte carlo techniques that utilize importance sam... | [['longrange', 'interactions', 'in', 'finite', 'density', 'qcd', 'necessitate', 'a', 'nonperturbative', 'approach', 'in', 'order', 'to', 'reliably', 'map', 'out', 'the', 'key', 'features', 'and', 'spectrum', 'of', 'the', 'qcd', 'phase', 'diagram', 'however', 'the', 'complex', 'nature', 'of', 'the', 'fermion', 'determin... | [-0.08850166810307282, 0.14602034325870844, -0.12214971772816687, 0.07228817534213466, -0.022873885294019774, -0.06008197776637636, 0.0725786753548393, 0.37760623388395115, -0.25069272311127466, -0.3071124084495209, 0.09596656427848749, -0.27528852252037944, -0.10977569194762288, 0.09740304247148938, -0.000323012028873... |
710.0141 | Dense gas in luminous infrared galaxies | Molecules that trace the high-density regions of the interstellar medium have
been observed in (ultra-)luminous (far-)infrared galaxies, in order to initiate
multiple-molecule multiple-transition studies to evaluate the physical and
chemical environment of the nuclear medium and its response to the ongoing
nuclear ac... | astro-ph | molecules that trace the highdensity regions of the interstellar medium have been observed in ultraluminous farinfrared galaxies in order to initiate multiplemolecule multipletransition studies to evaluate the physical and chemical environment of the nuclear medium and its response to the ongoing nuclear activity the h... | [['molecules', 'that', 'trace', 'the', 'highdensity', 'regions', 'of', 'the', 'interstellar', 'medium', 'have', 'been', 'observed', 'in', 'ultraluminous', 'farinfrared', 'galaxies', 'in', 'order', 'to', 'initiate', 'multiplemolecule', 'multipletransition', 'studies', 'to', 'evaluate', 'the', 'physical', 'and', 'chemica... | [-0.04655952379914981, 0.05286007816356545, -0.03677647582368355, 0.08667800568294512, -0.012599922672204802, -0.01984825946465996, -0.001771886219308211, 0.5081807310030811, -0.11468322238127157, -0.3196918606445882, 0.07323812359992436, -0.292015712169898, -0.019242465490679865, 0.13116748158004393, 0.047295621547069... |
710.0142 | LDPC codes in the McEliece cryptosystem: attacks and countermeasures | The McEliece cryptosystem is a public-key cryptosystem based on coding theory
that has successfully resisted cryptanalysis for thirty years. The original
version, based on Goppa codes, is able to guarantee a high level of security,
and is faster than competing solutions, like RSA. Despite this, it has been
rarely con... | cs.IT math.IT | the mceliece cryptosystem is a publickey cryptosystem based on coding theory that has successfully resisted cryptanalysis for thirty years the original version based on goppa codes is able to guarantee a high level of security and is faster than competing solutions like rsa despite this it has been rarely considered in... | [['the', 'mceliece', 'cryptosystem', 'is', 'a', 'publickey', 'cryptosystem', 'based', 'on', 'coding', 'theory', 'that', 'has', 'successfully', 'resisted', 'cryptanalysis', 'for', 'thirty', 'years', 'the', 'original', 'version', 'based', 'on', 'goppa', 'codes', 'is', 'able', 'to', 'guarantee', 'a', 'high', 'level', 'of'... | [-0.1642961627246974, 0.003821278298828151, -0.08346773601843877, 0.09388097335507158, -0.028810954074791298, -0.302656133721763, 0.031553557386949455, 0.3425427091293214, -0.28152370286034234, -0.28054480112006835, 0.1716948667708637, -0.2507653088353044, -0.16535327435570507, 0.22128385813490822, -0.18943993417498298... |
710.0143 | Generalized Taylor's Theorem | The Euclidean algorithm makes possible a simple but powerful generalization
of Taylor's theorem. Instead of expanding a function in a series around a
single point, one spreads out the spectrum to include any number of points with
given multiplicities. Taken together with a simple expression for the
remainder, this th... | math.NA | the euclidean algorithm makes possible a simple but powerful generalization of taylors theorem instead of expanding a function in a series around a single point one spreads out the spectrum to include any number of points with given multiplicities taken together with a simple expression for the remainder this theorem b... | [['the', 'euclidean', 'algorithm', 'makes', 'possible', 'a', 'simple', 'but', 'powerful', 'generalization', 'of', 'taylors', 'theorem', 'instead', 'of', 'expanding', 'a', 'function', 'in', 'a', 'series', 'around', 'a', 'single', 'point', 'one', 'spreads', 'out', 'the', 'spectrum', 'to', 'include', 'any', 'number', 'of'... | [-0.09530748616837498, 0.009625077944448484, -0.1989249629234629, 0.1295775721830848, -0.07796291435536529, -0.15045363140691603, 0.11391825781070761, 0.31674853919872215, -0.252909792454115, -0.23627022712358406, 0.08967582833886678, -0.2546153237045343, -0.14626868404448032, 0.2570782199585145, -0.029703119304031134,... |
710.0144 | Two Digit Theorems | We prove that if p is a prime with a primitive root 2 then S_p(2^p)=p and
give a sufficient condition for an equality of kind S_p(2^p)=+or-p.
| math.NT | we prove that if p is a prime with a primitive root 2 then s_p2pp and give a sufficient condition for an equality of kind s_p2porp | [['we', 'prove', 'that', 'if', 'p', 'is', 'a', 'prime', 'with', 'a', 'primitive', 'root', '2', 'then', 's_p2pp', 'and', 'give', 'a', 'sufficient', 'condition', 'for', 'an', 'equality', 'of', 'kind', 's_p2porp']] | [-0.18485373724251986, 0.14213156741425337, -0.14601035066880286, 0.07940136911444522, -0.08404257451184094, -0.21713180096897608, -0.007145622609338413, 0.2485206005318711, -0.3226914778351784, -0.2190652156326299, 0.1220338920247741, -0.23376704876621565, -0.16748917855632803, 0.18902811237300435, -0.0778580575327699... |
710.0145 | Applications of integral transforms in fractional diffusion processes | The fundamental solution (Green function) for the Cauchy problem of the
space-time fractional diffusion equation is investigated with respect to its
scaling and similarity properties, starting from its Fourier-Laplace
representation. Then, by using the Mellin transform, a general representation
of the Green function ... | math.PR math.CV | the fundamental solution green function for the cauchy problem of the spacetime fractional diffusion equation is investigated with respect to its scaling and similarity properties starting from its fourierlaplace representation then by using the mellin transform a general representation of the green function in terms o... | [['the', 'fundamental', 'solution', 'green', 'function', 'for', 'the', 'cauchy', 'problem', 'of', 'the', 'spacetime', 'fractional', 'diffusion', 'equation', 'is', 'investigated', 'with', 'respect', 'to', 'its', 'scaling', 'and', 'similarity', 'properties', 'starting', 'from', 'its', 'fourierlaplace', 'representation', ... | [-0.09017755467952653, -0.016463848205839657, -0.15718825815801885, 0.09874012766786935, -0.11528101684707036, -0.021517897575077684, 0.037855255018387525, 0.33089675860745565, -0.3148806063676035, -0.21828146818072788, 0.1128629193015324, -0.24974527940862395, -0.20109017299754278, 0.17130745898980598, -0.036607374618... |
710.0146 | Anisotropic Lavine's formula and symmetrised time delay in scattering
theory | We consider, in quantum scattering theory, symmetrised time delay defined in
terms of sojourn times in arbitrary spatial regions symmetric with respect to
the origin. For potentials decaying more rapidly than $|x|^{-4}$ at infinity,
we show the existence of symmetrised time delay, and prove that it satisfies an
aniso... | math-ph math.FA math.MP | we consider in quantum scattering theory symmetrised time delay defined in terms of sojourn times in arbitrary spatial regions symmetric with respect to the origin for potentials decaying more rapidly than x4 at infinity we show the existence of symmetrised time delay and prove that it satisfies an anisotropic version ... | [['we', 'consider', 'in', 'quantum', 'scattering', 'theory', 'symmetrised', 'time', 'delay', 'defined', 'in', 'terms', 'of', 'sojourn', 'times', 'in', 'arbitrary', 'spatial', 'regions', 'symmetric', 'with', 'respect', 'to', 'the', 'origin', 'for', 'potentials', 'decaying', 'more', 'rapidly', 'than', 'x4', 'at', 'infini... | [-0.1687862404736705, 0.1179031176341971, -0.09251191881707027, 0.0820786812922932, 0.016702988554560948, -0.12651857665725172, -0.03589176934855502, 0.38185718267904745, -0.25533956394249957, -0.20608739507299598, 0.06987882845310701, -0.290922907491525, -0.1394397646469611, 0.18794416843189132, -0.031683380242496256,... |
710.0147 | Polymer Translocation out of Planar Confinements | Polymer translocation in three dimensions out of planar confinements is
studied in this paper. Three membranes are located at $z=-h$, $z=0$ and
$z=h_1$. These membranes are impenetrable, except for the middle one at $z=0$,
which has a narrow pore. A polymer with length $N$ is initially sandwiched
between the membrane... | cond-mat.soft cond-mat.stat-mech | polymer translocation in three dimensions out of planar confinements is studied in this paper three membranes are located at zh z0 and zh_1 these membranes are impenetrable except for the middle one at z0 which has a narrow pore a polymer with length n is initially sandwiched between the membranes placed at zh and z0 a... | [['polymer', 'translocation', 'in', 'three', 'dimensions', 'out', 'of', 'planar', 'confinements', 'is', 'studied', 'in', 'this', 'paper', 'three', 'membranes', 'are', 'located', 'at', 'zh', 'z0', 'and', 'zh_1', 'these', 'membranes', 'are', 'impenetrable', 'except', 'for', 'the', 'middle', 'one', 'at', 'z0', 'which', 'h... | [-0.11818410388056051, 0.1953196040747032, -0.04915932877554075, 0.02100850332041133, 0.02190428193204786, -0.18413042603707355, -0.012088533330016717, 0.41713409902014836, -0.2006848940687228, -0.2610726394233535, 0.05389503025529579, -0.2823595330744326, -0.11355511399422001, 0.19128445313415593, -0.00548804400885408... |
710.0148 | D1-brane in beta-Deformed Background | We study various configurations of rotating and wound D1-brane in AdS_5\times
S^5 background and in its beta deformed version. We find giant magnon and spike
solutions on the world-volume of D1-brane in AdS_5\times S^5 background. We
also analyse the equations of motion of D1-brane in beta-deformed background.
We sho... | hep-th | we study various configurations of rotating and wound d1brane in ads_5times s5 background and in its beta deformed version we find giant magnon and spike solutions on the worldvolume of d1brane in ads_5times s5 background we also analyse the equations of motion of d1brane in betadeformed background we show that in the ... | [['we', 'study', 'various', 'configurations', 'of', 'rotating', 'and', 'wound', 'd1brane', 'in', 'ads_5times', 's5', 'background', 'and', 'in', 'its', 'beta', 'deformed', 'version', 'we', 'find', 'giant', 'magnon', 'and', 'spike', 'solutions', 'on', 'the', 'worldvolume', 'of', 'd1brane', 'in', 'ads_5times', 's5', 'back... | [-0.17316440331718225, 0.15480065207635418, -0.006440823936960503, 0.07892384264994873, -0.04809308529235004, -0.07019146058310786, -0.031360820814799725, 0.3367989773160956, -0.12103914241358806, -0.2458300903371504, 0.09938221849537758, -0.3052374091878366, -0.15319780593089175, 0.1575239670483835, -0.119883018718467... |
710.0149 | Multi-Channel Selective Femtosecond Coherent Control Based on Symmetry
Properties | We present and implement a new scheme for extended multi-channel selective
femtosecond coherent control based on symmetry properties of the excitation
channels. Here, an atomic non-resonant two-photon absorption channel is
coherently incorporated in a resonance-mediated (2+1) three-photon absorption
channel. By prope... | physics.atom-ph | we present and implement a new scheme for extended multichannel selective femtosecond coherent control based on symmetry properties of the excitation channels here an atomic nonresonant twophoton absorption channel is coherently incorporated in a resonancemediated 21 threephoton absorption channel by proper pulse shapi... | [['we', 'present', 'and', 'implement', 'a', 'new', 'scheme', 'for', 'extended', 'multichannel', 'selective', 'femtosecond', 'coherent', 'control', 'based', 'on', 'symmetry', 'properties', 'of', 'the', 'excitation', 'channels', 'here', 'an', 'atomic', 'nonresonant', 'twophoton', 'absorption', 'channel', 'is', 'coherentl... | [-0.1349694995647844, 0.17125985085132175, -0.06477917042588267, -0.005916120743324213, -0.02084265837774557, -0.20900836107595003, 0.08162007857497562, 0.5453143143697696, -0.26089978349559445, -0.2413958791643381, -0.04935069696238155, -0.2036097202778739, -0.045082078189315165, 0.1791234029813067, 0.0412543491460382... |
710.015 | Phase heterogeneities of lipidic aggregates | We propose a model for explanation the "domain-wall" type configuration
states in binary lipid mixtures of cationic and neutral lipids, associated with
observed relaxation effects in their aggregates. We apply the analogy with
formation of Kibble-\.Zurek topological defects, which we suppose connected
with structural... | cond-mat.soft cond-mat.other | we propose a model for explanation the domainwall type configuration states in binary lipid mixtures of cationic and neutral lipids associated with observed relaxation effects in their aggregates we apply the analogy with formation of kibblezurek topological defects which we suppose connected with structural dynamics o... | [['we', 'propose', 'a', 'model', 'for', 'explanation', 'the', 'domainwall', 'type', 'configuration', 'states', 'in', 'binary', 'lipid', 'mixtures', 'of', 'cationic', 'and', 'neutral', 'lipids', 'associated', 'with', 'observed', 'relaxation', 'effects', 'in', 'their', 'aggregates', 'we', 'apply', 'the', 'analogy', 'with... | [-0.14691807528587936, 0.20478541232809863, -0.058425442154711, 0.042549136820632744, 0.061274986522381794, -0.10392603625351672, 0.04316264063955339, 0.3785272328840459, -0.23265766079181477, -0.2663095335352837, 0.002103210990111727, -0.2722733045298168, -0.18357667522094048, 0.04951022623914897, 0.012715749098467366... |
710.0151 | Charm Mixing - Theory | We discuss Standard Model (SM) and New Physics (NP) descriptions of D0
mixing. The SM part of the discussion addresses both quark level and hadron
level contributions. The NP part describes our recent works on the rate
difference Delta Gamma_D and the mass difference Delta M_D. In particular, we
describe how the rece... | hep-ph | we discuss standard model sm and new physics np descriptions of d0 mixing the sm part of the discussion addresses both quark level and hadron level contributions the np part describes our recent works on the rate difference delta gamma_d and the mass difference delta m_d in particular we describe how the recent experim... | [['we', 'discuss', 'standard', 'model', 'sm', 'and', 'new', 'physics', 'np', 'descriptions', 'of', 'd0', 'mixing', 'the', 'sm', 'part', 'of', 'the', 'discussion', 'addresses', 'both', 'quark', 'level', 'and', 'hadron', 'level', 'contributions', 'the', 'np', 'part', 'describes', 'our', 'recent', 'works', 'on', 'the', 'r... | [-0.09448764218194854, 0.15939473681196215, -0.001902435396221422, 0.10828061652552735, -0.061178403263468115, -0.13852088567468204, 0.08108741539624698, 0.2519613970514564, -0.21098055524219358, -0.30272814513938057, 0.024769154055753632, -0.30750744286481113, -0.07242467476143724, 0.14600512287524042, -0.039253577911... |
710.0152 | On minimal non-potentially closed subsets of the plane | We study the Borel subsets of the plane that can be made closed by refining
the Polish topology on the real line. These sets are called potentially closed.
We first compare Borel subsets of the plane using products of continuous
functions. We show the existence of a perfect antichain made of minimal sets
among non-po... | math.LO math.GN | we study the borel subsets of the plane that can be made closed by refining the polish topology on the real line these sets are called potentially closed we first compare borel subsets of the plane using products of continuous functions we show the existence of a perfect antichain made of minimal sets among nonpotentia... | [['we', 'study', 'the', 'borel', 'subsets', 'of', 'the', 'plane', 'that', 'can', 'be', 'made', 'closed', 'by', 'refining', 'the', 'polish', 'topology', 'on', 'the', 'real', 'line', 'these', 'sets', 'are', 'called', 'potentially', 'closed', 'we', 'first', 'compare', 'borel', 'subsets', 'of', 'the', 'plane', 'using', 'pr... | [-0.1926283433543224, 0.07692059100556531, -0.05702874802641179, 0.11501019123917151, -0.09695003665983677, -0.02256766602789101, 0.10202420379378294, 0.40477250767626655, -0.2713444622527612, -0.20366760787407034, 0.10501402213948925, -0.2857581840631993, -0.1258122784649267, 0.24523151387509548, -0.10440860680108399,... |
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