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708.3949 | Categorification of Wedderburn's basis for \mathbb{C}[S_n] | M. Neunh{\"o}ffer studies in \cite{Ne} a certain basis of $\mathbb{C}[S_n]$
with the origins in \cite{Lu} and shows that this basis is in fact Wedderburn's
basis. In particular, in this basis the right regular representation of $S_n$
decomposes into a direct sum of irreducible representations (i.e. Specht or
cell mod... | math.RT math.GR | m neunhoffer studies in citene a certain basis of mathbbcs_n with the origins in citelu and shows that this basis is in fact wedderburns basis in particular in this basis the right regular representation of s_n decomposes into a direct sum of irreducible representations ie specht or cell modules in the present paper we... | [['m', 'neunhoffer', 'studies', 'in', 'citene', 'a', 'certain', 'basis', 'of', 'mathbbcs_n', 'with', 'the', 'origins', 'in', 'citelu', 'and', 'shows', 'that', 'this', 'basis', 'is', 'in', 'fact', 'wedderburns', 'basis', 'in', 'particular', 'in', 'this', 'basis', 'the', 'right', 'regular', 'representation', 'of', 's_n',... | [-0.13904911803058836, 0.03352002525090328, -0.08056476434132645, 0.04371440201473481, -0.092343146505707, -0.10808990084585714, 0.00018638127949088812, 0.3554277475272025, -0.33533890834534086, -0.17176555414273814, 0.0871800410128166, -0.20139975213212485, -0.17386513034213932, 0.18212822535550677, -0.108497796618457... |
708.395 | Noncommutative Minisuperspace Cosmology | We consider the noncommutative minisuperspace classical and quantum
cosmologies.
| hep-th | we consider the noncommutative minisuperspace classical and quantum cosmologies | [['we', 'consider', 'the', 'noncommutative', 'minisuperspace', 'classical', 'and', 'quantum', 'cosmologies']] | [-0.16307885944843292, 0.15901545942243603, -0.09789778768188423, 0.2597746555176046, -0.10579260273112191, -0.2685537238915761, -0.14574224556175372, 0.27453409673439133, -0.2738395581642787, -0.14926205896255043, -0.03395700174021638, -0.22178981653673369, -0.17080802718798319, 0.10568581666383478, -0.159868958923551... |
708.3951 | Gauge Model in D=3, N=5 Harmonic Superspace | We construct the Grassmann-analytic gauge superfields in D=3, N=5 harmonic
superspace using the SO(5)/U(1)xU(1) harmonics. These gauge N=5 superfields
contain an infinite number of bosonic and fermionic fields arising from
decompositions in harmonics and Grassmann coordinates. The bosonic sector of
this supermultiple... | hep-th | we construct the grassmannanalytic gauge superfields in d3 n5 harmonic superspace using the so5u1xu1 harmonics these gauge n5 superfields contain an infinite number of bosonic and fermionic fields arising from decompositions in harmonics and grassmann coordinates the bosonic sector of this supermultiplet includes the g... | [['we', 'construct', 'the', 'grassmannanalytic', 'gauge', 'superfields', 'in', 'd3', 'n5', 'harmonic', 'superspace', 'using', 'the', 'so5u1xu1', 'harmonics', 'these', 'gauge', 'n5', 'superfields', 'contain', 'an', 'infinite', 'number', 'of', 'bosonic', 'and', 'fermionic', 'fields', 'arising', 'from', 'decompositions', ... | [-0.24086152438016595, 0.29432848181829124, -0.006520695401835724, 0.07739953187297914, -0.11925845952386889, -0.14352334297240474, -0.1238223198104592, 0.32056243974686593, -0.1611784939805782, -0.27458543159553145, 0.04790981021951595, -0.2562623422289657, -0.15772074662408855, 0.052564283399283165, -0.00483834906661... |
708.3952 | Liftable D_4-Covers | Let k be an algebraically closed field of characteristic p and let G be a
subgroup of Aut(k[[t]]) be a faithful action on a local power series ring over
k. Let R be a discrete valuation ring of characteristic 0 with residue field k.
One asks, whether it is possible to find a faithful action G inside Aut(R[[t]])
which... | math.AG math.NT | let k be an algebraically closed field of characteristic p and let g be a subgroup of autkt be a faithful action on a local power series ring over k let r be a discrete valuation ring of characteristic 0 with residue field k one asks whether it is possible to find a faithful action g inside autrt which reduces to the g... | [['let', 'k', 'be', 'an', 'algebraically', 'closed', 'field', 'of', 'characteristic', 'p', 'and', 'let', 'g', 'be', 'a', 'subgroup', 'of', 'autkt', 'be', 'a', 'faithful', 'action', 'on', 'a', 'local', 'power', 'series', 'ring', 'over', 'k', 'let', 'r', 'be', 'a', 'discrete', 'valuation', 'ring', 'of', 'characteristic',... | [-0.23327448987171495, 0.13307222026520718, -0.14358732773286134, -0.02265179291307594, -0.12113871381129368, -0.20806000057589447, -0.011088141682788287, 0.3609112449137881, -0.3771448141646267, -0.21052888210973528, 0.03875576990822533, -0.2121297745725675, -0.09131665374290678, 0.1762979241263232, -0.079625695214219... |
708.3953 | Taking the Measure of the Universe: Precision Astrometry with SIM
PlanetQuest | Precision astrometry at microarcsecond accuracy has application to a wide
range of astrophysical problems. This paper is a study of the science questions
that can be addressed using an instrument that delivers parallaxes at about 4
microarcsec on targets as faint as V = 20, differential accuracy of 0.6
microarcsec on... | astro-ph | precision astrometry at microarcsecond accuracy has application to a wide range of astrophysical problems this paper is a study of the science questions that can be addressed using an instrument that delivers parallaxes at about 4 microarcsec on targets as faint as v 20 differential accuracy of 06 microarcsec on bright... | [['precision', 'astrometry', 'at', 'microarcsecond', 'accuracy', 'has', 'application', 'to', 'a', 'wide', 'range', 'of', 'astrophysical', 'problems', 'this', 'paper', 'is', 'a', 'study', 'of', 'the', 'science', 'questions', 'that', 'can', 'be', 'addressed', 'using', 'an', 'instrument', 'that', 'delivers', 'parallaxes',... | [-0.07326261292827976, 0.1544114776643999, -0.048591132355389983, 0.07414966556814856, -0.1264808179557905, -0.06562804465517956, 0.04774297857297875, 0.38205440991236156, -0.1818985460783947, -0.42838196420772034, 0.10349324640868142, -0.296929028875378, -0.024423373340313984, 0.2795846096662368, -0.0786316473674043, ... |
708.3954 | Non-commutative phase space and its space-time symmetry | First a description of 2+1 dimensional non-commutative(NC) phase space is
presented, where the deformation of the planck constant is given. We find that
in this new formulation, generalized Bopp's shift has a symmetric
representation and one can easily and straightforwardly define the star product
on NC phase space. ... | hep-th | first a description of 21 dimensional noncommutativenc phase space is presented where the deformation of the planck constant is given we find that in this new formulation generalized bopps shift has a symmetric representation and one can easily and straightforwardly define the star product on nc phase space then we def... | [['first', 'a', 'description', 'of', '21', 'dimensional', 'noncommutativenc', 'phase', 'space', 'is', 'presented', 'where', 'the', 'deformation', 'of', 'the', 'planck', 'constant', 'is', 'given', 'we', 'find', 'that', 'in', 'this', 'new', 'formulation', 'generalized', 'bopps', 'shift', 'has', 'a', 'symmetric', 'represe... | [-0.1209462959280548, 0.18932394308891767, -0.10938697445089929, 0.06763475390228753, -0.08185218225601905, -0.10613382370987286, 0.04579372029790344, 0.3680004727987883, -0.2615430195243486, -0.22683851588711454, 0.08984144672649563, -0.17441800295879753, -0.2069606969404655, 0.12794271096936427, -0.07966024907121512,... |
708.3955 | Evolution of geometric structures in intense turbulence | We report measurements of the evolution of lines, planes, and volumes in an
intensely turbulent laboratory flow using high-speed particle tracking. We find
that the classical characteristic time scale of an eddy at the initial scale of
the object considered is the natural time scale for the subsequent evolution.
The ... | physics.flu-dyn | we report measurements of the evolution of lines planes and volumes in an intensely turbulent laboratory flow using highspeed particle tracking we find that the classical characteristic time scale of an eddy at the initial scale of the object considered is the natural time scale for the subsequent evolution the initial... | [['we', 'report', 'measurements', 'of', 'the', 'evolution', 'of', 'lines', 'planes', 'and', 'volumes', 'in', 'an', 'intensely', 'turbulent', 'laboratory', 'flow', 'using', 'highspeed', 'particle', 'tracking', 'we', 'find', 'that', 'the', 'classical', 'characteristic', 'time', 'scale', 'of', 'an', 'eddy', 'at', 'the', '... | [-0.1744859183861597, 0.22940354790842174, -0.10268074928663319, 0.1016417505011919, -0.0021884304666388277, -0.04402717252299693, -0.07006584291623251, 0.3351181562788583, -0.3037266497424728, -0.34175286718921083, 0.13438449297855432, -0.18693633130877405, -0.008558484823191288, 0.21882711442319575, 0.019861671950894... |
708.3956 | The asymptotic behaviour of recurrence coefficients for orthogonal
polynomials with varying exponential weights | We consider orthogonal polynomials $\{p_{n,N}(x)\}_{n=0}^{\infty}$ on the
real line with respect to a weight $w(x)=e^{-NV(x)}$ and in particular the
asymptotic behaviour of the coefficients $a_{n,N}$ and $b_{n,N}$ in the three
term recurrence $x \pi_{n,N}(x) = \pi_{n+1,N}(x) + b_{n,N} \pi_{n,N}(x) +
a_{n,N} \pi_{n-1,... | math.CA math.CV | we consider orthogonal polynomials p_nnx_n0infty on the real line with respect to a weight wxenvx and in particular the asymptotic behaviour of the coefficients a_nn and b_nn in the three term recurrence x pi_nnx pi_n1nx b_nn pi_nnx a_nn pi_n1nx for onecut regular v we show using the deiftzhou method of steepest descen... | [['we', 'consider', 'orthogonal', 'polynomials', 'p_nnx_n0infty', 'on', 'the', 'real', 'line', 'with', 'respect', 'to', 'a', 'weight', 'wxenvx', 'and', 'in', 'particular', 'the', 'asymptotic', 'behaviour', 'of', 'the', 'coefficients', 'a_nn', 'and', 'b_nn', 'in', 'the', 'three', 'term', 'recurrence', 'x', 'pi_nnx', 'pi... | [-0.16793265015728873, 0.057079309584853584, -0.06612152437845321, 0.03807512038763715, -0.018180510705362442, -0.13961800789358478, 0.008342409965722528, 0.36044261034271896, -0.2796440719792696, -0.1375691610275232, 0.11111877294901554, -0.3389199735622292, -0.16051669414027606, 0.1841091284247702, -0.002799415756782... |
708.3957 | Hyperon decay form factors in chiral perturbation theory | We present a complete calculation of the SU(3)-breaking corrections to the
hyperon vector form factors up to O(p^4) in covariant baryon chiral
perturbation theory. Partial higher-order contributions are obtained, and we
discuss chiral extrapolations of the vector form factor at zero momentum
transfer. In addition we ... | hep-ph hep-ex hep-lat | we present a complete calculation of the su3breaking corrections to the hyperon vector form factors up to op4 in covariant baryon chiral perturbation theory partial higherorder contributions are obtained and we discuss chiral extrapolations of the vector form factor at zero momentum transfer in addition we derive lowen... | [['we', 'present', 'a', 'complete', 'calculation', 'of', 'the', 'su3breaking', 'corrections', 'to', 'the', 'hyperon', 'vector', 'form', 'factors', 'up', 'to', 'op4', 'in', 'covariant', 'baryon', 'chiral', 'perturbation', 'theory', 'partial', 'higherorder', 'contributions', 'are', 'obtained', 'and', 'we', 'discuss', 'ch... | [-0.14761497131953744, 0.2303636892280285, -0.040505864596723215, 0.14910612721671013, -0.11270169483875667, -0.04013762188454469, 0.0658461777864537, 0.29076797698718915, -0.20001246208878423, -0.2131957983787077, -0.05814527847594919, -0.3659319675568005, -0.03710428816333845, 0.04258131806441731, 0.12180941588366809... |
708.3958 | Cruising through molecular bound state manifolds with radio frequency | The emerging field of ultracold molecules with their rich internal structure
is currently attracting a lot of interest. Various methods have been developed
to produce ultracold molecules in pre-set quantum states. For future
experiments it will be important to efficiently transfer these molecules from
their initial q... | quant-ph | the emerging field of ultracold molecules with their rich internal structure is currently attracting a lot of interest various methods have been developed to produce ultracold molecules in preset quantum states for future experiments it will be important to efficiently transfer these molecules from their initial quantu... | [['the', 'emerging', 'field', 'of', 'ultracold', 'molecules', 'with', 'their', 'rich', 'internal', 'structure', 'is', 'currently', 'attracting', 'a', 'lot', 'of', 'interest', 'various', 'methods', 'have', 'been', 'developed', 'to', 'produce', 'ultracold', 'molecules', 'in', 'preset', 'quantum', 'states', 'for', 'future... | [-0.09761447558627913, 0.17877589790863746, -0.07359235383926627, 0.04065656798493477, -0.02460561824652056, -0.18150965113158304, 0.08513672366726821, 0.41553873423900867, -0.2645390776250465, -0.3146175945861794, 0.05912091103411153, -0.24939617990619606, -0.10670838326095017, 0.24759029968135796, 0.01190939376038717... |
708.3959 | Surface Plasmon Polariton Self-Focusing by Ponderomotive Forces | Nonlinear properties of Surface Plasmon Polaritons stemming from the inherent
electron plasma nonlinearity of the metal layers are investigated. A
fluid-mechanics plasma model is used to describe the electron motion in metals.
The nonlinear ponderomotive force repels the electrons from the high field
intensity region... | physics.optics | nonlinear properties of surface plasmon polaritons stemming from the inherent electron plasma nonlinearity of the metal layers are investigated a fluidmechanics plasma model is used to describe the electron motion in metals the nonlinear ponderomotive force repels the electrons from the high field intensity region effe... | [['nonlinear', 'properties', 'of', 'surface', 'plasmon', 'polaritons', 'stemming', 'from', 'the', 'inherent', 'electron', 'plasma', 'nonlinearity', 'of', 'the', 'metal', 'layers', 'are', 'investigated', 'a', 'fluidmechanics', 'plasma', 'model', 'is', 'used', 'to', 'describe', 'the', 'electron', 'motion', 'in', 'metals'... | [-0.09526916317242597, 0.19728768920148945, -0.02375047914683819, 0.054337434203452654, -0.05378705903311216, -0.12414978702242176, -0.012783225993847564, 0.39143616489711264, -0.2518150234240152, -0.29444456605152003, -0.004488108093140736, -0.29702443311966603, -0.16524794842338278, 0.23440053500678568, 0.00360812920... |
708.396 | Quantum indirect estimation theory and joint estimate of all moments of
two incompatible observables | We introduce the quantum indirect estimation theory, which provides a general
framework to address the problem of which ensemble averages can be estimated by
means of an available set of measuring apparatuses, e. g. estimate the ensemble
average of an observable by measuring other observable. A main ingredient in
thi... | quant-ph | we introduce the quantum indirect estimation theory which provides a general framework to address the problem of which ensemble averages can be estimated by means of an available set of measuring apparatuses e g estimate the ensemble average of an observable by measuring other observable a main ingredient in this appro... | [['we', 'introduce', 'the', 'quantum', 'indirect', 'estimation', 'theory', 'which', 'provides', 'a', 'general', 'framework', 'to', 'address', 'the', 'problem', 'of', 'which', 'ensemble', 'averages', 'can', 'be', 'estimated', 'by', 'means', 'of', 'an', 'available', 'set', 'of', 'measuring', 'apparatuses', 'e', 'g', 'est... | [-0.11224542762717131, 0.13811991298678747, -0.09042792608160644, 0.0580861232455547, -0.02993586905312481, -0.13608608539898398, 0.05226309945106886, 0.3261089856057149, -0.2654662620466036, -0.3164380097370239, 0.10348802442650554, -0.2663535627411904, -0.11231698764296795, 0.2042390569617414, -0.05198452938763294, 0... |
708.3961 | Chess, Chance and Conspiracy | Chess and chance are seemingly strange bedfellows. Luck and/or randomness
have no apparent role in move selection when the game is played at the highest
levels. However, when competition is at the ultimate level, that of the World
Chess Championship (WCC), chess and conspiracy are not strange bedfellows,
there being ... | stat.ME | chess and chance are seemingly strange bedfellows luck andor randomness have no apparent role in move selection when the game is played at the highest levels however when competition is at the ultimate level that of the world chess championship wcc chess and conspiracy are not strange bedfellows there being a long and ... | [['chess', 'and', 'chance', 'are', 'seemingly', 'strange', 'bedfellows', 'luck', 'andor', 'randomness', 'have', 'no', 'apparent', 'role', 'in', 'move', 'selection', 'when', 'the', 'game', 'is', 'played', 'at', 'the', 'highest', 'levels', 'however', 'when', 'competition', 'is', 'at', 'the', 'ultimate', 'level', 'that', ... | [-0.06271025510914859, 0.11937649657229714, -0.1300088281387393, 0.11395812519231471, -0.07555169894934029, -0.15814045220672054, 0.08620920014983546, 0.39481628801872803, -0.22317128985792212, -0.34849087210992974, 0.10286138469789692, -0.29910886269101195, -0.11409364962282609, 0.1343294488025958, -0.0993693183240650... |
708.3962 | A course on Combinatorial Algorithms | The paper presents a course on Combinatorial Algorithms that is based on the
drafts of the author that he used while teaching the course in the Department
of Informatics and Applied Mathematics of Yerevan State University, Armenia
from February 2007 to June 2007.
| cs.DM | the paper presents a course on combinatorial algorithms that is based on the drafts of the author that he used while teaching the course in the department of informatics and applied mathematics of yerevan state university armenia from february 2007 to june 2007 | [['the', 'paper', 'presents', 'a', 'course', 'on', 'combinatorial', 'algorithms', 'that', 'is', 'based', 'on', 'the', 'drafts', 'of', 'the', 'author', 'that', 'he', 'used', 'while', 'teaching', 'the', 'course', 'in', 'the', 'department', 'of', 'informatics', 'and', 'applied', 'mathematics', 'of', 'yerevan', 'state', 'u... | [0.05188277537046477, 0.03615429213400497, -0.18131262111629165, 0.011063465905419095, -0.13071452115857324, -0.09035825368753353, 0.062231232566477425, 0.27104258145270654, -0.15481973902950452, -0.4229915264214194, 0.1498260848240407, -0.2524634520414957, -0.15494507265298865, 0.23914783933134967, -0.1939133229167308... |
708.3963 | Localization of light in a lamellar structure with left-handed medium :
the light wheel | The contra-directional coupling between a left-handed monomode waveguide and
a right-handed monomode waveguide is rigorously studied using a complex plane
analysis. Light is shown to rotate in this lamellar structure forming a very
exotic mode which we have called a light wheel. The light wheel can be excited
using e... | physics.optics | the contradirectional coupling between a lefthanded monomode waveguide and a righthanded monomode waveguide is rigorously studied using a complex plane analysis light is shown to rotate in this lamellar structure forming a very exotic mode which we have called a light wheel the light wheel can be excited using evanesce... | [['the', 'contradirectional', 'coupling', 'between', 'a', 'lefthanded', 'monomode', 'waveguide', 'and', 'a', 'righthanded', 'monomode', 'waveguide', 'is', 'rigorously', 'studied', 'using', 'a', 'complex', 'plane', 'analysis', 'light', 'is', 'shown', 'to', 'rotate', 'in', 'this', 'lamellar', 'structure', 'forming', 'a',... | [-0.16337729789289263, 0.22107173613656092, -0.09449595342225889, 0.002175335445003036, -0.14195133123327705, -0.19340382645673612, 0.026946058421505287, 0.46238995619556483, -0.25285295928444934, -0.25762313175467116, 0.07453443289953558, -0.25319837749771335, -0.14251053976716802, 0.19341980468426995, 0.0273698195595... |
708.3964 | Separation of the strain and finite size effect on the ferromagnetic
properties of La_{0.5}Sr_{0.5}CoO_3 thin films | The ferromagnetic properties of epitaxial La$_{0.5}$Sr$_{0.5}$CoO$_3$ thin
films have been studied. The magnetic transition is affected by both strain and
finite thickness. We have used a series of films of different thickness and on
different substrates in order to quantitatively determine the change in Curie
temper... | cond-mat.mtrl-sci | the ferromagnetic properties of epitaxial la_05sr_05coo_3 thin films have been studied the magnetic transition is affected by both strain and finite thickness we have used a series of films of different thickness and on different substrates in order to quantitatively determine the change in curie temperature contribute... | [['the', 'ferromagnetic', 'properties', 'of', 'epitaxial', 'la_05sr_05coo_3', 'thin', 'films', 'have', 'been', 'studied', 'the', 'magnetic', 'transition', 'is', 'affected', 'by', 'both', 'strain', 'and', 'finite', 'thickness', 'we', 'have', 'used', 'a', 'series', 'of', 'films', 'of', 'different', 'thickness', 'and', 'o... | [-0.13538780284947471, 0.2773850969798667, -0.04134163312417896, -0.0630530572520863, -0.03350988251990394, -0.11864816747899902, 0.07777516561511316, 0.4703760185524037, -0.29538450901837726, -0.27341366225951597, 0.03431611055336697, -0.25687244969763257, -0.09258154296855393, 0.17601412121010454, 0.0370961593267949,... |
708.3965 | Maty's Biography of Abraham De Moivre, Translated, Annotated and
Augmented | November 27, 2004, marked the 250th anniversary of the death of Abraham De
Moivre, best known in statistical circles for his famous large-sample
approximation to the binomial distribution, whose generalization is now
referred to as the Central Limit Theorem. De Moivre was one of the great
pioneers of classical probab... | stat.ME | november 27 2004 marked the 250th anniversary of the death of abraham de moivre best known in statistical circles for his famous largesample approximation to the binomial distribution whose generalization is now referred to as the central limit theorem de moivre was one of the great pioneers of classical probability th... | [['november', '27', '2004', 'marked', 'the', '250th', 'anniversary', 'of', 'the', 'death', 'of', 'abraham', 'de', 'moivre', 'best', 'known', 'in', 'statistical', 'circles', 'for', 'his', 'famous', 'largesample', 'approximation', 'to', 'the', 'binomial', 'distribution', 'whose', 'generalization', 'is', 'now', 'referred'... | [-0.0557493143120325, 0.03997064738286485, -0.12594335113832955, 0.10235799431194477, -0.12456725523539101, -0.09608465161429142, 0.042187168623870175, 0.2658620354880264, -0.17744546976248673, -0.3356383665458118, 0.08398161042588863, -0.3109642781799646, -0.13784906047516965, 0.21882090740334645, -0.16474272866847275... |
708.3966 | PAC Fields over Finitely Generated Fields | We prove the following theorem for a finitely generated field $K$: Let $M$ be
a Galois extension of $K$ which is not separably closed. Then $M$ is not PAC
over $K$.
| math.NT | we prove the following theorem for a finitely generated field k let m be a galois extension of k which is not separably closed then m is not pac over k | [['we', 'prove', 'the', 'following', 'theorem', 'for', 'a', 'finitely', 'generated', 'field', 'k', 'let', 'm', 'be', 'a', 'galois', 'extension', 'of', 'k', 'which', 'is', 'not', 'separably', 'closed', 'then', 'm', 'is', 'not', 'pac', 'over', 'k']] | [-0.2275072433234703, 0.18801655322914163, -0.15743462729357904, -0.02323132145759319, -0.13132729023815162, -0.20503338471415541, -0.007377096001178988, 0.35228865930149633, -0.36301695939994627, -0.21955073367984546, 0.02167487022797427, -0.20437908322820741, -0.057336892850036104, 0.26599852162443344, -0.11507133862... |
708.3967 | The dynamical viability of scalar-tensor gravity theories | We establish the dynamical attractor behavior in scalar-tensor theories of
dark energy, providing a powerful framework to analyze classes of theories,
predicting common evolutionary characteristics that can be compared against
cosmological constraints. In the Jordan frame the theories are viewed as a
coupling between... | astro-ph gr-qc | we establish the dynamical attractor behavior in scalartensor theories of dark energy providing a powerful framework to analyze classes of theories predicting common evolutionary characteristics that can be compared against cosmological constraints in the jordan frame the theories are viewed as a coupling between a sca... | [['we', 'establish', 'the', 'dynamical', 'attractor', 'behavior', 'in', 'scalartensor', 'theories', 'of', 'dark', 'energy', 'providing', 'a', 'powerful', 'framework', 'to', 'analyze', 'classes', 'of', 'theories', 'predicting', 'common', 'evolutionary', 'characteristics', 'that', 'can', 'be', 'compared', 'against', 'cos... | [-0.18528201359123747, 0.1499446216987997, -0.09037878088096063, 0.10553980977637968, -0.05597193869329863, -0.20054848888154114, -0.052557365484496396, 0.32407516320452157, -0.2072400442503377, -0.3093608484096542, 0.03880013893152104, -0.21459029046307762, -0.09310479915429708, 0.15159719912354924, 0.0264861277692149... |
708.3968 | Spectral evolution of GRB 060904A observed with Swift and Suzaku --
Possibility of Inefficient Electron Acceleration | We observed an X-ray afterglow of GRB 060904A with the Swift and Suzaku
satellites. We found rapid spectral softening during both the prompt tail phase
and the decline phase of an X-ray flare in the BAT and XRT data. The observed
spectra were fit by power-law photon indices which rapidly changed from $\Gamma
= 1.51^{... | astro-ph | we observed an xray afterglow of grb 060904a with the swift and suzaku satellites we found rapid spectral softening during both the prompt tail phase and the decline phase of an xray flare in the bat and xrt data the observed spectra were fit by powerlaw photon indices which rapidly changed from gamma 151004_003 to gam... | [['we', 'observed', 'an', 'xray', 'afterglow', 'of', 'grb', '060904a', 'with', 'the', 'swift', 'and', 'suzaku', 'satellites', 'we', 'found', 'rapid', 'spectral', 'softening', 'during', 'both', 'the', 'prompt', 'tail', 'phase', 'and', 'the', 'decline', 'phase', 'of', 'an', 'xray', 'flare', 'in', 'the', 'bat', 'and', 'xr... | [-0.03531665117360461, 0.19627183868208406, -0.12648128623640909, 0.1596692789033833, -0.07310304124651974, -0.14440023210309036, 0.03215911871183923, 0.4788282205702075, -0.24812187355407428, -0.33837191439011977, 0.04849579657305155, -0.3301780885597179, 0.0029687461385250963, 0.20423537079669576, 0.00341838167983724... |
708.3969 | Asymmetric quantum error correction via code conversion | In many physical systems it is expected that environmental decoherence will
exhibit an asymmetry between dephasing and relaxation that may result in qubits
experiencing discrete phase errors more frequently than discrete bit errors. In
the presence of such an error asymmetry, an appropriately asymmetric quantum
code ... | quant-ph | in many physical systems it is expected that environmental decoherence will exhibit an asymmetry between dephasing and relaxation that may result in qubits experiencing discrete phase errors more frequently than discrete bit errors in the presence of such an error asymmetry an appropriately asymmetric quantum code that... | [['in', 'many', 'physical', 'systems', 'it', 'is', 'expected', 'that', 'environmental', 'decoherence', 'will', 'exhibit', 'an', 'asymmetry', 'between', 'dephasing', 'and', 'relaxation', 'that', 'may', 'result', 'in', 'qubits', 'experiencing', 'discrete', 'phase', 'errors', 'more', 'frequently', 'than', 'discrete', 'bit... | [-0.1631752192983792, 0.1563296073625679, -0.08559701578633394, 0.13211512206471526, -0.009889770733813445, -0.23795335777880003, 0.050287242447181295, 0.39936149676019944, -0.2583849431636433, -0.27819131494810184, 0.10195247381246493, -0.22588624708199254, -0.13563072982166582, 0.24306130457359057, -0.118849390201891... |
708.397 | Pseudo-Dirac Bino Dark Matter | While the bino-dominated lightest neutralino of the minimal supersymmetric
Standard Model (MSSM) is an interesting and widely-studied candidate of the
dark matter, the p-wave suppression of its annihilation cross section requires
fine-tunings of the MSSM spectra to be consistent with WMAP observations. We
propose pse... | hep-ph | while the binodominated lightest neutralino of the minimal supersymmetric standard model mssm is an interesting and widelystudied candidate of the dark matter the pwave suppression of its annihilation cross section requires finetunings of the mssm spectra to be consistent with wmap observations we propose pseudodirac b... | [['while', 'the', 'binodominated', 'lightest', 'neutralino', 'of', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'is', 'an', 'interesting', 'and', 'widelystudied', 'candidate', 'of', 'the', 'dark', 'matter', 'the', 'pwave', 'suppression', 'of', 'its', 'annihilation', 'cross', 'section', 'requires', '... | [-0.1361332210724178, 0.24219555824273467, -0.018411957105352737, 0.17296665795006919, -0.12188191949550448, -0.17420420868739742, 0.004602377519718018, 0.28991176955530357, -0.20317664874942395, -0.34586312246091405, 0.012583162690761724, -0.26458573964793747, -0.014464024442312276, 0.1144161901972658, 0.0126472924522... |
708.3971 | Nematic cells with defect-patterned alignment layers | Using Monte Carlo simulations of the Lebwohl--Lasher model we study the
director ordering in a nematic cell where the top and bottom surfaces are
patterned with a lattice of $\pm 1$ point topological defects of lattice
spacing $a$. We find that the nematic order depends crucially on the ratio of
the height of the cel... | cond-mat.soft | using monte carlo simulations of the lebwohllasher model we study the director ordering in a nematic cell where the top and bottom surfaces are patterned with a lattice of pm 1 point topological defects of lattice spacing a we find that the nematic order depends crucially on the ratio of the height of the cell h to a w... | [['using', 'monte', 'carlo', 'simulations', 'of', 'the', 'lebwohllasher', 'model', 'we', 'study', 'the', 'director', 'ordering', 'in', 'a', 'nematic', 'cell', 'where', 'the', 'top', 'and', 'bottom', 'surfaces', 'are', 'patterned', 'with', 'a', 'lattice', 'of', 'pm', '1', 'point', 'topological', 'defects', 'of', 'lattic... | [-0.15398014743730207, 0.1911085782909033, -0.012743975449463023, 0.01465802177280078, 0.007967014112235868, -0.13275113679906902, 0.1043837905409472, 0.3796690959045116, -0.24919662757174058, -0.27585604098789834, 0.08042325119227718, -0.3000664956073332, -0.12670998364166522, 0.1286141823107541, 0.01655325913692222, ... |
708.3972 | Ultrashort intense-field optical vortices produced with laser-etched
mirrors | We introduce a simple and practical method to create ultrashort intense
optical vortices for applications involving high-intensity lasers. Our method
utilizes femtosecond laser pulses to laser-etch grating lines into
laser-quality gold mirrors. These grating lines holographically encode an
optical vortex. We derive m... | physics.optics physics.atom-ph | we introduce a simple and practical method to create ultrashort intense optical vortices for applications involving highintensity lasers our method utilizes femtosecond laser pulses to laseretch grating lines into laserquality gold mirrors these grating lines holographically encode an optical vortex we derive mathemati... | [['we', 'introduce', 'a', 'simple', 'and', 'practical', 'method', 'to', 'create', 'ultrashort', 'intense', 'optical', 'vortices', 'for', 'applications', 'involving', 'highintensity', 'lasers', 'our', 'method', 'utilizes', 'femtosecond', 'laser', 'pulses', 'to', 'laseretch', 'grating', 'lines', 'into', 'laserquality', '... | [-0.09962456216964558, 0.1289372802021085, -0.06973359868897282, 0.011021053949051061, -0.06613988168395431, -0.1980156212056923, 0.019611671029319915, 0.5505276612496672, -0.2087923663629233, -0.31176622224019, 0.029198462269731038, -0.2599684365292769, -0.10553876180486142, 0.24275332810321668, -0.08718692941168138, ... |
708.3973 | Evidence of orbital reconstruction at interfaces in La0.67Sr0.33MnO3
films | Electronic properties of transition metal oxides at interfaces are influenced
by strain, electric polarization and oxygen diffusion. Linear dichroism (LD)
x-ray absorption, diffraction, transport and magnetization on thin
La0.7Sr0.3MnO3 films, allow identification of a peculiar universal interface
effect. We report t... | cond-mat.str-el cond-mat.mtrl-sci | electronic properties of transition metal oxides at interfaces are influenced by strain electric polarization and oxygen diffusion linear dichroism ld xray absorption diffraction transport and magnetization on thin la07sr03mno3 films allow identification of a peculiar universal interface effect we report the ld signatu... | [['electronic', 'properties', 'of', 'transition', 'metal', 'oxides', 'at', 'interfaces', 'are', 'influenced', 'by', 'strain', 'electric', 'polarization', 'and', 'oxygen', 'diffusion', 'linear', 'dichroism', 'ld', 'xray', 'absorption', 'diffraction', 'transport', 'and', 'magnetization', 'on', 'thin', 'la07sr03mno3', 'fi... | [-0.19462496141950864, 0.21584788254963663, -0.026404468247141592, -0.0022394765968410633, -0.06233001788122914, -0.15363918411402175, 0.11577292485162616, 0.44906344747123045, -0.3298593496856017, -0.29117610444052094, -0.02567553181702701, -0.31417197846353817, -0.1135715996989837, 0.14117300851891437, 0.102967230686... |
708.3974 | A Conversation with Robert V. Hogg | Robert Vincent Hogg was born on November 8, 1924 in Hannibal, Missouri. He
earned a Ph.D. in statistics at the University of Iowa in 1950, where his
advisor was Allen Craig. Following graduation, he joined the mathematics
faculty at the University of Iowa. He was the founding Chair when the
Department of Statistics w... | stat.ME | robert vincent hogg was born on november 8 1924 in hannibal missouri he earned a phd in statistics at the university of iowa in 1950 where his advisor was allen craig following graduation he joined the mathematics faculty at the university of iowa he was the founding chair when the department of statistics was created ... | [['robert', 'vincent', 'hogg', 'was', 'born', 'on', 'november', '8', '1924', 'in', 'hannibal', 'missouri', 'he', 'earned', 'a', 'phd', 'in', 'statistics', 'at', 'the', 'university', 'of', 'iowa', 'in', '1950', 'where', 'his', 'advisor', 'was', 'allen', 'craig', 'following', 'graduation', 'he', 'joined', 'the', 'mathema... | [0.025667418398407433, 0.0683882046216268, -0.1422702641188531, 0.049317147158473955, -0.0886992615089766, -0.13921835210628164, 0.1260682863518974, 0.25711562534983906, -0.135969417021364, -0.43047420955192167, 0.11702201302992983, -0.3577682050465025, -0.08160532281147836, 0.133721753839063, -0.20374646586446366, -0.... |
708.3975 | Absence of local magnetic moments in Ru and Rh impurities and clusters
on Ag(100) and Pt(997) | The magnetism of quench-condensed Ru and Rh impurities and metal films on
Ag(100) and Pt(997) has been studied using x-ray magnetic circular dichroism.
In the coverage range between 0.22 ML and 2.0 ML no dichroic signal was
detected at the M3,2 absorption edges of Ru on Ag(100) at a temperature of 5 K
in the presence... | cond-mat.other | the magnetism of quenchcondensed ru and rh impurities and metal films on ag100 and pt997 has been studied using xray magnetic circular dichroism in the coverage range between 022 ml and 20 ml no dichroic signal was detected at the m32 absorption edges of ru on ag100 at a temperature of 5 k in the presence of an applied... | [['the', 'magnetism', 'of', 'quenchcondensed', 'ru', 'and', 'rh', 'impurities', 'and', 'metal', 'films', 'on', 'ag100', 'and', 'pt997', 'has', 'been', 'studied', 'using', 'xray', 'magnetic', 'circular', 'dichroism', 'in', 'the', 'coverage', 'range', 'between', '022', 'ml', 'and', '20', 'ml', 'no', 'dichroic', 'signal',... | [-0.09994473869877833, 0.14447996615522748, 0.030620907757569243, 0.025204779369825566, 0.041166687630875796, -0.12975912814683938, 0.08694821083098996, 0.45021212401765365, -0.20999305773595417, -0.4001271353413661, 0.009467885668251526, -0.38671725312316857, -0.052305334704686644, 0.15405939926427822, 0.0538179969001... |
708.3976 | Geometry reconstruction of fluorescence detectors revisited | The experimental technique of fluorescence light observation is used in
current and planned air shower experiments that aim at understanding the origin
of ultra-high energy cosmic rays. In the fluorescence technique, the geometry
of the shower is reconstructed based on the correlation between viewing angle
and arriva... | astro-ph | the experimental technique of fluorescence light observation is used in current and planned air shower experiments that aim at understanding the origin of ultrahigh energy cosmic rays in the fluorescence technique the geometry of the shower is reconstructed based on the correlation between viewing angle and arrival tim... | [['the', 'experimental', 'technique', 'of', 'fluorescence', 'light', 'observation', 'is', 'used', 'in', 'current', 'and', 'planned', 'air', 'shower', 'experiments', 'that', 'aim', 'at', 'understanding', 'the', 'origin', 'of', 'ultrahigh', 'energy', 'cosmic', 'rays', 'in', 'the', 'fluorescence', 'technique', 'the', 'geo... | [-0.06829186593052881, 0.16538171859502176, -0.10124770609507634, 0.09414586737512931, -0.05420298949049334, -0.0622980707358106, -0.021035429013110476, 0.4161016730723914, -0.22786294924888825, -0.3568259087451816, 0.10950225989882609, -0.2899138300222229, -0.11037526285749745, 0.23928810472561587, -0.0073837108314919... |
708.3977 | The Lie algebra perturbation lemma | Let g be a differential graded Lie algebra and suppose given a contraction of
chain complexes of g onto a general chain complex M. We show that the data
determine an sh-Lie algebra structure on M, that is, a coalgebra perturbation
of the coalgebra differential on the cofree coaugmented differential graded
cocommutati... | math.AG math.AC | let g be a differential graded lie algebra and suppose given a contraction of chain complexes of g onto a general chain complex m we show that the data determine an shlie algebra structure on m that is a coalgebra perturbation of the coalgebra differential on the cofree coaugmented differential graded cocommutative coa... | [['let', 'g', 'be', 'a', 'differential', 'graded', 'lie', 'algebra', 'and', 'suppose', 'given', 'a', 'contraction', 'of', 'chain', 'complexes', 'of', 'g', 'onto', 'a', 'general', 'chain', 'complex', 'm', 'we', 'show', 'that', 'the', 'data', 'determine', 'an', 'shlie', 'algebra', 'structure', 'on', 'm', 'that', 'is', 'a... | [-0.20763574086424127, 0.04018576713882366, -0.06783010499716244, -0.005757132797632092, -0.16969900473486632, -0.1137567857033847, -0.043506326050299, 0.3588886107181144, -0.4086705268898239, -0.2220960113370572, 0.10730835202112383, -0.2116451471537242, -0.11927490105153993, 0.1483437296393437, -0.137470089684939, -0... |
708.3978 | Path-Integral Formulation of Pseudo-Hermitian Quantum Mechanics and the
Role of the Metric Operator | We provide a careful analysis of the generating functional in the path
integral formulation of pseudo-Hermitian and in particular PT-symmetric quantum
mechanics and show how the metric operator enters the expression for the
generating functional.
| quant-ph gr-qc hep-th math-ph math.MP | we provide a careful analysis of the generating functional in the path integral formulation of pseudohermitian and in particular ptsymmetric quantum mechanics and show how the metric operator enters the expression for the generating functional | [['we', 'provide', 'a', 'careful', 'analysis', 'of', 'the', 'generating', 'functional', 'in', 'the', 'path', 'integral', 'formulation', 'of', 'pseudohermitian', 'and', 'in', 'particular', 'ptsymmetric', 'quantum', 'mechanics', 'and', 'show', 'how', 'the', 'metric', 'operator', 'enters', 'the', 'expression', 'for', 'the... | [-0.1412147481260555, 0.070320686371997, -0.15978335070290736, 0.09633296041616372, -0.06405023772801671, -0.09993104970614825, 0.00986055337291743, 0.3313810834395034, -0.23721684286636965, -0.2347184625587293, 0.044726512374888575, -0.28589056006499697, -0.315699601984982, 0.18264317863753865, -0.04054842801498515, 0... |
708.3979 | Constraining the nature of High Frequency Peakers. I. The spectral
variability | We investigate the spectral characteristics of 51 candidate High Frequency
Peakers (HFPs), from the ``bright'' HFP sample, in order to determine the
nature of each object, and to obtain a smaller sample of genuine young radio
sources. Simultaneous multi-frequency VLA observations carried out at various
epochs have be... | astro-ph | we investigate the spectral characteristics of 51 candidate high frequency peakers hfps from the bright hfp sample in order to determine the nature of each object and to obtain a smaller sample of genuine young radio sources simultaneous multifrequency vla observations carried out at various epochs have been used to de... | [['we', 'investigate', 'the', 'spectral', 'characteristics', 'of', '51', 'candidate', 'high', 'frequency', 'peakers', 'hfps', 'from', 'the', 'bright', 'hfp', 'sample', 'in', 'order', 'to', 'determine', 'the', 'nature', 'of', 'each', 'object', 'and', 'to', 'obtain', 'a', 'smaller', 'sample', 'of', 'genuine', 'young', 'r... | [-0.08388824593259389, 0.08588895695327733, -0.07912094771486003, 0.10274840509103603, -0.10564924958883457, -0.08872202920897955, 0.059731638204402554, 0.4386581697549339, -0.1972001032038054, -0.36676934142400264, 0.10254680159547641, -0.26416491643643714, -0.04078186935627125, 0.17784011344744566, -0.018687357087324... |
708.398 | On a characterization of PPT states | We present two different descriptions of positive partially transposed (PPT)
states. One is based on the theory of positive maps while the second
description provides a characterization of PPT states in terms of Hilbert space
vectors. Our note is based on our previous results.
| quant-ph | we present two different descriptions of positive partially transposed ppt states one is based on the theory of positive maps while the second description provides a characterization of ppt states in terms of hilbert space vectors our note is based on our previous results | [['we', 'present', 'two', 'different', 'descriptions', 'of', 'positive', 'partially', 'transposed', 'ppt', 'states', 'one', 'is', 'based', 'on', 'the', 'theory', 'of', 'positive', 'maps', 'while', 'the', 'second', 'description', 'provides', 'a', 'characterization', 'of', 'ppt', 'states', 'in', 'terms', 'of', 'hilbert',... | [-0.13280889877668497, 0.10512177860999311, -0.08319624496454542, 0.006630331150848757, 0.008859870997680859, -0.08887626889124724, 0.02174655716622841, 0.2942920281678777, -0.17773760509126904, -0.2139282969927246, 0.11022328106760555, -0.30743615750477393, -0.1543968107382005, 0.18090070166032424, -0.060158267384395,... |
708.3981 | Gaps in the differential forms spectrum on cyclic coverings | We are interested in the spectrum of the Hodge-de Rham operator on a cyclic
covering $X$ over a compact manifold $M$ of dimension $n+1$. Let $\Sigma$ be a
hypersurface in $M$ which does not disconnect $M$ and such that $M-\Sigma$ is a
fundamental domain of the covering. If the cohomology group $H^{n/2 (\Sigma)$
is tr... | math.DG | we are interested in the spectrum of the hodgede rham operator on a cyclic covering x over a compact manifold m of dimension n1 let sigma be a hypersurface in m which does not disconnect m and such that msigma is a fundamental domain of the covering if the cohomology group hn2 sigma is trivial we can construct for each... | [['we', 'are', 'interested', 'in', 'the', 'spectrum', 'of', 'the', 'hodgede', 'rham', 'operator', 'on', 'a', 'cyclic', 'covering', 'x', 'over', 'a', 'compact', 'manifold', 'm', 'of', 'dimension', 'n1', 'let', 'sigma', 'be', 'a', 'hypersurface', 'in', 'm', 'which', 'does', 'not', 'disconnect', 'm', 'and', 'such', 'that'... | [-0.24439341341633172, 0.09224777184205041, -0.09500300491206526, 0.0561752236426054, -0.07551054387974242, -0.16130812339307296, -0.029295825727638745, 0.3377261814905242, -0.2579678885638714, -0.21774586725846998, 0.09707796166961392, -0.2884913384914398, -0.11602540518201533, 0.15923506484056513, -0.1194832853972911... |
708.3982 | Atomic-charge distribution in glasses by terahertz spectroscopy | It is demonstrated that the width of the uncorrelated atomic-charge
distribution in glasses can be extracted from the frequency dependence of the
coupling coefficient for the far-infrared absorption measured experimentally by
the time-domain terahertz spectroscopy technique. This value for As2S3 glass is
found to be ... | cond-mat.dis-nn | it is demonstrated that the width of the uncorrelated atomiccharge distribution in glasses can be extracted from the frequency dependence of the coupling coefficient for the farinfrared absorption measured experimentally by the timedomain terahertz spectroscopy technique this value for as2s3 glass is found to be 012 e ... | [['it', 'is', 'demonstrated', 'that', 'the', 'width', 'of', 'the', 'uncorrelated', 'atomiccharge', 'distribution', 'in', 'glasses', 'can', 'be', 'extracted', 'from', 'the', 'frequency', 'dependence', 'of', 'the', 'coupling', 'coefficient', 'for', 'the', 'farinfrared', 'absorption', 'measured', 'experimentally', 'by', '... | [-0.07502477930583915, 0.17055879078316885, -0.14869987321864875, 0.012597395691135134, -0.005367090437011641, -0.11302035852320126, 0.025450002799024346, 0.4598650675816614, -0.25220018336702077, -0.2650692853160569, 0.016256069556474077, -0.2966382140751745, -0.1521442249783727, 0.186467222071665, 0.08026785930221686... |
708.3983 | Unifying inflation and dark matter with neutrino masses | We propose a simple model where a {\it gauge invariant inflaton} is
responsible for cosmic inflation and generates the seed for structure
formation, while its relic {\it thermal} abundance explains the missing matter
of the universe in the form of cold dark matter. The inflaton self-coupling
also explains the observe... | hep-ph astro-ph gr-qc hep-th | we propose a simple model where a it gauge invariant inflaton is responsible for cosmic inflation and generates the seed for structure formation while its relic it thermal abundance explains the missing matter of the universe in the form of cold dark matter the inflaton selfcoupling also explains the observed neutrino ... | [['we', 'propose', 'a', 'simple', 'model', 'where', 'a', 'it', 'gauge', 'invariant', 'inflaton', 'is', 'responsible', 'for', 'cosmic', 'inflation', 'and', 'generates', 'the', 'seed', 'for', 'structure', 'formation', 'while', 'its', 'relic', 'it', 'thermal', 'abundance', 'explains', 'the', 'missing', 'matter', 'of', 'th... | [-0.13891315682981673, 0.22700735426720217, -0.11921172264159065, 0.18393572215228976, -0.1033233693782346, -0.08869613401210782, -0.043100693824023685, 0.3303346809645353, -0.24082960044457155, -0.33530212598006154, 0.033057002680090423, -0.21552020449995657, -0.0858062452382662, 0.1590836862557229, 0.0253694974976083... |
708.3984 | Lectures on Nongeometric Flux Compactifications | These notes present a pedagogical review of nongeometric flux
compactifications. We begin by reviewing well-known geometric flux
compactifications in Type II string theory, and argue that one must include
nongeometric "fluxes" in order to have a superpotential which is invariant
under T-duality. Additionally, we disc... | hep-th | these notes present a pedagogical review of nongeometric flux compactifications we begin by reviewing wellknown geometric flux compactifications in type ii string theory and argue that one must include nongeometric fluxes in order to have a superpotential which is invariant under tduality additionally we discuss some e... | [['these', 'notes', 'present', 'a', 'pedagogical', 'review', 'of', 'nongeometric', 'flux', 'compactifications', 'we', 'begin', 'by', 'reviewing', 'wellknown', 'geometric', 'flux', 'compactifications', 'in', 'type', 'ii', 'string', 'theory', 'and', 'argue', 'that', 'one', 'must', 'include', 'nongeometric', 'fluxes', 'in... | [-0.10343573134658592, 0.20233882003064665, -0.08904709498664098, 0.16681067324409793, -0.12013139236452323, -0.16847845249410187, -0.01175344165115218, 0.30465609494463675, -0.11934084817767143, -0.3034762965781348, 0.12651063911284188, -0.2708496672633503, -0.18185831199350236, 0.12447827238855617, -0.233307969250849... |
708.3985 | Transient x-ray absorption spectroscopy of hydrated halogen atom | Time-resolved x-ray absorption spectroscopy monitors the transient species
generated by one-photon detachment of an electron from aqueous bromide.
Hydrated bromine atoms with a lifetime of ca. 17 ns were observed, nearly half
of which react with excess Br- to form Br2-. The K-edge spectra of the Br atom
and Br2- anio... | physics.chem-ph | timeresolved xray absorption spectroscopy monitors the transient species generated by onephoton detachment of an electron from aqueous bromide hydrated bromine atoms with a lifetime of ca 17 ns were observed nearly half of which react with excess br to form br2 the kedge spectra of the br atom and br2 anion exhibit dis... | [['timeresolved', 'xray', 'absorption', 'spectroscopy', 'monitors', 'the', 'transient', 'species', 'generated', 'by', 'onephoton', 'detachment', 'of', 'an', 'electron', 'from', 'aqueous', 'bromide', 'hydrated', 'bromine', 'atoms', 'with', 'a', 'lifetime', 'of', 'ca', '17', 'ns', 'were', 'observed', 'nearly', 'half', 'o... | [-0.05193788997001118, 0.19128193818695663, 0.010529847874487233, 0.01952766670146957, 0.07452678218380444, -0.17039311760519113, 0.07468729031776698, 0.45700077948470913, -0.22075164591402022, -0.3033539465550954, -0.04023861427299885, -0.409130062473317, -0.022959769998366634, 0.1004992655530158, 0.07397664818498824,... |
708.3986 | In-situ studies of bulk deformation structures: Static properties under
load and Dynamics during deformation | (Abridged, full abstract available in the text)
The main goal of the study presented in this thesis was to perform in-situ
investigations on deformation structures in plastically deformed
polycrystalline copper at low degrees (<5%) of tensile deformation. Copper is
taken as a model system for pure fcc metals.
A n... | cond-mat.mtrl-sci | abridged full abstract available in the text the main goal of the study presented in this thesis was to perform insitu investigations on deformation structures in plastically deformed polycrystalline copper at low degrees 5 of tensile deformation copper is taken as a model system for pure fcc metals a novel synchrotron... | [['abridged', 'full', 'abstract', 'available', 'in', 'the', 'text', 'the', 'main', 'goal', 'of', 'the', 'study', 'presented', 'in', 'this', 'thesis', 'was', 'to', 'perform', 'insitu', 'investigations', 'on', 'deformation', 'structures', 'in', 'plastically', 'deformed', 'polycrystalline', 'copper', 'at', 'low', 'degrees... | [-0.07338520478968677, 0.11942116338556093, -0.08132448622732948, 0.010460016286225886, -0.008220444724747474, -0.0709236593728712, 0.03299236697872561, 0.4246548978927357, -0.25830066566930604, -0.2714381082876601, 0.07959074347694735, -0.26097832472692434, -0.1382154046807214, 0.1647729004842682, -0.01806921459215342... |
708.3987 | Background reduction and sensitivity for germanium double beta decay
experiments | Germanium detectors have very good capabilities for the investigation of rare
phenomena like the neutrinoless double beta decay. Rejection of the background
entangling the expected signal is one primary goal in this kind of experiments.
Here, the attainable background reduction in the energy region where the
neutrino... | nucl-ex | germanium detectors have very good capabilities for the investigation of rare phenomena like the neutrinoless double beta decay rejection of the background entangling the expected signal is one primary goal in this kind of experiments here the attainable background reduction in the energy region where the neutrinoless ... | [['germanium', 'detectors', 'have', 'very', 'good', 'capabilities', 'for', 'the', 'investigation', 'of', 'rare', 'phenomena', 'like', 'the', 'neutrinoless', 'double', 'beta', 'decay', 'rejection', 'of', 'the', 'background', 'entangling', 'the', 'expected', 'signal', 'is', 'one', 'primary', 'goal', 'in', 'this', 'kind',... | [-0.04262798356123754, 0.16008072823682834, -0.03809353944806922, 0.10076284164028275, -0.016379859952356655, -0.1449832701952246, 0.043604080185029634, 0.3673512360863608, -0.17820497685712736, -0.37282251754015155, 0.07276975061157553, -0.3366479749938393, -0.02846375837393061, 0.21190002704171476, -0.013218549079159... |
708.3988 | Semiclassical Evolution of Dissipative Markovian Systems | A semiclassical approximation for an evolving density operator, driven by a
"closed" hamiltonian operator and "open" markovian Lindblad operators, is
obtained. The theory is based on the chord function, i.e. the Fourier transform
of the Wigner function. It reduces to an exact solution of the Lindblad master
equation ... | quant-ph math-ph math.MP math.SG | a semiclassical approximation for an evolving density operator driven by a closed hamiltonian operator and open markovian lindblad operators is obtained the theory is based on the chord function ie the fourier transform of the wigner function it reduces to an exact solution of the lindblad master equation if the hamilt... | [['a', 'semiclassical', 'approximation', 'for', 'an', 'evolving', 'density', 'operator', 'driven', 'by', 'a', 'closed', 'hamiltonian', 'operator', 'and', 'open', 'markovian', 'lindblad', 'operators', 'is', 'obtained', 'the', 'theory', 'is', 'based', 'on', 'the', 'chord', 'function', 'ie', 'the', 'fourier', 'transform',... | [-0.1584212443938003, 0.1269320264208453, -0.09801386007916034, 0.10071825966062557, -0.058560612433003305, -0.1128605987265345, 0.010780537268659716, 0.2961752391933148, -0.30332581971726885, -0.18690511049284284, 0.06643266709457821, -0.26571058090940314, -0.1781682265237269, 0.16992533557313916, -0.03479997768225292... |
708.3989 | Time-delay in a multi-channel formalism | We reexamine the time-delay formalism of Wigner, Eisenbud and Smith, which
was developed to analyze both elastic and inelastic resonances. An error in the
paper of Smith has propagated through the literature. We correct this error and
show how the results of Eisenbud and Smith are related. We also comment on some
rec... | nucl-th hep-ph | we reexamine the timedelay formalism of wigner eisenbud and smith which was developed to analyze both elastic and inelastic resonances an error in the paper of smith has propagated through the literature we correct this error and show how the results of eisenbud and smith are related we also comment on some recent time... | [['we', 'reexamine', 'the', 'timedelay', 'formalism', 'of', 'wigner', 'eisenbud', 'and', 'smith', 'which', 'was', 'developed', 'to', 'analyze', 'both', 'elastic', 'and', 'inelastic', 'resonances', 'an', 'error', 'in', 'the', 'paper', 'of', 'smith', 'has', 'propagated', 'through', 'the', 'literature', 'we', 'correct', '... | [-0.11388178767811041, 0.02781752251235048, -0.12659306485875277, 0.10082593434162845, -0.10003231418340874, -0.0843766527614207, 0.062059397941993666, 0.33682671579299495, -0.20745193649054272, -0.2383617996238172, 0.09218886450798891, -0.25091422714467626, -0.26727282503270544, 0.20744179470420931, -0.135105984169058... |
708.399 | Extreme values of zeta and L-functions | We introduce a "resonance" method to produce large values of
$|\zeta(1/2+it)|$ and large and small central values of $L$-functions.
| math.NT math.CA | we introduce a resonance method to produce large values of zeta12it and large and small central values of lfunctions | [['we', 'introduce', 'a', 'resonance', 'method', 'to', 'produce', 'large', 'values', 'of', 'zeta12it', 'and', 'large', 'and', 'small', 'central', 'values', 'of', 'lfunctions']] | [-0.16456257983257896, 0.09348276478091352, -0.053955075085947386, 0.10027481772397694, -0.05850635321908876, -0.10475991105072592, 0.029622851307258793, 0.2548776056960617, -0.18009615238559873, -0.35083181175746414, 0.0849156460822805, -0.23134229018499977, -0.06329682488974772, 0.23075610423754706, -0.07825893433274... |
708.3991 | On ground fields of arithmetic hyperbolic reflection groups | Using authors's methods of 1980, 1981, some explicit finite sets of number
fields containing ground fields of arithmetic hyperbolic reflection groups are
defined, and good bounds of their degrees (over Q) are obtained. For example,
degree of the ground field of any arithmetic hyperbolic reflection group in
dimension ... | math.AG math.GT | using authorss methods of 1980 1981 some explicit finite sets of number fields containing ground fields of arithmetic hyperbolic reflection groups are defined and good bounds of their degrees over q are obtained for example degree of the ground field of any arithmetic hyperbolic reflection group in dimension at least 6... | [['using', 'authorss', 'methods', 'of', '1980', '1981', 'some', 'explicit', 'finite', 'sets', 'of', 'number', 'fields', 'containing', 'ground', 'fields', 'of', 'arithmetic', 'hyperbolic', 'reflection', 'groups', 'are', 'defined', 'and', 'good', 'bounds', 'of', 'their', 'degrees', 'over', 'q', 'are', 'obtained', 'for', ... | [-0.18002219246593357, 0.13170339900936032, -0.07187095778491134, 0.07384109517008108, -0.075395224484797, -0.12288890226112528, 0.029076102339587677, 0.35779868998703945, -0.2307640976304638, -0.3343260006004966, 0.14451861383939354, -0.231966846314762, -0.11909839414038706, 0.2515032385508048, -0.1128580054782074, 0.... |
708.3992 | The group of automorphisms of a real rational surface is n-transitive | Let X be a rational nonsingular compact connected real algebraic surface. Denote by Aut(X) the group of real algebraic automorphisms of X. We show that the group Aut(X) acts n-transitively on X, for all natural integers n. As an application we give a new and simpler proof of the fact that two rational nonsingular com... | math.AG | let x be a rational nonsingular compact connected real algebraic surface denote by autx the group of real algebraic automorphisms of x we show that the group autx acts ntransitively on x for all natural integers n as an application we give a new and simpler proof of the fact that two rational nonsingular compact connec... | [['let', 'x', 'be', 'a', 'rational', 'nonsingular', 'compact', 'connected', 'real', 'algebraic', 'surface', 'denote', 'by', 'autx', 'the', 'group', 'of', 'real', 'algebraic', 'automorphisms', 'of', 'x', 'we', 'show', 'that', 'the', 'group', 'autx', 'acts', 'ntransitively', 'on', 'x', 'for', 'all', 'natural', 'integers'... | [-0.23325675899084186, 0.12849813867151297, -0.10127218324743525, 0.029853284881207566, -0.1609827223968443, -0.18724925295305503, -0.0354138584020482, 0.3553224985658283, -0.3280634420438552, -0.1471064770463067, 0.10908478689970265, -0.29615121612876233, -0.19876453583292716, 0.27418335052338283, -0.14502286459778396... |
708.3993 | Propagators in the continuum limit: from molecules to scalar fields | The propagator of linear molecules whose constituents interact through
oscillator potentials can be obtained in a closed form for $N$ atoms as long as
$N \leq 4$. We compute the propagator for arbitrary $N$ in the approximation $N
\gg 1$. Taking advantage of this result it is possible to analyze the limit in
which th... | quant-ph | the propagator of linear molecules whose constituents interact through oscillator potentials can be obtained in a closed form for n atoms as long as n leq 4 we compute the propagator for arbitrary n in the approximation n gg 1 taking advantage of this result it is possible to analyze the limit in which the molecule has... | [['the', 'propagator', 'of', 'linear', 'molecules', 'whose', 'constituents', 'interact', 'through', 'oscillator', 'potentials', 'can', 'be', 'obtained', 'in', 'a', 'closed', 'form', 'for', 'n', 'atoms', 'as', 'long', 'as', 'n', 'leq', '4', 'we', 'compute', 'the', 'propagator', 'for', 'arbitrary', 'n', 'in', 'the', 'app... | [-0.16715709635645598, 0.21005841555547977, -0.07374620986067587, 0.0409028464420818, -0.02608231894679877, -0.1270272817231842, 0.003797300621612459, 0.30322497558947176, -0.23676018044352531, -0.2864036733746274, 0.0658990766775484, -0.26996991258019054, -0.11122649745084345, 0.13243448446628153, 0.028021463491500188... |
708.3994 | BFKL at NNLO | We present a recent determination of an approximate expression for the
O(alpha_s^3) contribution chi_2 to the kernel of the BFKL equation. This
includes all collinear and anticollinear singular contributions and is derived
using duality relations between the GLAP and BFKL kernels.
| hep-ph | we present a recent determination of an approximate expression for the oalpha_s3 contribution chi_2 to the kernel of the bfkl equation this includes all collinear and anticollinear singular contributions and is derived using duality relations between the glap and bfkl kernels | [['we', 'present', 'a', 'recent', 'determination', 'of', 'an', 'approximate', 'expression', 'for', 'the', 'oalpha_s3', 'contribution', 'chi_2', 'to', 'the', 'kernel', 'of', 'the', 'bfkl', 'equation', 'this', 'includes', 'all', 'collinear', 'and', 'anticollinear', 'singular', 'contributions', 'and', 'is', 'derived', 'us... | [-0.11622913751052692, 0.025417190060034046, -0.14230549414642155, 0.1413920627674088, -0.08192458207486197, -0.03383057530736551, -0.02129398313118145, 0.31671977527439593, -0.2264238579198718, -0.19928783550858498, 0.024860845477087425, -0.3466712858527899, -0.12302367226220667, 0.14748992854729295, 0.084251519129611... |
708.3995 | Thermodynamic properties of binary HCP solution phases from special
quasirandom structures | Three different special quasirandom structures (SQS) of the substitutional
hcp $A_{1-x}B_x$ binary random solutions ($x=0.25$, 0.5, and 0.75) are
presented. These structures are able to mimic the most important pair and
multi-site correlation functions corresponding to perfectly random hcp
solutions at those composit... | cond-mat.mtrl-sci cond-mat.stat-mech | three different special quasirandom structures sqs of the substitutional hcp a_1xb_x binary random solutions x025 05 and 075 are presented these structures are able to mimic the most important pair and multisite correlation functions corresponding to perfectly random hcp solutions at those compositions due to the relat... | [['three', 'different', 'special', 'quasirandom', 'structures', 'sqs', 'of', 'the', 'substitutional', 'hcp', 'a_1xb_x', 'binary', 'random', 'solutions', 'x025', '05', 'and', '075', 'are', 'presented', 'these', 'structures', 'are', 'able', 'to', 'mimic', 'the', 'most', 'important', 'pair', 'and', 'multisite', 'correlati... | [-0.07366185108336007, 0.1415600346098938, -0.04400913761802679, 0.09312413735726917, -0.029180641273297822, -0.09427492798124326, 0.034407936459657076, 0.44333774796346337, -0.26772546449962936, -0.3035012592288961, 0.08004723016950642, -0.31282451454828286, -0.1521146452372394, 0.14909901319457808, 0.0409903096279311... |
708.3996 | Models of crustal heating in accreting neutron stars | Heating associated with non-equilibrium nuclear reactions in accreting
neutron-star crusts is reconsidered, taking into account suppression of
neutrino losses demonstrated recently by Gupta et al. Two initial compositions
of the nuclear burning ashes, A=56 and A=106, are considered. Dependence of the
integrated crust... | astro-ph | heating associated with nonequilibrium nuclear reactions in accreting neutronstar crusts is reconsidered taking into account suppression of neutrino losses demonstrated recently by gupta et al two initial compositions of the nuclear burning ashes a56 and a106 are considered dependence of the integrated crustal heating ... | [['heating', 'associated', 'with', 'nonequilibrium', 'nuclear', 'reactions', 'in', 'accreting', 'neutronstar', 'crusts', 'is', 'reconsidered', 'taking', 'into', 'account', 'suppression', 'of', 'neutrino', 'losses', 'demonstrated', 'recently', 'by', 'gupta', 'et', 'al', 'two', 'initial', 'compositions', 'of', 'the', 'nu... | [-0.024611599977566477, 0.24823875196058962, -0.04165744922921637, 0.0840423822409802, -0.02605029278304702, -0.004308511068537722, 0.05196754416752168, 0.3081033422447303, -0.16972133864046018, -0.36038159881444537, -0.006119467388592003, -0.30434609671835516, 0.03581128219580826, 0.20033992489060276, -0.0184099134496... |
708.3997 | The Charged Z(4433): Towards a New Spectroscopy | We identify the newly found Z(4433) with the first radial excitation of the
tetraquark basic supermultiplet to which X(3872) and X(3876) belong.
Experimental predictions following from this hypothesis are spelled out.
| hep-ph | we identify the newly found z4433 with the first radial excitation of the tetraquark basic supermultiplet to which x3872 and x3876 belong experimental predictions following from this hypothesis are spelled out | [['we', 'identify', 'the', 'newly', 'found', 'z4433', 'with', 'the', 'first', 'radial', 'excitation', 'of', 'the', 'tetraquark', 'basic', 'supermultiplet', 'to', 'which', 'x3872', 'and', 'x3876', 'belong', 'experimental', 'predictions', 'following', 'from', 'this', 'hypothesis', 'are', 'spelled', 'out']] | [-0.04215987497009337, 0.10869300561025738, -0.12141404170542955, 0.10482097263059889, -0.09406751108666261, -0.16213983713338773, 0.07208940380563339, 0.3448432799428701, -0.17327558607794344, -0.24981892680128415, -0.013082660641521216, -0.2523419267808398, -0.09735055986481408, 0.06888197891724607, 0.065292456808189... |
708.3998 | High-pressure infrared spectroscopy: tuning of the low-energy
excitations in correlated electron systems | We have extended the range of the high-pressure optical spectroscopy to the
far-infrared region keeping the accuracy of ambient-pressure experiments. The
newly-developed method offers a powerful tool for the study of pressure-induced
phase transitions and electronic-structural changes in correlated electron
systems. ... | cond-mat.str-el | we have extended the range of the highpressure optical spectroscopy to the farinfrared region keeping the accuracy of ambientpressure experiments the newlydeveloped method offers a powerful tool for the study of pressureinduced phase transitions and electronicstructural changes in correlated electron systems the novelt... | [['we', 'have', 'extended', 'the', 'range', 'of', 'the', 'highpressure', 'optical', 'spectroscopy', 'to', 'the', 'farinfrared', 'region', 'keeping', 'the', 'accuracy', 'of', 'ambientpressure', 'experiments', 'the', 'newlydeveloped', 'method', 'offers', 'a', 'powerful', 'tool', 'for', 'the', 'study', 'of', 'pressureindu... | [-0.13183440755299097, 0.22452832825442065, -0.058022237436441505, -0.047115669166056535, -0.008908128249458969, -0.11197097201549791, 0.15611621081648322, 0.39490447179904503, -0.2693152882550892, -0.2930071716944344, 0.05929798346646988, -0.30109921900264836, -0.0859775578780835, 0.1674538657887177, 0.059410676603491... |
708.3999 | Spin Diagrams for Equal-Mass Black-Hole Binaries with Aligned Spins | Binary black-hole systems with spins aligned with the orbital angular
momentum are of special interest as they may be the preferred end-state of the
inspiral of generic supermassive binary black-hole systems. In view of this, we
have computed the inspiral and merger of a large set of binary systems of
equal-mass blac... | gr-qc astro-ph | binary blackhole systems with spins aligned with the orbital angular momentum are of special interest as they may be the preferred endstate of the inspiral of generic supermassive binary blackhole systems in view of this we have computed the inspiral and merger of a large set of binary systems of equalmass black holes ... | [['binary', 'blackhole', 'systems', 'with', 'spins', 'aligned', 'with', 'the', 'orbital', 'angular', 'momentum', 'are', 'of', 'special', 'interest', 'as', 'they', 'may', 'be', 'the', 'preferred', 'endstate', 'of', 'the', 'inspiral', 'of', 'generic', 'supermassive', 'binary', 'blackhole', 'systems', 'in', 'view', 'of', ... | [-0.18872416713577886, 0.17978644257835377, -0.03483351158371907, 0.06788201537645777, -0.06822110441460358, -0.10916163190835859, -0.01132303995280943, 0.3527268010922291, -0.17086791056321887, -0.3291945688244773, 0.07407060060536534, -0.29640352017458194, -0.005537495422139158, 0.20580015076718072, 0.016672943378003... |
708.4 | Coherent Schwinger Interaction from Darboux Transformation | The exactly solvable scalar-tensor potential of the four-component Dirac
equation has been obtained by the Darboux transformation method. The
constructed potential has been interpreted in terms of nucleon-nucleon and
Schwinger interactions of neutral particles with lattice sites during their
channeling Hamiltonians o... | hep-th | the exactly solvable scalartensor potential of the fourcomponent dirac equation has been obtained by the darboux transformation method the constructed potential has been interpreted in terms of nucleonnucleon and schwinger interactions of neutral particles with lattice sites during their channeling hamiltonians of a sc... | [['the', 'exactly', 'solvable', 'scalartensor', 'potential', 'of', 'the', 'fourcomponent', 'dirac', 'equation', 'has', 'been', 'obtained', 'by', 'the', 'darboux', 'transformation', 'method', 'the', 'constructed', 'potential', 'has', 'been', 'interpreted', 'in', 'terms', 'of', 'nucleonnucleon', 'and', 'schwinger', 'inte... | [-0.1666570066028651, 0.1418339141759358, -0.07099252516062522, 0.06241319582746555, -0.04441286353011654, -0.13530265708925993, -0.018547728552470263, 0.337714515422305, -0.247453771276425, -0.22424640639187537, 0.017562805845606308, -0.29243225752286717, -0.1463211157346425, 0.1471356107049609, 0.08078274872051934, 0... |
708.4001 | Critical points of inner functions, nonlinear partial differential
equations, and an extension of Liouville's theorem | We establish an extension of Liouville's classical representation theorem for
solutions of the partial differential equation $\Delta u=4 e^{2u}$ and combine
this result with methods from nonlinear elliptic PDE to construct holomorphic
maps with prescribed critical points and specified boundary behaviour. For
instance... | math.CV math.AP | we establish an extension of liouvilles classical representation theorem for solutions of the partial differential equation delta u4 e2u and combine this result with methods from nonlinear elliptic pde to construct holomorphic maps with prescribed critical points and specified boundary behaviour for instance we show th... | [['we', 'establish', 'an', 'extension', 'of', 'liouvilles', 'classical', 'representation', 'theorem', 'for', 'solutions', 'of', 'the', 'partial', 'differential', 'equation', 'delta', 'u4', 'e2u', 'and', 'combine', 'this', 'result', 'with', 'methods', 'from', 'nonlinear', 'elliptic', 'pde', 'to', 'construct', 'holomorph... | [-0.14332890798291767, 0.0039263215150618005, -0.07162490757422976, 0.03124039515387267, -0.08211726512483976, -0.14639408117229188, -0.000651601953489453, 0.30035801107684773, -0.3429007848414282, -0.20796733092010758, 0.1280882375093499, -0.328727337135071, -0.16758928005583584, 0.19787220321135757, -0.11677923425744... |
708.4002 | Evidence for evolution from pure states to mixed states in pion creation
process pi(-) p -> pi(-)pi(+) n on polarized target and its physical
interpretation | In 1982 Hawking suggested that quantum fluctuations of space-time metric will
induce a non-unitary evolution from pure initial states to mixed final states
in particle interactions at any energy. This hypothesis can be tested using
existing CERN data on pi(-) p -> pi(-)pi(+) n on polarized target at 17.2
GeV/c. The p... | hep-ph gr-qc | in 1982 hawking suggested that quantum fluctuations of spacetime metric will induce a nonunitary evolution from pure initial states to mixed final states in particle interactions at any energy this hypothesis can be tested using existing cern data on pi p pipi n on polarized target at 172 gevc the purity of the final s... | [['in', '1982', 'hawking', 'suggested', 'that', 'quantum', 'fluctuations', 'of', 'spacetime', 'metric', 'will', 'induce', 'a', 'nonunitary', 'evolution', 'from', 'pure', 'initial', 'states', 'to', 'mixed', 'final', 'states', 'in', 'particle', 'interactions', 'at', 'any', 'energy', 'this', 'hypothesis', 'can', 'be', 'te... | [-0.12521222109868252, 0.2796447967011985, -0.1367232479738502, 0.0767951401071434, 0.02489216737067926, -0.14142250433313655, 0.03954690665330694, 0.3226860747808776, -0.21598375675796766, -0.2710898306454962, -0.0012346287400935565, -0.2973392957832381, -0.013855166343852268, 0.14246565865132174, 0.03697598720383313,... |
708.4003 | Mixed Higgsino Dark Matter from a Large SU(2) Gaugino Mass | We observe that in SUSY models with non-universal GUT scale gaugino mass
parameters, raising the GUT scale SU(2) gaugino mass |M_2| from its unified
value results in a smaller value of -m_{H_u}^2 at the weak scale. By the
electroweak symmetry breaking conditions, this implies a reduced value of \mu^2
{\it vis \`a vis... | hep-ph | we observe that in susy models with nonuniversal gut scale gaugino mass parameters raising the gut scale su2 gaugino mass m_2 from its unified value results in a smaller value of m_h_u2 at the weak scale by the electroweak symmetry breaking conditions this implies a reduced value of mu2 it vis a vis models with gaugino... | [['we', 'observe', 'that', 'in', 'susy', 'models', 'with', 'nonuniversal', 'gut', 'scale', 'gaugino', 'mass', 'parameters', 'raising', 'the', 'gut', 'scale', 'su2', 'gaugino', 'mass', 'm_2', 'from', 'its', 'unified', 'value', 'results', 'in', 'a', 'smaller', 'value', 'of', 'm_h_u2', 'at', 'the', 'weak', 'scale', 'by', ... | [-0.0905636574331785, 0.302368628380305, -0.05206321831792593, 0.2047702356415028, -0.08469129941039817, -0.17067824348985675, 0.015031021314257003, 0.3262797919528044, -0.19949395127118902, -0.36405742523518014, 0.046551016960392134, -0.2599561696356915, 0.07290043318049705, 0.1480918133076518, 0.024873018743311787, 0... |
708.4004 | Energy of bond defects in quantum spin chains obtained from local
approximations and from exact diagonalization | We study the influence of ferromagnetic and antiferromagnetic bond defects on
the ground-state energy of antiferromagnetic spin chains. In the absence of
translational invariance, the energy spectrum of the full Hamiltonian is
obtained numerically, by an iterative modification of the power algorithm. In
parallel, app... | cond-mat.mtrl-sci cond-mat.stat-mech cond-mat.str-el | we study the influence of ferromagnetic and antiferromagnetic bond defects on the groundstate energy of antiferromagnetic spin chains in the absence of translational invariance the energy spectrum of the full hamiltonian is obtained numerically by an iterative modification of the power algorithm in parallel approximate... | [['we', 'study', 'the', 'influence', 'of', 'ferromagnetic', 'and', 'antiferromagnetic', 'bond', 'defects', 'on', 'the', 'groundstate', 'energy', 'of', 'antiferromagnetic', 'spin', 'chains', 'in', 'the', 'absence', 'of', 'translational', 'invariance', 'the', 'energy', 'spectrum', 'of', 'the', 'full', 'hamiltonian', 'is'... | [-0.1560528374452522, 0.107114171435714, -0.05572173180922434, 0.07508306004160988, 0.0019382681643617325, -0.08987164761250217, 0.09189738353471393, 0.3995375067697487, -0.23219044014568563, -0.3214351233310889, 0.011740600152035662, -0.28354283238666644, -0.09363486207481744, 0.11627342093034067, 0.08407355833501703,... |
708.4005 | Metastable Kinks in the Orbifold | We consider static configurations of bulk scalar fields in extra dimensional
models in which the fifth dimension is an $S^1/Z_2$ orbifold. There may exist a
finite number of such configurations, with total number depending on the size
of the orbifold interval. We perform a detailed Sturm-Liouville stability
analysis ... | hep-ph hep-th | we consider static configurations of bulk scalar fields in extra dimensional models in which the fifth dimension is an s1z_2 orbifold there may exist a finite number of such configurations with total number depending on the size of the orbifold interval we perform a detailed sturmliouville stability analysis that demon... | [['we', 'consider', 'static', 'configurations', 'of', 'bulk', 'scalar', 'fields', 'in', 'extra', 'dimensional', 'models', 'in', 'which', 'the', 'fifth', 'dimension', 'is', 'an', 's1z_2', 'orbifold', 'there', 'may', 'exist', 'a', 'finite', 'number', 'of', 'such', 'configurations', 'with', 'total', 'number', 'depending',... | [-0.18463358193236803, 0.09712823947927626, -0.05928272700957244, 0.06813609162789015, -0.07653828916982526, -0.1326639803303849, 0.02493647529322299, 0.36175179394582907, -0.1783036052559813, -0.2865667528871979, 0.11822746797309568, -0.255801743428622, -0.14164271804592793, 0.1683192979278309, -0.026671462395184097, ... |
708.4006 | The Drinfel'd Double and Twisting in Stringy Orbifold Theory | This paper exposes the fundamental role that the Drinfel'd double $\dkg$ of
the group ring of a finite group $G$ and its twists $\dbkg$, $\beta \in
Z^3(G,\uk)$ as defined by Dijkgraaf--Pasquier--Roche play in stringy orbifold
theories and their twistings.
The results pertain to three different aspects of the theory... | math.AG math.KT math.QA | this paper exposes the fundamental role that the drinfeld double dkg of the group ring of a finite group g and its twists dbkg beta in z3guk as defined by dijkgraafpasquierroche play in stringy orbifold theories and their twistings the results pertain to three different aspects of the theory first we show that gfrobeni... | [['this', 'paper', 'exposes', 'the', 'fundamental', 'role', 'that', 'the', 'drinfeld', 'double', 'dkg', 'of', 'the', 'group', 'ring', 'of', 'a', 'finite', 'group', 'g', 'and', 'its', 'twists', 'dbkg', 'beta', 'in', 'z3guk', 'as', 'defined', 'by', 'dijkgraafpasquierroche', 'play', 'in', 'stringy', 'orbifold', 'theories'... | [-0.18293956729406813, 0.0427881284060235, -0.10745381477995422, 0.08009768739187469, -0.08269860624367821, -0.12753968135903365, -0.009080228510837274, 0.31071730568903316, -0.37024080849737034, -0.22216232306184783, 0.11694633763286168, -0.1908351799192833, -0.18160031403243626, 0.18760458361384214, -0.17255770857939... |
708.4007 | A critical constant for the k nearest neighbour model | Let P be a Poisson process of intensity one in a square S_n of area n. For a
fixed integer k, join every point of P to its k nearest neighbours, creating an
undirected random geometric graph G_{n,k}. We prove that there exists a
critical constant c such that for c'<c, G_{n,c'log n} is disconnected with
probability te... | math.PR math.CO | let p be a poisson process of intensity one in a square s_n of area n for a fixed integer k join every point of p to its k nearest neighbours creating an undirected random geometric graph g_nk we prove that there exists a critical constant c such that for cc g_nclog n is disconnected with probability tending to 1 as n ... | [['let', 'p', 'be', 'a', 'poisson', 'process', 'of', 'intensity', 'one', 'in', 'a', 'square', 's_n', 'of', 'area', 'n', 'for', 'a', 'fixed', 'integer', 'k', 'join', 'every', 'point', 'of', 'p', 'to', 'its', 'k', 'nearest', 'neighbours', 'creating', 'an', 'undirected', 'random', 'geometric', 'graph', 'g_nk', 'we', 'prov... | [-0.1810973547399044, 0.16798862482808932, -0.03914262452738339, 0.0006185920244278033, -0.043842403053337434, -0.2619723395622346, 0.1252925099407354, 0.342114750630735, -0.29033189647820556, -0.2524910483226766, 0.04212184364284818, -0.35839473644501707, -0.09538522022880949, 0.07172152630231354, -0.05155701481663946... |
708.4008 | Existence and Stability of Non-Trivial Scalar Field Configurations in
Orbifolded Extra Dimensions | We consider the existence and stability of static configurations of a scalar
field in a five dimensional spacetime in which the extra spatial dimension is
compactified on an $S^1/Z_2$ orbifold. For a wide class of potentials with
multiple minima there exist a finite number of such configurations, with total
number de... | hep-ph hep-th | we consider the existence and stability of static configurations of a scalar field in a five dimensional spacetime in which the extra spatial dimension is compactified on an s1z_2 orbifold for a wide class of potentials with multiple minima there exist a finite number of such configurations with total number depending ... | [['we', 'consider', 'the', 'existence', 'and', 'stability', 'of', 'static', 'configurations', 'of', 'a', 'scalar', 'field', 'in', 'a', 'five', 'dimensional', 'spacetime', 'in', 'which', 'the', 'extra', 'spatial', 'dimension', 'is', 'compactified', 'on', 'an', 's1z_2', 'orbifold', 'for', 'a', 'wide', 'class', 'of', 'pot... | [-0.18509227943429926, 0.11267656861920416, -0.07050654895936757, 0.06933088834230944, -0.06542710098607914, -0.17371221180039928, 0.018687061501503753, 0.3380810176787123, -0.19107774534962907, -0.2804055667421135, 0.13731225126297178, -0.2448956614308591, -0.13789093950899303, 0.21134382189951673, -0.0263053669940925... |
708.4009 | Generation of spin currents and spin densities in systems with reduced
symmetry | We show that the spin-current response of a semiconductor crystal to an
external electric field is considerably more complex than previously assumed.
While in systems of high symmetry only the spin-Hall components are allowed, in
systems of lower symmetry other non-spin-Hall components may be present. We
argue that, ... | cond-mat.mes-hall | we show that the spincurrent response of a semiconductor crystal to an external electric field is considerably more complex than previously assumed while in systems of high symmetry only the spinhall components are allowed in systems of lower symmetry other nonspinhall components may be present we argue that when spino... | [['we', 'show', 'that', 'the', 'spincurrent', 'response', 'of', 'a', 'semiconductor', 'crystal', 'to', 'an', 'external', 'electric', 'field', 'is', 'considerably', 'more', 'complex', 'than', 'previously', 'assumed', 'while', 'in', 'systems', 'of', 'high', 'symmetry', 'only', 'the', 'spinhall', 'components', 'are', 'all... | [-0.1751294377790138, 0.17237014769006154, -0.05256291297095644, 0.06388565724394715, -0.0769522867689864, -0.1157977553554067, -0.001548195828120185, 0.4263107796207446, -0.2543280616856548, -0.3073472357002877, 0.019582404702228783, -0.2894030956457518, -0.16611380054529348, 0.2035327293643994, -0.003498899218227182,... |
708.401 | On the fifth order KdV equation: local well-posedness and lack of
uniform continuity of the solution map | In this paper we prove that the fifth order equation arising from the KdV
hierarchy $ \partial_tu + \partial_x^5u + c_1\partial_x u\partial_x^2u +
c_2u\partial_x^3u = 0 $ is locally well-posed in $ H^s(\mathbb{R}) $ for $ s>
5/2. Also, we prove the solution map of the equation is not uniformly
continuous for $s>0$.
| math.AP | in this paper we prove that the fifth order equation arising from the kdv hierarchy partial_tu partial_x5u c_1partial_x upartial_x2u c_2upartial_x3u 0 is locally wellposed in hsmathbbr for s 52 also we prove the solution map of the equation is not uniformly continuous for s0 | [['in', 'this', 'paper', 'we', 'prove', 'that', 'the', 'fifth', 'order', 'equation', 'arising', 'from', 'the', 'kdv', 'hierarchy', 'partial_tu', 'partial_x5u', 'c_1partial_x', 'upartial_x2u', 'c_2upartial_x3u', '0', 'is', 'locally', 'wellposed', 'in', 'hsmathbbr', 'for', 's', '52', 'also', 'we', 'prove', 'the', 'soluti... | [-0.15869426964171707, 0.06369873604214774, -0.04879958390417259, 0.06806591045531649, -0.06013267123844565, -0.13214886433831075, -0.04831406712338964, 0.2715760891030474, -0.371873750919249, -0.1536698956496832, 0.16612056942043327, -0.3354920789417697, -0.1342268452593466, 0.1449388848481382, -0.03867388721101168, 0... |
708.4011 | Functionalized nanopore-embedded electrodes for rapid DNA sequencing | The determination of a patient's DNA sequence can, in principle, reveal an
increased risk to fall ill with particular diseases [1,2] and help to design
"personalized medicine" [3]. Moreover, statistical studies and comparison of
genomes [4] of a large number of individuals are crucial for the analysis of
mutations [5... | physics.bio-ph cond-mat.soft q-bio.BM | the determination of a patients dna sequence can in principle reveal an increased risk to fall ill with particular diseases 12 and help to design personalized medicine 3 moreover statistical studies and comparison of genomes 4 of a large number of individuals are crucial for the analysis of mutations 5 and hereditary d... | [['the', 'determination', 'of', 'a', 'patients', 'dna', 'sequence', 'can', 'in', 'principle', 'reveal', 'an', 'increased', 'risk', 'to', 'fall', 'ill', 'with', 'particular', 'diseases', '12', 'and', 'help', 'to', 'design', 'personalized', 'medicine', '3', 'moreover', 'statistical', 'studies', 'and', 'comparison', 'of',... | [-0.07736933319001563, 0.079901138696328, -0.03934498140510793, 0.056362936603618435, -0.04072012087330222, -0.15704264032964904, 0.08492992563276655, 0.37296956073078846, -0.2277655948781305, -0.3159318999076883, 0.08811039890835269, -0.2531126417219639, -0.16027186536178406, 0.23400249781294002, -0.09868842562453614,... |
708.4012 | Spin-charge separation in a strongly correlated spin-polarized chain | We combine the first-quantized path-integral formalism and bosonization to
develop a phenomenological theory for spin-charge coupled dynamics in
one-dimensional (1D) ferromagnetic systems with strong interparticle repulsion,
at low temperatures. We assume an effective spin-charge separation and retain
the standard Lu... | cond-mat.str-el cond-mat.mes-hall | we combine the firstquantized pathintegral formalism and bosonization to develop a phenomenological theory for spincharge coupled dynamics in onedimensional 1d ferromagnetic systems with strong interparticle repulsion at low temperatures we assume an effective spincharge separation and retain the standard luttingerliqu... | [['we', 'combine', 'the', 'firstquantized', 'pathintegral', 'formalism', 'and', 'bosonization', 'to', 'develop', 'a', 'phenomenological', 'theory', 'for', 'spincharge', 'coupled', 'dynamics', 'in', 'onedimensional', '1d', 'ferromagnetic', 'systems', 'with', 'strong', 'interparticle', 'repulsion', 'at', 'low', 'temperat... | [-0.17011883052285104, 0.211114537566341, -0.08460171292558787, 0.07266819368997662, -0.058796864452625754, -0.1899548295164006, 0.0037646237281425033, 0.334728248216504, -0.2450546698807967, -0.2266893776809322, -0.06505552182709068, -0.302656448427953, -0.14704742842678017, 0.12928437146668634, 0.09995601687457084, 0... |
708.4013 | The Axis of Opportunity: The Large-Scale Correlation of Elliptical
Galaxies | This paper has been withdrawn by the author due to the discovery of a serious
bias resulting from the systematic dimming of galaxies with larger
ellipticities away from the North Galactic Pole. Thus the conclusion that there
is a special axis along which the elliptical galaxies tend to be aligned is
incorrect.
| astro-ph | this paper has been withdrawn by the author due to the discovery of a serious bias resulting from the systematic dimming of galaxies with larger ellipticities away from the north galactic pole thus the conclusion that there is a special axis along which the elliptical galaxies tend to be aligned is incorrect | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'author', 'due', 'to', 'the', 'discovery', 'of', 'a', 'serious', 'bias', 'resulting', 'from', 'the', 'systematic', 'dimming', 'of', 'galaxies', 'with', 'larger', 'ellipticities', 'away', 'from', 'the', 'north', 'galactic', 'pole', 'thus', 'the', 'conclusion', ... | [-0.06879831121030013, 0.054611810500948474, -0.10478193888691469, 0.05226750010311102, -0.18351098844924799, -0.05412468961171376, 0.019991257104825657, 0.3800006233012447, -0.20561992103019014, -0.31613974742448103, 0.08422926096962048, -0.3098405974675328, -0.08133071739799701, 0.14717883245947844, -0.12303330648977... |
708.4014 | Spectral energy distributions of submm/radio bright gamma-ray burst host
galaxies | We present optical to radio spectral energy distribution fitting of the host
galaxies of four long gamma-ray bursts: 980703, 000210, 000418 and 010222,
which were detected at submillimetre and/or radio wavelengths. We find that
only very young starburst galaxy models are consistent with the data having
both blue opti... | astro-ph | we present optical to radio spectral energy distribution fitting of the host galaxies of four long gammaray bursts 980703 000210 000418 and 010222 which were detected at submillimetre andor radio wavelengths we find that only very young starburst galaxy models are consistent with the data having both blue optical color... | [['we', 'present', 'optical', 'to', 'radio', 'spectral', 'energy', 'distribution', 'fitting', 'of', 'the', 'host', 'galaxies', 'of', 'four', 'long', 'gammaray', 'bursts', '980703', '000210', '000418', 'and', '010222', 'which', 'were', 'detected', 'at', 'submillimetre', 'andor', 'radio', 'wavelengths', 'we', 'find', 'th... | [-0.020787274390657213, 0.11793142159350534, -0.05249600666277903, 0.10817933675060247, -0.09043232072144747, -0.11095723504710824, 0.036213549059577924, 0.5365909128449857, -0.12207666671081902, -0.36733647459682, 0.06659052943057836, -0.3276170543989444, 0.01160246934345428, 0.19896630165315768, -0.002148111375603587... |
708.4015 | Energetic Impact of Jet Inflated Cocoons in Relaxed Galaxy Clusters | Jets from active galactic nuclei (AGN) in the cores of galaxy clusters have
the potential to be a major contributor to the energy budget of the
intracluster medium (ICM). To study the dependence of the interaction between
the AGN jets and the ICM on the parameters of the jets themselves, we present a
parameter survey... | astro-ph | jets from active galactic nuclei agn in the cores of galaxy clusters have the potential to be a major contributor to the energy budget of the intracluster medium icm to study the dependence of the interaction between the agn jets and the icm on the parameters of the jets themselves we present a parameter survey of twod... | [['jets', 'from', 'active', 'galactic', 'nuclei', 'agn', 'in', 'the', 'cores', 'of', 'galaxy', 'clusters', 'have', 'the', 'potential', 'to', 'be', 'a', 'major', 'contributor', 'to', 'the', 'energy', 'budget', 'of', 'the', 'intracluster', 'medium', 'icm', 'to', 'study', 'the', 'dependence', 'of', 'the', 'interaction', '... | [-0.09722411160460483, 0.17448776612714442, -0.06244754939953881, 0.1069958092425209, -0.04337899950041901, -0.017793075972638853, 0.027517000500004295, 0.3770278357339769, -0.22764565969489262, -0.3519630584527146, 0.02975001541463743, -0.2925271670524539, 0.03175270915116099, 0.19415407994529232, 0.05394223558621227,... |
708.4016 | Glueballs, Hybrids, Multiquarks. Experimental facts versus QCD inspired
concepts | The spectroscopy of light and heavy mesons is reviewed with emphasis on
glueballs, hybrids, and tetraquarks.
| hep-ph | the spectroscopy of light and heavy mesons is reviewed with emphasis on glueballs hybrids and tetraquarks | [['the', 'spectroscopy', 'of', 'light', 'and', 'heavy', 'mesons', 'is', 'reviewed', 'with', 'emphasis', 'on', 'glueballs', 'hybrids', 'and', 'tetraquarks']] | [-0.033919582987437025, 0.3893849326414056, -0.14830222562886775, 0.19658002028154442, -0.0340218844357878, -0.25450206897221506, 0.09927179652731866, 0.41052885772660375, -0.026966110803186893, -0.15953028528019786, -0.014003228396177292, -0.45155719853937626, 0.017182795330882072, 0.05813634488731623, 0.0494015527656... |
708.4017 | Hot GRB-selected Submillimeter Galaxies | Using detailed spectral energy distribution fits we present evidence that
submillimeter- and radio-bright gamma-ray burst host galaxies are hotter
counterparts to submillimeter galaxies. This hypothesis makes them of special
interest since hotter submm galaxies are difficult to find and are believed to
contribute sig... | astro-ph | using detailed spectral energy distribution fits we present evidence that submillimeter and radiobright gammaray burst host galaxies are hotter counterparts to submillimeter galaxies this hypothesis makes them of special interest since hotter submm galaxies are difficult to find and are believed to contribute significa... | [['using', 'detailed', 'spectral', 'energy', 'distribution', 'fits', 'we', 'present', 'evidence', 'that', 'submillimeter', 'and', 'radiobright', 'gammaray', 'burst', 'host', 'galaxies', 'are', 'hotter', 'counterparts', 'to', 'submillimeter', 'galaxies', 'this', 'hypothesis', 'makes', 'them', 'of', 'special', 'interest'... | [-0.014969045699287493, 0.09049169061024888, -0.0830720713845669, 0.20428246050813378, -0.22185651889930552, -0.05995053971463886, 0.002345862256613775, 0.5223319685229888, -0.05514734080777718, -0.345174228772521, 0.010948787210509181, -0.3085789404352769, -0.02153973589436366, 0.2006187685407125, -0.0227079215244605,... |
708.4018 | Concealed Quantum Information | We study the teleportation scheme performed by means of a partially entangled
pure state. We found that the information belonging to the quantum channel can
be distributed into both the system of the transmitter and the system of the
receiver. Thus, in order to complete the teleportation process it is required
to per... | quant-ph | we study the teleportation scheme performed by means of a partially entangled pure state we found that the information belonging to the quantum channel can be distributed into both the system of the transmitter and the system of the receiver thus in order to complete the teleportation process it is required to perform ... | [['we', 'study', 'the', 'teleportation', 'scheme', 'performed', 'by', 'means', 'of', 'a', 'partially', 'entangled', 'pure', 'state', 'we', 'found', 'that', 'the', 'information', 'belonging', 'to', 'the', 'quantum', 'channel', 'can', 'be', 'distributed', 'into', 'both', 'the', 'system', 'of', 'the', 'transmitter', 'and'... | [-0.1504911325847298, 0.15855920571977533, -0.1316889670702654, 0.029973532289413678, -3.477718748219378e-05, -0.23449458874057275, 0.10026127981600931, 0.37519770699578364, -0.29226259947628586, -0.2687574671329679, 0.09118007340988664, -0.23799260693346885, -0.09489141022870401, 0.15325988480938715, -0.04573479406367... |
708.4019 | Comparing $GL_n$-Representations by Characteristic-Free Isomorphisms
between Generalized Schur Algebras | Isomorphisms are constructed between generalized Schur algebras in different
degrees. The construction covers both the classical case (of general linear
groups over infinite fields of arbitrary characteristic) and the quantized case
(in type $A$, for any non-zero value of the quantum parameter $q$). The
construction ... | math.RT | isomorphisms are constructed between generalized schur algebras in different degrees the construction covers both the classical case of general linear groups over infinite fields of arbitrary characteristic and the quantized case in type a for any nonzero value of the quantum parameter q the construction does not depen... | [['isomorphisms', 'are', 'constructed', 'between', 'generalized', 'schur', 'algebras', 'in', 'different', 'degrees', 'the', 'construction', 'covers', 'both', 'the', 'classical', 'case', 'of', 'general', 'linear', 'groups', 'over', 'infinite', 'fields', 'of', 'arbitrary', 'characteristic', 'and', 'the', 'quantized', 'ca... | [-0.1701242488783759, 0.10932263565409156, -0.05499616928759392, 0.04587040534494696, -0.10815413265388359, -0.14407354327304675, 0.008440313221014163, 0.3098235916900071, -0.3393636020865325, -0.2424665881469762, 0.09512452733795251, -0.19417703425226449, -0.14387216944843195, 0.20179750973165775, -0.09358479398898445... |
708.402 | Yields from single AGB stars | In order to understand the composition of planetary nebulae we first need to
study the nucleosynthesis occurring in the progenitor star during the
thermally-pulsing Asymptotic Giant Branch (AGB) phase. I present an overview of
single AGB evolution, with an emphasis on the mixing processes that alter the
envelope comp... | astro-ph | in order to understand the composition of planetary nebulae we first need to study the nucleosynthesis occurring in the progenitor star during the thermallypulsing asymptotic giant branch agb phase i present an overview of single agb evolution with an emphasis on the mixing processes that alter the envelope composition... | [['in', 'order', 'to', 'understand', 'the', 'composition', 'of', 'planetary', 'nebulae', 'we', 'first', 'need', 'to', 'study', 'the', 'nucleosynthesis', 'occurring', 'in', 'the', 'progenitor', 'star', 'during', 'the', 'thermallypulsing', 'asymptotic', 'giant', 'branch', 'agb', 'phase', 'i', 'present', 'an', 'overview',... | [-0.04738402937258047, 0.13791458777730384, -0.10696164421027615, 0.0473895345533651, -0.1217308539956335, 0.021811894178094846, 0.06350169866345823, 0.38830258555355524, -0.16102515660976577, -0.3257719895669392, 0.060346224245482256, -0.22565612569451332, -0.06648693588517961, 0.1414124527724371, -0.07171547657529277... |
708.4021 | \emph{In situ} measurement of three-dimensional ion densities in focused
femtosecond pulses | We image spatial distributions of Xe$^{q+}$ ions in the focus of a laser beam
of ultrashort, intense pulses in all three dimensions, with a resolution of
$\sim$3 $\mu$m and $\sim$12 $\mu$m in the two transverse directions. This
allows for studying ionization processes without spatially averaging ion
yields. Our \emph... | physics.atom-ph | we image spatial distributions of xeq ions in the focus of a laser beam of ultrashort intense pulses in all three dimensions with a resolution of sim3 mum and sim12 mum in the two transverse directions this allows for studying ionization processes without spatially averaging ion yields our emphin situ ion imaging is al... | [['we', 'image', 'spatial', 'distributions', 'of', 'xeq', 'ions', 'in', 'the', 'focus', 'of', 'a', 'laser', 'beam', 'of', 'ultrashort', 'intense', 'pulses', 'in', 'all', 'three', 'dimensions', 'with', 'a', 'resolution', 'of', 'sim3', 'mum', 'and', 'sim12', 'mum', 'in', 'the', 'two', 'transverse', 'directions', 'this', ... | [-0.07741554209259244, 0.18435012611066948, -0.05994906232986903, 0.05454075291909619, 0.03796976280626746, -0.14834707419920182, -0.048775666868504215, 0.5265623898226388, -0.19829867485606548, -0.3027477842489524, 0.01778109801210919, -0.2776995844004868, 0.028211936285441302, 0.22323618829250336, -0.0181178814394171... |
708.4022 | Time reversal invariance in finance | Time reversal invariance can be summarized as follows: no difference can be
measured if a sequence of events is run forward or backward in time. Because
price time series are dominated by a randomness that hides possible structures
and orders, the existence of time reversal invariance requires care to be
investigated... | q-fin.ST physics.soc-ph q-fin.CP | time reversal invariance can be summarized as follows no difference can be measured if a sequence of events is run forward or backward in time because price time series are dominated by a randomness that hides possible structures and orders the existence of time reversal invariance requires care to be investigated diff... | [['time', 'reversal', 'invariance', 'can', 'be', 'summarized', 'as', 'follows', 'no', 'difference', 'can', 'be', 'measured', 'if', 'a', 'sequence', 'of', 'events', 'is', 'run', 'forward', 'or', 'backward', 'in', 'time', 'because', 'price', 'time', 'series', 'are', 'dominated', 'by', 'a', 'randomness', 'that', 'hides', ... | [-0.13430005130389291, 0.1617886580951862, -0.1361850152798497, 0.18340451005724084, -0.10076363355658899, -0.13971636789357103, 0.027920936125693154, 0.4472219918435752, -0.3295530149439309, -0.2758072225014435, 0.14219809380038048, -0.25395705623102166, -0.10140509644787736, 0.20269696456817723, -0.02941873786586568,... |
708.4023 | A limited resource model of fault-tolerant capability against cascading
failure of complex network | We propose a novel capacity model for complex networks against cascading
failure. In this model, vertices with both higher loads and larger degrees
should be paid more extra capacities, i.e. the allocation of extra capacity on
vertex $i$ will be proportional to $ k_{i}^{\gamma} $, where $ k_{i}$ is the
degree of vert... | physics.soc-ph physics.data-an | we propose a novel capacity model for complex networks against cascading failure in this model vertices with both higher loads and larger degrees should be paid more extra capacities ie the allocation of extra capacity on vertex i will be proportional to k_igamma where k_i is the degree of vertex i and gamma0 is a free... | [['we', 'propose', 'a', 'novel', 'capacity', 'model', 'for', 'complex', 'networks', 'against', 'cascading', 'failure', 'in', 'this', 'model', 'vertices', 'with', 'both', 'higher', 'loads', 'and', 'larger', 'degrees', 'should', 'be', 'paid', 'more', 'extra', 'capacities', 'ie', 'the', 'allocation', 'of', 'extra', 'capac... | [-0.12927365024026566, 0.09587791187504491, 0.0016752877477351782, 0.04205458289252819, -0.07273065855030666, -0.24640606004990392, 0.06068748478255757, 0.4005439541415199, -0.24395471641404942, -0.29398978209880355, 0.08745929373013736, -0.28803577437833117, -0.17323602118355397, 0.11742506844533997, -0.11281753788512... |
708.4024 | ac Losses in a Finite Z Stack Using an Anisotropic Homogeneous-Medium
Approximation | A finite stack of thin superconducting tapes, all carrying a fixed current I,
can be approximated by an anisotropic superconducting bar with critical current
density Jc=Ic/2aD, where Ic is the critical current of each tape, 2a is the
tape width, and D is the tape-to-tape periodicity. The current density J must
obey t... | cond-mat.supr-con | a finite stack of thin superconducting tapes all carrying a fixed current i can be approximated by an anisotropic superconducting bar with critical current density jcic2ad where ic is the critical current of each tape 2a is the tape width and d is the tapetotape periodicity the current density j must obey the constrain... | [['a', 'finite', 'stack', 'of', 'thin', 'superconducting', 'tapes', 'all', 'carrying', 'a', 'fixed', 'current', 'i', 'can', 'be', 'approximated', 'by', 'an', 'anisotropic', 'superconducting', 'bar', 'with', 'critical', 'current', 'density', 'jcic2ad', 'where', 'ic', 'is', 'the', 'critical', 'current', 'of', 'each', 'ta... | [-0.17524299402345356, 0.13475224818266154, -0.021237975404067425, 0.018512321344259376, -0.047084067869856285, -0.18533280339183897, 0.07245918372938318, 0.39356742991393456, -0.24115970940851175, -0.23621724554517143, 0.07044759708469224, -0.2614892309619273, -0.032417719412413365, 0.19858912712238697, -0.01287964231... |
708.4025 | Black holes as mirrors: quantum information in random subsystems | We study information retrieval from evaporating black holes, assuming that
the internal dynamics of a black hole is unitary and rapidly mixing, and
assuming that the retriever has unlimited control over the emitted Hawking
radiation. If the evaporation of the black hole has already proceeded past the
"half-way" point... | hep-th gr-qc quant-ph | we study information retrieval from evaporating black holes assuming that the internal dynamics of a black hole is unitary and rapidly mixing and assuming that the retriever has unlimited control over the emitted hawking radiation if the evaporation of the black hole has already proceeded past the halfway point where h... | [['we', 'study', 'information', 'retrieval', 'from', 'evaporating', 'black', 'holes', 'assuming', 'that', 'the', 'internal', 'dynamics', 'of', 'a', 'black', 'hole', 'is', 'unitary', 'and', 'rapidly', 'mixing', 'and', 'assuming', 'that', 'the', 'retriever', 'has', 'unlimited', 'control', 'over', 'the', 'emitted', 'hawki... | [-0.13535826669638634, 0.15014342041882936, -0.1196794400522879, 0.11470947385922199, -0.04161280365152494, -0.21617434917322792, 0.09349497772333487, 0.3289917658811147, -0.242886252911158, -0.28225033288874046, 0.1389722259449576, -0.353795054221106, -0.04933723401725883, 0.1897895597675684, -0.06414091771363582, 0.0... |
708.4026 | The Evolution of Oxygen and Magnesium in the Bulge and Disk of the Milky
Way | We show that the Galactic bulge and disk share a similar, strong, decline in
[O/Mg] ratio with [Mg/H]. The similarity of the [O/Mg] trend in these two,
markedly different, populations suggests a metallicity-dependent modulation of
the stellar yields from massive stars, by mass loss from winds, and related to
the Wolf... | astro-ph | we show that the galactic bulge and disk share a similar strong decline in omg ratio with mgh the similarity of the omg trend in these two markedly different populations suggests a metallicitydependent modulation of the stellar yields from massive stars by mass loss from winds and related to the wolfrayet phenomenon as... | [['we', 'show', 'that', 'the', 'galactic', 'bulge', 'and', 'disk', 'share', 'a', 'similar', 'strong', 'decline', 'in', 'omg', 'ratio', 'with', 'mgh', 'the', 'similarity', 'of', 'the', 'omg', 'trend', 'in', 'these', 'two', 'markedly', 'different', 'populations', 'suggests', 'a', 'metallicitydependent', 'modulation', 'of... | [-0.015299124921511975, 0.08935730834653961, -0.07466555802323326, 0.12445103201181544, -0.07546584418326217, -0.06206673745847573, 0.0858250586435523, 0.405367268282654, -0.15336285771835328, -0.3986044631845808, -0.047212812562065665, -0.2734928559844515, -0.0769328586985856, 0.21714817482721369, -0.11654491950633071... |
708.4027 | Predictions for masses of bottom baryons | The recent observation of Sigma_b^{+-} (uub and ddb) and Xi_b^- (dsb) baryons
at the Tevatron within 2 MeV of our theoretical predictions provides a strong
motivation for applying the same theoretical approach, based on modeling the
color hyperfine interaction, to predict the masses of other bottom baryons
which migh... | hep-ph | the recent observation of sigma_b uub and ddb and xi_b dsb baryons at the tevatron within 2 mev of our theoretical predictions provides a strong motivation for applying the same theoretical approach based on modeling the color hyperfine interaction to predict the masses of other bottom baryons which might be observed i... | [['the', 'recent', 'observation', 'of', 'sigma_b', 'uub', 'and', 'ddb', 'and', 'xi_b', 'dsb', 'baryons', 'at', 'the', 'tevatron', 'within', '2', 'mev', 'of', 'our', 'theoretical', 'predictions', 'provides', 'a', 'strong', 'motivation', 'for', 'applying', 'the', 'same', 'theoretical', 'approach', 'based', 'on', 'modelin... | [-0.041841646671255533, 0.25953112144340224, -0.04569112580081329, 0.13206785991094372, -0.03168809255386921, -0.1433713805237587, 0.13593999561952783, 0.37681282569277796, -0.166058291264988, -0.3465367196613249, -0.0792611906604663, -0.3420649334352384, 0.10223752452912642, 0.12998336641999714, 0.10611669012429589, 0... |
708.4028 | Spontaneous soliton symmetry breaking in two-dimensional coupled
Bose-Einstein condensates supported by optical lattices | Models of two-dimensional (2D) traps, with the double-well structure in the
third direction, for Bose-Einstein condensate (BEC) are introduced, with
attractive or repulsive interactions between atoms. The models are based on
systems of linearly coupled 2D Gross-Pitaevskii equations (GPEs), where the
coupling accounts... | nlin.PS | models of twodimensional 2d traps with the doublewell structure in the third direction for boseeinstein condensate bec are introduced with attractive or repulsive interactions between atoms the models are based on systems of linearly coupled 2d grosspitaevskii equations gpes where the coupling accounts for tunneling be... | [['models', 'of', 'twodimensional', '2d', 'traps', 'with', 'the', 'doublewell', 'structure', 'in', 'the', 'third', 'direction', 'for', 'boseeinstein', 'condensate', 'bec', 'are', 'introduced', 'with', 'attractive', 'or', 'repulsive', 'interactions', 'between', 'atoms', 'the', 'models', 'are', 'based', 'on', 'systems', ... | [-0.20279772904794663, 0.18247200590145077, -0.054970392863499, 0.05926505774166435, -0.02112426096946001, -0.2223049336820841, -0.006949145052582026, 0.3531053262911737, -0.23158729870343814, -0.2250782433175482, 0.07397857985738665, -0.3062720048762858, -0.12965322492085396, 0.13144185655005275, 0.02945975014939904, ... |
708.4029 | Ultrapowers of Banach algebras and modules | The Arens products are the standard way of extending the product from a
Banach algebra $\mc A$ to its bidual $\mc A''$. Ultrapowers provide another
method which is more symmetric, but one that in general will only give a
bilinear map, which may not be associative. We show that if $\mc A$ is Arens
regular, then there ... | math.FA | the arens products are the standard way of extending the product from a banach algebra mc a to its bidual mc a ultrapowers provide another method which is more symmetric but one that in general will only give a bilinear map which may not be associative we show that if mc a is arens regular then there is at least one wa... | [['the', 'arens', 'products', 'are', 'the', 'standard', 'way', 'of', 'extending', 'the', 'product', 'from', 'a', 'banach', 'algebra', 'mc', 'a', 'to', 'its', 'bidual', 'mc', 'a', 'ultrapowers', 'provide', 'another', 'method', 'which', 'is', 'more', 'symmetric', 'but', 'one', 'that', 'in', 'general', 'will', 'only', 'gi... | [-0.08611955030202088, 0.04724286647163623, -0.1279394512197801, 0.10149643854186921, -0.13124312830904683, -0.13365625694475985, -0.02431576438555187, 0.38508426320258077, -0.37980355551609624, -0.1674234235741116, 0.18761770720568047, -0.2319732781622436, -0.13740460665712317, 0.21968916231500252, -0.1216502250632741... |
708.403 | Deep ACS Imaging in the Globular Cluster NGC 6397: The Cluster Color
Magnitude Diagram and Luminosity Function | We present the CMD from deep HST imaging in the globular cluster NGC 6397.
The ACS was used for 126 orbits to image a single field in two colors (F814W,
F606W) 5 arcmin SE of the cluster center. The field observed overlaps that of
archival WFPC2 data from 1994 and 1997 which were used to proper motion (PM)
clean the ... | astro-ph | we present the cmd from deep hst imaging in the globular cluster ngc 6397 the acs was used for 126 orbits to image a single field in two colors f814w f606w 5 arcmin se of the cluster center the field observed overlaps that of archival wfpc2 data from 1994 and 1997 which were used to proper motion pm clean the data appl... | [['we', 'present', 'the', 'cmd', 'from', 'deep', 'hst', 'imaging', 'in', 'the', 'globular', 'cluster', 'ngc', '6397', 'the', 'acs', 'was', 'used', 'for', '126', 'orbits', 'to', 'image', 'a', 'single', 'field', 'in', 'two', 'colors', 'f814w', 'f606w', '5', 'arcmin', 'se', 'of', 'the', 'cluster', 'center', 'the', 'field'... | [-0.019161588651008463, 0.057408842682232515, -0.1347440655525942, 0.12005856209887295, -0.08881127839817458, -0.04600222520012823, 0.07763231309905273, 0.42580273705405286, -0.1897924268634799, -0.38318183277240475, 0.04036772122263857, -0.28715984541324563, -0.04479985158104682, 0.19816641558391743, -0.08355880315422... |
708.4031 | BDDC and FETI-DP under Minimalist Assumptions | The FETI-DP, BDDC and P-FETI-DP preconditioners are derived in a particulary
simple abstract form. It is shown that their properties can be obtained from
only on a very small set of algebraic assumptions. The presentation is purely
algebraic and it does not use any particular definition of method components,
such as ... | math.NA | the fetidp bddc and pfetidp preconditioners are derived in a particulary simple abstract form it is shown that their properties can be obtained from only on a very small set of algebraic assumptions the presentation is purely algebraic and it does not use any particular definition of method components such as substruct... | [['the', 'fetidp', 'bddc', 'and', 'pfetidp', 'preconditioners', 'are', 'derived', 'in', 'a', 'particulary', 'simple', 'abstract', 'form', 'it', 'is', 'shown', 'that', 'their', 'properties', 'can', 'be', 'obtained', 'from', 'only', 'on', 'a', 'very', 'small', 'set', 'of', 'algebraic', 'assumptions', 'the', 'presentation... | [-0.10915098716202003, 0.07422596051138107, -0.12462134633546437, 0.09617237023520851, -0.11924481539176852, -0.13167419626445667, -0.013540950060511628, 0.32974177129506094, -0.29984971917257075, -0.2874144505845701, 0.13046708959438724, -0.22095905647166375, -0.14868192603964003, 0.20262706501606276, -0.0941234972078... |
708.4032 | Coherent ultrafast core-hole correlation spectroscopy: x-ray analogues
of multidimensional NMR | We propose two dimensional x-ray coherent correlation spectroscopy (2DXCS)
for the study of interactions between core-electron and valence transitions.
This technique might find experimental applications in the future when very
high intensity x-ray sources become available. Spectra obtained by varying two
delay perio... | quant-ph | we propose two dimensional xray coherent correlation spectroscopy 2dxcs for the study of interactions between coreelectron and valence transitions this technique might find experimental applications in the future when very high intensity xray sources become available spectra obtained by varying two delay periods betwee... | [['we', 'propose', 'two', 'dimensional', 'xray', 'coherent', 'correlation', 'spectroscopy', '2dxcs', 'for', 'the', 'study', 'of', 'interactions', 'between', 'coreelectron', 'and', 'valence', 'transitions', 'this', 'technique', 'might', 'find', 'experimental', 'applications', 'in', 'the', 'future', 'when', 'very', 'high... | [-0.12254862670873314, 0.21881427992741728, -0.06151668555820686, 0.10663554602340514, 0.015074653399371824, -0.12768476444491467, 0.055016212425259656, 0.45437345419858777, -0.2643391917524643, -0.3222566458212515, 0.014385010719537562, -0.34413181115544217, -0.1314548263380434, 0.18896408873707662, 0.0861139556847859... |
708.4033 | New Prediction For Leptonic Theta_13 | An extension of the neutrino sector with two right handed singlet neutrinos
responsible for Dirac neutrino masses is discussed. We show that this setup
with flavor symmetry can give large solar and atmospheric neutrino mixings and
suppressed Theta_13. The flavor symmetry U(1) x S_4 is shown to lead to
Theta_23 = \pi/... | hep-ph | an extension of the neutrino sector with two right handed singlet neutrinos responsible for dirac neutrino masses is discussed we show that this setup with flavor symmetry can give large solar and atmospheric neutrino mixings and suppressed theta_13 the flavor symmetry u1 x s_4 is shown to lead to theta_23 pi4 and a ne... | [['an', 'extension', 'of', 'the', 'neutrino', 'sector', 'with', 'two', 'right', 'handed', 'singlet', 'neutrinos', 'responsible', 'for', 'dirac', 'neutrino', 'masses', 'is', 'discussed', 'we', 'show', 'that', 'this', 'setup', 'with', 'flavor', 'symmetry', 'can', 'give', 'large', 'solar', 'and', 'atmospheric', 'neutrino'... | [-0.1390494344426164, 0.3966753602515382, 0.0655826679430902, 0.2199362152973966, -0.12006161551301678, -0.22385459755702566, 0.04470677071561416, 0.3247474969985584, -0.19965670080273412, -0.2711919030174613, 0.029170193796016975, -0.2734691195655614, -0.03810474826314021, 0.1388500617739434, -0.0006651376800922056, -... |
708.4034 | Tate motives and the fundamental group | Let k be a number field, and let S be a finite set of k-rational points of
P^1. We relate the Deligne-Goncharov contruction of the motivic fundamental
group of X:=P^1_k- S to the Tannaka group scheme of the category of mixed Tate
motives over X.
| math.AG math.KT | let k be a number field and let s be a finite set of krational points of p1 we relate the delignegoncharov contruction of the motivic fundamental group of xp1_k s to the tannaka group scheme of the category of mixed tate motives over x | [['let', 'k', 'be', 'a', 'number', 'field', 'and', 'let', 's', 'be', 'a', 'finite', 'set', 'of', 'krational', 'points', 'of', 'p1', 'we', 'relate', 'the', 'delignegoncharov', 'contruction', 'of', 'the', 'motivic', 'fundamental', 'group', 'of', 'xp1_k', 's', 'to', 'the', 'tannaka', 'group', 'scheme', 'of', 'the', 'categ... | [-0.26848585022136917, 0.06433957743696696, -0.21065284324766592, -0.030853215171847234, -0.07404672765974389, -0.15607898528579361, 0.07139763568506338, 0.2779512274144001, -0.4076217121856157, -0.20325527307414992, 0.041289075840871, -0.19474925395361212, -0.04027030599671741, 0.20946167398590682, -0.1950878840979448... |
708.4035 | Three-dimensional coherent X-ray diffraction imaging of a ceramic
nanofoam: determination of structural deformation mechanisms | Ultra-low density polymers, metals, and ceramic nanofoams are valued for
their high strength-to-weight ratio, high surface area and insulating
properties ascribed to their structural geometry. We obtain the labrynthine
internal structure of a tantalum oxide nanofoam by X-ray diffractive imaging.
Finite element analys... | cond-mat.mtrl-sci physics.optics | ultralow density polymers metals and ceramic nanofoams are valued for their high strengthtoweight ratio high surface area and insulating properties ascribed to their structural geometry we obtain the labrynthine internal structure of a tantalum oxide nanofoam by xray diffractive imaging finite element analysis from the... | [['ultralow', 'density', 'polymers', 'metals', 'and', 'ceramic', 'nanofoams', 'are', 'valued', 'for', 'their', 'high', 'strengthtoweight', 'ratio', 'high', 'surface', 'area', 'and', 'insulating', 'properties', 'ascribed', 'to', 'their', 'structural', 'geometry', 'we', 'obtain', 'the', 'labrynthine', 'internal', 'struct... | [-0.083995164302807, 0.17536396027945383, -0.06488999506660006, 0.026802955362064815, -0.033180614304099534, -0.12029324566341333, 0.11144609150722169, 0.4283864780303997, -0.2663558408164898, -0.30983371575790886, 0.049143030075356364, -0.3527742101231942, -0.09988149218701732, 0.09468018754095947, 0.00379993547559589... |
708.4036 | Whittaker unitary dual of affine graded Hecke algebras of type E | This paper gives the classification of the Whittaker unitary dual for affine
graded Hecke algebras of type E. By the Iwahori-Matsumoto involution, this is
equivalent also to the classification of the spherical unitary dual for type E.
This work completes the classification of the Whittaker Iwahori-spherical
unitary d... | math.RT | this paper gives the classification of the whittaker unitary dual for affine graded hecke algebras of type e by the iwahorimatsumoto involution this is equivalent also to the classification of the spherical unitary dual for type e this work completes the classification of the whittaker iwahorispherical unitary dual or ... | [['this', 'paper', 'gives', 'the', 'classification', 'of', 'the', 'whittaker', 'unitary', 'dual', 'for', 'affine', 'graded', 'hecke', 'algebras', 'of', 'type', 'e', 'by', 'the', 'iwahorimatsumoto', 'involution', 'this', 'is', 'equivalent', 'also', 'to', 'the', 'classification', 'of', 'the', 'spherical', 'unitary', 'dua... | [-0.12193684168159961, 0.06333619801638027, -0.10069662624349197, 0.0351174024050124, -0.14291319567710162, -0.16941894177968303, -0.04417848051331627, 0.27573985476046803, -0.35077586517824483, -0.11857334990830472, 0.06724030763531724, -0.15301379018152753, -0.15843510320798185, 0.16600451555956777, -0.17530905873087... |
708.4037 | Dynamics of Rotating Accretion Flows Irradiated by a Quasar | We study the axisymmetric, time-dependent hydrodynamics of rotating flows
that are under the influence of supermassive black hole gravity and radiation
from an accretion disk surrounding the black hole. This work is an extension of
the earlier work presented by Proga, where nonrotating flows were studied.
Here, we co... | astro-ph | we study the axisymmetric timedependent hydrodynamics of rotating flows that are under the influence of supermassive black hole gravity and radiation from an accretion disk surrounding the black hole this work is an extension of the earlier work presented by proga where nonrotating flows were studied here we consider e... | [['we', 'study', 'the', 'axisymmetric', 'timedependent', 'hydrodynamics', 'of', 'rotating', 'flows', 'that', 'are', 'under', 'the', 'influence', 'of', 'supermassive', 'black', 'hole', 'gravity', 'and', 'radiation', 'from', 'an', 'accretion', 'disk', 'surrounding', 'the', 'black', 'hole', 'this', 'work', 'is', 'an', 'ex... | [-0.0962600708146175, 0.1599360455671916, -0.055497038670525446, 0.07015679852290796, -0.058915739025935894, -0.07829428918098603, -0.031093016537822416, 0.37859681470044815, -0.20313912152396668, -0.30053814859835615, 0.09316401674744261, -0.2675872448121854, -0.02133407299864854, 0.20879771057172816, -0.0383028552494... |
708.4038 | Studies of magnetogyration in cubic Bi12GeO20 crystals using
small-angular magnetooptic polarimetry | We present the results of studies for magnetogyration (MG) effect in
non-centro-symmetric, non-polar Bi12GeO20 crystals performed with the
small-angular polarimetric mapping technique. The magnitude of MG rotation
obtained with the small-angular mapping is close to the corresponding values
obtained recently on the ba... | physics.optics | we present the results of studies for magnetogyration mg effect in noncentrosymmetric nonpolar bi12geo20 crystals performed with the smallangular polarimetric mapping technique the magnitude of mg rotation obtained with the smallangular mapping is close to the corresponding values obtained recently on the basis of sing... | [['we', 'present', 'the', 'results', 'of', 'studies', 'for', 'magnetogyration', 'mg', 'effect', 'in', 'noncentrosymmetric', 'nonpolar', 'bi12geo20', 'crystals', 'performed', 'with', 'the', 'smallangular', 'polarimetric', 'mapping', 'technique', 'the', 'magnitude', 'of', 'mg', 'rotation', 'obtained', 'with', 'the', 'sma... | [-0.09610992515393134, 0.08553083026310473, -0.040104787125961765, -0.008176311836688824, -0.009197238683035331, -0.08717348655530562, 0.024175773820995044, 0.40706617788722116, -0.19332749183688844, -0.3293017544561908, 0.08974682214431509, -0.2784038555054438, -0.12904563027301005, 0.24391993627484357, -0.00155571951... |
708.4039 | Combinatorial fiber bundles and fragmentation of a fiberwise
PL-homeomorphism | With a compact PL manifold X we associate a category T(X). The objects of
T(X) are all combinatorial manifolds of type X, and morphisms are combinatorial
assemblies. We prove that the homotopy equivalence BT (X) \approx BPL(X) holds,
where PL(X) is the simplicial group of PL-homeomorphisms. Thus the space BT(X)
is a ... | math.GT math.CO math.CT | with a compact pl manifold x we associate a category tx the objects of tx are all combinatorial manifolds of type x and morphisms are combinatorial assemblies we prove that the homotopy equivalence bt x approx bplx holds where plx is the simplicial group of plhomeomorphisms thus the space btx is a canonical countable a... | [['with', 'a', 'compact', 'pl', 'manifold', 'x', 'we', 'associate', 'a', 'category', 'tx', 'the', 'objects', 'of', 'tx', 'are', 'all', 'combinatorial', 'manifolds', 'of', 'type', 'x', 'and', 'morphisms', 'are', 'combinatorial', 'assemblies', 'we', 'prove', 'that', 'the', 'homotopy', 'equivalence', 'bt', 'x', 'approx', ... | [-0.17036823627401004, 0.06600877831193362, -0.1060419197612511, 0.06466735422037784, -0.09890508118594342, -0.15997253922762833, 0.05532507624863043, 0.3678412907325697, -0.3141315313383799, -0.21619599175917553, 0.06524723343399172, -0.26441152890765807, -0.14211391997243347, 0.18020622855557897, -0.16687820445211535... |
708.404 | Effective equidistribution for closed orbits of semisimple groups on
homogeneous spaces | We prove effective equidistribution, with polynomial rate, for large closed
orbits of semisimple groups on homogeneous spaces, under certain technical
restrictions (notably, the acting group should have finite centralizer in the
ambient group). The proofs make extensive use of spectral gaps, and also of a
closing lem... | math.DS math.NT | we prove effective equidistribution with polynomial rate for large closed orbits of semisimple groups on homogeneous spaces under certain technical restrictions notably the acting group should have finite centralizer in the ambient group the proofs make extensive use of spectral gaps and also of a closing lemma for suc... | [['we', 'prove', 'effective', 'equidistribution', 'with', 'polynomial', 'rate', 'for', 'large', 'closed', 'orbits', 'of', 'semisimple', 'groups', 'on', 'homogeneous', 'spaces', 'under', 'certain', 'technical', 'restrictions', 'notably', 'the', 'acting', 'group', 'should', 'have', 'finite', 'centralizer', 'in', 'the', '... | [-0.21708547843038103, 0.11787406409159303, -0.13868110577575862, 0.07971359267830849, -0.12419185265898705, -0.10805768060497939, 0.0613110414147377, 0.38881449107080696, -0.28038298364728687, -0.2355474646668881, 0.17557772813597694, -0.19923957252409308, -0.10710571149364113, 0.2544111225940287, -0.13593693544156848... |
708.4041 | Integrable KdV Hierarchies on T^2=S^1\times S^1 | Following our previous works on extended higher spin symmetries on the torus
we focus in the present contribution to make a setup of the integrable KdV
hierarchies on $T^{2} = S^{1} \times S^{1}$. Actually two particular systems
are considered, namely the KdV and the Burgers non linear integrable model
associated to ... | hep-th | following our previous works on extended higher spin symmetries on the torus we focus in the present contribution to make a setup of the integrable kdv hierarchies on t2 s1 times s1 actually two particular systems are considered namely the kdv and the burgers non linear integrable model associated to currents of confor... | [['following', 'our', 'previous', 'works', 'on', 'extended', 'higher', 'spin', 'symmetries', 'on', 'the', 'torus', 'we', 'focus', 'in', 'the', 'present', 'contribution', 'to', 'make', 'a', 'setup', 'of', 'the', 'integrable', 'kdv', 'hierarchies', 'on', 't2', 's1', 'times', 's1', 'actually', 'two', 'particular', 'system... | [-0.1788011437902848, 0.08664272647195806, -0.00342325075632996, 0.10142891094761176, -0.031766571409793366, -0.18391675702813598, -0.05016824736570318, 0.36363810954822434, -0.2373555451631546, -0.2062860479992297, 0.1455711744298848, -0.2952311681635264, -0.12969123543524702, 0.18286262767958558, -0.01566166331299933... |
708.4042 | Moments of the critical values of families of elliptic curves, with
applications | We make conjectures on the moments of the central values of the family of all
elliptic curves and on the moments of the first derivative of the central
values of a large family of positive rank curves. In both cases the order of
magnitude is the same as that of the moments of the central values of an
orthogonal famil... | math.NT | we make conjectures on the moments of the central values of the family of all elliptic curves and on the moments of the first derivative of the central values of a large family of positive rank curves in both cases the order of magnitude is the same as that of the moments of the central values of an orthogonal family o... | [['we', 'make', 'conjectures', 'on', 'the', 'moments', 'of', 'the', 'central', 'values', 'of', 'the', 'family', 'of', 'all', 'elliptic', 'curves', 'and', 'on', 'the', 'moments', 'of', 'the', 'first', 'derivative', 'of', 'the', 'central', 'values', 'of', 'a', 'large', 'family', 'of', 'positive', 'rank', 'curves', 'in', ... | [-0.15514338712221873, 0.07207432149326491, -0.07727231679800481, 0.06836081668908305, -0.046393948784376034, -0.07434206787469004, 0.0018292067128532468, 0.2894142417709774, -0.24499035832722352, -0.27146348393341496, 0.1247605910688055, -0.29990707163928326, -0.11673362307083696, 0.24818470980277035, -0.0528779600455... |
708.4043 | Broadening of band-gap in photonic crystals with optically saturated
media | Due to strong absorption of the incident light, the media with high
refractive index are considered restrictive for applications in photonic
crystals (PhCs). The possibility to resolve this problem by optical saturation
effectively minimizing the absorption of the PhC medium is discussed. Such
approach might be promi... | physics.optics physics.ins-det | due to strong absorption of the incident light the media with high refractive index are considered restrictive for applications in photonic crystals phcs the possibility to resolve this problem by optical saturation effectively minimizing the absorption of the phc medium is discussed such approach might be promising fo... | [['due', 'to', 'strong', 'absorption', 'of', 'the', 'incident', 'light', 'the', 'media', 'with', 'high', 'refractive', 'index', 'are', 'considered', 'restrictive', 'for', 'applications', 'in', 'photonic', 'crystals', 'phcs', 'the', 'possibility', 'to', 'resolve', 'this', 'problem', 'by', 'optical', 'saturation', 'effec... | [-0.09999210454354232, 0.14667358557608995, -0.001506851003928618, 0.007996118097269739, -0.09672997924075885, -0.1635510521348227, 0.03118910952047868, 0.5004971853711389, -0.2934732783247124, -0.33721902627836575, 0.054585402736186305, -0.3069730746983127, -0.12612940289757468, 0.18913283329457045, -0.032410836592316... |
708.4044 | Mutual Coherence of Polarized Light in Disordered Media: Two-Frequency
Method Extended | The paper addresses the two-point correlations of electromagnetic waves in
general random, bi-anisotropic media whose constitutive tensors are complex
Hermitian, positive- or negative-definite matrices. A simplified version of the
two-frequency Wigner distribution (2f-WD) for polarized waves is introduced and
the clo... | physics.optics | the paper addresses the twopoint correlations of electromagnetic waves in general random bianisotropic media whose constitutive tensors are complex hermitian positive or negativedefinite matrices a simplified version of the twofrequency wigner distribution 2fwd for polarized waves is introduced and the closed form wign... | [['the', 'paper', 'addresses', 'the', 'twopoint', 'correlations', 'of', 'electromagnetic', 'waves', 'in', 'general', 'random', 'bianisotropic', 'media', 'whose', 'constitutive', 'tensors', 'are', 'complex', 'hermitian', 'positive', 'or', 'negativedefinite', 'matrices', 'a', 'simplified', 'version', 'of', 'the', 'twofre... | [-0.18024774544127287, 0.20354544735618402, -0.020626802541315555, 0.07770647188555449, -0.09509125082474201, -0.12071884293295443, -0.09987158783711493, 0.3378473353236914, -0.2566544675976038, -0.19275059446319937, 0.06261872253660113, -0.30004489233158527, -0.16321830463781953, 0.15198310728929937, 0.086397055068518... |
708.4045 | Stable rank for inclusions of C*-algebras | When a unital \ca $A$ has topological stable rank one (write $\tsr(A) = 1$),
we know that $\tsr(pAp) \leq 1$ for a non-zero projection $p \in A$. When,
however, $\tsr(A) \geq 2$, it is generally faluse. We prove that if a unital
C*-algebra $A$ has a simple unital C*-subalgebra $D$ of $A$ with common unit
such that $D... | math.OA | when a unital ca a has topological stable rank one write tsra 1 we know that tsrpap leq 1 for a nonzero projection p in a when however tsra geq 2 it is generally faluse we prove that if a unital calgebra a has a simple unital csubalgebra d of a with common unit such that d has psp and sup_pin pdtsrpap infty then tsra l... | [['when', 'a', 'unital', 'ca', 'a', 'has', 'topological', 'stable', 'rank', 'one', 'write', 'tsra', '1', 'we', 'know', 'that', 'tsrpap', 'leq', '1', 'for', 'a', 'nonzero', 'projection', 'p', 'in', 'a', 'when', 'however', 'tsra', 'geq', '2', 'it', 'is', 'generally', 'faluse', 'we', 'prove', 'that', 'if', 'a', 'unital', ... | [-0.10663871072068974, 0.17510770605816275, -0.05118859245615837, -0.008198274415917695, -0.025868094398302365, -0.29206367793933047, 0.01483428476194104, 0.4028208185189434, -0.3279861136861555, -0.15776190079830504, 0.10901879887019826, -0.31420665643699874, -0.09325743688700291, 0.14509246150379654, -0.1019148756442... |
708.4046 | Super Gelfand-Dickey Algebra And Integrable Models | We present in this work a systematic study of integrable models and
supersymmetric extensions of the Gelfand-Dickey algebra of pseudo differential
operators. We describe in detail the relation existing between the algebra of
super pseudo-differential operators on the ring of superfields
$u_{\frac{s}{2}}(z,\theta),s\i... | hep-th | we present in this work a systematic study of integrable models and supersymmetric extensions of the gelfanddickey algebra of pseudo differential operators we describe in detail the relation existing between the algebra of super pseudodifferential operators on the ring of superfields u_fracs2zthetasin z and the higher ... | [['we', 'present', 'in', 'this', 'work', 'a', 'systematic', 'study', 'of', 'integrable', 'models', 'and', 'supersymmetric', 'extensions', 'of', 'the', 'gelfanddickey', 'algebra', 'of', 'pseudo', 'differential', 'operators', 'we', 'describe', 'in', 'detail', 'the', 'relation', 'existing', 'between', 'the', 'algebra', 'o... | [-0.14032835696103438, 0.07516022321750533, -0.027083630902024935, 0.12084059368704779, -0.09366356116666827, -0.09288548125516412, -0.058467457022623355, 0.31296102316030916, -0.27280282143960305, -0.2236379953628441, 0.13789961158456104, -0.29088770134269065, -0.16765038774542088, 0.13871581112649642, -0.066228547660... |
708.4047 | An Approximate Solution of the Master Equation with the Dissipator being
a Set of Projectors | In this paper we consider a quantum open system and treat the master equation
with some restricted dissipator which consists of a set of projection operators
(projectors). The exact solution is given under the commutable approximation
(in our terminology). This is the first step for constructing a general
solution.
| quant-ph math-ph math.MP | in this paper we consider a quantum open system and treat the master equation with some restricted dissipator which consists of a set of projection operators projectors the exact solution is given under the commutable approximation in our terminology this is the first step for constructing a general solution | [['in', 'this', 'paper', 'we', 'consider', 'a', 'quantum', 'open', 'system', 'and', 'treat', 'the', 'master', 'equation', 'with', 'some', 'restricted', 'dissipator', 'which', 'consists', 'of', 'a', 'set', 'of', 'projection', 'operators', 'projectors', 'the', 'exact', 'solution', 'is', 'given', 'under', 'the', 'commutab... | [-0.13613695499240136, 0.029941347313626687, -0.06840128558022636, 0.01574272377302452, -0.026087512019831612, -0.12239678474903411, 0.04788910169201922, 0.27579789890014395, -0.27003551932165815, -0.21121670271517062, 0.12417262476602835, -0.2634002079008793, -0.14709262748971125, 0.1514432483295701, -0.06420519391112... |
708.4048 | Further insight into gravitational recoil | We test the accuracy of our recently proposed empirical formula to model the
recoil velocity imparted to the merger remnant of spinning, unequal-mass
black-hole binaries. We study three families of black-hole binary
configurations, all with mass ratio q=3/8 (to maximize the unequal-mass
contribution to the kick) and ... | gr-qc astro-ph | we test the accuracy of our recently proposed empirical formula to model the recoil velocity imparted to the merger remnant of spinning unequalmass blackhole binaries we study three families of blackhole binary configurations all with mass ratio q38 to maximize the unequalmass contribution to the kick and spins aligned... | [['we', 'test', 'the', 'accuracy', 'of', 'our', 'recently', 'proposed', 'empirical', 'formula', 'to', 'model', 'the', 'recoil', 'velocity', 'imparted', 'to', 'the', 'merger', 'remnant', 'of', 'spinning', 'unequalmass', 'blackhole', 'binaries', 'we', 'study', 'three', 'families', 'of', 'blackhole', 'binary', 'configurat... | [-0.15164744359855023, 0.13699349023065427, -0.0415503975269126, 0.08056600015455236, -0.0836535405057172, -0.0990968474587943, 0.029157651813066978, 0.37606557078995845, -0.180530022910615, -0.35389258847054506, -0.02835456666070968, -0.30344026802857926, -0.036132230454111576, 0.22337072934735464, 0.00487404190547143... |
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