id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
706.1414 | Absence of long-range Ni/Mn ordering in ferromagnetic La2NiMnO6 thin
films | Epitaxial La2NiMnO6 thin films have been grown on (001)-oriented SrTiO3 using
the PLD technique. The thin films are semiconducting and FM with a TC close to
270K, a coercive field of 920Oe, and a saturation magnetization of 5muB per
f.u. TEM, conducted at RT, reveals a majority phase having "I-centered"
structure wit... | cond-mat.mtrl-sci cond-mat.str-el | epitaxial la2nimno6 thin films have been grown on 001oriented srtio3 using the pld technique the thin films are semiconducting and fm with a tc close to 270k a coercive field of 920oe and a saturation magnetization of 5mub per fu tem conducted at rt reveals a majority phase having icentered structure with ac14asub and ... | [['epitaxial', 'la2nimno6', 'thin', 'films', 'have', 'been', 'grown', 'on', '001oriented', 'srtio3', 'using', 'the', 'pld', 'technique', 'the', 'thin', 'films', 'are', 'semiconducting', 'and', 'fm', 'with', 'a', 'tc', 'close', 'to', '270k', 'a', 'coercive', 'field', 'of', '920oe', 'and', 'a', 'saturation', 'magnetizati... | [-0.16245977008217122, 0.16906066134918568, -0.03339286293119712, -0.09897448145649071, -0.035382331977056904, -0.1476666071603811, 0.12466508358023888, 0.4856311775050884, -0.22968677221526673, -0.27859552346743904, 0.049400062978451766, -0.34376033664096234, -0.08993381948405227, 0.1967909491924179, 0.032496556179424... |
706.1415 | Approximate joint measurements of qubit observables | Joint measurements of qubit observables have recently been studied in
conjunction with quantum information processing tasks such as cloning.
Considerations of such joint measurements have until now been restricted to a
certain class of observables that can be characterized by a form of covariance.
Here we investigate... | quant-ph | joint measurements of qubit observables have recently been studied in conjunction with quantum information processing tasks such as cloning considerations of such joint measurements have until now been restricted to a certain class of observables that can be characterized by a form of covariance here we investigate con... | [['joint', 'measurements', 'of', 'qubit', 'observables', 'have', 'recently', 'been', 'studied', 'in', 'conjunction', 'with', 'quantum', 'information', 'processing', 'tasks', 'such', 'as', 'cloning', 'considerations', 'of', 'such', 'joint', 'measurements', 'have', 'until', 'now', 'been', 'restricted', 'to', 'a', 'certai... | [-0.1138766882049435, 0.09750648516606777, -0.0897961741987061, 0.0692625514542063, -0.05037982026544393, -0.15589602119520518, 0.02899385946274385, 0.3883611135026242, -0.2627203099244664, -0.2996996886737592, 0.07277923579004111, -0.24049502216834337, -0.07739034833399751, 0.21453512620497892, -0.08424745269899145, 0... |
706.1416 | Anatomy of Malicious Singularities | As well known, the b-boundaries of the closed Friedman world model and of
Schwarzschild solution consist of a single point. We study this phenomenon in a
broader context of differential and structured spaces. We show that it is an
equivalence relation $\rho $, defined on the Cauchy completed total space
$\bar{E}$ of ... | gr-qc | as well known the bboundaries of the closed friedman world model and of schwarzschild solution consist of a single point we study this phenomenon in a broader context of differential and structured spaces we show that it is an equivalence relation rho defined on the cauchy completed total space bare of the frame bundle... | [['as', 'well', 'known', 'the', 'bboundaries', 'of', 'the', 'closed', 'friedman', 'world', 'model', 'and', 'of', 'schwarzschild', 'solution', 'consist', 'of', 'a', 'single', 'point', 'we', 'study', 'this', 'phenomenon', 'in', 'a', 'broader', 'context', 'of', 'differential', 'and', 'structured', 'spaces', 'we', 'show', ... | [-0.14657358769136408, 0.07172513781620182, -0.09785136560185492, 0.08556922207814448, -0.090410781052924, -0.16857543982284065, 0.010807375588531917, 0.3069440619953336, -0.29871251216294087, -0.22356797691463726, 0.08507723881969771, -0.2735061354773431, -0.17421631918477942, 0.17874049669262604, -0.11705178208103462... |
706.1417 | Spatially resolved THz response as a characterization concept for
nanowire FETs | In this paper, we propose a THz probe technique to obtain spatially resolved
information about the electronic spectra inside nanowire-based FETs. This
spectroscopic approach employs a segmented multi-gate design for the local
detection of quantum transitions between few-electron states within the FET
channel. We simu... | cond-mat.other | in this paper we propose a thz probe technique to obtain spatially resolved information about the electronic spectra inside nanowirebased fets this spectroscopic approach employs a segmented multigate design for the local detection of quantum transitions between fewelectron states within the fet channel we simulate the... | [['in', 'this', 'paper', 'we', 'propose', 'a', 'thz', 'probe', 'technique', 'to', 'obtain', 'spatially', 'resolved', 'information', 'about', 'the', 'electronic', 'spectra', 'inside', 'nanowirebased', 'fets', 'this', 'spectroscopic', 'approach', 'employs', 'a', 'segmented', 'multigate', 'design', 'for', 'the', 'local', ... | [-0.0961457003839983, 0.07726440620983298, -0.08946895681792634, 0.012592261825720298, -0.0003075636120448852, -0.17214580347504596, 0.08975777547437183, 0.3814235293659671, -0.25173936606031555, -0.30321842444867925, -0.005425012746729471, -0.2550603704334333, -0.1729167057709747, 0.22086195122977803, 0.00236491475992... |
706.1418 | Generalized Banach contraction in probabilistic metric/normed spaces | In this paper, we present the generalization of B-contraction and
C-contraction due to Sehgal and Hicks respectively. We also study some
properties of C-contraction in probabilistic metric space.
| math.FA | in this paper we present the generalization of bcontraction and ccontraction due to sehgal and hicks respectively we also study some properties of ccontraction in probabilistic metric space | [['in', 'this', 'paper', 'we', 'present', 'the', 'generalization', 'of', 'bcontraction', 'and', 'ccontraction', 'due', 'to', 'sehgal', 'and', 'hicks', 'respectively', 'we', 'also', 'study', 'some', 'properties', 'of', 'ccontraction', 'in', 'probabilistic', 'metric', 'space']] | [-0.0675020843744278, 0.03541614476591349, -0.06721147418022155, 0.048901218413375316, -0.07380220748484134, -0.0014728976786136628, 0.08242810934316366, 0.3861391621828079, -0.2554671037197113, -0.27473505079746247, 0.11323256864212454, -0.24073650386184453, -0.2721340817213058, 0.18019449084997177, -0.186308370828628... |
706.1419 | Regularization by free additive convolution, square and rectangular
cases | The free convolution is the binary operation on the set of probability
measures on the real line which allows to deduce, from the individual spectral
distributions, the spectral distribution of a sum of independent unitarily
invariant square random matrices or of a sum of free operators in a non
commutative probabili... | math.PR | the free convolution is the binary operation on the set of probability measures on the real line which allows to deduce from the individual spectral distributions the spectral distribution of a sum of independent unitarily invariant square random matrices or of a sum of free operators in a non commutative probability s... | [['the', 'free', 'convolution', 'is', 'the', 'binary', 'operation', 'on', 'the', 'set', 'of', 'probability', 'measures', 'on', 'the', 'real', 'line', 'which', 'allows', 'to', 'deduce', 'from', 'the', 'individual', 'spectral', 'distributions', 'the', 'spectral', 'distribution', 'of', 'a', 'sum', 'of', 'independent', 'un... | [-0.10692831998734924, 0.13503303291839652, -0.07733439844609662, 0.06063462216960644, -0.03257272715869171, -0.09864604503561097, 0.044106405109315266, 0.3799402136909222, -0.2698154910658877, -0.1818124723998859, 0.09963392437243561, -0.28623405482037517, -0.09273473135850203, 0.16282680042990047, -0.0589585425983463... |
706.142 | Asymptotic form of molecular continuum wave function for system of
non-overlapping atomic potentials | The asymptotic behavior of the molecular continuum wave function has been
analyzed within a model of non-overlapping atomic potentials. It is been shown
that the representation of the wave function far from a molecule as a plane
wave and single spherical wave emitted by the molecular center cannot be
corrected. Becau... | physics.atom-ph physics.atm-clus | the asymptotic behavior of the molecular continuum wave function has been analyzed within a model of nonoverlapping atomic potentials it is been shown that the representation of the wave function far from a molecule as a plane wave and single spherical wave emitted by the molecular center cannot be corrected because of... | [['the', 'asymptotic', 'behavior', 'of', 'the', 'molecular', 'continuum', 'wave', 'function', 'has', 'been', 'analyzed', 'within', 'a', 'model', 'of', 'nonoverlapping', 'atomic', 'potentials', 'it', 'is', 'been', 'shown', 'that', 'the', 'representation', 'of', 'the', 'wave', 'function', 'far', 'from', 'a', 'molecule', ... | [-0.10655887181430494, 0.08770888677019983, -0.0799449381597136, 0.061970222820902615, 0.006335961536746727, -0.06597120927212989, -0.0034872716075855575, 0.3621905087812306, -0.20785931811017327, -0.25503420075146505, 0.04317688176963376, -0.30128316708827674, -0.13426962131570566, 0.15830156990256772, 0.0718653513782... |
706.1421 | On electromagnetic contributions in WIMP quests | The effect pointed out by A. B. Migdal in the 40's (hereafter named Migdal
effect) has so far been usually neglected in the direct searches for WIMP Dark
Matter candidates. This effect consists in the ionization and the excitation of
bound atomic electrons induced by the recoiling atomic nucleus. In the present
paper... | astro-ph | the effect pointed out by a b migdal in the 40s hereafter named migdal effect has so far been usually neglected in the direct searches for wimp dark matter candidates this effect consists in the ionization and the excitation of bound atomic electrons induced by the recoiling atomic nucleus in the present paper the rela... | [['the', 'effect', 'pointed', 'out', 'by', 'a', 'b', 'migdal', 'in', 'the', '40s', 'hereafter', 'named', 'migdal', 'effect', 'has', 'so', 'far', 'been', 'usually', 'neglected', 'in', 'the', 'direct', 'searches', 'for', 'wimp', 'dark', 'matter', 'candidates', 'this', 'effect', 'consists', 'in', 'the', 'ionization', 'and... | [-0.0887438136140828, 0.16076263786571754, -0.07207436530621021, 0.11185000825661247, -0.061806587006461314, -0.07946434200366402, 0.054639165130951864, 0.32410310890961, -0.20819788348752183, -0.30445903520305434, 0.028594694493411035, -0.275328113915181, -0.10768291101996581, 0.17488005345493748, 0.015533656123783681... |
706.1422 | Inverse Conductivity Problem for a Parabolic Equation using a Carlemen
Estimate with one Observation | For the heat equation in a bounded domain we give a stability result for a
smooth diffusion coefficient. The key ingredients are a global Carleman-type
estimate, a Poincar\'e-type estimate and an energy estimate with a single
observation acting on a part of the boundary.
| math.AP | for the heat equation in a bounded domain we give a stability result for a smooth diffusion coefficient the key ingredients are a global carlemantype estimate a poincaretype estimate and an energy estimate with a single observation acting on a part of the boundary | [['for', 'the', 'heat', 'equation', 'in', 'a', 'bounded', 'domain', 'we', 'give', 'a', 'stability', 'result', 'for', 'a', 'smooth', 'diffusion', 'coefficient', 'the', 'key', 'ingredients', 'are', 'a', 'global', 'carlemantype', 'estimate', 'a', 'poincaretype', 'estimate', 'and', 'an', 'energy', 'estimate', 'with', 'a', ... | [-0.13608120162759654, 0.03679211934352431, -0.11046405657279221, 0.037767356086988, -0.09493149095214903, -0.07632580631285567, 0.02343064015307887, 0.2701310793107206, -0.2835221823982217, -0.22727780052545396, 0.19195118749418974, -0.26444036907262425, -0.0928778473634421, 0.2278627622025934, -0.04859508030031892, 0... |
706.1423 | Spiral phases and two-particle bound states from a systematic low-energy
effective theory for magnons, electrons, and holes in an antiferromagnet | We have constructed a systematic low-energy effective theory for hole- and
electron-doped antiferromagnets, where holes reside in momentum space pockets
centered at $(\pm\frac{\pi}{2a},\pm\frac{\pi}{2a})$ and where electrons live in
pockets centered at $(\frac{\pi}{a},0)$ or $(0,\frac{\pi}{a})$. The effective
theory ... | cond-mat.str-el | we have constructed a systematic lowenergy effective theory for hole and electrondoped antiferromagnets where holes reside in momentum space pockets centered at pmfracpi2apmfracpi2a and where electrons live in pockets centered at fracpia0 or 0fracpia the effective theory is used to investigate the magnonmediated bindin... | [['we', 'have', 'constructed', 'a', 'systematic', 'lowenergy', 'effective', 'theory', 'for', 'hole', 'and', 'electrondoped', 'antiferromagnets', 'where', 'holes', 'reside', 'in', 'momentum', 'space', 'pockets', 'centered', 'at', 'pmfracpi2apmfracpi2a', 'and', 'where', 'electrons', 'live', 'in', 'pockets', 'centered', '... | [-0.13133825129398735, 0.19014400003433493, -0.043469309035728695, 0.14346017194436161, -0.009230829209529905, -0.16980141318172856, 0.08580965806244402, 0.34794572979131694, -0.21430699899542316, -0.2644073114159607, 0.0014240964608747632, -0.4122187895500051, -0.13138244751094771, 0.1279645065065994, 0.07162251563802... |
706.1424 | Theory of antibound states in partially filled narrow band systems | We present a theory of the dynamical two-particle response function in the
Hubbard model based on the time-dependent Gutzwiller approximation. The results
are in excellent agreement with exact diagonalization on small clusters and
give reliable results even for high densities, where the usual ladder
approximation bre... | cond-mat.str-el | we present a theory of the dynamical twoparticle response function in the hubbard model based on the timedependent gutzwiller approximation the results are in excellent agreement with exact diagonalization on small clusters and give reliable results even for high densities where the usual ladder approximation breaks do... | [['we', 'present', 'a', 'theory', 'of', 'the', 'dynamical', 'twoparticle', 'response', 'function', 'in', 'the', 'hubbard', 'model', 'based', 'on', 'the', 'timedependent', 'gutzwiller', 'approximation', 'the', 'results', 'are', 'in', 'excellent', 'agreement', 'with', 'exact', 'diagonalization', 'on', 'small', 'clusters'... | [-0.06907384570067128, 0.11053054301689068, -0.09033271285394827, 0.13379158860227713, -0.020820808438584207, -0.11545080134179443, 0.08236133544861028, 0.34466697884102665, -0.19514123044908047, -0.28264436416948835, 0.03769192956077556, -0.3155466289476802, -0.11963123143369254, 0.15188644197769463, 0.056608143020809... |
706.1425 | Combined Effect of Bond- and Potential-Disorder in Half-Doped Manganites | We analyze the effects of both bond- and potential-disorder in the vicinity
of a first-order metal insulator transition in a two-band model for manganites
using a real-space Monte Carlo method. Our results reveal a novel
charge-ordered state coexisting with spin-glass behavior. We provide the basis
for understanding ... | cond-mat.str-el cond-mat.dis-nn | we analyze the effects of both bond and potentialdisorder in the vicinity of a firstorder metal insulator transition in a twoband model for manganites using a realspace monte carlo method our results reveal a novel chargeordered state coexisting with spinglass behavior we provide the basis for understanding the phase d... | [['we', 'analyze', 'the', 'effects', 'of', 'both', 'bond', 'and', 'potentialdisorder', 'in', 'the', 'vicinity', 'of', 'a', 'firstorder', 'metal', 'insulator', 'transition', 'in', 'a', 'twoband', 'model', 'for', 'manganites', 'using', 'a', 'realspace', 'monte', 'carlo', 'method', 'our', 'results', 'reveal', 'a', 'novel'... | [-0.13589252541078167, 0.14528140698530478, -0.09716811359976418, 0.06118778143718373, 0.008910394564736634, -0.10653772059595212, 0.15196193793963175, 0.37387947738170624, -0.2271173554690904, -0.260825426899828, 0.03168011721209041, -0.3467470661198604, -0.21103023731848225, 0.12667852491358644, 0.09597120742546394, ... |
706.1426 | Is Sr2RuO4 a triplet superconductor? | The field dependence of the specific heat \gamma(H) at lower temperatures in
Sr2RuO4 is analyzed by solving microscopic Eilenberger equation numerically. We
find that systematic \gamma(H) behaviors from a concaved \sqrt H to a convex
H^{\alpha} (\alpha>1) under H orientation change are understood by taking
account of... | cond-mat.supr-con | the field dependence of the specific heat gammah at lower temperatures in sr2ruo4 is analyzed by solving microscopic eilenberger equation numerically we find that systematic gammah behaviors from a concaved sqrt h to a convex halpha alpha1 under h orientation change are understood by taking account of the pauli paramag... | [['the', 'field', 'dependence', 'of', 'the', 'specific', 'heat', 'gammah', 'at', 'lower', 'temperatures', 'in', 'sr2ruo4', 'is', 'analyzed', 'by', 'solving', 'microscopic', 'eilenberger', 'equation', 'numerically', 'we', 'find', 'that', 'systematic', 'gammah', 'behaviors', 'from', 'a', 'concaved', 'sqrt', 'h', 'to', 'a... | [-0.1307511224088052, 0.18532342835225993, -0.06570012998353277, 0.08755473403855124, -0.11096132896426651, -0.16751897261581486, 0.06784534062155419, 0.380597250836177, -0.26382245753063926, -0.26476239090164505, 0.002845918269465781, -0.29711639010104895, -0.06410056678836959, 0.16907372648711316, 0.01802838497484723... |
706.1427 | Estimating the annihilation decay B_s -> rho gamma with factorization | The branching ratio for the rare two-body B_s -> rho gamma decay is
calculated using the factorization assumption. This transition is dominated by
the annihilation diagrams and, in principle, prone to receiving substantial
contributions from new physics. We estimate Br(B_s -> rho gamma) = 1.6 x 10^-9
within the Stand... | hep-ph | the branching ratio for the rare twobody b_s rho gamma decay is calculated using the factorization assumption this transition is dominated by the annihilation diagrams and in principle prone to receiving substantial contributions from new physics we estimate brb_s rho gamma 16 x 109 within the standard model and invest... | [['the', 'branching', 'ratio', 'for', 'the', 'rare', 'twobody', 'b_s', 'rho', 'gamma', 'decay', 'is', 'calculated', 'using', 'the', 'factorization', 'assumption', 'this', 'transition', 'is', 'dominated', 'by', 'the', 'annihilation', 'diagrams', 'and', 'in', 'principle', 'prone', 'to', 'receiving', 'substantial', 'contr... | [-0.06660288877816853, 0.2317821416208177, -0.035398200583797924, 0.10598329744116376, -0.032025304252227535, -0.12492063420019972, 0.1040376835792027, 0.27997434184009445, -0.24996087405021367, -0.27587847809479077, 0.031339559820480645, -0.3117796470076569, -0.06066595071540169, 0.13776335855086957, 0.034765792242025... |
706.1428 | SILEM : a new gaseous detector with integrated x-y readout plane | This works reports on gaseous detectors developments made in the frame of the
EXO double-beta decay experiment. LEM (Large Electron Multiplication) are
electron amplification grids based on GEM. They were developed in Neuchatel and
showed remarquable resistance to sparks. The new SILEM grid combines the
properties of... | physics.ins-det | this works reports on gaseous detectors developments made in the frame of the exo doublebeta decay experiment lem large electron multiplication are electron amplification grids based on gem they were developed in neuchatel and showed remarquable resistance to sparks the new silem grid combines the properties of the sta... | [['this', 'works', 'reports', 'on', 'gaseous', 'detectors', 'developments', 'made', 'in', 'the', 'frame', 'of', 'the', 'exo', 'doublebeta', 'decay', 'experiment', 'lem', 'large', 'electron', 'multiplication', 'are', 'electron', 'amplification', 'grids', 'based', 'on', 'gem', 'they', 'were', 'developed', 'in', 'neuchate... | [-0.11156930042696851, 0.1234472847071948, -0.03432082591877718, 0.0017005833116807527, -0.03033128504145455, -0.14570297554207892, 0.014687058606559967, 0.3495783405015608, -0.20625774270262232, -0.3044638339091431, 0.08266028012723553, -0.338999019172224, -0.04588250961009558, 0.24272158089571622, -0.0450512035689377... |
706.1429 | Q-Ball Condensation | Q-balls arise in particle theories with U(1) global symmetry. The coupling of
the corresponding scalar field to fermions leads to Q-ball evaporation. In this
paper we consider the oposite problem, the case where a Q-ball absorbs
particles to grow. In particular we shall use the exact quantum mechanical
description of... | hep-th hep-ph | qballs arise in particle theories with u1 global symmetry the coupling of the corresponding scalar field to fermions leads to qball evaporation in this paper we consider the oposite problem the case where a qball absorbs particles to grow in particular we shall use the exact quantum mechanical description of fermions i... | [['qballs', 'arise', 'in', 'particle', 'theories', 'with', 'u1', 'global', 'symmetry', 'the', 'coupling', 'of', 'the', 'corresponding', 'scalar', 'field', 'to', 'fermions', 'leads', 'to', 'qball', 'evaporation', 'in', 'this', 'paper', 'we', 'consider', 'the', 'oposite', 'problem', 'the', 'case', 'where', 'a', 'qball', ... | [-0.16609666408629906, 0.24233207573399315, -0.07014222948116736, 0.10571005698260655, -0.09831962912855013, -0.1497260294854641, -0.00011112006433622938, 0.2910396828198097, -0.23767732600615898, -0.25639000616338053, 0.029293816790811087, -0.2760268843299906, -0.10266759131812084, 0.06722247212449692, -0.024036595256... |
706.143 | Arc-like distribution of high CO(J=3-2)/CO(J=1-0) ratio gas surrounding
the central star cluster of the supergiant HII region NGC 604 | We report the discovery of a high CO(J=3-2)/CO(J=1-0) ratio gas with an
arc-like distribution (``high-ratio gas arc'') surrounding the central star
cluster of the supergiant HII region NGC 604 in the nearby spiral galaxy M 33,
based on multi-J CO observations of a 5' $\times$ 5' region of NGC 604
conducted using the ... | astro-ph | we report the discovery of a high coj32coj10 ratio gas with an arclike distribution highratio gas arc surrounding the central star cluster of the supergiant hii region ngc 604 in the nearby spiral galaxy m 33 based on multij co observations of a 5 times 5 region of ngc 604 conducted using the aste 10m and nro 45m teles... | [['we', 'report', 'the', 'discovery', 'of', 'a', 'high', 'coj32coj10', 'ratio', 'gas', 'with', 'an', 'arclike', 'distribution', 'highratio', 'gas', 'arc', 'surrounding', 'the', 'central', 'star', 'cluster', 'of', 'the', 'supergiant', 'hii', 'region', 'ngc', '604', 'in', 'the', 'nearby', 'spiral', 'galaxy', 'm', '33', '... | [-0.0962565820238563, 0.07996578963533837, 0.002666504842793113, 0.022796830062263754, -0.03574588408778792, -0.03326991177164018, 0.05932748375683635, 0.41644027224311264, -0.11201329791157316, -0.35006188302330915, 0.07759549445034536, -0.2857675773331956, 0.03663428932377037, 0.1319048275203464, 0.006437599895708513... |
706.1431 | Observation of squeezed light with 10dB quantum noise reduction | Squeezing of light's quantum noise requires temporal rearranging of photons.
This again corresponds to creation of quantum correlations between individual
photons. Squeezed light is a non-classical manifestation of light with great
potential in high-precision quantum measurements, for example in the detection
of grav... | quant-ph | squeezing of lights quantum noise requires temporal rearranging of photons this again corresponds to creation of quantum correlations between individual photons squeezed light is a nonclassical manifestation of light with great potential in highprecision quantum measurements for example in the detection of gravitationa... | [['squeezing', 'of', 'lights', 'quantum', 'noise', 'requires', 'temporal', 'rearranging', 'of', 'photons', 'this', 'again', 'corresponds', 'to', 'creation', 'of', 'quantum', 'correlations', 'between', 'individual', 'photons', 'squeezed', 'light', 'is', 'a', 'nonclassical', 'manifestation', 'of', 'light', 'with', 'great... | [-0.1433914125040506, 0.215215269480333, -0.0849532624758597, 0.04659730502680759, -0.032579455304325426, -0.17320289422475202, 0.06578153035869556, 0.4012539785222283, -0.20038424932447793, -0.3144076825036401, 0.050982381388686396, -0.2751093964657879, -0.13881885620711337, 0.30262822130628464, -0.06848949043030318, ... |
706.1432 | Reconstruction of 5D Cosmological Model From Recent Observations | We use a parameterized equation of state (EOS) of dark energy to a 5D
Ricci-flat cosmological solution and suppose the universe contains two major
components: dark matter and dark energy. Using the recent observational
datasets: the latest 182 type Ia Supernovae Gold data, the 3-year WMAP CMB
shift parameter and the ... | astro-ph | we use a parameterized equation of state eos of dark energy to a 5d ricciflat cosmological solution and suppose the universe contains two major components dark matter and dark energy using the recent observational datasets the latest 182 type ia supernovae gold data the 3year wmap cmb shift parameter and the sdss baryo... | [['we', 'use', 'a', 'parameterized', 'equation', 'of', 'state', 'eos', 'of', 'dark', 'energy', 'to', 'a', '5d', 'ricciflat', 'cosmological', 'solution', 'and', 'suppose', 'the', 'universe', 'contains', 'two', 'major', 'components', 'dark', 'matter', 'and', 'dark', 'energy', 'using', 'the', 'recent', 'observational', 'd... | [-0.0833373504659179, 0.0656277808616191, -0.07691315370295378, 0.1102254138061397, -0.15263463388967385, -0.08886692476757233, 0.034904793996671304, 0.31205445008117305, -0.18936618281871948, -0.37493849482423475, 0.03856179900173532, -0.3617001917683384, 0.04028792993066091, 0.16952733590394187, 0.05790446938101137, ... |
706.1433 | IGR J00234+6141 : a new INTEGRAL source identified as an Intermediate
polar | Following an extensive survey of the galactic plane by the INTEGRAL
satellite, new hard X-ray sources are discovered with a significant fraction of
Cataclysmic Variables (CVs) among them. We report here the identification of
one of these hard X-ray sources, IGR J00234+6141, as an accreting magnetic
white dwarf of int... | astro-ph | following an extensive survey of the galactic plane by the integral satellite new hard xray sources are discovered with a significant fraction of cataclysmic variables cvs among them we report here the identification of one of these hard xray sources igr j002346141 as an accreting magnetic white dwarf of intermediate p... | [['following', 'an', 'extensive', 'survey', 'of', 'the', 'galactic', 'plane', 'by', 'the', 'integral', 'satellite', 'new', 'hard', 'xray', 'sources', 'are', 'discovered', 'with', 'a', 'significant', 'fraction', 'of', 'cataclysmic', 'variables', 'cvs', 'among', 'them', 'we', 'report', 'here', 'the', 'identification', 'o... | [-0.13783497148662066, 0.0844939819569192, -0.07074982846776644, 0.07735684430883386, -0.10425381520285439, -0.0717283334583044, 0.10006176172755658, 0.4076095448568081, -0.2032713416014583, -0.34539178009100185, 0.10181050901181805, -0.3116850750449185, -0.08876902396575763, 0.25089733083613025, -0.045620711556134314,... |
706.1434 | Nonlinear Dynamics of Infectious Diseases Transfer with Possible
Applications for Tubercular Infection | In this paper, we model a nonlinear dynamics of infectious diseases transfer.
Particularly, we study possible applications to tubercular infection in models
with different profiles (peak values) of the population density dependence on
spatial coordinates. Our approach is based on the well known method of
instantons w... | physics.med-ph physics.data-an | in this paper we model a nonlinear dynamics of infectious diseases transfer particularly we study possible applications to tubercular infection in models with different profiles peak values of the population density dependence on spatial coordinates our approach is based on the well known method of instantons which has... | [['in', 'this', 'paper', 'we', 'model', 'a', 'nonlinear', 'dynamics', 'of', 'infectious', 'diseases', 'transfer', 'particularly', 'we', 'study', 'possible', 'applications', 'to', 'tubercular', 'infection', 'in', 'models', 'with', 'different', 'profiles', 'peak', 'values', 'of', 'the', 'population', 'density', 'dependen... | [-0.08894886734793918, 0.11083274535933295, -0.07444656714319418, 0.060800594062013075, -0.04350828449391068, -0.12085263726588052, 0.05096854594422695, 0.3683498139636448, -0.23000020368729168, -0.2999379036183923, 0.07734956864106397, -0.2902856794430707, -0.19334836793132126, 0.1935884511554972, -0.04895766390930079... |
706.1435 | A Critical String Theory in 3+1 Dimensions | Redefining the vacuum state of a free twofold N=1 covariant supersymmetric
string action as the one with all the world sheet fermionic excited states
occupied, makes the theory anomaly free in D=4 with Minkowski signature. The
theory thus describes a critical string in 3+1 dimensions as opposed to earlier
N=2 supersy... | hep-th | redefining the vacuum state of a free twofold n1 covariant supersymmetric string action as the one with all the world sheet fermionic excited states occupied makes the theory anomaly free in d4 with minkowski signature the theory thus describes a critical string in 31 dimensions as opposed to earlier n2 supersymmetric ... | [['redefining', 'the', 'vacuum', 'state', 'of', 'a', 'free', 'twofold', 'n1', 'covariant', 'supersymmetric', 'string', 'action', 'as', 'the', 'one', 'with', 'all', 'the', 'world', 'sheet', 'fermionic', 'excited', 'states', 'occupied', 'makes', 'the', 'theory', 'anomaly', 'free', 'in', 'd4', 'with', 'minkowski', 'signat... | [-0.1356880759814255, 0.24761656702007623, -0.027706335389642716, 0.11860334368428714, -0.02838743471820516, -0.16700098108427197, -0.016965730487082907, 0.27131341510981904, -0.14996888129331828, -0.2826443825851444, 0.04868664659005803, -0.3203734107729461, -0.1057486474731145, 0.06608498363688685, -0.013683067652962... |
706.1436 | Hybrid inflation followed by modular inflation | Inflationary models with a superheavy scale F-term hybrid inflation followed
by an intermediate scale modular inflation are considered. The restrictions on
the power spectrum P_R of curvature perturbation and the spectral index n_s
from the recent data within the power-law cosmological model with cold dark
matter and... | hep-ph astro-ph | inflationary models with a superheavy scale fterm hybrid inflation followed by an intermediate scale modular inflation are considered the restrictions on the power spectrum p_r of curvature perturbation and the spectral index n_s from the recent data within the powerlaw cosmological model with cold dark matter and a co... | [['inflationary', 'models', 'with', 'a', 'superheavy', 'scale', 'fterm', 'hybrid', 'inflation', 'followed', 'by', 'an', 'intermediate', 'scale', 'modular', 'inflation', 'are', 'considered', 'the', 'restrictions', 'on', 'the', 'power', 'spectrum', 'p_r', 'of', 'curvature', 'perturbation', 'and', 'the', 'spectral', 'inde... | [-0.1586634183661659, 0.2472213582947791, -0.06676294487213193, 0.1246363502482768, -0.06353570705164054, -0.17648267748254334, -0.047099539730089166, 0.300380847404644, -0.23475683396956062, -0.37212113357982995, 0.1098304068048795, -0.1991415005055518, -0.015877590685157605, 0.1497796661390929, -0.03370132808743982, ... |
706.1437 | Spiking Optical Patterns and Synchronization | We analyze the time resolved spike statistics of a solitary and two mutually
interacting chaotic semiconductor lasers whose chaos is characterized by
apparently random, short intensity spikes. Repulsion between two successive
spikes is observed, resulting in a refractory period which is largest at laser
threshold. Fo... | physics.optics physics.bio-ph | we analyze the time resolved spike statistics of a solitary and two mutually interacting chaotic semiconductor lasers whose chaos is characterized by apparently random short intensity spikes repulsion between two successive spikes is observed resulting in a refractory period which is largest at laser threshold for time... | [['we', 'analyze', 'the', 'time', 'resolved', 'spike', 'statistics', 'of', 'a', 'solitary', 'and', 'two', 'mutually', 'interacting', 'chaotic', 'semiconductor', 'lasers', 'whose', 'chaos', 'is', 'characterized', 'by', 'apparently', 'random', 'short', 'intensity', 'spikes', 'repulsion', 'between', 'two', 'successive', '... | [-0.1930573756585447, 0.21233517790913395, -0.06792260877278855, 0.09569467018733618, 0.01855591811547927, -0.1735734955869153, 0.029614863421419543, 0.4408595094309865, -0.2812470912584941, -0.26964045734071046, 0.04823027894054975, -0.27792385132085506, -0.1684671341568875, 0.21042135707982113, -0.020670634634095988,... |
706.1438 | 3-quasi-Sasakian manifolds | In the present paper we carry on a systematic study of 3-quasi-Sasakian
manifolds. In particular we prove that the three Reeb vector fields generate an
involutive distribution determining a canonical totally geodesic and Riemannian
foliation. Locally, the leaves of this foliation turn out to be Lie groups:
either the... | math.DG | in the present paper we carry on a systematic study of 3quasisasakian manifolds in particular we prove that the three reeb vector fields generate an involutive distribution determining a canonical totally geodesic and riemannian foliation locally the leaves of this foliation turn out to be lie groups either the orthogo... | [['in', 'the', 'present', 'paper', 'we', 'carry', 'on', 'a', 'systematic', 'study', 'of', '3quasisasakian', 'manifolds', 'in', 'particular', 'we', 'prove', 'that', 'the', 'three', 'reeb', 'vector', 'fields', 'generate', 'an', 'involutive', 'distribution', 'determining', 'a', 'canonical', 'totally', 'geodesic', 'and', '... | [-0.2262023890317224, 0.08415791879455319, -0.14431020764560246, 0.10398778911348026, -0.08298215476132118, -0.10325277515567176, -0.006667462759651244, 0.39510282242237266, -0.2791938411237875, -0.20661373145066866, 0.10698267385262147, -0.24545671798445579, -0.14651946445217007, 0.16484114531621263, -0.09854423908728... |
706.1439 | The plasmon Talbot effect | The plasmon analog of the self-imaging Talbot effect is described and
theoretically analyzed. Rich plasmon carpets containing hot spots are shown to
be produced by a row of periodically-spaced surface features. A row of holes
drilled in a metal film and illuminated from the back side is discussed as a
realizable impl... | cond-mat.other | the plasmon analog of the selfimaging talbot effect is described and theoretically analyzed rich plasmon carpets containing hot spots are shown to be produced by a row of periodicallyspaced surface features a row of holes drilled in a metal film and illuminated from the back side is discussed as a realizable implementa... | [['the', 'plasmon', 'analog', 'of', 'the', 'selfimaging', 'talbot', 'effect', 'is', 'described', 'and', 'theoretically', 'analyzed', 'rich', 'plasmon', 'carpets', 'containing', 'hot', 'spots', 'are', 'shown', 'to', 'be', 'produced', 'by', 'a', 'row', 'of', 'periodicallyspaced', 'surface', 'features', 'a', 'row', 'of', ... | [-0.12088867400940645, 0.1748501078588614, -0.04913235562665196, 0.03861433510096771, -0.03585263643831508, -0.13935805560664877, 0.03074408951215446, 0.4220792146738591, -0.3015775901149027, -0.2913988042718676, 0.09807089191385518, -0.29498610323485885, -0.13819463296985143, 0.2313951705034603, -0.0554721655053607, 0... |
706.144 | One loop renormalization of the non-local gauge invariant operator min_U
(A^U_mu)^2 in QCD | We compute the one loop anomalous dimension of the gauge invariant dimension
two operator min_U (A^U_mu)^2, where U is an element of the gauge group, by
exploiting Zwanziger's expansion of the operator in terms of gauge invariant
non-local n leg operators. The computation is performed in an arbitrary linear
covariant... | hep-th | we compute the one loop anomalous dimension of the gauge invariant dimension two operator min_u au_mu2 where u is an element of the gauge group by exploiting zwanzigers expansion of the operator in terms of gauge invariant nonlocal n leg operators the computation is performed in an arbitrary linear covariant gauge and ... | [['we', 'compute', 'the', 'one', 'loop', 'anomalous', 'dimension', 'of', 'the', 'gauge', 'invariant', 'dimension', 'two', 'operator', 'min_u', 'au_mu2', 'where', 'u', 'is', 'an', 'element', 'of', 'the', 'gauge', 'group', 'by', 'exploiting', 'zwanzigers', 'expansion', 'of', 'the', 'operator', 'in', 'terms', 'of', 'gauge... | [-0.20342080247971941, 0.21251763898968312, -0.04809352504637311, 0.07936944447129088, -0.06312679574715302, -0.135552030473071, -0.04116937128060004, 0.29463244963656454, -0.22500238725367713, -0.2147706042372567, 0.06480409053756911, -0.2598788745701313, -0.1400344831732047, 0.07639657549340935, -0.006849032809944166... |
706.1441 | On Shadow of the Moon in Extensive Air Shower Data | A new technique has been devised for the analysis of extensive air shower
data in observing the effect of the moon on this data. In this technique the
number of EAS events with arrival directions falling in error circles centered
about the moving moon is compared to the mean number of events falling in error
circles ... | astro-ph | a new technique has been devised for the analysis of extensive air shower data in observing the effect of the moon on this data in this technique the number of eas events with arrival directions falling in error circles centered about the moving moon is compared to the mean number of events falling in error circles wit... | [['a', 'new', 'technique', 'has', 'been', 'devised', 'for', 'the', 'analysis', 'of', 'extensive', 'air', 'shower', 'data', 'in', 'observing', 'the', 'effect', 'of', 'the', 'moon', 'on', 'this', 'data', 'in', 'this', 'technique', 'the', 'number', 'of', 'eas', 'events', 'with', 'arrival', 'directions', 'falling', 'in', '... | [-0.10092297078170363, 0.10393001940101385, -0.12377316761581648, 0.07522167132701725, -0.04825283790067319, -0.01402484803130069, 0.02334806203537981, 0.38085657173106746, -0.20717094920635704, -0.38619669046132793, 0.11645981842021068, -0.3203030255052351, -0.06561021051039138, 0.2022794505551217, -0.0870713798021296... |
706.1442 | Searching for New Physics in Future Neutrino Factory Experiments | An extension of the New Standard Model, by introducing a mixing of the low
mass ``active'' neutrinos with heavy ones, or by any model with lepton flavor
violation, is considered. This leads to non-orthogonal neutrino production and
detection states and to modifications of neutrino oscillations in both, vacuum
and mat... | hep-ph | an extension of the new standard model by introducing a mixing of the low mass active neutrinos with heavy ones or by any model with lepton flavor violation is considered this leads to nonorthogonal neutrino production and detection states and to modifications of neutrino oscillations in both vacuum and matter the poss... | [['an', 'extension', 'of', 'the', 'new', 'standard', 'model', 'by', 'introducing', 'a', 'mixing', 'of', 'the', 'low', 'mass', 'active', 'neutrinos', 'with', 'heavy', 'ones', 'or', 'by', 'any', 'model', 'with', 'lepton', 'flavor', 'violation', 'is', 'considered', 'this', 'leads', 'to', 'nonorthogonal', 'neutrino', 'prod... | [-0.11849830939243428, 0.2491199449833799, 0.013776147026473132, 0.12577306169849367, -0.045534661376418976, -0.15672662589125907, 0.06222344967476928, 0.31782643583436043, -0.20583158563106105, -0.31790722002490207, 0.08684323378122197, -0.29991769862767215, -0.044341190523491836, 0.19936537057525502, 0.05918722381160... |
706.1443 | Spin chain from membrane and the Neumann-Rosochatius integrable system | We find membrane configurations in AdS_4 x S^7, which correspond to the
continuous limit of the SU(2) integrable spin chain, considered as a limit of
the SU(3) spin chain, arising in N=4 SYM in four dimensions, dual to strings in
AdS_5 x S^5. We also discuss the relationship with the Neumann-Rosochatius
integrable sy... | hep-th nlin.SI | we find membrane configurations in ads_4 x s7 which correspond to the continuous limit of the su2 integrable spin chain considered as a limit of the su3 spin chain arising in n4 sym in four dimensions dual to strings in ads_5 x s5 we also discuss the relationship with the neumannrosochatius integrable system at the lev... | [['we', 'find', 'membrane', 'configurations', 'in', 'ads_4', 'x', 's7', 'which', 'correspond', 'to', 'the', 'continuous', 'limit', 'of', 'the', 'su2', 'integrable', 'spin', 'chain', 'considered', 'as', 'a', 'limit', 'of', 'the', 'su3', 'spin', 'chain', 'arising', 'in', 'n4', 'sym', 'in', 'four', 'dimensions', 'dual', '... | [-0.15663783994023106, 0.17119946975071798, -0.00047688484119134955, 0.10692153582931496, 0.00873485766351223, -0.13688181622273987, -0.03150981373983086, 0.36344710845150985, -0.16092226212640526, -0.1643563469115179, 0.1344092153958627, -0.3062682731397217, -0.11548073272570036, 0.09105170960538089, -0.02499539988639... |
706.1444 | Representations of tame quivers and affine canonical bases | An integral PBW-basis of type $A_1^{(1)}$ has been constructed by Zhang [Z]
and Chen [C] using the Auslander-Reiten quiver of the Kronecker quiver. We
associate a geometric order to elements in this basis following an idea of
Lusztig [L1] in the case of finite type. This leads to an algebraic realization
of a bar-inv... | math.QA | an integral pbwbasis of type a_11 has been constructed by zhang z and chen c using the auslanderreiten quiver of the kronecker quiver we associate a geometric order to elements in this basis following an idea of lusztig l1 in the case of finite type this leads to an algebraic realization of a barinvariant basis of uq2 ... | [['an', 'integral', 'pbwbasis', 'of', 'type', 'a_11', 'has', 'been', 'constructed', 'by', 'zhang', 'z', 'and', 'chen', 'c', 'using', 'the', 'auslanderreiten', 'quiver', 'of', 'the', 'kronecker', 'quiver', 'we', 'associate', 'a', 'geometric', 'order', 'to', 'elements', 'in', 'this', 'basis', 'following', 'an', 'idea', '... | [-0.14253442298784783, 0.06969319284386681, -0.07033488679358184, 0.01304875293377942, -0.11986474065687852, -0.12018629984905366, -0.040095977540692766, 0.3394037624821067, -0.3704626673867029, -0.15674264655562756, 0.1194657583346944, -0.18534231616218608, -0.1527325258511054, 0.1347046057603115, -0.14498253531874744... |
706.1445 | Form factors in finite volume I: form factor bootstrap and truncated
conformal space | We describe the volume dependence of matrix elements of local fields to all
orders in inverse powers of the volume (i.e. only neglecting contributions that
decay exponentially with volume). Using the scaling Lee-Yang model and the
Ising model in a magnetic field as testing ground, we compare them to matrix
elements e... | hep-th cond-mat.other hep-lat | we describe the volume dependence of matrix elements of local fields to all orders in inverse powers of the volume ie only neglecting contributions that decay exponentially with volume using the scaling leeyang model and the ising model in a magnetic field as testing ground we compare them to matrix elements extracted ... | [['we', 'describe', 'the', 'volume', 'dependence', 'of', 'matrix', 'elements', 'of', 'local', 'fields', 'to', 'all', 'orders', 'in', 'inverse', 'powers', 'of', 'the', 'volume', 'ie', 'only', 'neglecting', 'contributions', 'that', 'decay', 'exponentially', 'with', 'volume', 'using', 'the', 'scaling', 'leeyang', 'model',... | [-0.06457583326846361, 0.1191756818357995, -0.0736131928719555, 0.05938848950884405, -0.03241232073570073, -0.06659765818433182, 0.03293395075849509, 0.34242705196595274, -0.2347852852497552, -0.2523762677934625, 0.08748680585366045, -0.27244266138311374, -0.14413162532287674, 0.18654919538735035, 0.040563721720261396,... |
706.1446 | Non-forward Balitsky-Kovchegov equation and Vector Mesons | Considering the Balitsky-Kovchegov QCD evolution equation in full momentum
space, we derive the travelling wave solutions expressing the nonlinear
saturation constraints on the dipole scattering amplitude at non-zero momentum
transfer. A phenomenological application to elastic vector meson production
shows the compat... | hep-ph | considering the balitskykovchegov qcd evolution equation in full momentum space we derive the travelling wave solutions expressing the nonlinear saturation constraints on the dipole scattering amplitude at nonzero momentum transfer a phenomenological application to elastic vector meson production shows the compatibilit... | [['considering', 'the', 'balitskykovchegov', 'qcd', 'evolution', 'equation', 'in', 'full', 'momentum', 'space', 'we', 'derive', 'the', 'travelling', 'wave', 'solutions', 'expressing', 'the', 'nonlinear', 'saturation', 'constraints', 'on', 'the', 'dipole', 'scattering', 'amplitude', 'at', 'nonzero', 'momentum', 'transfe... | [-0.18487326630221848, 0.17484318557518153, -0.10383987733670934, 0.12710182624869049, -0.12752276015552608, -0.027242454171011395, -0.005158479871567, 0.30054427859458055, -0.2907425170214, -0.24124055775729092, 0.011129750808785584, -0.32086362450976263, -0.010268419574607503, 0.07909054214727472, 0.1496960639784282,... |
706.1447 | Star clusters as diaries of galaxies | Most if not all stars form in star clusters. Thus the distribution of star
clusters preserves the information on the star formation history of a galaxy.
Massive clusters form only during episodes of high star formation activity
whereas periods of low star formation activity cannot produce them. We present
here the me... | astro-ph | most if not all stars form in star clusters thus the distribution of star clusters preserves the information on the star formation history of a galaxy massive clusters form only during episodes of high star formation activity whereas periods of low star formation activity cannot produce them we present here the method ... | [['most', 'if', 'not', 'all', 'stars', 'form', 'in', 'star', 'clusters', 'thus', 'the', 'distribution', 'of', 'star', 'clusters', 'preserves', 'the', 'information', 'on', 'the', 'star', 'formation', 'history', 'of', 'a', 'galaxy', 'massive', 'clusters', 'form', 'only', 'during', 'episodes', 'of', 'high', 'star', 'forma... | [-0.06321929122550764, 0.10546698149941537, -0.11767992655328219, 0.10812483716459162, -0.1473246830906989, 0.03296675150404158, 0.06279134929544576, 0.405435621900403, -0.14624502170203335, -0.36815383984450845, 0.05845592896946692, -0.2455984777319616, -0.05241622786591019, 0.14043551012941136, -0.045306630952256746,... |
706.1448 | Rational points on certain hyperelliptic curves over finite fields | Let $K$ be a field, $a, b\in K$ and $ab\neq 0$. Let us consider the
polynomials $g_{1}(x)=x^n+ax+b, g_{2}(x)=x^n+ax^2+bx$, where $n$ is a fixed
positive integer. In this paper we show that for each $k\geq 2$ the
hypersurface given by the equation \begin{equation*} S_{k}^{i}:
u^2=\prod_{j=1}^{k}g_{i}(x_{j}),\quad i=1,... | math.NT | let k be a field a bin k and abneq 0 let us consider the polynomials g_1xxnaxb g_2xxnax2bx where n is a fixed positive integer in this paper we show that for each kgeq 2 the hypersurface given by the equation beginequation s_ki u2prod_j1kg_ix_jquad i1 2 endequation contains a rational curve using the above and woestijn... | [['let', 'k', 'be', 'a', 'field', 'a', 'bin', 'k', 'and', 'abneq', '0', 'let', 'us', 'consider', 'the', 'polynomials', 'g_1xxnaxb', 'g_2xxnax2bx', 'where', 'n', 'is', 'a', 'fixed', 'positive', 'integer', 'in', 'this', 'paper', 'we', 'show', 'that', 'for', 'each', 'kgeq', '2', 'the', 'hypersurface', 'given', 'by', 'the'... | [-0.1969199029866744, 0.12557045389527316, -0.0967248070433184, -0.01755450373906412, -0.03409487597736312, -0.21987674942952984, 0.022970758069502075, 0.3041009458793718, -0.3067178219832756, -0.1888750946942579, 0.07913922813698006, -0.3365064949533086, -0.12477646471737068, 0.16460216785838575, -0.03661707381683367,... |
706.1449 | Detector dead-time effects and paralyzability in high-speed quantum key
distribution | Recent advances in quantum key distribution (QKD) have given rise to systems
that operate at transmission periods significantly shorter than the dead times
of their component single-photon detectors. As systems continue to increase in
transmission rate, security concerns associated with detector dead times can
limit ... | quant-ph | recent advances in quantum key distribution qkd have given rise to systems that operate at transmission periods significantly shorter than the dead times of their component singlephoton detectors as systems continue to increase in transmission rate security concerns associated with detector dead times can limit the pro... | [['recent', 'advances', 'in', 'quantum', 'key', 'distribution', 'qkd', 'have', 'given', 'rise', 'to', 'systems', 'that', 'operate', 'at', 'transmission', 'periods', 'significantly', 'shorter', 'than', 'the', 'dead', 'times', 'of', 'their', 'component', 'singlephoton', 'detectors', 'as', 'systems', 'continue', 'to', 'in... | [-0.21968788027655906, 0.10123659497688865, -0.06247946058208935, -0.006776158922525027, 0.06608840518702681, -0.1942138341971888, 0.08672348867791395, 0.36238825893125093, -0.2232099616756806, -0.2900218408411512, 0.10098124043687652, -0.3046203077765546, -0.08267039190888262, 0.2616731215548964, -0.14081080385650963,... |
706.145 | Nuclei embedded in an electron gas | The properties of nuclei embedded in an electron gas are studied within the
relativistic mean-field approach. These studies are relevant for nuclear
properties in astrophysical environments such as neutron-star crusts and
supernova explosions. The electron gas is treated as a constant background in
the Wigner-Seitz c... | nucl-th | the properties of nuclei embedded in an electron gas are studied within the relativistic meanfield approach these studies are relevant for nuclear properties in astrophysical environments such as neutronstar crusts and supernova explosions the electron gas is treated as a constant background in the wignerseitz cell app... | [['the', 'properties', 'of', 'nuclei', 'embedded', 'in', 'an', 'electron', 'gas', 'are', 'studied', 'within', 'the', 'relativistic', 'meanfield', 'approach', 'these', 'studies', 'are', 'relevant', 'for', 'nuclear', 'properties', 'in', 'astrophysical', 'environments', 'such', 'as', 'neutronstar', 'crusts', 'and', 'super... | [-0.029816034611680413, 0.2326953213105818, -0.0330637830575662, 0.18043702861676658, 0.029900352676798192, -0.08844765045339176, 0.039220427140493744, 0.38076798103616705, -0.19796628769753236, -0.24465097413548, 0.006982627440343744, -0.32456040385711404, 0.003396901548174875, 0.1757676758903212, 0.06499799798142963,... |
706.1451 | Spin Injection into a Graphene Thin Film at Room Temperature | We demonstrate spin injection into a graphene thin film with high reliability
by using non-local magnetoresistance (MR) measurements, in which the electric
current path is completely separated from the spin current path. Using these
non-local measurements, an obvious MR effect was observed at room temperature;
and th... | cond-mat.mtrl-sci | we demonstrate spin injection into a graphene thin film with high reliability by using nonlocal magnetoresistance mr measurements in which the electric current path is completely separated from the spin current path using these nonlocal measurements an obvious mr effect was observed at room temperature and the mr effec... | [['we', 'demonstrate', 'spin', 'injection', 'into', 'a', 'graphene', 'thin', 'film', 'with', 'high', 'reliability', 'by', 'using', 'nonlocal', 'magnetoresistance', 'mr', 'measurements', 'in', 'which', 'the', 'electric', 'current', 'path', 'is', 'completely', 'separated', 'from', 'the', 'spin', 'current', 'path', 'using... | [-0.1605657863266328, 0.1988706422272919, -0.05133659278645235, -0.07828532458858235, -0.05223587523488438, -0.14056557615780654, 0.04238948617678355, 0.41633927212918503, -0.28027617921504905, -0.32612222557997, 0.018676702501526213, -0.2893728117732441, -0.06263339066439692, 0.23651817108997528, 0.04541927003027762, ... |
706.1452 | Reconstructing vibrational states in warm molecules using four-wave
mixing with femtosecond laser pulses | We propose a method to reconstruct the vibrational quantum state of molecules
excited by a general excitation laser pulse. Unlike existing methods, we do not
require the molecules before excitation to be in a pure state, allowing us to
treat the important case of initially thermally excited molecules. Even if only
a ... | quant-ph | we propose a method to reconstruct the vibrational quantum state of molecules excited by a general excitation laser pulse unlike existing methods we do not require the molecules before excitation to be in a pure state allowing us to treat the important case of initially thermally excited molecules even if only a single... | [['we', 'propose', 'a', 'method', 'to', 'reconstruct', 'the', 'vibrational', 'quantum', 'state', 'of', 'molecules', 'excited', 'by', 'a', 'general', 'excitation', 'laser', 'pulse', 'unlike', 'existing', 'methods', 'we', 'do', 'not', 'require', 'the', 'molecules', 'before', 'excitation', 'to', 'be', 'in', 'a', 'pure', '... | [-0.09101541174324945, 0.19115453041208988, -0.09399327839402338, 0.04425135802011937, -0.023614127095788716, -0.1506184158882556, 0.04446073022106877, 0.4544800063738456, -0.2362652574880765, -0.32468050746247173, 0.04884116416304515, -0.24344134737576287, -0.024949755067399774, 0.17839933101920627, -0.016086224771033... |
706.1453 | The crucial importance of the $t_{2g}$--$e_g$ hybridization in
transition metal oxides | We studied the influence of the trigonal distortion of the regular octahedron
along the (111) direction, found in the $\rm CoO_2$ layers. Under such a
distortion the $t_{2g}$ orbitals split into one $a_{1g}$ and two degenerated
$e_g^\prime$ orbitals. We focused on the relative order of these orbitals.
Using quantum c... | cond-mat.str-el | we studied the influence of the trigonal distortion of the regular octahedron along the 111 direction found in the rm coo_2 layers under such a distortion the t_2g orbitals split into one a_1g and two degenerated e_gprime orbitals we focused on the relative order of these orbitals using quantum chemical calculations of... | [['we', 'studied', 'the', 'influence', 'of', 'the', 'trigonal', 'distortion', 'of', 'the', 'regular', 'octahedron', 'along', 'the', '111', 'direction', 'found', 'in', 'the', 'rm', 'coo_2', 'layers', 'under', 'such', 'a', 'distortion', 'the', 't_2g', 'orbitals', 'split', 'into', 'one', 'a_1g', 'and', 'two', 'degenerated... | [-0.18226640808894495, 0.167250427620774, -0.017014150627442753, 0.07299022540297609, 0.01712753014101214, -0.08356320029649307, 0.06303354044375993, 0.37504432245459357, -0.28332205519447445, -0.2628752148093682, -0.05254149223058025, -0.3169030368634095, -0.11101347638267867, 0.07227761023776265, 0.052115100862222236... |
706.1454 | Heterogeneity and Increasing Returns May Drive Socio-Economic
Transitions | There are clear benefits associated with a particular consumer choice for
many current markets. For example, as we consider here, some products might
carry environmental or `green' benefits. Some consumers might value these
benefits while others do not. However, as evidenced by myriad failed attempts
of environmental... | q-fin.GN physics.soc-ph | there are clear benefits associated with a particular consumer choice for many current markets for example as we consider here some products might carry environmental or green benefits some consumers might value these benefits while others do not however as evidenced by myriad failed attempts of environmental products ... | [['there', 'are', 'clear', 'benefits', 'associated', 'with', 'a', 'particular', 'consumer', 'choice', 'for', 'many', 'current', 'markets', 'for', 'example', 'as', 'we', 'consider', 'here', 'some', 'products', 'might', 'carry', 'environmental', 'or', 'green', 'benefits', 'some', 'consumers', 'might', 'value', 'these', '... | [-0.097453897770191, 0.10438653506376837, -0.06751626024434212, 0.10658368243305229, -0.12259204175355735, -0.15948347478352357, 0.0839037882126218, 0.44386823311296486, -0.2869447036495711, -0.306372557336608, 0.13749468435064977, -0.2960331059795524, -0.16240752731628585, 0.18667669538516812, -0.12667053764371938, -0... |
706.1455 | Geometrical locus of massive test particle orbits in the space of
physical parameters in Kerr space-time | Gravitational radiation of binary systems can be studied by using the
adiabatic approximation in General Relativity. In this approach a small
astrophysical object follows a trajectory consisting of a chained series of
bounded geodesics (orbits) in the outer region of a Kerr Black Hole,
representing the space time cre... | gr-qc | gravitational radiation of binary systems can be studied by using the adiabatic approximation in general relativity in this approach a small astrophysical object follows a trajectory consisting of a chained series of bounded geodesics orbits in the outer region of a kerr black hole representing the space time created b... | [['gravitational', 'radiation', 'of', 'binary', 'systems', 'can', 'be', 'studied', 'by', 'using', 'the', 'adiabatic', 'approximation', 'in', 'general', 'relativity', 'in', 'this', 'approach', 'a', 'small', 'astrophysical', 'object', 'follows', 'a', 'trajectory', 'consisting', 'of', 'a', 'chained', 'series', 'of', 'boun... | [-0.17885640352784146, 0.10850334162373215, -0.10070595677130886, 0.05869769265785092, -0.06615656689710675, -0.058821803136097806, 0.012457998569363788, 0.31765585975240795, -0.22071626575122918, -0.3022779007111826, 0.08603078206219981, -0.21502632181791048, -0.11092093689667602, 0.26316467756705897, -0.0746660194680... |
706.1456 | A Generic Model of Contracts for Embedded Systems | We present the mathematical foundations of the contract-based model developed
in the framework of the SPEEDS project. SPEEDS aims at developing methods and
tools to support "speculative design", a design methodology in which
distributed designers develop different aspects of the overall system, in a
concurrent but co... | cs.SE | we present the mathematical foundations of the contractbased model developed in the framework of the speeds project speeds aims at developing methods and tools to support speculative design a design methodology in which distributed designers develop different aspects of the overall system in a concurrent but controlled... | [['we', 'present', 'the', 'mathematical', 'foundations', 'of', 'the', 'contractbased', 'model', 'developed', 'in', 'the', 'framework', 'of', 'the', 'speeds', 'project', 'speeds', 'aims', 'at', 'developing', 'methods', 'and', 'tools', 'to', 'support', 'speculative', 'design', 'a', 'design', 'methodology', 'in', 'which',... | [-0.11260198474694746, 0.05761290553799075, -0.10965463846596836, 0.015270696967851315, -0.0858801343557337, -0.1215333769203357, 0.06974660403771712, 0.33785947569522934, -0.2732718661954662, -0.3255478540646299, 0.0990024889601869, -0.17788679905692642, -0.17300171050174987, 0.19381193457037332, -0.07311656414794754,... |
706.1457 | Universality of traveling waves with QCD running coupling | ``Geometric scaling'', i.e. the dependence of DIS cross-sections on the ratio
Q/Q_S, where Q_S(Y) is the rapidity-dependent \saturation scale, can be
theoretically obtained from universal ``traveling wave'' solutions of the
nonlinear Balitsky-Kovchegov (BK) QCD evolution equation at fixed coupling. We
examine the sim... | hep-ph | geometric scaling ie the dependence of dis crosssections on the ratio qq_s where q_sy is the rapiditydependent saturation scale can be theoretically obtained from universal traveling wave solutions of the nonlinear balitskykovchegov bk qcd evolution equation at fixed coupling we examine the similar meanfield prediction... | [['geometric', 'scaling', 'ie', 'the', 'dependence', 'of', 'dis', 'crosssections', 'on', 'the', 'ratio', 'qq_s', 'where', 'q_sy', 'is', 'the', 'rapiditydependent', 'saturation', 'scale', 'can', 'be', 'theoretically', 'obtained', 'from', 'universal', 'traveling', 'wave', 'solutions', 'of', 'the', 'nonlinear', 'balitskyk... | [-0.13325193850323558, 0.15818372264970093, -0.1486069404054433, 0.14383927922463044, -0.08450857087504118, -0.07517668772954494, -0.014317905195057393, 0.2769130392745137, -0.2546267026662827, -0.25212453737854956, 0.03876451431773603, -0.3264371159765869, -0.04595101332291961, 0.10787489179521799, 0.15518045190023258... |
706.1458 | Impurity scattering in strongly correlated metals close to the Mott
transition | This work explores a simple approximation to describe isolated impurity
scattering in a strongly correlated metal. The approximation combines
conventional one electron scattering theory and the Dynamic Mean Field Theory
to describe strong correlations in the host. It becomes exact in several
limits, including those o... | cond-mat.str-el | this work explores a simple approximation to describe isolated impurity scattering in a strongly correlated metal the approximation combines conventional one electron scattering theory and the dynamic mean field theory to describe strong correlations in the host it becomes exact in several limits including those of ver... | [['this', 'work', 'explores', 'a', 'simple', 'approximation', 'to', 'describe', 'isolated', 'impurity', 'scattering', 'in', 'a', 'strongly', 'correlated', 'metal', 'the', 'approximation', 'combines', 'conventional', 'one', 'electron', 'scattering', 'theory', 'and', 'the', 'dynamic', 'mean', 'field', 'theory', 'to', 'de... | [-0.13045840906573736, 0.13736388255207937, -0.07190149828068357, 0.15584868570774832, -0.02608234942593473, -0.21217056047765814, 0.06274916670728534, 0.3853955354858586, -0.2681064329238886, -0.2834387695357362, 8.507012488677147e-06, -0.3415741614521818, -0.1526812116437136, 0.16587360683788963, 0.02981666324937597,... |
706.1459 | Transversity Signals in Two-Hadron Production at COMPASS | New results on single spin asymmetries of identified charged pion and kaon
pairs produced in deep-inelastic scattering of muons on a transversely
polarized 6LiD target are presented. The data were taken in the years 2003 and
2004 with the COMPASS spectrometer at CERN with a 160 GeV muon beam from the
CERN SPS acceler... | hep-ex | new results on single spin asymmetries of identified charged pion and kaon pairs produced in deepinelastic scattering of muons on a transversely polarized 6lid target are presented the data were taken in the years 2003 and 2004 with the compass spectrometer at cern with a 160 gev muon beam from the cern sps accelerator... | [['new', 'results', 'on', 'single', 'spin', 'asymmetries', 'of', 'identified', 'charged', 'pion', 'and', 'kaon', 'pairs', 'produced', 'in', 'deepinelastic', 'scattering', 'of', 'muons', 'on', 'a', 'transversely', 'polarized', '6lid', 'target', 'are', 'presented', 'the', 'data', 'were', 'taken', 'in', 'the', 'years', '2... | [-0.05809222826592661, 0.28313801679121076, -0.11862534026651844, 0.1436636740108952, -0.003713158114502827, -0.08331235063116194, -0.021816510684313437, 0.38513730444452343, -0.18443577294694444, -0.25558067259250905, -0.044208566867061615, -0.3520525489550303, 0.11140444074008687, 0.1848318040023978, 0.07925134297122... |
706.146 | Uncertainty in the Fluctuations of the Price of Stocks | We report on a study of the Tehran Price Index (TEPIX) from 2001 to 2006 as
an emerging market that has been affected by several political crises during
the recent years, and analyze the non-Gaussian probability density function
(PDF) of the log returns of the stocks' prices. We show that while the average
of the ind... | q-fin.ST physics.data-an physics.soc-ph | we report on a study of the tehran price index tepix from 2001 to 2006 as an emerging market that has been affected by several political crises during the recent years and analyze the nongaussian probability density function pdf of the log returns of the stocks prices we show that while the average of the index did not... | [['we', 'report', 'on', 'a', 'study', 'of', 'the', 'tehran', 'price', 'index', 'tepix', 'from', '2001', 'to', '2006', 'as', 'an', 'emerging', 'market', 'that', 'has', 'been', 'affected', 'by', 'several', 'political', 'crises', 'during', 'the', 'recent', 'years', 'and', 'analyze', 'the', 'nongaussian', 'probability', 'd... | [-0.10326619168950452, 0.11994824053016837, -0.1598683317526357, 0.07465223712087782, 0.0002532694488763809, -0.03341060879605788, 0.08795722092467326, 0.37166160292647504, -0.2394273816616516, -0.29999828052413824, 0.12826317789860897, -0.2905518018502604, -0.15216188956983387, 0.20469035215813805, -0.0969259361632996... |
706.1461 | Gap solitons in spatiotemporal photonic crystals | We generalize the concept of nonlinear periodic structures to systems that
show arbitrary spacetime variations of the refractive index. Nonlinear pulse
propagation through these spatiotemporal photonic crystals can be described,
for shallow nonstationary gratings, by coupled mode equations which are a
generalization ... | physics.optics | we generalize the concept of nonlinear periodic structures to systems that show arbitrary spacetime variations of the refractive index nonlinear pulse propagation through these spatiotemporal photonic crystals can be described for shallow nonstationary gratings by coupled mode equations which are a generalization of th... | [['we', 'generalize', 'the', 'concept', 'of', 'nonlinear', 'periodic', 'structures', 'to', 'systems', 'that', 'show', 'arbitrary', 'spacetime', 'variations', 'of', 'the', 'refractive', 'index', 'nonlinear', 'pulse', 'propagation', 'through', 'these', 'spatiotemporal', 'photonic', 'crystals', 'can', 'be', 'described', '... | [-0.17009098474158063, 0.1673642614595814, -0.08013575375523596, 0.07825437423750936, -0.10169146074691698, -0.21544540039308013, -0.042218783690172824, 0.42230749536039575, -0.2549115047080531, -0.28184630617588047, 0.056851179768619614, -0.2602810238160947, -0.19789371549684023, 0.17810058408871382, 0.001334509479680... |
706.1462 | MiniBooNE Results and Neutrino Schemes with 2 sterile Neutrinos:
Possible Mass Orderings and Observables related to Neutrino Masses | The MiniBooNE and LSND experiments are compatible with each other when two
sterile neutrinos are added to the three active ones. In this case there are
eight possible mass orderings. In two of them both sterile neutrinos are
heavier than the three active ones. In the next two scenarios both sterile
neutrinos are ligh... | hep-ph astro-ph hep-ex | the miniboone and lsnd experiments are compatible with each other when two sterile neutrinos are added to the three active ones in this case there are eight possible mass orderings in two of them both sterile neutrinos are heavier than the three active ones in the next two scenarios both sterile neutrinos are lighter t... | [['the', 'miniboone', 'and', 'lsnd', 'experiments', 'are', 'compatible', 'with', 'each', 'other', 'when', 'two', 'sterile', 'neutrinos', 'are', 'added', 'to', 'the', 'three', 'active', 'ones', 'in', 'this', 'case', 'there', 'are', 'eight', 'possible', 'mass', 'orderings', 'in', 'two', 'of', 'them', 'both', 'sterile', '... | [-0.09755839715025534, 0.31000748783546056, 0.02973593054094205, 0.216567860671172, -0.043964738641424396, -0.2002219409044636, 0.0339344780604159, 0.3551293762694848, -0.1740920887965905, -0.3549730529043652, 0.04673790437916882, -0.3815091960132122, -0.013370928337405387, 0.21675026901066302, 0.09208571888310345, 0.0... |
706.1463 | Nernst Effect in NdBa_2[Cu_{1-y}Ni_y]_3O_{7-\delta} | In NdBa_2[Cu_{1-y}Ni_y]_3O_{7-\delta}, magnetic Ni-impurities suppress Tc but
at the same time the pseudogap is strongly enhanced. This unique feature makes
it an ideal system to study possible relations between the anomalous Nernst
effect, superconductivity and the pseudogap. We present Nernst effect
measurements on... | cond-mat.supr-con cond-mat.str-el | in ndba_2cu_1yni_y_3o_7delta magnetic niimpurities suppress tc but at the same time the pseudogap is strongly enhanced this unique feature makes it an ideal system to study possible relations between the anomalous nernst effect superconductivity and the pseudogap we present nernst effect measurements on a series of opt... | [['in', 'ndba_2cu_1yni_y_3o_7delta', 'magnetic', 'niimpurities', 'suppress', 'tc', 'but', 'at', 'the', 'same', 'time', 'the', 'pseudogap', 'is', 'strongly', 'enhanced', 'this', 'unique', 'feature', 'makes', 'it', 'an', 'ideal', 'system', 'to', 'study', 'possible', 'relations', 'between', 'the', 'anomalous', 'nernst', '... | [-0.11855289131571634, 0.2115159965577209, -0.02038814222044128, 0.02312714128395704, -0.06384380862454143, -0.14313532942979354, 0.13505564384184426, 0.3398267371162009, -0.28525660478135967, -0.29446467111165836, 0.00045666424328402624, -0.46747119173290225, -0.060266217275515316, 0.1361087473241363, -0.0139072476327... |
706.1464 | Testing thermal reprocessing in AGN accretion discs | The thermal reprocessing hypothesis in AGN, where EUV/X-ray photons are
reprocessed by the accretion disc into optical/UV photons, predicts
wavelength-dependent time delays between the optical continuum at different
wavelengths. Recent photometric monitoring by Sergeev et al. has shown that the
time-delay is observed... | astro-ph | the thermal reprocessing hypothesis in agn where euvxray photons are reprocessed by the accretion disc into opticaluv photons predicts wavelengthdependent time delays between the optical continuum at different wavelengths recent photometric monitoring by sergeev et al has shown that the timedelay is observed in 14 agn ... | [['the', 'thermal', 'reprocessing', 'hypothesis', 'in', 'agn', 'where', 'euvxray', 'photons', 'are', 'reprocessed', 'by', 'the', 'accretion', 'disc', 'into', 'opticaluv', 'photons', 'predicts', 'wavelengthdependent', 'time', 'delays', 'between', 'the', 'optical', 'continuum', 'at', 'different', 'wavelengths', 'recent',... | [-0.06395154251640633, 0.103651554127282, -0.04738813000221853, 0.08445395287071733, -0.02838715489997412, -0.12220397733108257, 0.05223275058961008, 0.44181210042734165, -0.19244351266388549, -0.3572820722765755, 0.07414167391561932, -0.2901694091851823, 0.005446792447401094, 0.22066396240006725, -0.06419368709612172,... |
706.1465 | Supercurrents in an atom-molecule gas in an optical ring lattice | Atom and molecule currents in a Fermi gas in the neighborhood of a Feshbach
resonance are studied in a one-dimensional optical ring lattice by directly
diagonalizing small models. A rotational analogy of flux quantization is used
to show that fraction of the current is carried by particles with twice the
mass of an a... | quant-ph | atom and molecule currents in a fermi gas in the neighborhood of a feshbach resonance are studied in a onedimensional optical ring lattice by directly diagonalizing small models a rotational analogy of flux quantization is used to show that fraction of the current is carried by particles with twice the mass of an atom ... | [['atom', 'and', 'molecule', 'currents', 'in', 'a', 'fermi', 'gas', 'in', 'the', 'neighborhood', 'of', 'a', 'feshbach', 'resonance', 'are', 'studied', 'in', 'a', 'onedimensional', 'optical', 'ring', 'lattice', 'by', 'directly', 'diagonalizing', 'small', 'models', 'a', 'rotational', 'analogy', 'of', 'flux', 'quantizatio... | [-0.17423808016770884, 0.20748579625057065, -0.02617828356954506, 0.047785080736503005, 0.01799260832811311, -0.12681455951247175, 0.08723335815356824, 0.368323626501833, -0.22666696552187204, -0.259356123379479, 0.0018605082473417713, -0.26351029785760377, -0.0590321675763797, 0.15630595016656285, 0.03371294576011724,... |
706.1466 | The absolute Galois group acts faithfully on the connected components of
the moduli space of surfaces of general type | We show that the Galois group $Gal(\bar{\Q} /\Q)$ operates faithfully on the
set of connected components of the moduli spaces of surfaces of general type,
and also that for each element $\sigma \in Gal(\bar{\Q} /\Q)$ different from
the identity and from complex conjugation, there is a surface of general type
such tha... | math.AG math.NT | we show that the galois group galbarq q operates faithfully on the set of connected components of the moduli spaces of surfaces of general type and also that for each element sigma in galbarq q different from the identity and from complex conjugation there is a surface of general type such that x and the galois conjuga... | [['we', 'show', 'that', 'the', 'galois', 'group', 'galbarq', 'q', 'operates', 'faithfully', 'on', 'the', 'set', 'of', 'connected', 'components', 'of', 'the', 'moduli', 'spaces', 'of', 'surfaces', 'of', 'general', 'type', 'and', 'also', 'that', 'for', 'each', 'element', 'sigma', 'in', 'galbarq', 'q', 'different', 'from'... | [-0.1577071423152796, 0.10217929521026328, -0.11097702852939853, 0.03423126180878638, -0.1262056332959149, -0.14972466696352243, 0.008030998430256613, 0.3195917235078433, -0.3051918523590594, -0.26275940096149075, 0.09549594432628976, -0.24201451127047244, -0.19148342298248258, 0.24258990061636537, -0.15672171251096118... |
706.1467 | The Quantum-Classical Transition and Wave Packet Dispersion | Two recent studies have presented new information relevant to the transition
from quantum behavior to classical behavior, and related this to parameters
characterizing the universe as a whole. The present study based on a separate
approach has developed similar results that appear to substantiate aspects of
earlier w... | physics.gen-ph | two recent studies have presented new information relevant to the transition from quantum behavior to classical behavior and related this to parameters characterizing the universe as a whole the present study based on a separate approach has developed similar results that appear to substantiate aspects of earlier work ... | [['two', 'recent', 'studies', 'have', 'presented', 'new', 'information', 'relevant', 'to', 'the', 'transition', 'from', 'quantum', 'behavior', 'to', 'classical', 'behavior', 'and', 'related', 'this', 'to', 'parameters', 'characterizing', 'the', 'universe', 'as', 'a', 'whole', 'the', 'present', 'study', 'based', 'on', '... | [-0.02822414074431766, 0.07976421426812356, -0.16184513742019507, 0.038910664395767854, -0.11448336087844589, -0.11420121142132715, 0.048293116747994316, 0.3050992194224488, -0.2218367386863313, -0.3029104174876755, 0.10274370862382719, -0.239111944491213, -0.22443485964428295, 0.22923910949717868, -0.0616478938778693,... |
706.1468 | Enhanced Pressure Dependence of Magnetic Exchange in A2+[V2]O4 Spinels
Approaching the Itinerant Electron Limit | We report a systematic enhancement of the pressure dependence of TN in
A2+[V2]O4 spinels as the V-V separation approaches the critical separation for
a transition to itinerant-electron behavior. An intermediate phase between
localized and itinerant electron behavior is identified in Zn[V2]O4 and
Mg[V2]O4 exhibiting m... | cond-mat.str-el | we report a systematic enhancement of the pressure dependence of tn in a2v2o4 spinels as the vv separation approaches the critical separation for a transition to itinerantelectron behavior an intermediate phase between localized and itinerant electron behavior is identified in znv2o4 and mgv2o4 exhibiting mobile holes ... | [['we', 'report', 'a', 'systematic', 'enhancement', 'of', 'the', 'pressure', 'dependence', 'of', 'tn', 'in', 'a2v2o4', 'spinels', 'as', 'the', 'vv', 'separation', 'approaches', 'the', 'critical', 'separation', 'for', 'a', 'transition', 'to', 'itinerantelectron', 'behavior', 'an', 'intermediate', 'phase', 'between', 'lo... | [-0.18355286214229932, 0.23766526446808373, -0.02003945998825826, 0.05275462194871114, -0.015574045034618181, -0.14543102920423587, 0.08896241025176159, 0.3774441191710012, -0.21779926181879156, -0.28665302087401234, 0.021071341198728267, -0.3522761378350646, -0.11632868342729676, 0.15418918990681685, 0.038098888764114... |
706.1469 | N=4 Supersymmetric MICZ-Kepler systems on S3 | Proceeding from the superfield action for $N=4, d=1$ nonlinear
supermultiplet, equipped with the most general potential term, we find the
action describing a charged particle on the sphere $S^3$ in the field of $n$
fixed Dirac dyons. We construct the supercharges and Hamiltonian and analyze
some particulary interesti... | hep-th | proceeding from the superfield action for n4 d1 nonlinear supermultiplet equipped with the most general potential term we find the action describing a charged particle on the sphere s3 in the field of n fixed dirac dyons we construct the supercharges and hamiltonian and analyze some particulary interesting potentials c... | [['proceeding', 'from', 'the', 'superfield', 'action', 'for', 'n4', 'd1', 'nonlinear', 'supermultiplet', 'equipped', 'with', 'the', 'most', 'general', 'potential', 'term', 'we', 'find', 'the', 'action', 'describing', 'a', 'charged', 'particle', 'on', 'the', 'sphere', 's3', 'in', 'the', 'field', 'of', 'n', 'fixed', 'dir... | [-0.1644180444606508, 0.126726819967063, -0.0015112889787325492, 0.10440984026242334, -0.062246633818946205, -0.2207498741049606, -0.09061931254198918, 0.2910917657785691, -0.12624138868234766, -0.2421981751191197, 0.07226001764468562, -0.36587085437316164, -0.19838288575769045, 0.0867360146662507, -0.02373164557995131... |
706.147 | Fast mode of rotating atoms in one-dimensional lattice rings | We study the rotation of atoms in one-dimensional lattice rings. In
particular, the "fast mode", where the ground state atoms rotate faster than
the stirring rotating the atoms, is studied both analytically and numerically.
The conditions for the transition to the fast mode are found to be very
different from that in... | quant-ph | we study the rotation of atoms in onedimensional lattice rings in particular the fast mode where the ground state atoms rotate faster than the stirring rotating the atoms is studied both analytically and numerically the conditions for the transition to the fast mode are found to be very different from that in continuum... | [['we', 'study', 'the', 'rotation', 'of', 'atoms', 'in', 'onedimensional', 'lattice', 'rings', 'in', 'particular', 'the', 'fast', 'mode', 'where', 'the', 'ground', 'state', 'atoms', 'rotate', 'faster', 'than', 'the', 'stirring', 'rotating', 'the', 'atoms', 'is', 'studied', 'both', 'analytically', 'and', 'numerically', ... | [-0.1506076160488495, 0.24597532095503993, -0.040874101008133344, 0.06220807527643046, -0.0018121167692394617, -0.14094658326454615, 0.06514057168290795, 0.4135072100907564, -0.2439111856801901, -0.22231740697558658, 0.08139272054540925, -0.24624301841807514, -0.09812470288792004, 0.16170618973167925, 0.033044894385966... |
706.1471 | Singular unitarity in "quantization commutes with reduction" | Let $M$ be a connected compact quantizable K\"ahler manifold equipped with a
Hamiltonian action of a connected compact Lie group $G$. Let
$M//G=\phi^{-1}(0)/G=M_0$ be the symplectic quotient at value 0 of the moment
map $\phi$. The space $M_0$ may in general not be smooth. It is known that, as
vector spaces, there is... | math.SG | let m be a connected compact quantizable kahler manifold equipped with a hamiltonian action of a connected compact lie group g let mgphi10gm_0 be the symplectic quotient at value 0 of the moment map phi the space m_0 may in general not be smooth it is known that as vector spaces there is a natural isomorphism between t... | [['let', 'm', 'be', 'a', 'connected', 'compact', 'quantizable', 'kahler', 'manifold', 'equipped', 'with', 'a', 'hamiltonian', 'action', 'of', 'a', 'connected', 'compact', 'lie', 'group', 'g', 'let', 'mgphi10gm_0', 'be', 'the', 'symplectic', 'quotient', 'at', 'value', '0', 'of', 'the', 'moment', 'map', 'phi', 'the', 'sp... | [-0.20361895094988228, 0.1461686388703191, -0.09451113830014836, 0.0666912648274087, -0.10846426029412345, -0.11156246327005952, -0.013538300671582714, 0.35400182504974703, -0.33992395012547044, -0.21650876118339427, 0.09296712052620919, -0.21195307799849575, -0.11272085608047155, 0.20810736684868011, -0.12179427269760... |
706.1472 | On Lesieur's Measured Quantum Groupoids | In his thesis ([L1]), which is published in an expended and revised version
([L2]), Franck Lesieur had introduced a notion of measured quantum groupoid, in
the setting of von Neumann algebras, using intensively the notion of
pseudo-multiplicative unitary, which had been introduced in a previous article
of the author,... | math.OA | in his thesis l1 which is published in an expended and revised version l2 franck lesieur had introduced a notion of measured quantum groupoid in the setting of von neumann algebras using intensively the notion of pseudomultiplicative unitary which had been introduced in a previous article of the author in collaboration... | [['in', 'his', 'thesis', 'l1', 'which', 'is', 'published', 'in', 'an', 'expended', 'and', 'revised', 'version', 'l2', 'franck', 'lesieur', 'had', 'introduced', 'a', 'notion', 'of', 'measured', 'quantum', 'groupoid', 'in', 'the', 'setting', 'of', 'von', 'neumann', 'algebras', 'using', 'intensively', 'the', 'notion', 'of... | [-0.08465193327405114, 0.11290498544073685, -0.10939710716883749, 0.05741020120722033, -0.07277099403323356, -0.1310567722252723, -0.021735796131499445, 0.3179615781010031, -0.2170092922412971, -0.28558525412496344, 0.08546209911148606, -0.2553642534636962, -0.10811281876999941, 0.16425143055089597, -0.2246407356891614... |
706.1473 | Generalized St\"ackel Transform and Reciprocal Transformations for
Finite-Dimensional Integrable Systems | We present a multiparameter generalization of the St\"ackel transform (the
latter is also known as the coupling-constant metamorphosis) and show that
under certain conditions this generalized St\"ackel transform preserves the
Liouville integrability, noncommutative integrability and superintegrability.
The correspond... | nlin.SI hep-th math-ph math.MP | we present a multiparameter generalization of the stackel transform the latter is also known as the couplingconstant metamorphosis and show that under certain conditions this generalized stackel transform preserves the liouville integrability noncommutative integrability and superintegrability the corresponding transfo... | [['we', 'present', 'a', 'multiparameter', 'generalization', 'of', 'the', 'stackel', 'transform', 'the', 'latter', 'is', 'also', 'known', 'as', 'the', 'couplingconstant', 'metamorphosis', 'and', 'show', 'that', 'under', 'certain', 'conditions', 'this', 'generalized', 'stackel', 'transform', 'preserves', 'the', 'liouvill... | [-0.14216676362253644, 0.08991578876663445, -0.13988398886083261, 0.10456503198213835, -0.11754485867846676, -0.12888880624719287, -0.028910988812719512, 0.3218498188273414, -0.34150376130381355, -0.20618750436393463, 0.11650569759734461, -0.1971084206471341, -0.25684391686935787, 0.1833658125453993, -0.084714895349664... |
706.1474 | Determination of the Jet Energy Scale | The uncertainty in jet energy scale is one of the dominating systematic
errors for many measurements at hadron colliders - most notably for the
measurement of the top-quark-mass, inclusive jet cross section measurements and
last but not least for events with large missing transverse energy as expected
in searches bey... | hep-ex | the uncertainty in jet energy scale is one of the dominating systematic errors for many measurements at hadron colliders most notably for the measurement of the topquarkmass inclusive jet cross section measurements and last but not least for events with large missing transverse energy as expected in searches beyond the... | [['the', 'uncertainty', 'in', 'jet', 'energy', 'scale', 'is', 'one', 'of', 'the', 'dominating', 'systematic', 'errors', 'for', 'many', 'measurements', 'at', 'hadron', 'colliders', 'most', 'notably', 'for', 'the', 'measurement', 'of', 'the', 'topquarkmass', 'inclusive', 'jet', 'cross', 'section', 'measurements', 'and', ... | [-0.0610158697427697, 0.17918683575746946, -0.0720255216392242, 0.1525159805043511, -0.050059656280871126, -0.1271137054307922, -0.012163299263442217, 0.3250170422794476, -0.22539701536840007, -0.3231246784992822, 0.07695368146332465, -0.3441261652066079, 0.09065165304361958, 0.22444864415742252, 0.05973981411525902, 0... |
706.1475 | Jacobi-Nijenhuis algebroids and their modular classes | Jacobi-Nijenhuis algebroids are defined as a natural generalization of
Poisson-Nijenhuis algebroids, in the case where there exists a Nijenhuis
operator on a Jacobi algebroid which is compatible with it. We study modular
classes of Jacobi and Jacobi-Nijenhuis algebroids.
| math.DG math.SG | jacobinijenhuis algebroids are defined as a natural generalization of poissonnijenhuis algebroids in the case where there exists a nijenhuis operator on a jacobi algebroid which is compatible with it we study modular classes of jacobi and jacobinijenhuis algebroids | [['jacobinijenhuis', 'algebroids', 'are', 'defined', 'as', 'a', 'natural', 'generalization', 'of', 'poissonnijenhuis', 'algebroids', 'in', 'the', 'case', 'where', 'there', 'exists', 'a', 'nijenhuis', 'operator', 'on', 'a', 'jacobi', 'algebroid', 'which', 'is', 'compatible', 'with', 'it', 'we', 'study', 'modular', 'clas... | [-0.25138419871463585, -0.007228440004645994, -0.024975225108822708, 0.16173826708568653, -0.21788572675646528, -0.15773689292224222, -0.08712789930991437, 0.4018084932314722, -0.3678422594737065, -0.2040120306498322, 0.05404564590916332, -0.22626151999850808, -0.29428962108336, 0.1930059799434323, -0.17896586918811264... |
706.1476 | Entanglement signatures of the quantum phase transition induced by a
magnetic impurity in a superconductor | The insertion of a magnetic impurity in a superconductor induces a first
order quantum phase transition as the coupling to the electronic spin density
increases. As the transition is crossed, a discontinuity is exhibited by
various quantities, like the total spin density, the total gap function and the
gap function a... | cond-mat.supr-con | the insertion of a magnetic impurity in a superconductor induces a first order quantum phase transition as the coupling to the electronic spin density increases as the transition is crossed a discontinuity is exhibited by various quantities like the total spin density the total gap function and the gap function at the ... | [['the', 'insertion', 'of', 'a', 'magnetic', 'impurity', 'in', 'a', 'superconductor', 'induces', 'a', 'first', 'order', 'quantum', 'phase', 'transition', 'as', 'the', 'coupling', 'to', 'the', 'electronic', 'spin', 'density', 'increases', 'as', 'the', 'transition', 'is', 'crossed', 'a', 'discontinuity', 'is', 'exhibited... | [-0.15821809938549997, 0.19568109224922955, -0.0690201121866703, 0.0697921783644706, 0.021153566159307958, -0.10955143510177731, 0.06611011150479316, 0.34669778461568057, -0.26468688348680736, -0.2856388084664941, 0.05752356316521764, -0.3663228814303875, -0.12229170925542712, 0.1001741535961628, 0.023939004123210907, ... |
706.1477 | VPSPACE and a transfer theorem over the complex field | We extend the transfer theorem of [KP2007] to the complex field. That is, we
investigate the links between the class VPSPACE of families of polynomials and
the Blum-Shub-Smale model of computation over C. Roughly speaking, a family of
polynomials is in VPSPACE if its coefficients can be computed in polynomial
space. ... | cs.CC | we extend the transfer theorem of kp2007 to the complex field that is we investigate the links between the class vpspace of families of polynomials and the blumshubsmale model of computation over c roughly speaking a family of polynomials is in vpspace if its coefficients can be computed in polynomial space our main re... | [['we', 'extend', 'the', 'transfer', 'theorem', 'of', 'kp2007', 'to', 'the', 'complex', 'field', 'that', 'is', 'we', 'investigate', 'the', 'links', 'between', 'the', 'class', 'vpspace', 'of', 'families', 'of', 'polynomials', 'and', 'the', 'blumshubsmale', 'model', 'of', 'computation', 'over', 'c', 'roughly', 'speaking'... | [-0.12419034654720679, 0.1102692426158851, -0.08882118856236965, 0.05438423047073092, -0.06373001404200532, -0.13945938299699617, -0.016483660693429096, 0.3648743729161866, -0.34149463690754744, -0.2773945769432056, 0.10223618803248435, -0.2158038463255688, -0.138537983772024, 0.2502953480232601, -0.07081502755422012, ... |
706.1478 | Coherent population transfer in a chain of tunnel coupled quantum dots | We consider the dynamics of a single electron in a chain of tunnel coupled
quantum dots, exploring the formal analogies of this system with some of the
laser-driven multilevel atomic or molecular systems studied by Bruce W. Shore
and collaborators over the last 30 years. In particular, we describe two
regimes for ach... | quant-ph | we consider the dynamics of a single electron in a chain of tunnel coupled quantum dots exploring the formal analogies of this system with some of the laserdriven multilevel atomic or molecular systems studied by bruce w shore and collaborators over the last 30 years in particular we describe two regimes for achieving ... | [['we', 'consider', 'the', 'dynamics', 'of', 'a', 'single', 'electron', 'in', 'a', 'chain', 'of', 'tunnel', 'coupled', 'quantum', 'dots', 'exploring', 'the', 'formal', 'analogies', 'of', 'this', 'system', 'with', 'some', 'of', 'the', 'laserdriven', 'multilevel', 'atomic', 'or', 'molecular', 'systems', 'studied', 'by', ... | [-0.14412685456778193, 0.1685956803139948, -0.05836108275391954, 0.017310147939897175, 0.05622448732726382, -0.15125472699655285, 0.06722955116325104, 0.364166334377113, -0.28707330420296245, -0.27772025456850197, 0.053874113799257745, -0.2341484608036195, -0.08452451894561766, 0.21860734460188458, -0.00757556969398163... |
706.1479 | SU(N) gauge theories in the presence of a topological term | We review recent results on the theta dependence of the ground-state energy
and spectrum of four-dimensional SU(N) gauge theories, where theta is the
coefficient of the CP-violating topological term F-Fdual in the Lagrangian. In
particular, we discuss the results obtained by Monte Carlo simulations of the
lattice for... | hep-th hep-lat | we review recent results on the theta dependence of the groundstate energy and spectrum of fourdimensional sun gauge theories where theta is the coefficient of the cpviolating topological term ffdual in the lagrangian in particular we discuss the results obtained by monte carlo simulations of the lattice formulation of... | [['we', 'review', 'recent', 'results', 'on', 'the', 'theta', 'dependence', 'of', 'the', 'groundstate', 'energy', 'and', 'spectrum', 'of', 'fourdimensional', 'sun', 'gauge', 'theories', 'where', 'theta', 'is', 'the', 'coefficient', 'of', 'the', 'cpviolating', 'topological', 'term', 'ffdual', 'in', 'the', 'lagrangian', '... | [-0.1558507213510735, 0.19227832468206305, -0.08869747824048871, 0.060262293571292466, -0.022510506556895765, -0.08721307213620647, 0.0476844940415543, 0.30824253582598077, -0.19066796787892995, -0.2991057613702572, 0.06148385657149408, -0.3009699601173887, -0.1284719926897315, 0.1502022162211411, 0.06324607283686814, ... |
706.148 | Some necessary and sufficient conditions for parastrophic invariance of
the associative law in quasigroups | Every quasigroup $(S,\cdot)$ belongs to a set of 6 quasigroups, called
parastrophes denoted by $(S,\pi_i)$, $i\in \{1,2,3,4,5,6\}$. It is shown that
isotopy-isomorphy is a necessary and sufficient condition for any two distinct
quasigroups $(S,\pi_i)$ and $(S,\pi_j)$, $i,j\in \{1,2,3,4,5,6\}$ to be
parastrophic invar... | math.GM | every quasigroup scdot belongs to a set of 6 quasigroups called parastrophes denoted by spi_i iin 123456 it is shown that isotopyisomorphy is a necessary and sufficient condition for any two distinct quasigroups spi_i and spi_j ijin 123456 to be parastrophic invariant relative to the associative law in addition a neces... | [['every', 'quasigroup', 'scdot', 'belongs', 'to', 'a', 'set', 'of', '6', 'quasigroups', 'called', 'parastrophes', 'denoted', 'by', 'spi_i', 'iin', '123456', 'it', 'is', 'shown', 'that', 'isotopyisomorphy', 'is', 'a', 'necessary', 'and', 'sufficient', 'condition', 'for', 'any', 'two', 'distinct', 'quasigroups', 'spi_i'... | [-0.16046925332551126, 0.16318086183914063, -0.02453702057206656, 0.05528991500614211, -0.0781725841826933, -0.23449857099676283, -0.003617439541365888, 0.3568389131608656, -0.28234625033150285, -0.16297733563519382, 0.12031158038426853, -0.2818286419861903, -0.07371012135053653, 0.11507419612992681, -0.117484833887320... |
706.1481 | Weak Inverse Property Loops and Some Isotopy-Isomorphy Properties | Two distinct isotopy-isomorphy conditions, different from those of J. M.
Osborn and Wilson's condition, for a weak inverse property loop(WIPL) are
shown. Only one of them characterizes isotopy-isomorphy in WIPLs while the
other is just a sufficient condition for isotopy-isomorphy. Under the
sufficient condition calle... | math.GR | two distinct isotopyisomorphy conditions different from those of j m osborn and wilsons condition for a weak inverse property loopwipl are shown only one of them characterizes isotopyisomorphy in wipls while the other is just a sufficient condition for isotopyisomorphy under the sufficient condition called the cal t co... | [['two', 'distinct', 'isotopyisomorphy', 'conditions', 'different', 'from', 'those', 'of', 'j', 'm', 'osborn', 'and', 'wilsons', 'condition', 'for', 'a', 'weak', 'inverse', 'property', 'loopwipl', 'are', 'shown', 'only', 'one', 'of', 'them', 'characterizes', 'isotopyisomorphy', 'in', 'wipls', 'while', 'the', 'other', '... | [-0.1739395197736649, 0.17454708395067786, -0.0628536973305077, 0.11068672914397673, -0.07480061446224935, -0.24811548267903386, -0.040338773952155814, 0.35760827026650555, -0.24952375033839805, -0.23477406260847558, 0.1125446622332436, -0.22616577759140827, -0.1113398359080807, 0.18633881925422027, -0.0683727211731135... |
706.1482 | On a Pair of Universal Weak Inverse Property Loops | A new condition called ${\cal T}$ condition is introduced for the first time
and used to study a pair of isotopic loops. Under this condition, a loop in the
pair is a WIPL if and only if the other loop is a WIPL. Furthermore, such WIPLs
are isomorphic. The translation elements $f$ and $g$ of a CIPL with the ${\cal
T}... | math.GM | a new condition called cal t condition is introduced for the first time and used to study a pair of isotopic loops under this condition a loop in the pair is a wipl if and only if the other loop is a wipl furthermore such wipls are isomorphic the translation elements f and g of a cipl with the cal t conditionsuch that ... | [['a', 'new', 'condition', 'called', 'cal', 't', 'condition', 'is', 'introduced', 'for', 'the', 'first', 'time', 'and', 'used', 'to', 'study', 'a', 'pair', 'of', 'isotopic', 'loops', 'under', 'this', 'condition', 'a', 'loop', 'in', 'the', 'pair', 'is', 'a', 'wipl', 'if', 'and', 'only', 'if', 'the', 'other', 'loop', 'is... | [-0.1660454015109942, 0.1991600442616883, -0.07885472779585556, 0.059616486927155744, -0.08619946065909144, -0.18503093200058424, -0.008642908175137232, 0.38034693324430424, -0.2653911402618343, -0.21546100875870747, 0.1023803299494003, -0.23620618974620647, -0.11939846683632244, 0.14827515281398188, -0.065008258900012... |
706.1483 | Unitary Representations of Wavelet Groups and Encoding of Iterated
Function Systems in Solenoids | For points in $d$ real dimensions, we introduce a geometry for general digit
sets. We introduce a positional number system where the basis for our
representation is a fixed $d$ by $d$ matrix over $\bz$. Our starting point is a
given pair $(A, \mathcal D)$ with the matrix $A$ assumed expansive, and
$\mathcal D$ a chos... | math.NT math.FA | for points in d real dimensions we introduce a geometry for general digit sets we introduce a positional number system where the basis for our representation is a fixed d by d matrix over bz our starting point is a given pair a mathcal d with the matrix a assumed expansive and mathcal d a chosen complete digit set ie i... | [['for', 'points', 'in', 'd', 'real', 'dimensions', 'we', 'introduce', 'a', 'geometry', 'for', 'general', 'digit', 'sets', 'we', 'introduce', 'a', 'positional', 'number', 'system', 'where', 'the', 'basis', 'for', 'our', 'representation', 'is', 'a', 'fixed', 'd', 'by', 'd', 'matrix', 'over', 'bz', 'our', 'starting', 'po... | [-0.15782052904633204, 0.0789736409519765, -0.08595387470400469, 0.03869444088636418, -0.016491368514099956, -0.10653568536273646, 0.06152357730774604, 0.3551901975814771, -0.28120571690978424, -0.2032251053376857, 0.09873344831526129, -0.2779675124993905, -0.1629919744839873, 0.19600421817346494, -0.08776487485466541,... |
706.1484 | Frames of subspaces and operators | We study the relationship between operators, orthonormal basis of subspaces
and frames of subspaces (also called fusion frames) for a separable Hilbert
space $\mathcal{H}$. We get sufficient conditions on an orthonormal basis of
subspaces $\mathcal{E} = \{E_i \}_{i\in I}$ of a Hilbert space $\mathcal{K}$
and a surjec... | math.FA math.OA | we study the relationship between operators orthonormal basis of subspaces and frames of subspaces also called fusion frames for a separable hilbert space mathcalh we get sufficient conditions on an orthonormal basis of subspaces mathcale e_i _iin i of a hilbert space mathcalk and a surjective tin lmathcalk mathcalh in... | [['we', 'study', 'the', 'relationship', 'between', 'operators', 'orthonormal', 'basis', 'of', 'subspaces', 'and', 'frames', 'of', 'subspaces', 'also', 'called', 'fusion', 'frames', 'for', 'a', 'separable', 'hilbert', 'space', 'mathcalh', 'we', 'get', 'sufficient', 'conditions', 'on', 'an', 'orthonormal', 'basis', 'of',... | [-0.14209226920380147, 0.09891500338593293, -0.03624278998858836, 0.022418963633334406, -0.043027912188399506, -0.09438115921053854, 0.03153343445953581, 0.40386029347204244, -0.308326150587812, -0.18065655045089202, 0.08257158576930919, -0.26628862915013535, -0.1250806220781084, 0.16603207167960912, -0.143088689834893... |
706.1485 | Bootstrapping confidence intervals for the change-point of time series | We study an AMOC time series model with an abrupt change in the mean and
dependent errors that fulfill certain mixing conditions. We obtain confidence
intervals for the unknown change-point via bootstrapping methods.
Precisely we use a block bootstrap of the estimated centered error sequence.
Then we reconstruct a ... | math.ST stat.TH | we study an amoc time series model with an abrupt change in the mean and dependent errors that fulfill certain mixing conditions we obtain confidence intervals for the unknown changepoint via bootstrapping methods precisely we use a block bootstrap of the estimated centered error sequence then we reconstruct a sequence... | [['we', 'study', 'an', 'amoc', 'time', 'series', 'model', 'with', 'an', 'abrupt', 'change', 'in', 'the', 'mean', 'and', 'dependent', 'errors', 'that', 'fulfill', 'certain', 'mixing', 'conditions', 'we', 'obtain', 'confidence', 'intervals', 'for', 'the', 'unknown', 'changepoint', 'via', 'bootstrapping', 'methods', 'prec... | [-0.05315769061337422, 0.03281004617386243, -0.15243034495081562, 0.12935736971434858, -0.014337887032378982, -0.09547406492965554, 0.10478922442267954, 0.4239925510474365, -0.27249124892273524, -0.30860536244364767, 0.1502044601586858, -0.2499602696973912, -0.0991076784493932, 0.17342401902109766, -0.07031786403734319... |
706.1486 | A Minimization Method for Relativistic Electrons in a Mean-Field
Approximation of Quantum Electrodynamics | We study a mean-field relativistic model which is able to describe both the
behavior of finitely many spin-1/2 particles like electrons and of the Dirac
sea which is self-consistently polarized in the presence of the real particles.
The model is derived from the QED Hamiltonian in Coulomb gauge neglecting the
photon ... | physics.atom-ph math-ph math.MP | we study a meanfield relativistic model which is able to describe both the behavior of finitely many spin12 particles like electrons and of the dirac sea which is selfconsistently polarized in the presence of the real particles the model is derived from the qed hamiltonian in coulomb gauge neglecting the photon field a... | [['we', 'study', 'a', 'meanfield', 'relativistic', 'model', 'which', 'is', 'able', 'to', 'describe', 'both', 'the', 'behavior', 'of', 'finitely', 'many', 'spin12', 'particles', 'like', 'electrons', 'and', 'of', 'the', 'dirac', 'sea', 'which', 'is', 'selfconsistently', 'polarized', 'in', 'the', 'presence', 'of', 'the', ... | [-0.09801376393685739, 0.23979672568384558, -0.08963315805109838, 0.1144872184668202, -0.016021340860364337, -0.11594603389967233, -0.04253764171929409, 0.3167362023455401, -0.1983852700330317, -0.28703427921670177, -0.0382991298683919, -0.33263575018694, -0.12390817869454622, 0.15991067527017247, 0.04766001566313207, ... |
706.1487 | Semiclassical theory of the Ehrenfest-time dependence of quantum
transport | In ballistic conductors, there is a low-time threshold for the appearance of
quantum effects in transport coefficients. This low-time threshold is the
Ehrenfest time. Most previous studies of the Ehrenfest-time dependence of
quantum transport assumed ergodic electron dynamics, so that they could be
applied to ballist... | cond-mat.mes-hall | in ballistic conductors there is a lowtime threshold for the appearance of quantum effects in transport coefficients this lowtime threshold is the ehrenfest time most previous studies of the ehrenfesttime dependence of quantum transport assumed ergodic electron dynamics so that they could be applied to ballistic quantu... | [['in', 'ballistic', 'conductors', 'there', 'is', 'a', 'lowtime', 'threshold', 'for', 'the', 'appearance', 'of', 'quantum', 'effects', 'in', 'transport', 'coefficients', 'this', 'lowtime', 'threshold', 'is', 'the', 'ehrenfest', 'time', 'most', 'previous', 'studies', 'of', 'the', 'ehrenfesttime', 'dependence', 'of', 'qu... | [-0.19781522882631283, 0.18407798809502487, -0.11765369271493575, 0.06101007152605673, 0.02509578075474021, -0.1730803157545455, 0.03016886063289411, 0.32331479608413133, -0.2891372532340238, -0.21480232983527855, 0.00023372840783933457, -0.3160439378143042, -0.16106864694912715, 0.22065477881810747, -0.034672148300912... |
706.1488 | Dynamical matrix of two-dimensional electron crystals | In a quantizing magnetic field, the two-dimensional electron (2DEG) gas has a
rich phase diagram with broken translational symmetry phases such as Wigner,
bubble, and stripe crystals. In this paper, we derive a method to get the
dynamical matrix of these crystals from a calculation of the density response
function pe... | cond-mat.mes-hall | in a quantizing magnetic field the twodimensional electron 2deg gas has a rich phase diagram with broken translational symmetry phases such as wigner bubble and stripe crystals in this paper we derive a method to get the dynamical matrix of these crystals from a calculation of the density response function performed in... | [['in', 'a', 'quantizing', 'magnetic', 'field', 'the', 'twodimensional', 'electron', '2deg', 'gas', 'has', 'a', 'rich', 'phase', 'diagram', 'with', 'broken', 'translational', 'symmetry', 'phases', 'such', 'as', 'wigner', 'bubble', 'and', 'stripe', 'crystals', 'in', 'this', 'paper', 'we', 'derive', 'a', 'method', 'to', ... | [-0.09182015105216124, 0.15690211521966071, -0.12829266588475244, -0.0022936161318890904, 0.009596422417719927, -0.07247349517759478, 0.07603145157190738, 0.3386121913887716, -0.2646869658801734, -0.25353693205397576, 0.05288707844374585, -0.26212734015037614, -0.1779292686454331, 0.12392835526892061, 0.058661047228573... |
706.1489 | New Asymptotic Profiles of Nonstationnary Solutions of the Navier-Stokes
System | We show that solutions $u(x,t)$ of the non-stationnary incompressible
Navier--Stokes system in $\R^d$ ($d\geq2$) starting from mild decaying data $a$
behave as $|x|\to\infty$ as a potential field: u(x,t) = e^{t\Delta}a(x) +
\gamma_d\nabla_x(\sum_{h,k} \frac{\delta_{h,k}|x|^2 - d x_h x_k}{d|x|^{d+2}}
K_{h,k}(t))+\math... | math.AP math-ph math.MP | we show that solutions uxt of the nonstationnary incompressible navierstokes system in rd dgeq2 starting from mild decaying data a behave as xtoinfty as a potential field uxt etdeltaax gamma_dnabla_xsum_hk fracdelta_hkx2 d x_h x_kdxd2 k_hktmathfrakofrac1xd1 where gamma_d is a constant and k_hkint_0tu_h u_k_l2 is the en... | [['we', 'show', 'that', 'solutions', 'uxt', 'of', 'the', 'nonstationnary', 'incompressible', 'navierstokes', 'system', 'in', 'rd', 'dgeq2', 'starting', 'from', 'mild', 'decaying', 'data', 'a', 'behave', 'as', 'xtoinfty', 'as', 'a', 'potential', 'field', 'uxt', 'etdeltaax', 'gamma_dnabla_xsum_hk', 'fracdelta_hkx2', 'd',... | [-0.15333064840416666, 0.15396748534489976, -0.05123208847578132, 0.04209558554511103, -0.011293788095591244, -0.18375829124340304, 0.03366982387120111, 0.27119071044338244, -0.26749431576441834, -0.2253128281035633, 0.12292103688944028, -0.3110265083335064, -0.043383485835942405, 0.20323202735744417, -0.00991839659400... |
706.149 | Radiative Fermion Mass Hierarchy in a Non-supersymmetric Unified Theory | In non-supersymmetric grand unified models a ``radiative fermion mass
hierarchy" can be achieved in which the spectrum of quark and lepton masses is
determined entirely by physics at the unification scale, with many relations
following from the unified gauge symmetry, and with the masses of the lightest
family arisin... | hep-ph | in nonsupersymmetric grand unified models a radiative fermion mass hierarchy can be achieved in which the spectrum of quark and lepton masses is determined entirely by physics at the unification scale with many relations following from the unified gauge symmetry and with the masses of the lightest family arising from l... | [['in', 'nonsupersymmetric', 'grand', 'unified', 'models', 'a', 'radiative', 'fermion', 'mass', 'hierarchy', 'can', 'be', 'achieved', 'in', 'which', 'the', 'spectrum', 'of', 'quark', 'and', 'lepton', 'masses', 'is', 'determined', 'entirely', 'by', 'physics', 'at', 'the', 'unification', 'scale', 'with', 'many', 'relatio... | [-0.0669689178696753, 0.23571296598486327, -0.02813367063846485, 0.18970722646055813, -0.05639639601433351, -0.12909545010979068, 0.04271836852493845, 0.2968559644018288, -0.24147603058336695, -0.36699163794149586, 0.04144693304799687, -0.19737849471929633, -0.06832056976121816, 0.13576830823238892, 0.0245086940948242,... |
706.1491 | Weather induced effects on extensive air showers observed with the
surface detector of the Pierre Auger Observatory | The rate of events measured with the surface detector of the Pierre Auger
Observatory is found to be modulated by the weather conditions. This effect is
due to the increasing amount of matter traversed by the shower as the ground
pressure increases and to the inverse proportionality of the Moliere radius to
the air d... | astro-ph | the rate of events measured with the surface detector of the pierre auger observatory is found to be modulated by the weather conditions this effect is due to the increasing amount of matter traversed by the shower as the ground pressure increases and to the inverse proportionality of the moliere radius to the air dens... | [['the', 'rate', 'of', 'events', 'measured', 'with', 'the', 'surface', 'detector', 'of', 'the', 'pierre', 'auger', 'observatory', 'is', 'found', 'to', 'be', 'modulated', 'by', 'the', 'weather', 'conditions', 'this', 'effect', 'is', 'due', 'to', 'the', 'increasing', 'amount', 'of', 'matter', 'traversed', 'by', 'the', 's... | [-0.10135951929100573, 0.22951455768963244, -0.059995581714870176, 0.08658120708463535, -0.016252133239392345, 0.016659794298753347, -0.0050967040516385065, 0.3387668917644514, -0.24699937673413183, -0.41974942901567236, 0.07300398536409212, -0.3250386116337286, -0.07375295854441516, 0.17784888740335528, 0.013875010691... |
706.1492 | How do trehalose, maltose and sucrose influence some structural and
dynamical properties of lysozyme ? An insight from Molecular Dynamics
simulations | The influence of three well-known disaccharides, namely trehalose, maltose
and sucrose, on some structural and dynamical properties of lysozyme has been
investigated by means of molecular dynamics computer simulations in the 37-60
wt % concentration range. The effects of sugars on the protein conformation are
found r... | physics.chem-ph cond-mat.soft q-bio.BM | the influence of three wellknown disaccharides namely trehalose maltose and sucrose on some structural and dynamical properties of lysozyme has been investigated by means of molecular dynamics computer simulations in the 3760 wt concentration range the effects of sugars on the protein conformation are found relatively ... | [['the', 'influence', 'of', 'three', 'wellknown', 'disaccharides', 'namely', 'trehalose', 'maltose', 'and', 'sucrose', 'on', 'some', 'structural', 'and', 'dynamical', 'properties', 'of', 'lysozyme', 'has', 'been', 'investigated', 'by', 'means', 'of', 'molecular', 'dynamics', 'computer', 'simulations', 'in', 'the', '376... | [-0.07941817432783117, 0.16129479357615523, -0.041317112641791776, 0.042772693527632785, 0.04781042438395934, -0.0795518888961141, 0.03409833501392899, 0.3815986218109523, -0.26494309849628844, -0.28493740204211376, 0.050288367353870905, -0.2833510165498273, -0.16858997959516023, 0.12735073256931484, 0.0096384851143963... |
706.1493 | Dynamical Screening of Atom Confined by Finite-Width Fullerene | This is an investigation on the dynamical screening of an atom confined
within a fullerene of finite width. The two surfaces of the fullerene lead to
the presence of two surface plasmon eigenmodes. It is shown that, in the
vicinity of these two eigenfrequencies, there is a large enhancement of the
confined atom's pho... | physics.atm-clus | this is an investigation on the dynamical screening of an atom confined within a fullerene of finite width the two surfaces of the fullerene lead to the presence of two surface plasmon eigenmodes it is shown that in the vicinity of these two eigenfrequencies there is a large enhancement of the confined atoms photoabsor... | [['this', 'is', 'an', 'investigation', 'on', 'the', 'dynamical', 'screening', 'of', 'an', 'atom', 'confined', 'within', 'a', 'fullerene', 'of', 'finite', 'width', 'the', 'two', 'surfaces', 'of', 'the', 'fullerene', 'lead', 'to', 'the', 'presence', 'of', 'two', 'surface', 'plasmon', 'eigenmodes', 'it', 'is', 'shown', 't... | [-0.1651102973973717, 0.17883264035124077, -0.03731468506157398, 0.004921707396649501, 0.045458022759042004, -0.06458111997397448, 0.0027627990750426594, 0.3867789399894801, -0.20962187702852217, -0.23678687335923315, -0.0058650830527767536, -0.3123600441962481, -0.1254294809292663, 0.1790286547927694, 0.02341352031904... |
706.1494 | Fluctuations of finite-time stability exponents in the standard map and
the detection of small islands | Some statistical properties of finite-time stability exponents in the
standard map can be estimated analytically. The mean exponent averaged over the
entire phase space behaves quite differently from all the other cumulants.
Whereas the mean carries information about the strength of the interaction, and
only indirect... | nlin.CD | some statistical properties of finitetime stability exponents in the standard map can be estimated analytically the mean exponent averaged over the entire phase space behaves quite differently from all the other cumulants whereas the mean carries information about the strength of the interaction and only indirect infor... | [['some', 'statistical', 'properties', 'of', 'finitetime', 'stability', 'exponents', 'in', 'the', 'standard', 'map', 'can', 'be', 'estimated', 'analytically', 'the', 'mean', 'exponent', 'averaged', 'over', 'the', 'entire', 'phase', 'space', 'behaves', 'quite', 'differently', 'from', 'all', 'the', 'other', 'cumulants', ... | [-0.14744617270337454, 0.15670883218678813, -0.09911637970591462, 0.11657917015431199, -0.019678259732505206, -0.09614656970734359, 0.038681782004070034, 0.29790285211856826, -0.2914651774086191, -0.3120439988519398, 0.10329191489914333, -0.3026133984162698, -0.1343054003134187, 0.17585625288588094, 0.01721704276029153... |
706.1495 | Study of the Cosmic Ray Composition above 0.4 EeV using the Longitudinal
Profiles of Showers observed at the Pierre Auger Observatory | The Pierre Auger Observatory has been collecting data in a stable manner
since January 2004. We present here a study of the cosmic ray composition using
events recorded in hybrid mode during the first years of data taking. These are
air showers observed by the fluorescence detector as well as the surface
detector, so... | astro-ph | the pierre auger observatory has been collecting data in a stable manner since january 2004 we present here a study of the cosmic ray composition using events recorded in hybrid mode during the first years of data taking these are air showers observed by the fluorescence detector as well as the surface detector so the ... | [['the', 'pierre', 'auger', 'observatory', 'has', 'been', 'collecting', 'data', 'in', 'a', 'stable', 'manner', 'since', 'january', '2004', 'we', 'present', 'here', 'a', 'study', 'of', 'the', 'cosmic', 'ray', 'composition', 'using', 'events', 'recorded', 'in', 'hybrid', 'mode', 'during', 'the', 'first', 'years', 'of', '... | [-0.0382474086847957, 0.2170352610263312, -0.08358701561342612, 0.09291020117914435, 0.011768444989607713, 0.023024211855274493, -0.04615151004378344, 0.4287988690433101, -0.2239617805418811, -0.43421564731642465, 0.057992596536108824, -0.3446476441458799, -0.03996033456925059, 0.19772734714750306, 0.006148783163663661... |
706.1496 | Time-Delayed Feedback control of a flashing ratchet | Closed-loop or feedback control ratchets use information about the state of
the system to operate with the aim of maximizing the performance of the system.
In this paper we investigate the effects of a time delay in the feedback for a
protocol that performs an instantaneous maximization of the center-of-mass
velocity... | cond-mat.stat-mech | closedloop or feedback control ratchets use information about the state of the system to operate with the aim of maximizing the performance of the system in this paper we investigate the effects of a time delay in the feedback for a protocol that performs an instantaneous maximization of the centerofmass velocity for t... | [['closedloop', 'or', 'feedback', 'control', 'ratchets', 'use', 'information', 'about', 'the', 'state', 'of', 'the', 'system', 'to', 'operate', 'with', 'the', 'aim', 'of', 'maximizing', 'the', 'performance', 'of', 'the', 'system', 'in', 'this', 'paper', 'we', 'investigate', 'the', 'effects', 'of', 'a', 'time', 'delay',... | [-0.18291839918398684, 0.08783768214743759, -0.059266132020576186, 0.03165776175115627, -0.03454408404248734, -0.16231064291135006, 0.07168555126278581, 0.354963773556439, -0.26252079501563425, -0.3028979120888458, 0.1155629747648571, -0.25465205600655816, -0.1366801833330477, 0.23755638190777972, -0.07205933323182856,... |
706.1497 | Power-free values, repulsion between points, differing beliefs and the
existence of error | Let f be a cubic polynomial. Then there are infinitely many primes p such
that f(p) is square-free.
| math.NT math.PR | let f be a cubic polynomial then there are infinitely many primes p such that fp is squarefree | [['let', 'f', 'be', 'a', 'cubic', 'polynomial', 'then', 'there', 'are', 'infinitely', 'many', 'primes', 'p', 'such', 'that', 'fp', 'is', 'squarefree']] | [-0.2686448151038753, 0.18163923859699732, -0.1582235793272654, 0.04884083070404207, -0.05959905218333006, -0.2597202337605672, -0.14493997560607064, 0.3130124256842666, -0.4285893850028515, -0.17185898903860813, 0.004092705849972036, -0.3396437917318609, -0.15301226410600874, 0.256827833958798, -0.05579724920810097, 0... |
706.1498 | On the derived category of 1-motives, I | We consider the category of Deligne 1-motives over a perfect field k of
exponential characteristic p and its derived category for a suitable exact
structure after inverting p. As a first result, we provide a fully faithful
embedding into an etale version of Voevodsky's triangulated category of
geometric motives. Our ... | math.AG | we consider the category of deligne 1motives over a perfect field k of exponential characteristic p and its derived category for a suitable exact structure after inverting p as a first result we provide a fully faithful embedding into an etale version of voevodskys triangulated category of geometric motives our second ... | [['we', 'consider', 'the', 'category', 'of', 'deligne', '1motives', 'over', 'a', 'perfect', 'field', 'k', 'of', 'exponential', 'characteristic', 'p', 'and', 'its', 'derived', 'category', 'for', 'a', 'suitable', 'exact', 'structure', 'after', 'inverting', 'p', 'as', 'a', 'first', 'result', 'we', 'provide', 'a', 'fully',... | [-0.1616666518702577, -3.9344737295458025e-05, -0.1593853673138828, 0.09263525353485925, -0.09800729296963524, -0.14194122077552257, -0.0015127076163750004, 0.3400447058994797, -0.3790625240481286, -0.1722460871786569, 0.08351701450926528, -0.1419933155110037, -0.13790707073941896, 0.2101158174789614, -0.19514556135982... |
706.1499 | Elementary Maps on Triangular Algebras | In this note we prove that elementary maps on triangular algebras are
automically additive.
| math.RA math.OA | in this note we prove that elementary maps on triangular algebras are automically additive | [['in', 'this', 'note', 'we', 'prove', 'that', 'elementary', 'maps', 'on', 'triangular', 'algebras', 'are', 'automically', 'additive']] | [-0.168238484658874, 0.1391348120254966, -0.07910269427184875, 0.14742975734854832, -0.03485954839449663, -0.09956699667068628, -0.0758329862012313, 0.48740796974072087, -0.3769831250493343, -0.12355043610128072, 0.14596352653685385, -0.2959967957666287, -0.25693623263550064, 0.17636670329822943, -0.22552614716383126, ... |
706.15 | X-ray Flares in Orion Low Mass Stars | Context. X-ray flares are common phenomena in pre-main sequence stars. Their
analysis gives insights into the physics at work in young stellar coronae. The
Orion Nebula Cluster offers a unique opportunity to study large samples of
young low mass stars. This work is part of the Chandra Orion Ultradeep project
(COUP), ... | astro-ph | context xray flares are common phenomena in premain sequence stars their analysis gives insights into the physics at work in young stellar coronae the orion nebula cluster offers a unique opportunity to study large samples of young low mass stars this work is part of the chandra orion ultradeep project coup an 10 day l... | [['context', 'xray', 'flares', 'are', 'common', 'phenomena', 'in', 'premain', 'sequence', 'stars', 'their', 'analysis', 'gives', 'insights', 'into', 'the', 'physics', 'at', 'work', 'in', 'young', 'stellar', 'coronae', 'the', 'orion', 'nebula', 'cluster', 'offers', 'a', 'unique', 'opportunity', 'to', 'study', 'large', '... | [-0.06520161171982332, 0.15068842575585858, -0.10304470065776516, 0.14148917143953366, -0.08346641977288628, -0.07792003452294477, 0.07254226388736824, 0.42721593022269155, -0.17750442377775005, -0.38834761551043157, 0.03987073030255922, -0.2853482908224461, -0.03732465818837755, 0.21456697478384476, -0.052780204906956... |
706.1501 | Longitudinal Shower Profile Reconstruction from Fluorescence and
Cherenkov Light | Traditionally, longitudinal shower profiles are reconstructed in fluorescence
light experiments by treating the Cherenkov light contribution as background.
Here we will argue that, due to universality of the energy spectra of electrons
and positrons, both fluorescence and Cherenkov light can be used simultaneously
as... | astro-ph | traditionally longitudinal shower profiles are reconstructed in fluorescence light experiments by treating the cherenkov light contribution as background here we will argue that due to universality of the energy spectra of electrons and positrons both fluorescence and cherenkov light can be used simultaneously as signa... | [['traditionally', 'longitudinal', 'shower', 'profiles', 'are', 'reconstructed', 'in', 'fluorescence', 'light', 'experiments', 'by', 'treating', 'the', 'cherenkov', 'light', 'contribution', 'as', 'background', 'here', 'we', 'will', 'argue', 'that', 'due', 'to', 'universality', 'of', 'the', 'energy', 'spectra', 'of', 'e... | [-0.011010846970707512, 0.15612884991268597, -0.14874734743786033, 0.11529909573453531, -0.05498724469517389, -0.07210887785414967, -0.04552666855756235, 0.4181568164671405, -0.23715001818713513, -0.36997507554426623, 0.08009262725035922, -0.3268918731469619, -0.09531010080421909, 0.19775315914093777, 0.006253420286340... |
706.1502 | Additivity of Maps on Triangular Algebras | We prove that every multiplicative bijective map, Jordan bijective map, and
Jordan triple bijective map from a triangular algebra onto any ring is
automatically additive.
| math.RA math.OA | we prove that every multiplicative bijective map jordan bijective map and jordan triple bijective map from a triangular algebra onto any ring is automatically additive | [['we', 'prove', 'that', 'every', 'multiplicative', 'bijective', 'map', 'jordan', 'bijective', 'map', 'and', 'jordan', 'triple', 'bijective', 'map', 'from', 'a', 'triangular', 'algebra', 'onto', 'any', 'ring', 'is', 'automatically', 'additive']] | [-0.19047368437051773, -0.0332598065212369, -0.06849309861660004, 0.021127574243582786, -0.15347830642014743, -0.2743830101005733, -0.001773516945540905, 0.3982432585954666, -0.5287477373331785, -0.018624974712729454, 0.06825856236740947, -0.229757756665349, -0.28937320291996005, 0.17891889210790396, -0.210340449474751... |
706.1503 | The law of the supremum of a stable L\'{e}vy process with no negative
jumps | Let $X=(X_t)_{t\ge0}$ be a stable L\'{e}vy process of index $\alpha \in(1,2)$
with no negative jumps and let $S_t=\sup_{0\le s\le t}X_s$ denote its running
supremum for $t>0$. We show that the density function $f_t$ of $S_t$ can be
characterized as the unique solution to a weakly singular Volterra integral
equation o... | math.PR | let xx_t_tge0 be a stable levy process of index alpha in12 with no negative jumps and let s_tsup_0le sle tx_s denote its running supremum for t0 we show that the density function f_t of s_t can be characterized as the unique solution to a weakly singular volterra integral equation of the first kind or equivalently as t... | [['let', 'xx_t_tge0', 'be', 'a', 'stable', 'levy', 'process', 'of', 'index', 'alpha', 'in12', 'with', 'no', 'negative', 'jumps', 'and', 'let', 's_tsup_0le', 'sle', 'tx_s', 'denote', 'its', 'running', 'supremum', 'for', 't0', 'we', 'show', 'that', 'the', 'density', 'function', 'f_t', 'of', 's_t', 'can', 'be', 'character... | [-0.14391074713251187, 0.11901866401884269, -0.13572354722819333, 0.028116086071308135, -0.08258451404340497, -0.14494668626986923, 0.01649608308184516, 0.3174418929041526, -0.3703436807071397, -0.18077895443442218, 0.11362515929381474, -0.30723587386822754, -0.0975290857855692, 0.16982974011852586, -0.0238926335571145... |
706.1504 | Free Energy of Activation for the Comorosan Effect | Initial reaction rate data for lactic dehydrogenase / pyruvate, lactic
dehydrogenase / lactate and malic dehydrogenase / malate enzyme reactions were
analyzed to obtain activation free energy changes of -329, -195 and -221
cal/mole, respectively, for rate increases associated with time-specific
irradiation of the cry... | q-bio.SC q-bio.BM | initial reaction rate data for lactic dehydrogenase pyruvate lactic dehydrogenase lactate and malic dehydrogenase malate enzyme reactions were analyzed to obtain activation free energy changes of 329 195 and 221 calmole respectively for rate increases associated with timespecific irradiation of the crystalline substrat... | [['initial', 'reaction', 'rate', 'data', 'for', 'lactic', 'dehydrogenase', 'pyruvate', 'lactic', 'dehydrogenase', 'lactate', 'and', 'malic', 'dehydrogenase', 'malate', 'enzyme', 'reactions', 'were', 'analyzed', 'to', 'obtain', 'activation', 'free', 'energy', 'changes', 'of', '329', '195', 'and', '221', 'calmole', 'resp... | [-0.05264175699706558, 0.2090655663269478, 0.008617456912355272, 0.020988509210526644, 0.04737493335800683, -0.14444607865977907, 0.09768222050503797, 0.38250399119651957, -0.23933714514148216, -0.33391908673732074, 0.015764942395050805, -0.32627002663610366, -0.04986219720652439, 0.17345916769926706, -0.02393439542752... |
706.1505 | Very High Energy Gamma-ray Radiation from the Stellar-mass Black Hole
Cygnus X-1 | We report on the results from the observations in very high energy band (VHE,
E_gamma > 100 GeV) of the black hole X-ray binary (BHXB) Cygnus X-1. The
observations were performed with the MAGIC telescope, for a total of 40 hours
during 26 nights, spanning the period between June and November 2006. Searches
for steady... | astro-ph | we report on the results from the observations in very high energy band vhe e_gamma 100 gev of the black hole xray binary bhxb cygnus x1 the observations were performed with the magic telescope for a total of 40 hours during 26 nights spanning the period between june and november 2006 searches for steady gammaray signa... | [['we', 'report', 'on', 'the', 'results', 'from', 'the', 'observations', 'in', 'very', 'high', 'energy', 'band', 'vhe', 'e_gamma', '100', 'gev', 'of', 'the', 'black', 'hole', 'xray', 'binary', 'bhxb', 'cygnus', 'x1', 'the', 'observations', 'were', 'performed', 'with', 'the', 'magic', 'telescope', 'for', 'a', 'total', '... | [-0.07514360841379795, 0.12283562806512288, -0.03848961512538004, 0.11336920035950582, -0.05909254483664932, -0.12315922750772916, 0.11104884863835135, 0.4111600103808236, -0.13596104821885707, -0.4425567720988483, 0.09287340676077355, -0.3529810517425629, -0.006580143935123692, 0.2574339433970309, 0.000244157512970087... |
706.1506 | Electronic transport in normal-conductor/graphene/normal-conductor
junctions and conditions for insulating behavior at a finite charge-carrier
density | We investigate the conductance of normal-conductor/graphene/normal-conductor
(NGN) junctions for arbitrary on-site potentials in the normal and graphitic
parts of the system. We find that a ballistic NGN junction can display
insulating behavior even when the charge-carrier density in the graphene part
is finite. This... | cond-mat.mes-hall | we investigate the conductance of normalconductorgraphenenormalconductor ngn junctions for arbitrary onsite potentials in the normal and graphitic parts of the system we find that a ballistic ngn junction can display insulating behavior even when the chargecarrier density in the graphene part is finite this effect orig... | [['we', 'investigate', 'the', 'conductance', 'of', 'normalconductorgraphenenormalconductor', 'ngn', 'junctions', 'for', 'arbitrary', 'onsite', 'potentials', 'in', 'the', 'normal', 'and', 'graphitic', 'parts', 'of', 'the', 'system', 'we', 'find', 'that', 'a', 'ballistic', 'ngn', 'junction', 'can', 'display', 'insulating... | [-0.2390165449561257, 0.15694407130190244, -0.07144472506877624, 0.02166760878539399, 0.014420721155444257, -0.1645003348509291, 0.08018092504261355, 0.39103347478728545, -0.2754026334836932, -0.26190266783692334, -0.001162322023638377, -0.3049389607567144, -0.15761943103647547, 0.15130228454884337, 0.01730669805593175... |
706.1507 | Scaling laws for soliton pulse compression by cascaded quadratic
nonlinearities | We present a detailed study of soliton compression of ultra-short pulses
based on phase-mismatched second-harmonic generation (\textit{i.e.}, the
cascaded quadratic nonlinearity) in bulk quadratic nonlinear media. The
single-cycle propagation equations in the temporal domain including
higher-order nonlinear terms are... | physics.optics | we present a detailed study of soliton compression of ultrashort pulses based on phasemismatched secondharmonic generation textitie the cascaded quadratic nonlinearity in bulk quadratic nonlinear media the singlecycle propagation equations in the temporal domain including higherorder nonlinear terms are presented the b... | [['we', 'present', 'a', 'detailed', 'study', 'of', 'soliton', 'compression', 'of', 'ultrashort', 'pulses', 'based', 'on', 'phasemismatched', 'secondharmonic', 'generation', 'textitie', 'the', 'cascaded', 'quadratic', 'nonlinearity', 'in', 'bulk', 'quadratic', 'nonlinear', 'media', 'the', 'singlecycle', 'propagation', '... | [-0.17275066115442164, 0.15763114106167198, -0.04758295577413105, 0.04704617768449267, -0.08146595252802614, -0.1365668554022217, -0.000291802762580325, 0.4148541731164627, -0.2701726347764896, -0.25517272132631275, 0.0809107010034345, -0.27852636435760436, -0.14475831852088078, 0.2658500300513907, 0.017632362653606945... |
706.1508 | Sequential weak measurement | The notion of weak measurement provides a formalism for extracting
information from a quantum system in the limit of vanishing disturbance to its
state. Here we extend this formalism to the measurement of sequences of
observables. When these observables do not commute, we may obtain information
about joint properties... | quant-ph | the notion of weak measurement provides a formalism for extracting information from a quantum system in the limit of vanishing disturbance to its state here we extend this formalism to the measurement of sequences of observables when these observables do not commute we may obtain information about joint properties of a... | [['the', 'notion', 'of', 'weak', 'measurement', 'provides', 'a', 'formalism', 'for', 'extracting', 'information', 'from', 'a', 'quantum', 'system', 'in', 'the', 'limit', 'of', 'vanishing', 'disturbance', 'to', 'its', 'state', 'here', 'we', 'extend', 'this', 'formalism', 'to', 'the', 'measurement', 'of', 'sequences', 'o... | [-0.15933955562171304, 0.11595960826000723, -0.14971724895265284, 0.08006729008453085, -0.06486902341152294, -0.12661981826671695, 0.07835775994860768, 0.3127002795757372, -0.27502474782964853, -0.27590701864631495, 0.06862900678740366, -0.24986457706818097, -0.10064996281473697, 0.20139573511072212, -0.097574315699557... |
706.1509 | Grassmann Integral Representation for Spanning Hyperforests | Given a hypergraph G, we introduce a Grassmann algebra over the vertex set,
and show that a class of Grassmann integrals permits an expansion in terms of
spanning hyperforests. Special cases provide the generating functions for
rooted and unrooted spanning (hyper)forests and spanning (hyper)trees. All
these results a... | math-ph cond-mat.stat-mech hep-lat math.CO math.MP | given a hypergraph g we introduce a grassmann algebra over the vertex set and show that a class of grassmann integrals permits an expansion in terms of spanning hyperforests special cases provide the generating functions for rooted and unrooted spanning hyperforests and spanning hypertrees all these results are general... | [['given', 'a', 'hypergraph', 'g', 'we', 'introduce', 'a', 'grassmann', 'algebra', 'over', 'the', 'vertex', 'set', 'and', 'show', 'that', 'a', 'class', 'of', 'grassmann', 'integrals', 'permits', 'an', 'expansion', 'in', 'terms', 'of', 'spanning', 'hyperforests', 'special', 'cases', 'provide', 'the', 'generating', 'func... | [-0.17013970653836927, 0.14378440094529651, -0.013690362473328908, 0.06316115453373641, -0.10937661989902457, -0.049853895219663776, 0.04019568102279057, 0.36938397998611133, -0.2591507378779352, -0.2786432865510384, 0.06443299256730825, -0.26727135479139785, -0.22782017948726813, 0.1882104971135656, -0.075218832368652... |
706.151 | Aromatic emission from the ionised mane of the Horsehead nebula | We study the evolution of the Aromatic Infrared Bands (AIBs) emitters across
the illuminated edge of the Horsehead nebula and especially their survival and
properties in the HII region. We present spectral mapping observations taken
with the Infrared Spectrograph (IRS) at wavelengths 5.2-38 microns. A strong
AIB at 1... | astro-ph | we study the evolution of the aromatic infrared bands aibs emitters across the illuminated edge of the horsehead nebula and especially their survival and properties in the hii region we present spectral mapping observations taken with the infrared spectrograph irs at wavelengths 5238 microns a strong aib at 113 microns... | [['we', 'study', 'the', 'evolution', 'of', 'the', 'aromatic', 'infrared', 'bands', 'aibs', 'emitters', 'across', 'the', 'illuminated', 'edge', 'of', 'the', 'horsehead', 'nebula', 'and', 'especially', 'their', 'survival', 'and', 'properties', 'in', 'the', 'hii', 'region', 'we', 'present', 'spectral', 'mapping', 'observa... | [-0.054110295411353065, 0.09660378484273749, -0.019913314172160326, 0.03015780165951931, 0.01792790923205218, -0.08298116902771749, 0.04772921520035767, 0.4685971479346022, -0.17789293709322454, -0.3449793998686748, 0.034578204391140975, -0.29927722060758816, -0.003008116687242494, 0.10966693424356826, -0.0314848475971... |
706.1511 | Pulsar Kicks With Modified URCA and Electrons in Landau Levels | We derive the energy asymmetry given the proto-neutron star during the time
when the neutrino sphere is near the surface of the proto-neutron star, using
the modified URCA process. The electrons produced with the anti-neutrinos are
in Landau levels due to the strong magnetic field, and this leads to asymmetry
in the ... | astro-ph | we derive the energy asymmetry given the protoneutron star during the time when the neutrino sphere is near the surface of the protoneutron star using the modified urca process the electrons produced with the antineutrinos are in landau levels due to the strong magnetic field and this leads to asymmetry in the neutrino... | [['we', 'derive', 'the', 'energy', 'asymmetry', 'given', 'the', 'protoneutron', 'star', 'during', 'the', 'time', 'when', 'the', 'neutrino', 'sphere', 'is', 'near', 'the', 'surface', 'of', 'the', 'protoneutron', 'star', 'using', 'the', 'modified', 'urca', 'process', 'the', 'electrons', 'produced', 'with', 'the', 'antine... | [-0.13373000390601117, 0.24885502985184635, -0.003941260701410372, 0.08812814354753239, -0.06083256793774765, -0.040777334125360123, 0.06225527361321666, 0.3407030802950062, -0.21537259921928667, -0.34428251105536883, 0.03810243314522243, -0.2618939761273764, 0.02874812386250375, 0.20196642427440933, 0.0308965809393132... |
706.1512 | Local stability of ergodic averages | The mean ergodic theorem is equivalent to the assertion that for every
function K and every epsilon, there is an n with the property that the ergodic
averages A_m f are stable to within epsilon on the interval [n,K(n)]. We show
that even though it is not generally possible to compute a bound on the rate of
convergenc... | math.DS math.LO | the mean ergodic theorem is equivalent to the assertion that for every function k and every epsilon there is an n with the property that the ergodic averages a_m f are stable to within epsilon on the interval nkn we show that even though it is not generally possible to compute a bound on the rate of convergence of a se... | [['the', 'mean', 'ergodic', 'theorem', 'is', 'equivalent', 'to', 'the', 'assertion', 'that', 'for', 'every', 'function', 'k', 'and', 'every', 'epsilon', 'there', 'is', 'an', 'n', 'with', 'the', 'property', 'that', 'the', 'ergodic', 'averages', 'a_m', 'f', 'are', 'stable', 'to', 'within', 'epsilon', 'on', 'the', 'interv... | [-0.1121511772232448, 0.11923669349542654, -0.13483618601353584, 0.09251061185196176, -0.02789840642028226, -0.1352133747374271, 0.0794544116862977, 0.36059570785411105, -0.2733893144184244, -0.24693579576117639, 0.12689316838151568, -0.27085905223750245, -0.1366857871521978, 0.24857300641377664, -0.10364999170666059, ... |
706.1513 | How to tell a gravastar from a black hole | Gravastars have been recently proposed as potential alternatives to explain
the astrophysical phenomenology traditionally associated to black holes,
raising the question of whether the two objects can be distinguished at all.
Leaving aside the debate about the processes that would lead to the formation
of a gravastar... | gr-qc astro-ph | gravastars have been recently proposed as potential alternatives to explain the astrophysical phenomenology traditionally associated to black holes raising the question of whether the two objects can be distinguished at all leaving aside the debate about the processes that would lead to the formation of a gravastar and... | [['gravastars', 'have', 'been', 'recently', 'proposed', 'as', 'potential', 'alternatives', 'to', 'explain', 'the', 'astrophysical', 'phenomenology', 'traditionally', 'associated', 'to', 'black', 'holes', 'raising', 'the', 'question', 'of', 'whether', 'the', 'two', 'objects', 'can', 'be', 'distinguished', 'at', 'all', '... | [-0.11194380695612148, 0.10134156298802334, -0.10985270918747626, 0.15192228378687422, -0.10372591247852501, -0.14463682762390478, 0.030337961501615166, 0.3257582168592963, -0.22351654641720098, -0.304976208406219, 0.13971479872761425, -0.28648731286832413, -0.1052971704115788, 0.19707346968840114, -0.05656334673606812... |
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