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 |
|---|---|---|---|---|---|---|
710.1453 | Hadron production in deuteron-gold collisions and nuclear parton
distributions | We calculate nuclear modification factors $R_{dAu}$, central-to-peripheral
ratios, $R_{CP}$, and pseudorapidity asymmetries $Y_{Asym}$ in deuteron-gold
collisions at $\sqrt{s} = 200$ GeV in the framework of leading-order (LO)
perturbative Quantum Chromodynamics. We use the Eskola-Kolhinen-Salgado (EKS),
the Frankfurt... | hep-ph | we calculate nuclear modification factors r_dau centraltoperipheral ratios r_cp and pseudorapidity asymmetries y_asym in deuterongold collisions at sqrts 200 gev in the framework of leadingorder lo perturbative quantum chromodynamics we use the eskolakolhinensalgado eks the frankfurtguzeystrikman fgs and the hiraikuman... | [['we', 'calculate', 'nuclear', 'modification', 'factors', 'r_dau', 'centraltoperipheral', 'ratios', 'r_cp', 'and', 'pseudorapidity', 'asymmetries', 'y_asym', 'in', 'deuterongold', 'collisions', 'at', 'sqrts', '200', 'gev', 'in', 'the', 'framework', 'of', 'leadingorder', 'lo', 'perturbative', 'quantum', 'chromodynamics... | [-0.004607634790638675, 0.1985851175487652, -0.21180814557296576, 0.1921491575289945, 0.04213999334692222, 0.005218784614908891, -0.04829235321872669, 0.39043292497880144, -0.1316510328381765, -0.27375713474647767, -0.09192603836446757, -0.4123484492301941, 0.085846695682553, 0.11820661668574102, 0.089384228838455, 0.1... |
710.1454 | Constraining Right-Handed Scale Through Kaon Mixing in SUSY Left-Right
Model | We study flavor-changing neutral current and CP violations in the minimal
supersymmetric left-right model. We calculate the beyond-standard-model
contributions to the neutral kaon mixing $\Delta M_K$ and $\epsilon$, and find
possible to have a numerical cancelation between the contributions from the
right-handed gaug... | hep-ph | we study flavorchanging neutral current and cp violations in the minimal supersymmetric leftright model we calculate the beyondstandardmodel contributions to the neutral kaon mixing delta m_k and epsilon and find possible to have a numerical cancelation between the contributions from the righthanded gauge boson and sup... | [['we', 'study', 'flavorchanging', 'neutral', 'current', 'and', 'cp', 'violations', 'in', 'the', 'minimal', 'supersymmetric', 'leftright', 'model', 'we', 'calculate', 'the', 'beyondstandardmodel', 'contributions', 'to', 'the', 'neutral', 'kaon', 'mixing', 'delta', 'm_k', 'and', 'epsilon', 'and', 'find', 'possible', 'to... | [-0.07720777191487806, 0.2770960568816268, 0.05568945949364986, 0.19689925414110934, -0.0781265230583293, -0.1727728136648823, 0.09494495705834456, 0.3054827969321715, -0.21000386620206493, -0.3241772164457611, 0.019837730988261422, -0.3239265470699008, -0.008219349677009241, 0.05606145587184334, 0.08562340429385326, 0... |
710.1455 | Superrecursive Features of Interactive Computation | Functioning and interaction of distributed devices and concurrent algorithms
are analyzed in the context of the theory of algorithms. Our main concern here
is how and under what conditions algorithmic interactive devices can be more
powerful than the recursive models of computation, such as Turing machines.
Realizati... | cs.DC cs.PF | functioning and interaction of distributed devices and concurrent algorithms are analyzed in the context of the theory of algorithms our main concern here is how and under what conditions algorithmic interactive devices can be more powerful than the recursive models of computation such as turing machines realization of... | [['functioning', 'and', 'interaction', 'of', 'distributed', 'devices', 'and', 'concurrent', 'algorithms', 'are', 'analyzed', 'in', 'the', 'context', 'of', 'the', 'theory', 'of', 'algorithms', 'our', 'main', 'concern', 'here', 'is', 'how', 'and', 'under', 'what', 'conditions', 'algorithmic', 'interactive', 'devices', 'c... | [-0.12912265658444497, 0.09513443875794281, -0.07835600709648065, 0.09649385109693163, -0.06592314988198988, -0.18940707804406728, 0.04226548772169066, 0.4089929264144234, -0.2463116964219876, -0.35009347178252803, 0.1329218171897151, -0.2157890998389361, -0.18963096659841402, 0.2774115522031866, -0.07832066390091193, ... |
710.1456 | Classification of the line-soliton solutions of KPII | In the previous papers (notably, Y. Kodama, J. Phys. A 37, 11169-11190
(2004), and G. Biondini and S. Chakravarty, J. Math. Phys. 47 033514 (2006)),
we found a large variety of line-soliton solutions of the
Kadomtsev-Petviashvili II (KPII) equation. The line-soliton solutions are
solitary waves which decay exponentia... | nlin.SI math-ph math.CO math.MP | in the previous papers notably y kodama j phys a 37 1116911190 2004 and g biondini and s chakravarty j math phys 47 033514 2006 we found a large variety of linesoliton solutions of the kadomtsevpetviashvili ii kpii equation the linesoliton solutions are solitary waves which decay exponentially in xyplane except along c... | [['in', 'the', 'previous', 'papers', 'notably', 'y', 'kodama', 'j', 'phys', 'a', '37', '1116911190', '2004', 'and', 'g', 'biondini', 'and', 's', 'chakravarty', 'j', 'math', 'phys', '47', '033514', '2006', 'we', 'found', 'a', 'large', 'variety', 'of', 'linesoliton', 'solutions', 'of', 'the', 'kadomtsevpetviashvili', 'ii... | [-0.15663766112321845, 0.06839349416115291, -0.06713883098787986, 0.034523749995239814, -0.06735554378438782, -0.13256475681459512, 0.04224053479137493, 0.28944922359353237, -0.23285044111684988, -0.3038502461942179, 0.054382172981174766, -0.3252966132905375, -0.17151347953048382, 0.1575868274750454, -0.069611649008488... |
710.1457 | Effective Coupling Constant in Renormalization Group for the Quantum
Electrodynamics | Effective coupling constant in quantum electrodynamics is investigated. A
pole appears in the effective coupling constant for the space-like momentum if
it is calculated by perturbation. The pole can be eliminated by the analytic
regularization. For QED the effective coupling constant is written in terms of
the scale... | hep-ph | effective coupling constant in quantum electrodynamics is investigated a pole appears in the effective coupling constant for the spacelike momentum if it is calculated by perturbation the pole can be eliminated by the analytic regularization for qed the effective coupling constant is written in terms of the scale param... | [['effective', 'coupling', 'constant', 'in', 'quantum', 'electrodynamics', 'is', 'investigated', 'a', 'pole', 'appears', 'in', 'the', 'effective', 'coupling', 'constant', 'for', 'the', 'spacelike', 'momentum', 'if', 'it', 'is', 'calculated', 'by', 'perturbation', 'the', 'pole', 'can', 'be', 'eliminated', 'by', 'the', '... | [-0.14935034149118323, 0.23269190326174524, -0.03715258641564782, 0.1175419793258659, -0.056537595334799684, -0.13619622310742419, -0.01988371342737624, 0.3183055191122471, -0.1805297757716889, -0.3186432895017788, 0.0626316016262516, -0.2566753251359184, -0.03450490704470096, 0.17470923026508473, 0.04688870921691365, ... |
710.1458 | Broad-line Balmer Decrements in Blue Active Galactic Nuclei | We have investigated the broad-line Balmer decrements (Halpha/Hbeta) for a
large, homogeneous sample of Seyfert 1 galaxies and QSOs using spectroscopic
data obtained in the Sloan Digital Sky Survey. The sample, drawn from the
Fourth Data Release, comprises 446 low redshift (z < 0.35) active galactic
nuclei (AGN) that... | astro-ph | we have investigated the broadline balmer decrements halphahbeta for a large homogeneous sample of seyfert 1 galaxies and qsos using spectroscopic data obtained in the sloan digital sky survey the sample drawn from the fourth data release comprises 446 low redshift z 035 active galactic nuclei agn that have blue optica... | [['we', 'have', 'investigated', 'the', 'broadline', 'balmer', 'decrements', 'halphahbeta', 'for', 'a', 'large', 'homogeneous', 'sample', 'of', 'seyfert', '1', 'galaxies', 'and', 'qsos', 'using', 'spectroscopic', 'data', 'obtained', 'in', 'the', 'sloan', 'digital', 'sky', 'survey', 'the', 'sample', 'drawn', 'from', 'the... | [0.0375085574774686, 0.05017867693110706, -0.01734364173906558, 0.13734059833009674, -0.0932570082910788, -0.11876888063989814, 0.07636622212466379, 0.5017093133586045, -0.09823731928868755, -0.3319999757539773, 0.0467363138651446, -0.35412118794562303, 0.04916227375113293, 0.2034823776025286, -0.05511033540260637, -0.... |
710.1459 | Geometry and complexity of O'Hara's algorithm | In this paper we analyze O'Hara's partition bijection. We present three type
of results. First, we show that O'Hara's bijection can be viewed geometrically
as a certain scissor congruence type result. Second, we obtain a number of new
complexity bounds, proving that O'Hara's bijection is efficient in several
special ... | math.CO | in this paper we analyze oharas partition bijection we present three type of results first we show that oharas bijection can be viewed geometrically as a certain scissor congruence type result second we obtain a number of new complexity bounds proving that oharas bijection is efficient in several special cases and mild... | [['in', 'this', 'paper', 'we', 'analyze', 'oharas', 'partition', 'bijection', 'we', 'present', 'three', 'type', 'of', 'results', 'first', 'we', 'show', 'that', 'oharas', 'bijection', 'can', 'be', 'viewed', 'geometrically', 'as', 'a', 'certain', 'scissor', 'congruence', 'type', 'result', 'second', 'we', 'obtain', 'a', '... | [-0.14393411251200763, 0.10631884292455479, -0.06793523670750715, 0.1097983613698965, -0.10708381264426169, -0.15336612410222492, 0.04461709951976359, 0.3527433100777368, -0.3233237745561859, -0.27269190489425366, 0.10067746124141627, -0.20402427804046533, -0.20492654713147895, 0.24711052154279536, -0.1283684687015401,... |
710.146 | Exact Static Solutions of a Generalized Discrete \phi^4 Model Including
Short-Periodic Solutions | For a five-parameter discrete $\phi^4$ model, we derive various exact static
solutions, including the staggered ones, in the form of the basic Jacobi
elliptic functions $\sn$, $\cn$, and $\dn$, and also in the form of their
hyperbolic function limits such as kink ($\tanh$) and single-humped pulse
($\sech$) solutions.... | nlin.SI nlin.PS | for a fiveparameter discrete phi4 model we derive various exact static solutions including the staggered ones in the form of the basic jacobi elliptic functions sn cn and dn and also in the form of their hyperbolic function limits such as kink tanh and singlehumped pulse sech solutions such solutions are admitted by th... | [['for', 'a', 'fiveparameter', 'discrete', 'phi4', 'model', 'we', 'derive', 'various', 'exact', 'static', 'solutions', 'including', 'the', 'staggered', 'ones', 'in', 'the', 'form', 'of', 'the', 'basic', 'jacobi', 'elliptic', 'functions', 'sn', 'cn', 'and', 'dn', 'and', 'also', 'in', 'the', 'form', 'of', 'their', 'hyper... | [-0.16091956490247578, 0.08714458381939216, -0.029155538053955973, 0.08571351388548841, -0.04659168914325319, -0.1727461738898078, -0.0214166609292123, 0.3661802459917054, -0.25097911009457097, -0.25641313275867483, 0.14388655014506474, -0.32716793821494256, -0.1634395024228114, 0.20491138446746712, 0.01386115302419767... |
710.1461 | A large deviation approach to optimal transport | A probabilistic method for solving the Monge-Kantorovich mass transport
problem on $R^d$ is introduced. A system of empirical measures of independent
particles is built in such a way that it obeys a doubly indexed large deviation
principle with an optimal transport cost as its rate function. As a
consequence, new app... | math.PR math.OC | a probabilistic method for solving the mongekantorovich mass transport problem on rd is introduced a system of empirical measures of independent particles is built in such a way that it obeys a doubly indexed large deviation principle with an optimal transport cost as its rate function as a consequence new approximatio... | [['a', 'probabilistic', 'method', 'for', 'solving', 'the', 'mongekantorovich', 'mass', 'transport', 'problem', 'on', 'rd', 'is', 'introduced', 'a', 'system', 'of', 'empirical', 'measures', 'of', 'independent', 'particles', 'is', 'built', 'in', 'such', 'a', 'way', 'that', 'it', 'obeys', 'a', 'doubly', 'indexed', 'large'... | [-0.10576456608058712, 0.07862337706649565, -0.10206873885826352, 0.09550286464263522, -0.02048316900858406, -0.10740440967732791, 0.10134448113937661, 0.32397734678167966, -0.35373024975631345, -0.2818354464894564, 0.08436741447196217, -0.2843880942571409, -0.1263469430358754, 0.2348635738773137, -0.07402143566437143,... |
710.1462 | Minimization of entropy functionals | Entropy functionals (i.e. convex integral functionals) and extensions of
these functionals are minimized on convex sets. This paper is aimed at reducing
as much as possible the assumptions on the constraint set. Dual equalities and
characterizations of the minimizers are obtained with weak constraint
qualifications.
| math.OC cs.IT math.IT math.PR | entropy functionals ie convex integral functionals and extensions of these functionals are minimized on convex sets this paper is aimed at reducing as much as possible the assumptions on the constraint set dual equalities and characterizations of the minimizers are obtained with weak constraint qualifications | [['entropy', 'functionals', 'ie', 'convex', 'integral', 'functionals', 'and', 'extensions', 'of', 'these', 'functionals', 'are', 'minimized', 'on', 'convex', 'sets', 'this', 'paper', 'is', 'aimed', 'at', 'reducing', 'as', 'much', 'as', 'possible', 'the', 'assumptions', 'on', 'the', 'constraint', 'set', 'dual', 'equalit... | [-0.11966850269171926, 0.041275743022561075, -0.06506245004841023, 0.15943703941173024, -0.06353875175118447, -0.11548120845109225, 0.05148965834588226, 0.3138572775655323, -0.3280870957507028, -0.27474661669176487, 0.1522193174705737, -0.3620064025123914, -0.0759805714038925, 0.21404372453689574, -0.11828964753852536,... |
710.1463 | Convex minimization problems with weak constraint qualifications | One revisits the standard saddle-point method based on conjugate duality for
solving convex minimization problems. Our aim is to reduce or remove
unnecessary topological restrictions on the constraint set. Dual equalities and
characterizations of the minimizers are obtained with weak or without
constraint qualificati... | math.OC | one revisits the standard saddlepoint method based on conjugate duality for solving convex minimization problems our aim is to reduce or remove unnecessary topological restrictions on the constraint set dual equalities and characterizations of the minimizers are obtained with weak or without constraint qualifications t... | [['one', 'revisits', 'the', 'standard', 'saddlepoint', 'method', 'based', 'on', 'conjugate', 'duality', 'for', 'solving', 'convex', 'minimization', 'problems', 'our', 'aim', 'is', 'to', 'reduce', 'or', 'remove', 'unnecessary', 'topological', 'restrictions', 'on', 'the', 'constraint', 'set', 'dual', 'equalities', 'and',... | [-0.1032002235962344, 0.002843777987263387, -0.09655482310058904, 0.12030024205783516, -0.14679635056693638, -0.13726883553733518, 0.05542472525987597, 0.3069887412157619, -0.34800505391432945, -0.31028584726820035, 0.1276395936022579, -0.3039414868412894, -0.14861088053744642, 0.18011629470025323, -0.1424975724048203,... |
710.1464 | Study of Hadron Scattering Using an Asymmetric Box | We propose to study hadron-hadron scattering using lattice QCD in an
asymmetric box which allows one to access more non-degenerate low-momentum
modes for a given volume. The conventional L\"{u}scher's formula applicable in
a symmetric box is modified accordingly. To illustrate the feasibility of this
approach, pion-p... | hep-lat | we propose to study hadronhadron scattering using lattice qcd in an asymmetric box which allows one to access more nondegenerate lowmomentum modes for a given volume the conventional luschers formula applicable in a symmetric box is modified accordingly to illustrate the feasibility of this approach pionpion elastic sc... | [['we', 'propose', 'to', 'study', 'hadronhadron', 'scattering', 'using', 'lattice', 'qcd', 'in', 'an', 'asymmetric', 'box', 'which', 'allows', 'one', 'to', 'access', 'more', 'nondegenerate', 'lowmomentum', 'modes', 'for', 'a', 'given', 'volume', 'the', 'conventional', 'luschers', 'formula', 'applicable', 'in', 'a', 'sy... | [-0.07485610838607086, 0.1915882120680511, -0.08478873276081603, 0.08889057106319921, -0.032969093902713874, -0.10588444799280049, 0.06365049151132883, 0.40940271807961504, -0.17337530303021512, -0.22589259467680345, 0.04048128373754232, -0.3170568771325138, -0.05742437102096367, 0.17811609830559147, 0.0244419515035009... |
710.1465 | Elasticity of Stiff Biopolymers | We present a statistical mechanical study of stiff polymers, motivated by
experiments on actin filaments and the considerable current interest in polymer
networks. We obtain simple, approximate analytical forms for the
force-extension relations and compare these with numerical treatments. We note
the important role o... | cond-mat.soft | we present a statistical mechanical study of stiff polymers motivated by experiments on actin filaments and the considerable current interest in polymer networks we obtain simple approximate analytical forms for the forceextension relations and compare these with numerical treatments we note the important role of bound... | [['we', 'present', 'a', 'statistical', 'mechanical', 'study', 'of', 'stiff', 'polymers', 'motivated', 'by', 'experiments', 'on', 'actin', 'filaments', 'and', 'the', 'considerable', 'current', 'interest', 'in', 'polymer', 'networks', 'we', 'obtain', 'simple', 'approximate', 'analytical', 'forms', 'for', 'the', 'forceext... | [-0.1394358763611445, 0.11874063602418349, -0.042930420085046724, 0.00838307063070236, -0.045312440130479074, -0.13064140980181996, 0.02969774258102701, 0.4215862610407414, -0.2430212936083716, -0.22303162695419404, 0.058245432034875914, -0.22744101964898647, -0.26811863444445116, 0.225050693177568, -0.0334537920982687... |
710.1466 | A note on the cone restriction conjecture in the cylindrically symmetric
case | In this note, we present two arguments showing that the classical
\textit{linear adjoint cone restriction conjecture} holds for the class of
functions supported on the cone and invariant under the spatial rotation in all
dimensions. The first is based on a dyadic restriction estimate, while the
second follows from a ... | math.CA math.AP | in this note we present two arguments showing that the classical textitlinear adjoint cone restriction conjecture holds for the class of functions supported on the cone and invariant under the spatial rotation in all dimensions the first is based on a dyadic restriction estimate while the second follows from a strength... | [['in', 'this', 'note', 'we', 'present', 'two', 'arguments', 'showing', 'that', 'the', 'classical', 'textitlinear', 'adjoint', 'cone', 'restriction', 'conjecture', 'holds', 'for', 'the', 'class', 'of', 'functions', 'supported', 'on', 'the', 'cone', 'and', 'invariant', 'under', 'the', 'spatial', 'rotation', 'in', 'all',... | [-0.11822524034505477, 0.07313743453414645, -0.11367121266084723, 0.09400398867728654, -0.07355810145236319, -0.10071461476036347, 0.026645122135960264, 0.3084726002853131, -0.2813956907921238, -0.1965095031191595, 0.1404334239923628, -0.22645886713507934, -0.1445946866124359, 0.23356866597896442, -0.10085476411040872,... |
710.1467 | Weight Distributions of Hamming Codes | We derive a recursive formula determing the weight distribution of the
[n=(q^m-1)/(q-1), n-m, 3] Hamming code H(m,q), when (m, q-1)=1. Here q is a
prime power. The proof is based on Moisio's idea of using Pless power moment
identity together with exponential sum techniques.
| cs.IT math.IT math.NT | we derive a recursive formula determing the weight distribution of the nqm1q1 nm 3 hamming code hmq when m q11 here q is a prime power the proof is based on moisios idea of using pless power moment identity together with exponential sum techniques | [['we', 'derive', 'a', 'recursive', 'formula', 'determing', 'the', 'weight', 'distribution', 'of', 'the', 'nqm1q1', 'nm', '3', 'hamming', 'code', 'hmq', 'when', 'm', 'q11', 'here', 'q', 'is', 'a', 'prime', 'power', 'the', 'proof', 'is', 'based', 'on', 'moisios', 'idea', 'of', 'using', 'pless', 'power', 'moment', 'ident... | [-0.15550778511651728, 0.06768518753707149, -0.12597077647440655, 0.04890988358339771, -0.08390225985542286, -0.20993218035978634, 0.061777492168868436, 0.31807892375387425, -0.27655095598920315, -0.27097969276960504, 0.07908876655016873, -0.2639992847432231, -0.08927631997611633, 0.16696949534897887, -0.04692471336010... |
710.1468 | Number of binomial coefficients divided by a fixed power of a prime | We state a general formula for the number of binomial coefficients $n$ choose
$k$ that are divided by a fixed power of a prime $p$, i.e., the number of
binomial coefficients divided by $p^j$ and not divided by $p^{j+1}$.
| math.GM | we state a general formula for the number of binomial coefficients n choose k that are divided by a fixed power of a prime p ie the number of binomial coefficients divided by pj and not divided by pj1 | [['we', 'state', 'a', 'general', 'formula', 'for', 'the', 'number', 'of', 'binomial', 'coefficients', 'n', 'choose', 'k', 'that', 'are', 'divided', 'by', 'a', 'fixed', 'power', 'of', 'a', 'prime', 'p', 'ie', 'the', 'number', 'of', 'binomial', 'coefficients', 'divided', 'by', 'pj', 'and', 'not', 'divided', 'by', 'pj1']] | [-0.17239169766636273, 0.1850505158746321, -0.06640781021039736, -0.018187752973876502, -0.008917633597248871, -0.2164223857444564, 0.08024590178147743, 0.2415350250360605, -0.28945455690355676, -0.2911237698832625, 0.014618225481459185, -0.26942714225304754, -0.0500995923679224, 0.22111361532619125, -0.023102193700125... |
710.1469 | Weight Distributions of Hamming Codes (II) | In a previous paper, we derived a recursive formula determining the weight
distributions of the [n=(q^m-1)/(q-1)] Hamming code H(m,q), when (m,q-1)=1.
Here q is a prime power. We note here that the formula actually holds for any
positive integer m and any prime power q, without the restriction (m, q-1)=1.
| cs.IT math.IT math.NT | in a previous paper we derived a recursive formula determining the weight distributions of the nqm1q1 hamming code hmq when mq11 here q is a prime power we note here that the formula actually holds for any positive integer m and any prime power q without the restriction m q11 | [['in', 'a', 'previous', 'paper', 'we', 'derived', 'a', 'recursive', 'formula', 'determining', 'the', 'weight', 'distributions', 'of', 'the', 'nqm1q1', 'hamming', 'code', 'hmq', 'when', 'mq11', 'here', 'q', 'is', 'a', 'prime', 'power', 'we', 'note', 'here', 'that', 'the', 'formula', 'actually', 'holds', 'for', 'any', '... | [-0.22375522380694746, 0.09941565312445164, -0.09294315986335278, 0.07123184309573843, -0.08019889816641808, -0.21138182018883525, 0.06858128810534253, 0.3124098711460829, -0.2621232228446752, -0.2509071286022663, 0.03439544881461188, -0.2449667757935822, -0.13192386474460363, 0.19280914566479623, -0.0800077772140503, ... |
710.147 | Asymmetry of near-critical percolation interfaces | We study the possible scaling limits of percolation interfaces in two
dimensions on the triangular lattice. When one lets the percolation parameter
p(N) vary with the size N of the box that one is considering, three
possibilities arise in the large-scale limit. It is known that when p(N) does
not converge to 1/2 fast... | math.PR | we study the possible scaling limits of percolation interfaces in two dimensions on the triangular lattice when one lets the percolation parameter pn vary with the size n of the box that one is considering three possibilities arise in the largescale limit it is known that when pn does not converge to 12 fast enough the... | [['we', 'study', 'the', 'possible', 'scaling', 'limits', 'of', 'percolation', 'interfaces', 'in', 'two', 'dimensions', 'on', 'the', 'triangular', 'lattice', 'when', 'one', 'lets', 'the', 'percolation', 'parameter', 'pn', 'vary', 'with', 'the', 'size', 'n', 'of', 'the', 'box', 'that', 'one', 'is', 'considering', 'three'... | [-0.12831523693375177, 0.16016503061696108, -0.05276716100191003, 0.059039517132037166, -0.0452795096450666, -0.1657759370230166, 0.06142283384618697, 0.3299136843754729, -0.25337688449019596, -0.23452848107632207, 0.14001727687393023, -0.31266097505637724, -0.10921140492949356, 0.20099699078822758, -0.0190638844375568... |
710.1471 | New determination of the size and bulk density of the binary asteroid 22
Kalliope from observations of mutual eclipses | In 2007, the M-type binary asteroid 22 Kalliope reached one of its annual
equinoxes. As a consequence, the orbit plane of its small moon, Linus, was
aligned closely to the Sun's line of sight, giving rise to a mutual eclipse
season. A dedicated international campaign of photometric observations, based
on amateur-prof... | astro-ph | in 2007 the mtype binary asteroid 22 kalliope reached one of its annual equinoxes as a consequence the orbit plane of its small moon linus was aligned closely to the suns line of sight giving rise to a mutual eclipse season a dedicated international campaign of photometric observations based on amateurprofessional coll... | [['in', '2007', 'the', 'mtype', 'binary', 'asteroid', '22', 'kalliope', 'reached', 'one', 'of', 'its', 'annual', 'equinoxes', 'as', 'a', 'consequence', 'the', 'orbit', 'plane', 'of', 'its', 'small', 'moon', 'linus', 'was', 'aligned', 'closely', 'to', 'the', 'suns', 'line', 'of', 'sight', 'giving', 'rise', 'to', 'a', 'm... | [-0.10692282353100786, 0.09597893672696088, -0.08529347822984254, 0.03952777031881474, -0.09060166810682632, -0.07047932430223557, 0.04193652567086944, 0.3373122704866791, -0.2008059135556144, -0.37480174545729483, 0.13359977189605873, -0.2866041696548385, -0.07608688771700574, 0.2096263203019556, -0.08744869270715429,... |
710.1472 | Optical Variability of the Radio Source J 1128+5925 | Very recently, J 1128+5925 was found to show strong intraday variability at
radio wavelengths and may be a new source with annual modulation of the
timescale of its radio variability. Therefore, its radio variability can be
best explained via interstellar scintillation. Here we present the properties
of its optical v... | astro-ph | very recently j 11285925 was found to show strong intraday variability at radio wavelengths and may be a new source with annual modulation of the timescale of its radio variability therefore its radio variability can be best explained via interstellar scintillation here we present the properties of its optical variabil... | [['very', 'recently', 'j', '11285925', 'was', 'found', 'to', 'show', 'strong', 'intraday', 'variability', 'at', 'radio', 'wavelengths', 'and', 'may', 'be', 'a', 'new', 'source', 'with', 'annual', 'modulation', 'of', 'the', 'timescale', 'of', 'its', 'radio', 'variability', 'therefore', 'its', 'radio', 'variability', 'ca... | [-0.13101425971090794, 0.13621256812661886, -0.13917937706410885, 0.08217762621119619, -0.11417203474789858, -0.12126384786143898, 0.08788959741406142, 0.517171152293682, -0.23386644153366798, -0.3043869045972824, 0.15186918055359275, -0.20948416231572628, -0.13971522066555916, 0.22662971667014062, -0.10142332711443305... |
710.1473 | Integrated properties of mass segregated star clusters | In this contribution we study integrated properties of dynamically segregated
star clusters. The observed core radii of segregated clusters can be 50%
smaller than the ``true'' core radius. In addition, the measured radius in the
red filters is smaller than those measured in blue filters. However, these
difference ar... | astro-ph | in this contribution we study integrated properties of dynamically segregated star clusters the observed core radii of segregated clusters can be 50 smaller than the true core radius in addition the measured radius in the red filters is smaller than those measured in blue filters however these difference are small less... | [['in', 'this', 'contribution', 'we', 'study', 'integrated', 'properties', 'of', 'dynamically', 'segregated', 'star', 'clusters', 'the', 'observed', 'core', 'radii', 'of', 'segregated', 'clusters', 'can', 'be', '50', 'smaller', 'than', 'the', 'true', 'core', 'radius', 'in', 'addition', 'the', 'measured', 'radius', 'in'... | [-0.03937211306168008, 0.16593717508866185, -0.10488490265977037, 0.1210320101038503, -0.05236600770773033, -0.04983134670848293, -0.010323602527413251, 0.42906886042536435, -0.18270095314073842, -0.36992812623170074, 0.06603172672787748, -0.30773255937466665, -0.0624059137522376, 0.19101371624024718, -0.04710725938119... |
710.1474 | Strong decays of heavy baryons in Bethe-Salpeter formalism | In this paper we study the properties of diquarks (composed of $u$ and/or $d$
quarks) in the Bethe-Salpeter formalism under the covariant instantaneous
approximation. We calculate their BS wave functions and study their effective
interaction with the pion. Using the effective coupling constant among the
diquarks and ... | hep-ph | in this paper we study the properties of diquarks composed of u andor d quarks in the bethesalpeter formalism under the covariant instantaneous approximation we calculate their bs wave functions and study their effective interaction with the pion using the effective coupling constant among the diquarks and the pion in ... | [['in', 'this', 'paper', 'we', 'study', 'the', 'properties', 'of', 'diquarks', 'composed', 'of', 'u', 'andor', 'd', 'quarks', 'in', 'the', 'bethesalpeter', 'formalism', 'under', 'the', 'covariant', 'instantaneous', 'approximation', 'we', 'calculate', 'their', 'bs', 'wave', 'functions', 'and', 'study', 'their', 'effecti... | [-0.13761355803359912, 0.22099602355657122, -0.08992198178002352, 0.13633962394522292, -0.0049770226631360714, -0.09243564166222946, 0.11689832765473454, 0.3495620783607039, -0.18283815432009817, -0.20185598027244023, -0.06873076921328902, -0.28718054926470865, -0.06101000336694378, 0.020221552729040762, 0.133046570670... |
710.1475 | Red-Shift Distribution of Gamma-ray Bursts and Their Progenitors | Gamma ray bursts have been divided into two classes, long-soft gamma ray
burst and short-hard gamma ray burst according to the bimodal distribution in
duration time. Due to the harder spectrum and the lack of afterglows of
short-hard bursts in optical and radio observations, different progenitors for
short-hard burst... | astro-ph | gamma ray bursts have been divided into two classes longsoft gamma ray burst and shorthard gamma ray burst according to the bimodal distribution in duration time due to the harder spectrum and the lack of afterglows of shorthard bursts in optical and radio observations different progenitors for shorthard bursts and lon... | [['gamma', 'ray', 'bursts', 'have', 'been', 'divided', 'into', 'two', 'classes', 'longsoft', 'gamma', 'ray', 'burst', 'and', 'shorthard', 'gamma', 'ray', 'burst', 'according', 'to', 'the', 'bimodal', 'distribution', 'in', 'duration', 'time', 'due', 'to', 'the', 'harder', 'spectrum', 'and', 'the', 'lack', 'of', 'aftergl... | [-0.03812975774722538, 0.16105368903078054, -0.07396870748750095, 0.2368122170827801, -0.14540676482626633, -0.09494247743538742, 0.06449718074337847, 0.5193165974830674, -0.14499372777585262, -0.3293640073067669, -0.01424985610473173, -0.3096363879800453, -0.010829721663104391, 0.2919678346457324, -0.00799408944955245... |
710.1476 | MACE -- Mach cones in heavy ion collisions | We study the propagation of sound-like perturbations created by a jet moving
with supersonic velocity through the quark-gluon-plasma created in heavy-ion
reactions within the model MACE (MAch Cone Evolution). Predictions for
heavy-ion reactions at RHIC energies (Au+Au-collisions) and for Pb+Pb reactions
at the LHC ($... | nucl-th | we study the propagation of soundlike perturbations created by a jet moving with supersonic velocity through the quarkgluonplasma created in heavyion reactions within the model mace mach cone evolution predictions for heavyion reactions at rhic energies auaucollisions and for pbpb reactions at the lhc sqrt s55a tev are... | [['we', 'study', 'the', 'propagation', 'of', 'soundlike', 'perturbations', 'created', 'by', 'a', 'jet', 'moving', 'with', 'supersonic', 'velocity', 'through', 'the', 'quarkgluonplasma', 'created', 'in', 'heavyion', 'reactions', 'within', 'the', 'model', 'mace', 'mach', 'cone', 'evolution', 'predictions', 'for', 'heavyi... | [-0.03323809936705787, 0.3090838029885949, -0.17308409598861205, 0.09628368888081888, 0.029928895376496397, -0.10585223188055522, -0.1197993336230619, 0.36969354928676357, -0.2043076658195232, -0.2578141287726871, -0.05267565712230122, -0.37824404579034804, 0.11873348304307309, 0.1729043585729738, 0.13432599628991368, ... |
710.1477 | Symplectic Connections of Ricci Type and Star Products | In this article we relate the construction of Ricci type symplectic
connections by reduction to the construction of star product by reduction
yielding rather explicit descriptions for the star product on the reduced
space.
| math.QA math.SG | in this article we relate the construction of ricci type symplectic connections by reduction to the construction of star product by reduction yielding rather explicit descriptions for the star product on the reduced space | [['in', 'this', 'article', 'we', 'relate', 'the', 'construction', 'of', 'ricci', 'type', 'symplectic', 'connections', 'by', 'reduction', 'to', 'the', 'construction', 'of', 'star', 'product', 'by', 'reduction', 'yielding', 'rather', 'explicit', 'descriptions', 'for', 'the', 'star', 'product', 'on', 'the', 'reduced', 'sp... | [-0.10441735715550535, 0.07566692354157567, -0.048167953603243566, 0.05863403099904056, -0.11265279407448628, -0.04276490030700669, 0.04100075451766744, 0.2865565100903897, -0.23136522883878036, -0.29300542372991056, 0.12567027438746983, -0.20070263309239902, -0.1612328118233777, 0.1938685956684982, -0.1373946533045348... |
710.1478 | Angular decorrelations in Mueller-Navelet jets and DIS | We discuss the azimuthal angle decorrelation of Mueller-Navelet jets at
hadron colliders and forward jets in Deep Inelastic Scattering within the BFKL
framework with a NLO kernel. We stress the need of collinear improvements to
obtain good perturbative convergence. We provide estimates of these
decorrelations for lar... | hep-ph | we discuss the azimuthal angle decorrelation of muellernavelet jets at hadron colliders and forward jets in deep inelastic scattering within the bfkl framework with a nlo kernel we stress the need of collinear improvements to obtain good perturbative convergence we provide estimates of these decorrelations for large ra... | [['we', 'discuss', 'the', 'azimuthal', 'angle', 'decorrelation', 'of', 'muellernavelet', 'jets', 'at', 'hadron', 'colliders', 'and', 'forward', 'jets', 'in', 'deep', 'inelastic', 'scattering', 'within', 'the', 'bfkl', 'framework', 'with', 'a', 'nlo', 'kernel', 'we', 'stress', 'the', 'need', 'of', 'collinear', 'improvem... | [-0.052000546104020696, 0.14016235702755778, -0.2097456808709963, 0.24088997637683696, -0.05975153234533288, -0.06788846515754068, -0.08107293128374625, 0.46101487898691135, -0.2090714574537494, -0.1891161500730298, -0.04134452517610043, -0.363300795734606, 0.0929755871268836, 0.11365030124275521, 0.10216386734338646, ... |
710.1479 | On superconformal projective hypermultiplets | Building on the five-dimensional constructions in hep-th/0601177, we provide
a unified description of four-dimensional N = 2 superconformal off-shell
multiplets in projective superspace, including a realization in terms of N = 1
superfields. In particular, superconformal polar multiplets are consistently
defined for ... | hep-th | building on the fivedimensional constructions in hepth0601177 we provide a unified description of fourdimensional n 2 superconformal offshell multiplets in projective superspace including a realization in terms of n 1 superfields in particular superconformal polar multiplets are consistently defined for the first time ... | [['building', 'on', 'the', 'fivedimensional', 'constructions', 'in', 'hepth0601177', 'we', 'provide', 'a', 'unified', 'description', 'of', 'fourdimensional', 'n', '2', 'superconformal', 'offshell', 'multiplets', 'in', 'projective', 'superspace', 'including', 'a', 'realization', 'in', 'terms', 'of', 'n', '1', 'superfiel... | [-0.1490442592791662, 0.1858327570134605, -0.025639209319168414, 0.07827006605647269, -0.10464209961888551, -0.19481797493390843, -0.0908980267843835, 0.31964276179435175, -0.18008736084530155, -0.26864759766326196, 0.0986553954762328, -0.24287228622723003, -0.211171558920399, 0.0908116971218014, -0.09760703786250047, ... |
710.148 | Density of neutral interstellar hydrogen at the termination shock from
Ulysses pickup ion observations | By reevaluating a 13-month stretch of Ulysses SWICS H pickup ion measurements
near 5 AU close to the ecliptic right after the previous solar minimum, this
paper presents a determination of the neutral interstellar H density at the
solar wind termination shock and implications for the density and ionization
degree of ... | astro-ph | by reevaluating a 13month stretch of ulysses swics h pickup ion measurements near 5 au close to the ecliptic right after the previous solar minimum this paper presents a determination of the neutral interstellar h density at the solar wind termination shock and implications for the density and ionization degree of hydr... | [['by', 'reevaluating', 'a', '13month', 'stretch', 'of', 'ulysses', 'swics', 'h', 'pickup', 'ion', 'measurements', 'near', '5', 'au', 'close', 'to', 'the', 'ecliptic', 'right', 'after', 'the', 'previous', 'solar', 'minimum', 'this', 'paper', 'presents', 'a', 'determination', 'of', 'the', 'neutral', 'interstellar', 'h',... | [-0.06401556125691547, 0.12706367952386044, -0.028789057688810293, 0.03631980885416496, 0.019872352259415315, -0.07521206474005494, 0.048984779306920245, 0.35331123477137627, -0.250296983106925, -0.3447277063799159, 0.036521562399973, -0.28810717820803206, 0.034993467111390356, 0.16832437870027384, 0.020497494428305, 0... |
710.1481 | What's in a Name? | This paper describes experiments on identifying the language of a single name
in isolation or in a document written in a different language. A new corpus has
been compiled and made available, matching names against languages. This corpus
is used in a series of experiments measuring the performance of general
language... | cs.CL cs.AI | this paper describes experiments on identifying the language of a single name in isolation or in a document written in a different language a new corpus has been compiled and made available matching names against languages this corpus is used in a series of experiments measuring the performance of general language mode... | [['this', 'paper', 'describes', 'experiments', 'on', 'identifying', 'the', 'language', 'of', 'a', 'single', 'name', 'in', 'isolation', 'or', 'in', 'a', 'document', 'written', 'in', 'a', 'different', 'language', 'a', 'new', 'corpus', 'has', 'been', 'compiled', 'and', 'made', 'available', 'matching', 'names', 'against', ... | [-0.0814972626535516, 0.002039225154409283, -0.0580326123212121, 0.11561095519849149, -0.13595003274906622, -0.14126900167106407, 0.04782145347960882, 0.41102267574322854, -0.24301407156806243, -0.34657978813997226, 0.047922469611818855, -0.3062525405499496, -0.07029628238248589, 0.24344348841542868, -0.080439006468575... |
710.1482 | Heap Reference Analysis for Functional Programs | Current garbage collectors leave a lot of garbage uncollected because they
conservatively approximate liveness by reachability from program variables. In
this paper, we describe a sequence of static analyses that takes as input a
program written in a first-order, eager functional programming language, and
finds at ea... | cs.PL cs.SE | current garbage collectors leave a lot of garbage uncollected because they conservatively approximate liveness by reachability from program variables in this paper we describe a sequence of static analyses that takes as input a program written in a firstorder eager functional programming language and finds at each prog... | [['current', 'garbage', 'collectors', 'leave', 'a', 'lot', 'of', 'garbage', 'uncollected', 'because', 'they', 'conservatively', 'approximate', 'liveness', 'by', 'reachability', 'from', 'program', 'variables', 'in', 'this', 'paper', 'we', 'describe', 'a', 'sequence', 'of', 'static', 'analyses', 'that', 'takes', 'as', 'i... | [-0.10486388929381951, 0.049026525348518826, -0.0841020253768676, 0.082358146704119, -0.08861775546600777, -0.14156646930080438, 0.09548510669167114, 0.36467927137875006, -0.2845434186228809, -0.37420108932424573, 0.12523678268214, -0.29197147180631505, -0.0837881751260681, 0.1902233309429452, -0.09121928813851618, 0.0... |
710.1483 | The complex of pant decompositions of a surface | We exhibit a set of edges (moves) and 2-cells (relations) making the complex
of pant decompositions on a surface a simply connected complex. Our
construction, unlike the previous ones, keeps the arguments concerning the
structural transformations independent from those deriving from the action of
the mapping class gr... | math.GT | we exhibit a set of edges moves and 2cells relations making the complex of pant decompositions on a surface a simply connected complex our construction unlike the previous ones keeps the arguments concerning the structural transformations independent from those deriving from the action of the mapping class group the mo... | [['we', 'exhibit', 'a', 'set', 'of', 'edges', 'moves', 'and', '2cells', 'relations', 'making', 'the', 'complex', 'of', 'pant', 'decompositions', 'on', 'a', 'surface', 'a', 'simply', 'connected', 'complex', 'our', 'construction', 'unlike', 'the', 'previous', 'ones', 'keeps', 'the', 'arguments', 'concerning', 'the', 'str... | [-0.16881235581205553, 0.11244949846001095, -0.10913350927946439, 0.009513776161685496, -0.12127948203124106, -0.09094540429784052, 0.07539716175566595, 0.3421502068010439, -0.300320723554097, -0.2985222648200859, 0.09325345008106656, -0.2920748117598649, -0.1691573574291879, 0.1912144104310547, -0.08065370493848999, -... |
710.1484 | The structure and modeling results of the parallel spatial switching
system | Problems of the switching parallel system designing provided spatial
switching of packets from random time are discussed. Results of modeling of
switching system as systems of mass service are resulted.
| cs.NI cs.DC | problems of the switching parallel system designing provided spatial switching of packets from random time are discussed results of modeling of switching system as systems of mass service are resulted | [['problems', 'of', 'the', 'switching', 'parallel', 'system', 'designing', 'provided', 'spatial', 'switching', 'of', 'packets', 'from', 'random', 'time', 'are', 'discussed', 'results', 'of', 'modeling', 'of', 'switching', 'system', 'as', 'systems', 'of', 'mass', 'service', 'are', 'resulted']] | [-0.28971477697292963, 0.10525303509396812, -0.008725339857240519, -0.031196085767199597, -0.009044491375486055, -0.18573833741247653, 0.03854468557983637, 0.4237036928534508, -0.27713546964029473, -0.319434421757857, 0.1393442195452129, -0.22294453081364432, -0.11071283730367819, 0.27448704143365227, -0.04704377390444... |
710.1485 | Quantum toboggans: models exhibiting a multisheeted PT symmetry | A generalization of the concept of PT-symmetric Hamiltonians H=p^2+V(x) is
described. It uses analytic potentials V(x) (with singularities) and a
generalized concept of PT-symmetric asymptotic boundary conditions. Nontrivial
toboggans are defined as integrated along topologically nontrivial paths of
coordinates runni... | quant-ph | a generalization of the concept of ptsymmetric hamiltonians hp2vx is described it uses analytic potentials vx with singularities and a generalized concept of ptsymmetric asymptotic boundary conditions nontrivial toboggans are defined as integrated along topologically nontrivial paths of coordinates running over several... | [['a', 'generalization', 'of', 'the', 'concept', 'of', 'ptsymmetric', 'hamiltonians', 'hp2vx', 'is', 'described', 'it', 'uses', 'analytic', 'potentials', 'vx', 'with', 'singularities', 'and', 'a', 'generalized', 'concept', 'of', 'ptsymmetric', 'asymptotic', 'boundary', 'conditions', 'nontrivial', 'toboggans', 'are', 'd... | [-0.2743383725578694, 0.10330780546950258, -0.10435913197453255, 0.06496153066046131, -0.10504707762384383, -0.17430430926058604, -0.058428191944308906, 0.37256194634929946, -0.19681446108481157, -0.1841474716835048, 0.0632447601781915, -0.2721184751464297, -0.23043222956197418, 0.20656986737056918, -0.0214620897060503... |
710.1486 | Type Ia supernovae as speed sensors at intermediate redshifts | The application of large scale peculiar velocity (LSPV), as a crucial probe
of dark matter, dark energy and gravity, is severely limited by measurement
obstacles. We show that fluctuations in type Ia supernovae (SNe Ia) fluxes
induced by LSPV offer a promising approach to measure LSPV at intermediate
redshifts. In th... | astro-ph | the application of large scale peculiar velocity lspv as a crucial probe of dark matter dark energy and gravity is severely limited by measurement obstacles we show that fluctuations in type ia supernovae sne ia fluxes induced by lspv offer a promising approach to measure lspv at intermediate redshifts in the 3d fourie... | [['the', 'application', 'of', 'large', 'scale', 'peculiar', 'velocity', 'lspv', 'as', 'a', 'crucial', 'probe', 'of', 'dark', 'matter', 'dark', 'energy', 'and', 'gravity', 'is', 'severely', 'limited', 'by', 'measurement', 'obstacles', 'we', 'show', 'that', 'fluctuations', 'in', 'type', 'ia', 'supernovae', 'sne', 'ia', '... | [-0.07898427614378273, 0.1326726624067155, -0.06656316293557303, 0.16907875865875155, -0.11683984490863364, -0.12759293656189577, 0.048809087113263684, 0.3581874545902834, -0.2573772308954952, -0.2988287893662212, 0.03462043041128392, -0.2738991946135776, -0.055405807484864095, 0.20401829497358942, -0.06305110399242023... |
710.1487 | Asymptotically isochronous systems | Mechanisms are elucidated underlying the existence of dynamical systems whose
generic solutions approach asymptotically (at large time) isochronous
evolutions: all their dependent variables tend asymptotically to functions
periodic with the same fixed period. We focus on two such mechanisms,
emphasizing their general... | nlin.SI math-ph math.DS math.MP | mechanisms are elucidated underlying the existence of dynamical systems whose generic solutions approach asymptotically at large time isochronous evolutions all their dependent variables tend asymptotically to functions periodic with the same fixed period we focus on two such mechanisms emphasizing their generality and... | [['mechanisms', 'are', 'elucidated', 'underlying', 'the', 'existence', 'of', 'dynamical', 'systems', 'whose', 'generic', 'solutions', 'approach', 'asymptotically', 'at', 'large', 'time', 'isochronous', 'evolutions', 'all', 'their', 'dependent', 'variables', 'tend', 'asymptotically', 'to', 'functions', 'periodic', 'with... | [-0.1485220305057186, 0.15179268792365688, -0.04241817002419872, 0.11197891033188713, -0.05733782785351981, -0.2238163818955666, -0.01733999930891312, 0.33998861220298393, -0.27240134885703976, -0.23835158969905942, 0.10630116311155936, -0.26157270917537234, -0.20169093726071144, 0.21686600598346706, 0.0238661121934501... |
710.1488 | Flavor Changing Neutral Current Processes in a SO(10) SUSY GUT with
Family Symmetry | We report on a detailed analysis of a SO(10) SUSY GUT model of Dermisek and
Raby (DR) with a D3 family symmetry. The model is completely specified in terms
of only 24 parameters and is able to successfully describe both quark and
lepton masses and mixings, except for |Vub| that turns out to be too low.
However, a glo... | hep-ph | we report on a detailed analysis of a so10 susy gut model of dermisek and raby dr with a d3 family symmetry the model is completely specified in terms of only 24 parameters and is able to successfully describe both quark and lepton masses and mixings except for vub that turns out to be too low however a global fit show... | [['we', 'report', 'on', 'a', 'detailed', 'analysis', 'of', 'a', 'so10', 'susy', 'gut', 'model', 'of', 'dermisek', 'and', 'raby', 'dr', 'with', 'a', 'd3', 'family', 'symmetry', 'the', 'model', 'is', 'completely', 'specified', 'in', 'terms', 'of', 'only', '24', 'parameters', 'and', 'is', 'able', 'to', 'successfully', 'de... | [-0.07647519300108728, 0.1658100276762823, -0.031813810383822735, 0.13075835544404676, -0.07513604795427195, -0.24360011792311273, 0.14702553823277228, 0.31843318553062294, -0.2133448063708967, -0.29484458018814313, 0.06347147822908338, -0.2534394699516667, -0.03427263178046746, 0.1182210229688418, -0.01733260940390584... |
710.1489 | Lepton Flavour Violating Effects on Chargino Production at the ILC | We review the influence of lepton flavour violation (LFV) on the production
processes e+e- -> ~chi+_i ~chi-_j at the International Linear Collider (ILC)
with longitudinal e+ and e- beam polarizations in the framework of the Minimal
Supersymmetric Standard Model (MSSM). The t-channel sneutrino exchange
contribution to... | hep-ph | we review the influence of lepton flavour violation lfv on the production processes ee chi_i chi_j at the international linear collider ilc with longitudinal e and e beam polarizations in the framework of the minimal supersymmetric standard model mssm the tchannel sneutrino exchange contribution to the processes ee chi... | [['we', 'review', 'the', 'influence', 'of', 'lepton', 'flavour', 'violation', 'lfv', 'on', 'the', 'production', 'processes', 'ee', 'chi_i', 'chi_j', 'at', 'the', 'international', 'linear', 'collider', 'ilc', 'with', 'longitudinal', 'e', 'and', 'e', 'beam', 'polarizations', 'in', 'the', 'framework', 'of', 'the', 'minima... | [-0.08618036473739836, 0.2805772911924035, 0.007806676262711633, 0.16009529417297289, -0.0632636042575894, -0.19900149481593452, 0.039528275708799986, 0.25846989008375626, -0.24521125265077423, -0.2542804687687043, -0.015611215008930094, -0.35141203333901716, 0.009831501773919966, 0.15625853485726654, 0.090427304857841... |
710.149 | Electrostatic control of quantum dot entanglement induced by coupling to
external reservoirs | We propose a quantum transport experiment to prepare and measure
charge-entanglement between two electrostatically defined quantum dots.
Coherent population trapping, as realized in cavity quantum electrodynamics,
can be carried out by using a third quantum dot to play the role of the optical
cavity. In our proposal,... | cond-mat.mes-hall | we propose a quantum transport experiment to prepare and measure chargeentanglement between two electrostatically defined quantum dots coherent population trapping as realized in cavity quantum electrodynamics can be carried out by using a third quantum dot to play the role of the optical cavity in our proposal a pumpi... | [['we', 'propose', 'a', 'quantum', 'transport', 'experiment', 'to', 'prepare', 'and', 'measure', 'chargeentanglement', 'between', 'two', 'electrostatically', 'defined', 'quantum', 'dots', 'coherent', 'population', 'trapping', 'as', 'realized', 'in', 'cavity', 'quantum', 'electrodynamics', 'can', 'be', 'carried', 'out',... | [-0.14308034492921823, 0.23963438877931884, -0.0875461895292452, -0.021300084191643316, 0.05785209033638239, -0.22312566938512413, 0.0809650903318039, 0.36786801245101947, -0.25810125133637146, -0.3033733418998645, 0.046726766966532954, -0.24913863641853184, -0.07880010914307126, 0.2564701220865563, 0.00212403389711662... |
710.1491 | Dust, pulsation, chromospheres and their role in driving mass loss from
red giants in Galactic globular clusters | Context: Mass loss from red giants in old globular clusters affects the
horizontal branch (HB) morphology and post-HB stellar evolution including the
production of ultraviolet-bright stars, dredge up of nucleosynthesis products
and replenishment of the intra-cluster medium. Studies of mass loss in globular
clusters a... | astro-ph | context mass loss from red giants in old globular clusters affects the horizontal branch hb morphology and posthb stellar evolution including the production of ultravioletbright stars dredge up of nucleosynthesis products and replenishment of the intracluster medium studies of mass loss in globular clusters also allows... | [['context', 'mass', 'loss', 'from', 'red', 'giants', 'in', 'old', 'globular', 'clusters', 'affects', 'the', 'horizontal', 'branch', 'hb', 'morphology', 'and', 'posthb', 'stellar', 'evolution', 'including', 'the', 'production', 'of', 'ultravioletbright', 'stars', 'dredge', 'up', 'of', 'nucleosynthesis', 'products', 'an... | [-0.03460160166628846, 0.109952695571227, -0.046687167550606486, 0.12166186857255966, -0.11093147550215662, -0.040414481658389734, 0.09645820754424979, 0.46886996761895716, -0.13137031923763448, -0.3436322748276518, -0.011886841381166243, -0.292835007655881, 0.027328254688958015, 0.21074904968731006, -0.083886235598390... |
710.1492 | Precise Formulation of Neutrino Oscillation in the Earth | We give a perturbation theory of neutrino oscillation in the Earth. The
perturbation theory is valid for neutrinos with energy $E \gsim 0.5$ GeV. It is
formulated using trajectory dependent average potential. Non-adiabatic
contributions are included as the first order effects in the perturbation
theory. We analyze ne... | hep-ph hep-ex | we give a perturbation theory of neutrino oscillation in the earth the perturbation theory is valid for neutrinos with energy e gsim 05 gev it is formulated using trajectory dependent average potential nonadiabatic contributions are included as the first order effects in the perturbation theory we analyze neutrino osci... | [['we', 'give', 'a', 'perturbation', 'theory', 'of', 'neutrino', 'oscillation', 'in', 'the', 'earth', 'the', 'perturbation', 'theory', 'is', 'valid', 'for', 'neutrinos', 'with', 'energy', 'e', 'gsim', '05', 'gev', 'it', 'is', 'formulated', 'using', 'trajectory', 'dependent', 'average', 'potential', 'nonadiabatic', 'con... | [-0.11800559101522796, 0.2350329545352401, -0.11351564369785289, 0.17607295860070735, -0.04630564109732707, -0.061518263366694255, 0.03466838835738599, 0.2743052485709389, -0.21918723742581075, -0.3377072172860304, 0.025978286609622755, -0.30408636745996775, -0.12550677841322289, 0.14687628909531567, 0.0237025440256628... |
710.1493 | Neutrinos from WIMP annihilations | We make an improved analysis on the flow of neutrinos originating from WIMP
annihilations inside the Sun and the Earth. We treat both neutrino interaction
and oscillation effects in a consistent framework. Our numerical simulations
are performed in an event based setting, which is useful for both theoretical
studies ... | hep-ph | we make an improved analysis on the flow of neutrinos originating from wimp annihilations inside the sun and the earth we treat both neutrino interaction and oscillation effects in a consistent framework our numerical simulations are performed in an event based setting which is useful for both theoretical studies and f... | [['we', 'make', 'an', 'improved', 'analysis', 'on', 'the', 'flow', 'of', 'neutrinos', 'originating', 'from', 'wimp', 'annihilations', 'inside', 'the', 'sun', 'and', 'the', 'earth', 'we', 'treat', 'both', 'neutrino', 'interaction', 'and', 'oscillation', 'effects', 'in', 'a', 'consistent', 'framework', 'our', 'numerical'... | [-0.08704345085037252, 0.2092464410176035, -0.09555589117051567, 0.16792080068650345, -0.0637868144425253, -0.08282999965672691, 0.029422414017220337, 0.3590023980701032, -0.1906597234805425, -0.29557469869653386, 0.04816259038634598, -0.3295417442917824, -0.06768343198734025, 0.25117992220407664, 0.054332283871869246,... |
710.1494 | Singular Scaling Functions in Clustering Phenomena | We study clustering in a stochastic system of particles sliding down a
fluctuating surface in one and two dimensions. In steady state, the
density-density correlation function is a scaling function of separation and
system size.This scaling function is singular for small argument -- it exhibits
a cusp singularity for... | cond-mat.stat-mech cond-mat.soft | we study clustering in a stochastic system of particles sliding down a fluctuating surface in one and two dimensions in steady state the densitydensity correlation function is a scaling function of separation and system sizethis scaling function is singular for small argument it exhibits a cusp singularity for particle... | [['we', 'study', 'clustering', 'in', 'a', 'stochastic', 'system', 'of', 'particles', 'sliding', 'down', 'a', 'fluctuating', 'surface', 'in', 'one', 'and', 'two', 'dimensions', 'in', 'steady', 'state', 'the', 'densitydensity', 'correlation', 'function', 'is', 'a', 'scaling', 'function', 'of', 'separation', 'and', 'syste... | [-0.1706643533808264, 0.20575095010836694, -0.17700183383104476, 0.09018354258415374, 0.011270503454249013, -0.14721730715933848, 0.028161278386886063, 0.3040698639794507, -0.2519725212488662, -0.25160313031890175, 0.07234856418270448, -0.3334290964190256, -0.12419885400344025, 0.13644995802526616, 0.030401793803850358... |
710.1495 | Limits of dihedral groups | We give a characterization of limits of dihedral groups in the space of
finitely generated marked groups.
We also describe the topological closure of dihedral groups in the space of
marked groups on a fixed number of generators.
| math.GR | we give a characterization of limits of dihedral groups in the space of finitely generated marked groups we also describe the topological closure of dihedral groups in the space of marked groups on a fixed number of generators | [['we', 'give', 'a', 'characterization', 'of', 'limits', 'of', 'dihedral', 'groups', 'in', 'the', 'space', 'of', 'finitely', 'generated', 'marked', 'groups', 'we', 'also', 'describe', 'the', 'topological', 'closure', 'of', 'dihedral', 'groups', 'in', 'the', 'space', 'of', 'marked', 'groups', 'on', 'a', 'fixed', 'number... | [-0.23227161811174532, 0.17780602625326106, -0.0949973689490243, 0.04189864359796047, -0.04353679643674312, -0.006153026424152286, 0.08134532538487722, 0.39294288140770633, -0.3079225086165886, -0.26804209696619136, 0.0643685915397088, -0.24680021321891168, -0.13177746816195154, 0.2610944123252442, -0.1289593918052943,... |
710.1496 | Self-organizing, two-temperature Ising model describing human
segregation | A two-temperature Ising-Schelling model is introduced and studied for
describing human segregation. The self-organized Ising model with Glauber
kinetics simulated by M\"uller et al. exhibits a phase transition between
segregated and mixed phases mimicking the change of tolerance (local
temperature) of individuals. Th... | physics.soc-ph cond-mat.stat-mech | a twotemperature isingschelling model is introduced and studied for describing human segregation the selforganized ising model with glauber kinetics simulated by muller et al exhibits a phase transition between segregated and mixed phases mimicking the change of tolerance local temperature of individuals the effect of ... | [['a', 'twotemperature', 'isingschelling', 'model', 'is', 'introduced', 'and', 'studied', 'for', 'describing', 'human', 'segregation', 'the', 'selforganized', 'ising', 'model', 'with', 'glauber', 'kinetics', 'simulated', 'by', 'muller', 'et', 'al', 'exhibits', 'a', 'phase', 'transition', 'between', 'segregated', 'and',... | [-0.11447358525104144, 0.21478790335066908, -0.07596272054769389, 0.030298074246263254, -0.041950709198589446, -0.16443418043169689, 0.08974346941844984, 0.34444211540719516, -0.21070234074753214, -0.3211025847001122, 0.0393695208522213, -0.25933850382442597, -0.16806768686450146, 0.0862604462686781, -0.027872323672371... |
710.1497 | Are galaxies with AGN a transition population? | We present the results of an analysis of a well-selected sample of galaxies
with active and inactive galactic nuclei from the Sloan Digital Sky Survey, in
the range 0.01 < z < 0.16. The SDSS galaxy catalogue was split into two classes
of active galaxies, Type~2 AGN and composites, and one set of inactive,
star-formin... | astro-ph | we present the results of an analysis of a wellselected sample of galaxies with active and inactive galactic nuclei from the sloan digital sky survey in the range 001 z 016 the sdss galaxy catalogue was split into two classes of active galaxies type2 agn and composites and one set of inactive starformingpassive galaxie... | [['we', 'present', 'the', 'results', 'of', 'an', 'analysis', 'of', 'a', 'wellselected', 'sample', 'of', 'galaxies', 'with', 'active', 'and', 'inactive', 'galactic', 'nuclei', 'from', 'the', 'sloan', 'digital', 'sky', 'survey', 'in', 'the', 'range', '001', 'z', '016', 'the', 'sdss', 'galaxy', 'catalogue', 'was', 'split'... | [-0.03564321016570693, 0.1165819727717793, -0.03820056944814963, 0.11324342447811583, -0.10765570605527094, -0.060105274920535856, 0.07878232704247293, 0.4888400688809766, -0.10020299665924354, -0.35880838725310954, 0.03544476194667957, -0.3334802563519405, -0.03304300616907596, 0.18399591369208376, -0.0368272081319345... |
710.1498 | Diffractive photoproduction of dijets in ep collisions at HERA | Diffractive photoproduction of dijets was measured with the ZEUS detector at
the ep collider HERA using an integrated luminosity of 77.2 pb-1. The
measurements were made in the kinematic range Q^2 < 1 GeV^2, 0.20 < y < 0.85
and x_pom < 0.025, where Q^2 is the photon virtuality, y is the inelasticity
and x_pom is the ... | hep-ex | diffractive photoproduction of dijets was measured with the zeus detector at the ep collider hera using an integrated luminosity of 772 pb1 the measurements were made in the kinematic range q2 1 gev2 020 y 085 and x_pom 0025 where q2 is the photon virtuality y is the inelasticity and x_pom is the fraction of the proton... | [['diffractive', 'photoproduction', 'of', 'dijets', 'was', 'measured', 'with', 'the', 'zeus', 'detector', 'at', 'the', 'ep', 'collider', 'hera', 'using', 'an', 'integrated', 'luminosity', 'of', '772', 'pb1', 'the', 'measurements', 'were', 'made', 'in', 'the', 'kinematic', 'range', 'q2', '1', 'gev2', '020', 'y', '085', ... | [-0.026568578864523285, 0.2397161665770303, -0.09298272437608994, 0.13968727094024788, -0.0028421491308993586, -0.04534856074170822, -0.025479927526887606, 0.41797117778175585, -0.1313362589089183, -0.33157201579704815, -0.07906305908145769, -0.4140658737411974, 0.20615076775419283, 0.15126676026832414, 0.0835096200965... |
710.1499 | Approximating max-min linear programs with local algorithms | A local algorithm is a distributed algorithm where each node must operate
solely based on the information that was available at system startup within a
constant-size neighbourhood of the node. We study the applicability of local
algorithms to max-min LPs where the objective is to maximise $\min_k \sum_v
c_{kv} x_v$ s... | cs.DC | a local algorithm is a distributed algorithm where each node must operate solely based on the information that was available at system startup within a constantsize neighbourhood of the node we study the applicability of local algorithms to maxmin lps where the objective is to maximise min_k sum_v c_kv x_v subject to s... | [['a', 'local', 'algorithm', 'is', 'a', 'distributed', 'algorithm', 'where', 'each', 'node', 'must', 'operate', 'solely', 'based', 'on', 'the', 'information', 'that', 'was', 'available', 'at', 'system', 'startup', 'within', 'a', 'constantsize', 'neighbourhood', 'of', 'the', 'node', 'we', 'study', 'the', 'applicability'... | [-0.170162427480574, 0.09825996005483878, 0.0017791537422607972, -0.023523224132731755, -0.04440524210788743, -0.22108488432846216, 0.06087354463451202, 0.40147475508736474, -0.2982511677626501, -0.24379700790381148, 0.043062293186300886, -0.3356441831088098, -0.07707189290326029, 0.09867033028787879, -0.03502529293727... |
710.15 | A 610-MHz survey of the ELAIS-N1 field with the Giant Metrewave Radio
Telescope - Observations, data analysis and source catalogue | Observations of the ELAIS-N1 field taken at 610 MHz with the Giant Metrewave
Radio Telescope are presented. Nineteen pointings were observed, covering a
total area of 9 square degrees with a resolution of 6" x 5", PA +45 deg. Four
of the pointings were deep observations with an rms of 40 microJy before
primary beam c... | astro-ph | observations of the elaisn1 field taken at 610 mhz with the giant metrewave radio telescope are presented nineteen pointings were observed covering a total area of 9 square degrees with a resolution of 6 x 5 pa 45 deg four of the pointings were deep observations with an rms of 40 microjy before primary beam correction ... | [['observations', 'of', 'the', 'elaisn1', 'field', 'taken', 'at', '610', 'mhz', 'with', 'the', 'giant', 'metrewave', 'radio', 'telescope', 'are', 'presented', 'nineteen', 'pointings', 'were', 'observed', 'covering', 'a', 'total', 'area', 'of', '9', 'square', 'degrees', 'with', 'a', 'resolution', 'of', '6', 'x', '5', 'p... | [-0.09411748061183177, 0.10039492851086493, 0.0004427483924133266, 0.03472182114496077, -0.03241579595565696, -0.07603888737503439, 0.07558509037711177, 0.4230405369761006, -0.13326162584251006, -0.4536238561053104, 0.14234983225615974, -0.35380020260110795, 0.01877283724181154, 0.20445496632308144, -0.0015772844343633... |
710.1501 | Horizons of stability in matrix Hamiltonians | Non-Hermitian Hamiltonians H possess the real (i.e., observable) spectra
inside certain specific domains of parameters D. In general, the determination
of their observability-horizon boundaries is difficult. We list the
pseudo-Hermitian real N by N matrix Hamiltonians for which the prototype
horizons are defined by c... | quant-ph | nonhermitian hamiltonians h possess the real ie observable spectra inside certain specific domains of parameters d in general the determination of their observabilityhorizon boundaries is difficult we list the pseudohermitian real n by n matrix hamiltonians for which the prototype horizons are defined by closed analyti... | [['nonhermitian', 'hamiltonians', 'h', 'possess', 'the', 'real', 'ie', 'observable', 'spectra', 'inside', 'certain', 'specific', 'domains', 'of', 'parameters', 'd', 'in', 'general', 'the', 'determination', 'of', 'their', 'observabilityhorizon', 'boundaries', 'is', 'difficult', 'we', 'list', 'the', 'pseudohermitian', 'r... | [-0.19851191402615412, 0.18208958714034373, 0.005312791904029639, 0.07114614124419978, -0.07607178147072377, -0.2246180354900982, -0.029853601170622784, 0.3818371696802585, -0.19915934947683758, -0.3045570992095315, 0.0875273407614061, -0.26483567557095183, -0.1475188631726348, 0.18305038579780122, -0.01235625125295685... |
710.1502 | Efficient 2-designs from bases exist | We show that in a complex d-dimensional vector space, one can find O(d) bases
whose elements form a 2-design. Such vector sets generalize the notion of a
maximal collection of mutually unbiased bases (MUBs). MUBs have manifold
applications in quantum information theory (e.g. in state tomography, cloning,
or cryptogra... | quant-ph | we show that in a complex ddimensional vector space one can find od bases whose elements form a 2design such vector sets generalize the notion of a maximal collection of mutually unbiased bases mubs mubs have manifold applications in quantum information theory eg in state tomography cloning or cryptography however it i... | [['we', 'show', 'that', 'in', 'a', 'complex', 'ddimensional', 'vector', 'space', 'one', 'can', 'find', 'od', 'bases', 'whose', 'elements', 'form', 'a', '2design', 'such', 'vector', 'sets', 'generalize', 'the', 'notion', 'of', 'a', 'maximal', 'collection', 'of', 'mutually', 'unbiased', 'bases', 'mubs', 'mubs', 'have', '... | [-0.12095999215644869, 0.10582614545829445, -0.04250341938088902, 0.02266471174185757, -0.06383813834664497, -0.14640433928421276, 0.045272091130556705, 0.33645991735075687, -0.24464231507683343, -0.24203225580806081, 0.09294619016899643, -0.26986680182374334, -0.1956705933373252, 0.20764148155523635, -0.10622143623503... |
710.1503 | Modeling the water line emission from the high-mass star-forming region
AFGL2591 | Context: observations of water lines are a sensitive probe of the geometry,
dynamics and chemical structure of dense molecular gas. The launch of Herschel
with on board HIFI and PACS allow to probe the behaviour of multiple water
lines with unprecedented sensitivity and resolution. Aims: we investigate the
diagnostic... | astro-ph | context observations of water lines are a sensitive probe of the geometry dynamics and chemical structure of dense molecular gas the launch of herschel with on board hifi and pacs allow to probe the behaviour of multiple water lines with unprecedented sensitivity and resolution aims we investigate the diagnostic value ... | [['context', 'observations', 'of', 'water', 'lines', 'are', 'a', 'sensitive', 'probe', 'of', 'the', 'geometry', 'dynamics', 'and', 'chemical', 'structure', 'of', 'dense', 'molecular', 'gas', 'the', 'launch', 'of', 'herschel', 'with', 'on', 'board', 'hifi', 'and', 'pacs', 'allow', 'to', 'probe', 'the', 'behaviour', 'of'... | [-0.060179841980016135, 0.11763082268640801, -0.03969119918656361, 0.07178251152481607, -0.05048505008335269, -0.10991051946439256, 0.02922428538568056, 0.4330525116311037, -0.1658348007422319, -0.33881798047696066, 0.08650051330414499, -0.2689978777743818, -0.03589939919575613, 0.14980847889819415, 0.03019223448916364... |
710.1504 | Searching for Mergers in Early-Type QSO Host Galaxies and a Control
Sample of Inactive Ellipticals | We present very deep HST/ACS images of five QSO host galaxies, classified as
undisturbed ellipticals in earlier studies. For four of the five objects, our
images reveal strong signs of interaction such as tidal tails, shells, and
other fine structure, suggesting that a large fraction of QSO host galaxies may
have exp... | astro-ph | we present very deep hstacs images of five qso host galaxies classified as undisturbed ellipticals in earlier studies for four of the five objects our images reveal strong signs of interaction such as tidal tails shells and other fine structure suggesting that a large fraction of qso host galaxies may have experienced ... | [['we', 'present', 'very', 'deep', 'hstacs', 'images', 'of', 'five', 'qso', 'host', 'galaxies', 'classified', 'as', 'undisturbed', 'ellipticals', 'in', 'earlier', 'studies', 'for', 'four', 'of', 'the', 'five', 'objects', 'our', 'images', 'reveal', 'strong', 'signs', 'of', 'interaction', 'such', 'as', 'tidal', 'tails', ... | [-0.10584787281884535, 0.026668874830057896, -0.10776069518682119, 0.11939234291580883, -0.13229403897767533, -0.0662786423140583, 0.0025766277528443448, 0.5090809808792295, -0.07228663591416301, -0.39094248298253564, 0.041021665430791374, -0.29824750619386703, -0.10300598240684013, 0.18584991059253445, -0.010060566936... |
710.1505 | Unparticle physics effects in (Lambda_b -> Lambda + missing energy)
processes | We study unparticle physics effects in (Lambda_b -> Lambda + missing energy)
decay with polarized $\Lambda_b$ and $\Lambda$ baryons. The sensitivity of the
branching ratio of this decay and polarizations of (Lambda_b) and (Lambda)
baryons on the scale dimension d_U and effective cut-off parameter (Lambda_U)
are discu... | hep-ph | we study unparticle physics effects in lambda_b lambda missing energy decay with polarized lambda_b and lambda baryons the sensitivity of the branching ratio of this decay and polarizations of lambda_b and lambda baryons on the scale dimension d_u and effective cutoff parameter lambda_u are discussed | [['we', 'study', 'unparticle', 'physics', 'effects', 'in', 'lambda_b', 'lambda', 'missing', 'energy', 'decay', 'with', 'polarized', 'lambda_b', 'and', 'lambda', 'baryons', 'the', 'sensitivity', 'of', 'the', 'branching', 'ratio', 'of', 'this', 'decay', 'and', 'polarizations', 'of', 'lambda_b', 'and', 'lambda', 'baryons'... | [-0.11492362851923746, 0.31542940150118537, -0.052889473136100505, 0.204328618847972, -0.10667870287886924, -0.12227797798501948, 0.010777815990149976, 0.2819711816807588, -0.22388582171665297, -0.22574989646673202, -0.0917702121582503, -0.33977316425492365, 0.06552866756295164, 0.02653778563770983, 0.2147281209213866,... |
710.1506 | Water vapor emission from IRC+10216 and other carbon-rich stars: model
predictions and prospects for multitransition observations | We have modeled the emission of H2O rotational lines from the extreme C-rich
star IRC+10216. Our treatment of the excitation of H2O emissions takes into
account the excitation of H2O both through collisions, and through the pumping
of the nu2 and nu3 vibrational states by dust emission and subsequent decay to
the gro... | astro-ph | we have modeled the emission of h2o rotational lines from the extreme crich star irc10216 our treatment of the excitation of h2o emissions takes into account the excitation of h2o both through collisions and through the pumping of the nu2 and nu3 vibrational states by dust emission and subsequent decay to the ground st... | [['we', 'have', 'modeled', 'the', 'emission', 'of', 'h2o', 'rotational', 'lines', 'from', 'the', 'extreme', 'crich', 'star', 'irc10216', 'our', 'treatment', 'of', 'the', 'excitation', 'of', 'h2o', 'emissions', 'takes', 'into', 'account', 'the', 'excitation', 'of', 'h2o', 'both', 'through', 'collisions', 'and', 'through... | [-0.037577410496465145, 0.1337134984776922, -0.0022887455035834553, 0.005908977650169743, -0.015150923651353919, -0.0723291319650364, 0.0680605823046009, 0.42382466676538666, -0.14551950904400382, -0.3089816477468671, 0.05751204447763372, -0.27988659844363795, -0.011143237457623424, 0.13235282431756354, 0.0502184057229... |
710.1507 | Critical Behavior of CP^1 at theta = pi, Haldane's Conjecture and the
Universality Class | Using an approach to analyze the theta dependence of systems with a
theta-term we recently proposed, the critical behavior of CP^1 at theta=pi is
studied. We find a region outside the strong coupling regime where Haldane's
conjecture is verified. The critical line however does not belong to the
universality class of ... | hep-lat cond-mat.stat-mech | using an approach to analyze the theta dependence of systems with a thetaterm we recently proposed the critical behavior of cp1 at thetapi is studied we find a region outside the strong coupling regime where haldanes conjecture is verified the critical line however does not belong to the universality class of the wessz... | [['using', 'an', 'approach', 'to', 'analyze', 'the', 'theta', 'dependence', 'of', 'systems', 'with', 'a', 'thetaterm', 'we', 'recently', 'proposed', 'the', 'critical', 'behavior', 'of', 'cp1', 'at', 'thetapi', 'is', 'studied', 'we', 'find', 'a', 'region', 'outside', 'the', 'strong', 'coupling', 'regime', 'where', 'hald... | [-0.19612338743530788, 0.12865824323492303, -0.06760664116053913, 0.030689591645764618, -0.04953949253003185, -0.21380816536167493, 0.06213541373323936, 0.30381625841479176, -0.22592512816190718, -0.26427848634238427, 0.06064837975785709, -0.27579919529290725, -0.18287761085308515, 0.15566553163628738, 0.00736457603365... |
710.1508 | Analysis of rare (B -> K_0*(1430) l^+ l^- decay) within QCD sum rules | Form factors of rare (B -> K_0*(1430) l^+ l^-$ decay) decay are calculated
within three-point QCD sum rules, with (K_0* (1430)) being the p-wave scalar
meson. The branching ratios are estimated when only short, as well as short and
long distance effects, are taken into account.It is obtained that the (B ->
K_0*(1430)... | hep-ph | form factors of rare b k_01430 l l decay decay are calculated within threepoint qcd sum rules with k_0 1430 being the pwave scalar meson the branching ratios are estimated when only short as well as short and long distance effects are taken into accountit is obtained that the b k_01430 l l lemu decay is measurable at l... | [['form', 'factors', 'of', 'rare', 'b', 'k_01430', 'l', 'l', 'decay', 'decay', 'are', 'calculated', 'within', 'threepoint', 'qcd', 'sum', 'rules', 'with', 'k_0', '1430', 'being', 'the', 'pwave', 'scalar', 'meson', 'the', 'branching', 'ratios', 'are', 'estimated', 'when', 'only', 'short', 'as', 'well', 'as', 'short', 'a... | [-0.15989148325891056, 0.3008143266086422, -0.031649687222116404, 0.17001411262511587, -0.1079510900336096, -0.2281306800986862, 0.05970005923882127, 0.3119945983358082, -0.2284719760396651, -0.17893033862734833, -0.01188027677458844, -0.321471887574132, 0.05070114055914538, 0.11111155855247662, 0.16917625470696726, 0.... |
710.1509 | Asymptotic Behavior of Inflated Lattice Polygons | We study the inflated phase of two dimensional lattice polygons with fixed
perimeter $N$ and variable area, associating a weight $\exp[pA - Jb ]$ to a
polygon with area $A$ and $b$ bends. For convex and column-convex polygons, we
show that $<A >/A_{max} = 1 - K(J)/\tilde{p}^2 +
\mathcal{O}(\rho^{-\tilde{p}})$, where ... | cond-mat.stat-mech | we study the inflated phase of two dimensional lattice polygons with fixed perimeter n and variable area associating a weight exppa jb to a polygon with area a and b bends for convex and columnconvex polygons we show that a a_max 1 kjtildep2 mathcalorhotildep where tildeppn gg 1 and rho1 the constant kj is found to be ... | [['we', 'study', 'the', 'inflated', 'phase', 'of', 'two', 'dimensional', 'lattice', 'polygons', 'with', 'fixed', 'perimeter', 'n', 'and', 'variable', 'area', 'associating', 'a', 'weight', 'exppa', 'jb', 'to', 'a', 'polygon', 'with', 'area', 'a', 'and', 'b', 'bends', 'for', 'convex', 'and', 'columnconvex', 'polygons', '... | [-0.15217115074554272, 0.1583652720514652, -0.05830297593554828, 0.0621635339777109, -0.04487847800282102, -0.23011148208340185, 0.08385459590802151, 0.4074873901755277, -0.2187801072192667, -0.23078905066590658, 0.0922360679215084, -0.33888485196944884, -0.10784031265926243, 0.15754387068636386, -0.07003028399055511, ... |
710.151 | On the growth of linear perturbations | We consider the linear growth of matter perturbations in various dark energy
(DE) models. We show the existence of a constraint valid at $z=0$ between the
background and dark energy parameters and the matter perturbations growth
parameters. For $\Lambda$CDM $\gamma'_0\equiv \frac{d\gamma}{dz}_0$ lies in a
very narrow... | astro-ph gr-qc | we consider the linear growth of matter perturbations in various dark energy de models we show the existence of a constraint valid at z0 between the background and dark energy parameters and the matter perturbations growth parameters for lambdacdm gamma_0equiv fracdgammadz_0 lies in a very narrow interval 00195 le gamm... | [['we', 'consider', 'the', 'linear', 'growth', 'of', 'matter', 'perturbations', 'in', 'various', 'dark', 'energy', 'de', 'models', 'we', 'show', 'the', 'existence', 'of', 'a', 'constraint', 'valid', 'at', 'z0', 'between', 'the', 'background', 'and', 'dark', 'energy', 'parameters', 'and', 'the', 'matter', 'perturbations... | [-0.12862214852721637, 0.17225149437742493, -0.10731454334890057, 0.13243291612078245, -0.078044886764793, -0.16808890626332118, 0.008947400498836664, 0.33579553763616743, -0.21545902942485026, -0.3286088879525889, 0.037449716691652896, -0.2723210040508336, -0.003908737125372841, 0.23665526496132708, 0.0027728486479124... |
710.1511 | Demographic growth and the distribution of language sizes | It is argued that the present log-normal distribution of language sizes is,
to a large extent, a consequence of demographic dynamics within the population
of speakers of each language. A two-parameter stochastic multiplicative process
is proposed as a model for the population dynamics of individual languages, and
app... | physics.data-an cs.CL physics.soc-ph | it is argued that the present lognormal distribution of language sizes is to a large extent a consequence of demographic dynamics within the population of speakers of each language a twoparameter stochastic multiplicative process is proposed as a model for the population dynamics of individual languages and applied ove... | [['it', 'is', 'argued', 'that', 'the', 'present', 'lognormal', 'distribution', 'of', 'language', 'sizes', 'is', 'to', 'a', 'large', 'extent', 'a', 'consequence', 'of', 'demographic', 'dynamics', 'within', 'the', 'population', 'of', 'speakers', 'of', 'each', 'language', 'a', 'twoparameter', 'stochastic', 'multiplicative... | [-0.06489958786828952, 0.06250646929679947, -0.1074858189010146, 0.12950547123494868, -0.033566575567238036, -0.08631854679604822, 0.07351895065512508, 0.34886801176365806, -0.264529094167731, -0.3198997217050584, 0.07579409907974133, -0.23602723555470054, -0.10796976845965467, 0.21100255410313945, -0.04345384054309265... |
710.1512 | Prompt dipole radiation in fusion reactions | The prompt gamma ray emission was investigated in the 16A MeV energy region
by means of the 36,40Ar+96,92Zr fusion reactions leading to a compound nucleus
in the vicinity of 132Ce. We show that the prompt radiation, which appears to
be still effective at such a high beam energy, has an angular distribution
pattern co... | nucl-ex | the prompt gamma ray emission was investigated in the 16a mev energy region by means of the 3640ar9692zr fusion reactions leading to a compound nucleus in the vicinity of 132ce we show that the prompt radiation which appears to be still effective at such a high beam energy has an angular distribution pattern consistent... | [['the', 'prompt', 'gamma', 'ray', 'emission', 'was', 'investigated', 'in', 'the', '16a', 'mev', 'energy', 'region', 'by', 'means', 'of', 'the', '3640ar9692zr', 'fusion', 'reactions', 'leading', 'to', 'a', 'compound', 'nucleus', 'in', 'the', 'vicinity', 'of', '132ce', 'we', 'show', 'that', 'the', 'prompt', 'radiation',... | [-0.08808674238280219, 0.16418688364374248, -0.09523592615478264, 0.08582992262672633, -0.008261934416441363, -0.03912637665926013, 0.0264928555523511, 0.40422006451990455, -0.2324468299280852, -0.2768339504254982, 0.008838524043676443, -0.3341423425008543, -0.001992170326411724, 0.1678885570348939, 0.04850374931957049... |
710.1513 | Passive Retrieval of Rayleigh Waves in Disordered Elastic Media | When averaged over sources or disorder, cross-correlation of diffuse fields
yield the Green's function between two passive sensors. This technique is
applied to elastic ultrasonic waves in an open scattering slab mimicking
seismic waves in the Earth's crust. It appears that the Rayleigh wave
reconstruction depends on... | cond-mat.other physics.class-ph | when averaged over sources or disorder crosscorrelation of diffuse fields yield the greens function between two passive sensors this technique is applied to elastic ultrasonic waves in an open scattering slab mimicking seismic waves in the earths crust it appears that the rayleigh wave reconstruction depends on the sca... | [['when', 'averaged', 'over', 'sources', 'or', 'disorder', 'crosscorrelation', 'of', 'diffuse', 'fields', 'yield', 'the', 'greens', 'function', 'between', 'two', 'passive', 'sensors', 'this', 'technique', 'is', 'applied', 'to', 'elastic', 'ultrasonic', 'waves', 'in', 'an', 'open', 'scattering', 'slab', 'mimicking', 'se... | [-0.17634108503598991, 0.20348224522728364, -0.07636809249113245, 0.07539454965835164, -0.11119334313950342, -0.057616328644543524, 0.0047548428041542445, 0.37456333471416703, -0.2888922310411567, -0.23401725885072133, 0.044557429549125276, -0.31296976772988805, -0.18793857584298565, 0.2250438909381401, 0.0323838200164... |
710.1514 | Intermediate rank and property RD | We introduce concepts of intermediate rank for countable groups that
"interpolate" between consecutive values of the classical (integer-valued)
rank. Various classes of groups are proved to have intermediate rank behaviors.
We are especially interested in interpolation between rank 1 and rank 2. For
instance, we cons... | math.MG math.GR math.KT math.OA | we introduce concepts of intermediate rank for countable groups that interpolate between consecutive values of the classical integervalued rank various classes of groups are proved to have intermediate rank behaviors we are especially interested in interpolation between rank 1 and rank 2 for instance we construct group... | [['we', 'introduce', 'concepts', 'of', 'intermediate', 'rank', 'for', 'countable', 'groups', 'that', 'interpolate', 'between', 'consecutive', 'values', 'of', 'the', 'classical', 'integervalued', 'rank', 'various', 'classes', 'of', 'groups', 'are', 'proved', 'to', 'have', 'intermediate', 'rank', 'behaviors', 'we', 'are'... | [-0.15163808126793, 0.13521952219424815, -0.056958962959714796, 0.1085998416651322, -0.024990581294928652, -0.21127392739417547, -0.006551185364545393, 0.3775514405878151, -0.30974883505166706, -0.24017734361906387, 0.11388869525203403, -0.2259398254452414, -0.18025919258938866, 0.15411531620418278, -0.0953802217831130... |
710.1515 | Ferromagnetic-like closure domains in ferroelectric ultrathin films | We simulate from first-principles the energetic, structural, and electronic
properties of ferroelectric domains in ultrathin capacitors made of a few unit
cells of BaTiO$_3$ between two metallic SrRuO$_3$ electrodes in short circuit.
The domains are stabilized down to two unit cells, adopting the form of a
domain of ... | cond-mat.mtrl-sci | we simulate from firstprinciples the energetic structural and electronic properties of ferroelectric domains in ultrathin capacitors made of a few unit cells of batio_3 between two metallic srruo_3 electrodes in short circuit the domains are stabilized down to two unit cells adopting the form of a domain of closure com... | [['we', 'simulate', 'from', 'firstprinciples', 'the', 'energetic', 'structural', 'and', 'electronic', 'properties', 'of', 'ferroelectric', 'domains', 'in', 'ultrathin', 'capacitors', 'made', 'of', 'a', 'few', 'unit', 'cells', 'of', 'batio_3', 'between', 'two', 'metallic', 'srruo_3', 'electrodes', 'in', 'short', 'circui... | [-0.16788420058088377, 0.16988852102086335, -0.007347055776044727, 0.0128760350185136, -0.03271036875744661, -0.17336236863707502, 0.05661931879352778, 0.4671294908225536, -0.28669117369689046, -0.25876831197490296, 0.028596502672104784, -0.3084149576195826, -0.12466888117836789, 0.19432513160010179, -0.000837758798152... |
710.1516 | Superselection Rules | This note provides a summary of the meaning of the term `Superselection Rule'
in Quantum Mechanics and Quantum-Field Theory. It is a slightly extended
version of a contribution to the Compendium of Quantum Physics: Concepts,
Experiments, History and Philosophy, edited by Friedel Weinert, Klaus
Hentschel, Daniel Green... | quant-ph | this note provides a summary of the meaning of the term superselection rule in quantum mechanics and quantumfield theory it is a slightly extended version of a contribution to the compendium of quantum physics concepts experiments history and philosophy edited by friedel weinert klaus hentschel daniel greenberger and b... | [['this', 'note', 'provides', 'a', 'summary', 'of', 'the', 'meaning', 'of', 'the', 'term', 'superselection', 'rule', 'in', 'quantum', 'mechanics', 'and', 'quantumfield', 'theory', 'it', 'is', 'a', 'slightly', 'extended', 'version', 'of', 'a', 'contribution', 'to', 'the', 'compendium', 'of', 'quantum', 'physics', 'conce... | [-0.07152502511627973, 0.1430463357269764, -0.18316468857228757, 0.10287579027935863, -0.12787133675068618, -0.14078609735704958, 0.06274033788358793, 0.18767905056476594, -0.24790834229439496, -0.2918047761172056, 0.047582642405759545, -0.29552083276212215, -0.19580234384164213, 0.15583556121215225, -0.138709261324256... |
710.1517 | Lattice QCD with two light Wilson quarks and maximally twisted mass | We summarise status and recent results of the European Twisted Mass
collaboration (ETMC). The collaboration has generated gauge configurations for
three different values of the lattice spacing smaller or equal 0.1 fm and
values of the charged pseudo scalar mass as low as 300 MeV with two flavours of
maximally twisted... | hep-lat | we summarise status and recent results of the european twisted mass collaboration etmc the collaboration has generated gauge configurations for three different values of the lattice spacing smaller or equal 01 fm and values of the charged pseudo scalar mass as low as 300 mev with two flavours of maximally twisted mass ... | [['we', 'summarise', 'status', 'and', 'recent', 'results', 'of', 'the', 'european', 'twisted', 'mass', 'collaboration', 'etmc', 'the', 'collaboration', 'has', 'generated', 'gauge', 'configurations', 'for', 'three', 'different', 'values', 'of', 'the', 'lattice', 'spacing', 'smaller', 'or', 'equal', '01', 'fm', 'and', 'v... | [-0.0899587879715444, 0.31896738446385126, -0.05109363685085893, 0.1201336880378306, -0.055961009718208346, -0.0973577021193409, 0.052763590842978166, 0.3537387251312476, -0.14077988640015382, -0.307413904013946, 0.05902319946827172, -0.3097060007627967, -0.03419879195584948, 0.10596414973423275, 0.02599146057375122, 0... |
710.1518 | Formation and evolution of bulges | After presenting three ways of defining a bulge component in disc galaxies,
we introduce the various types of bulges, namely the classical bulges, the
boxy/peanut bulges and the disc-like bulges. We then discuss three specific
topics linked to bulge formation and evolution, namely the coupled time
evolution of the ba... | astro-ph | after presenting three ways of defining a bulge component in disc galaxies we introduce the various types of bulges namely the classical bulges the boxypeanut bulges and the disclike bulges we then discuss three specific topics linked to bulge formation and evolution namely the coupled time evolution of the bar bucklin... | [['after', 'presenting', 'three', 'ways', 'of', 'defining', 'a', 'bulge', 'component', 'in', 'disc', 'galaxies', 'we', 'introduce', 'the', 'various', 'types', 'of', 'bulges', 'namely', 'the', 'classical', 'bulges', 'the', 'boxypeanut', 'bulges', 'and', 'the', 'disclike', 'bulges', 'we', 'then', 'discuss', 'three', 'spe... | [-0.11676531287786715, 0.03809755438979825, -0.10813563332125983, 0.1333614832803826, -0.08964435786337537, -0.04252216509570751, -0.05149059542728698, 0.38619503358324225, -0.22399581037461758, -0.2845151273889796, 0.009119678726967643, -0.2119855715701466, -0.09406522639534053, 0.13553443452452912, 0.0051908299244721... |
710.1519 | Strong Approximations of BSDEs in a domain | We study the strong approximation of a Backward SDE with finite stopping time
horizon, namely the first exit time of a forward SDE from a cylindrical domain.
We use the Euler scheme approach of Bouchard and Touzi, Zhang 04}. When the
domain is piecewise smooth and under a non-characteristic boundary condition,
we sho... | math.PR | we study the strong approximation of a backward sde with finite stopping time horizon namely the first exit time of a forward sde from a cylindrical domain we use the euler scheme approach of bouchard and touzi zhang 04 when the domain is piecewise smooth and under a noncharacteristic boundary condition we show that th... | [['we', 'study', 'the', 'strong', 'approximation', 'of', 'a', 'backward', 'sde', 'with', 'finite', 'stopping', 'time', 'horizon', 'namely', 'the', 'first', 'exit', 'time', 'of', 'a', 'forward', 'sde', 'from', 'a', 'cylindrical', 'domain', 'we', 'use', 'the', 'euler', 'scheme', 'approach', 'of', 'bouchard', 'and', 'touz... | [-0.1433123863065256, 0.08318140251529321, -0.10490806165902891, 0.0634807020766873, -0.08225512182699483, -0.14543988279949285, 0.04532374569884779, 0.38053507030647443, -0.2893299108887859, -0.24286142496694402, 0.15116951484314836, -0.22674598576492844, -0.08518392971324686, 0.17889318138712265, -0.04875813543861895... |
710.152 | Multicolor urn models with reducible replacement matrices | Consider the multicolored urn model where, after every draw, balls of the
different colors are added to the urn in a proportion determined by a given
stochastic replacement matrix. We consider some special replacement matrices
which are not irreducible. For three- and four-color urns, we derive the
asymptotic behavio... | math.PR | consider the multicolored urn model where after every draw balls of the different colors are added to the urn in a proportion determined by a given stochastic replacement matrix we consider some special replacement matrices which are not irreducible for three and fourcolor urns we derive the asymptotic behavior of line... | [['consider', 'the', 'multicolored', 'urn', 'model', 'where', 'after', 'every', 'draw', 'balls', 'of', 'the', 'different', 'colors', 'are', 'added', 'to', 'the', 'urn', 'in', 'a', 'proportion', 'determined', 'by', 'a', 'given', 'stochastic', 'replacement', 'matrix', 'we', 'consider', 'some', 'special', 'replacement', '... | [-0.0747897063644187, 0.15440116746201932, -0.06041937808786492, 0.07069742683212733, -0.017764817936870368, -0.15657936843356243, 0.05707201378270803, 0.38515377095312747, -0.23445787176589292, -0.23984846025614917, 0.1327772615974751, -0.30164955639804814, -0.10953858585178274, 0.1173607018206594, -0.1245297796355144... |
710.1521 | Algebraic quantum permutation groups | We discuss some algebraic aspects of quantum permutation groups, working over
arbitrary fields. If $K$ is any characteristic zero field, we show that there
exists a universal cosemisimple Hopf algebra coacting on the diagonal algebra
$K^n$: this is a refinement of Wang's universality theorem for the (compact)
quantum... | math.QA math.RA | we discuss some algebraic aspects of quantum permutation groups working over arbitrary fields if k is any characteristic zero field we show that there exists a universal cosemisimple hopf algebra coacting on the diagonal algebra kn this is a refinement of wangs universality theorem for the compact quantum permutation g... | [['we', 'discuss', 'some', 'algebraic', 'aspects', 'of', 'quantum', 'permutation', 'groups', 'working', 'over', 'arbitrary', 'fields', 'if', 'k', 'is', 'any', 'characteristic', 'zero', 'field', 'we', 'show', 'that', 'there', 'exists', 'a', 'universal', 'cosemisimple', 'hopf', 'algebra', 'coacting', 'on', 'the', 'diagon... | [-0.26509425798978875, 0.15701036466395155, -0.12611114053083036, 0.06256241556530928, -0.13851463568999486, -0.22349714461494893, 0.021021778092664832, 0.3516254668288371, -0.341701444873915, -0.1240018738214584, 0.11239957247915514, -0.1978403302253248, -0.16527302212574901, 0.21279756515560783, -0.08163186053142828,... |
710.1522 | Distributed spatial multiplexing with 1-bit feedback | We analyze a slow-fading interference network with MN non-cooperating
single-antenna sources and M non-cooperating single-antenna destinations. In
particular, we assume that the sources are divided into M mutually exclusive
groups of N sources each, every group is dedicated to transmit a common message
to a unique de... | cs.IT math.IT | we analyze a slowfading interference network with mn noncooperating singleantenna sources and m noncooperating singleantenna destinations in particular we assume that the sources are divided into m mutually exclusive groups of n sources each every group is dedicated to transmit a common message to a unique destination ... | [['we', 'analyze', 'a', 'slowfading', 'interference', 'network', 'with', 'mn', 'noncooperating', 'singleantenna', 'sources', 'and', 'm', 'noncooperating', 'singleantenna', 'destinations', 'in', 'particular', 'we', 'assume', 'that', 'the', 'sources', 'are', 'divided', 'into', 'm', 'mutually', 'exclusive', 'groups', 'of'... | [-0.23018546416523528, 0.05637870051443435, -0.053735652695723335, -0.027971240924671292, -0.078336700530043, -0.26676549500746044, 0.14275441962289867, 0.4241218422561601, -0.27466008810644255, -0.24343055657053728, 0.057805499052838535, -0.27332540259859855, -0.1479841720542354, 0.10536652166502312, -0.07080535746567... |
710.1523 | Extracting the CKM phase angle \gamma(\equiv \phi_3) from isospin
analysis in B\to K \pi decays | We propose a new method to extract the CKM phase angle \gamma (\equiv \phi_3)
from the isospin analysis in B \to K \pi decays. Unlike previously proposed
methods, we do not employ flavor SU(3) symmetry, so that this method is free
from the hadronic uncertainty coming from the SU(3) breaking effect. Neither we
adopt a... | hep-ph | we propose a new method to extract the ckm phase angle gamma equiv phi_3 from the isospin analysis in b to k pi decays unlike previously proposed methods we do not employ flavor su3 symmetry so that this method is free from the hadronic uncertainty coming from the su3 breaking effect neither we adopt any dalitzplot ana... | [['we', 'propose', 'a', 'new', 'method', 'to', 'extract', 'the', 'ckm', 'phase', 'angle', 'gamma', 'equiv', 'phi_3', 'from', 'the', 'isospin', 'analysis', 'in', 'b', 'to', 'k', 'pi', 'decays', 'unlike', 'previously', 'proposed', 'methods', 'we', 'do', 'not', 'employ', 'flavor', 'su3', 'symmetry', 'so', 'that', 'this', ... | [-0.11438491794536686, 0.22420418441665974, -0.08356162249852701, 0.08898010989583005, -0.11090305760742454, -0.1572540477762402, 0.13005102209253944, 0.3091194011837418, -0.26916725573277, -0.26480462632485124, 0.01385630438599888, -0.30123628593153423, -0.060908024087657185, 0.10131141196048617, 0.028800171424160925,... |
710.1524 | Gauge invariant nonlocal mass operator in YM theories | We briefly describe the construction of a renormalizable gauge model based on
the nonlocal gauge invariant mass operator F1/D^2F. We also take a look at the
unitarity of the resulting model.
| hep-th | we briefly describe the construction of a renormalizable gauge model based on the nonlocal gauge invariant mass operator f1d2f we also take a look at the unitarity of the resulting model | [['we', 'briefly', 'describe', 'the', 'construction', 'of', 'a', 'renormalizable', 'gauge', 'model', 'based', 'on', 'the', 'nonlocal', 'gauge', 'invariant', 'mass', 'operator', 'f1d2f', 'we', 'also', 'take', 'a', 'look', 'at', 'the', 'unitarity', 'of', 'the', 'resulting', 'model']] | [-0.11788122753302256, 0.17440214871118467, -0.1460655351014187, 0.1653500990321239, -0.07612886410206557, -0.16920812300716837, 0.022727736582358677, 0.3097936448951562, -0.18439307659864426, -0.20483526607664923, 0.052296445984393355, -0.22977809566849222, -0.17653005595008534, 0.0699192089183877, 0.01613940503448248... |
710.1525 | Efficient Optimally Lazy Algorithms for Minimal-Interval Semantics | Minimal-interval semantics associates with each query over a document a set
of intervals, called witnesses, that are incomparable with respect to inclusion
(i.e., they form an antichain): witnesses define the minimal regions of the
document satisfying the query. Minimal-interval semantics makes it easy to
define and ... | cs.DS cs.IR | minimalinterval semantics associates with each query over a document a set of intervals called witnesses that are incomparable with respect to inclusion ie they form an antichain witnesses define the minimal regions of the document satisfying the query minimalinterval semantics makes it easy to define and compute sever... | [['minimalinterval', 'semantics', 'associates', 'with', 'each', 'query', 'over', 'a', 'document', 'a', 'set', 'of', 'intervals', 'called', 'witnesses', 'that', 'are', 'incomparable', 'with', 'respect', 'to', 'inclusion', 'ie', 'they', 'form', 'an', 'antichain', 'witnesses', 'define', 'the', 'minimal', 'regions', 'of', ... | [-0.12350177891680804, 0.04052822455364199, -0.0533387364151004, 0.11541532202122304, -0.12132315399447599, -0.1451903770958336, 0.07893875149807755, 0.3955539165404983, -0.29190294678324463, -0.2808930633387391, 0.09055967499854234, -0.2867849381843534, -0.09918027203559923, 0.21118305842481697, -0.11433306443490064, ... |
710.1526 | Third Spectroscopy with a hint of superstrings | New regularities found in the pseudoscalar meson octet are reported. They
invite to reconsider models where elementary fermions and composite QCD open
strings can be grouped in common supermultiplets. It is proven that, with
fermions having the standard model charges, such grouping needs at least three
families.
| hep-ph | new regularities found in the pseudoscalar meson octet are reported they invite to reconsider models where elementary fermions and composite qcd open strings can be grouped in common supermultiplets it is proven that with fermions having the standard model charges such grouping needs at least three families | [['new', 'regularities', 'found', 'in', 'the', 'pseudoscalar', 'meson', 'octet', 'are', 'reported', 'they', 'invite', 'to', 'reconsider', 'models', 'where', 'elementary', 'fermions', 'and', 'composite', 'qcd', 'open', 'strings', 'can', 'be', 'grouped', 'in', 'common', 'supermultiplets', 'it', 'is', 'proven', 'that', 'w... | [-0.08506660195107156, 0.3032471358459047, -0.07986490782152147, 0.17351284979079712, -0.0961665789041906, -0.22614987277762688, 0.00012164239950002507, 0.37618408003386034, -0.19409775924175343, -0.301708996137406, 0.0036729569001955555, -0.3414024082507859, -0.06506336748010498, 0.04566495389519061, 0.012365748521257... |
710.1527 | Vertex-algebraic structure of the principal subspaces of certain
A_1^(1)-modules, II: higher level case | We give an a priori proof of the known presentations of (that is,
completeness of families of relations for) the principal subspaces of all the
standard A_1^(1)-modules. These presentations had been used by Capparelli,
Lepowsky and Milas for the purpose of obtaining the classical Rogers-Selberg
recursions for the gra... | math.QA hep-th math.RT | we give an a priori proof of the known presentations of that is completeness of families of relations for the principal subspaces of all the standard a_11modules these presentations had been used by capparelli lepowsky and milas for the purpose of obtaining the classical rogersselberg recursions for the graded dimensio... | [['we', 'give', 'an', 'a', 'priori', 'proof', 'of', 'the', 'known', 'presentations', 'of', 'that', 'is', 'completeness', 'of', 'families', 'of', 'relations', 'for', 'the', 'principal', 'subspaces', 'of', 'all', 'the', 'standard', 'a_11modules', 'these', 'presentations', 'had', 'been', 'used', 'by', 'capparelli', 'lepow... | [-0.11088766600808193, 0.045686649364958205, -0.08647487004255426, 0.05394557274171505, -0.07293477435275142, -0.06381645674239202, -0.010780985848496443, 0.29651228711009026, -0.2564808142066387, -0.24750690737032685, 0.11430300668018453, -0.23254774064467898, -0.15434273537890664, 0.23510956089815188, -0.139649839830... |
710.1528 | The energy release--stellar angular momentum independence in rotating
compact stars undergoing first-order phase transitions | We present the general relativistic calculation of the energy release
associated with a first order phase transition (PT) at the center of a rotating
neutron star (NS). The energy release, E_rel, is equal to the difference in
mass-energies between the initial (normal) phase configuration and the final
configuration c... | astro-ph | we present the general relativistic calculation of the energy release associated with a first order phase transition pt at the center of a rotating neutron star ns the energy release e_rel is equal to the difference in massenergies between the initial normal phase configuration and the final configuration containing a ... | [['we', 'present', 'the', 'general', 'relativistic', 'calculation', 'of', 'the', 'energy', 'release', 'associated', 'with', 'a', 'first', 'order', 'phase', 'transition', 'pt', 'at', 'the', 'center', 'of', 'a', 'rotating', 'neutron', 'star', 'ns', 'the', 'energy', 'release', 'e_rel', 'is', 'equal', 'to', 'the', 'differe... | [-0.09808958174113383, 0.16986428825042516, -0.062139674515742455, 0.08402986678193529, -0.049921499233326755, -0.07506859700465646, 0.03293780919021344, 0.3090251285995122, -0.1832397410571433, -0.33884007611688766, 0.0493282821457762, -0.264783734329514, 0.022680882761828763, 0.1779826960778788, 0.026290651386824102,... |
710.1529 | Optimum bias for fast-switching free energy calculations | We derive the bias function that minimizes the statistical error of free
energy differences calculated in work-biased fast-switching simulations. The
optimum bias function is compared to other bias functions using a particle
pulled through a viscous fluid as an illustrative example. Our analysis
indicates that the un... | cond-mat.stat-mech | we derive the bias function that minimizes the statistical error of free energy differences calculated in workbiased fastswitching simulations the optimum bias function is compared to other bias functions using a particle pulled through a viscous fluid as an illustrative example our analysis indicates that the uncertai... | [['we', 'derive', 'the', 'bias', 'function', 'that', 'minimizes', 'the', 'statistical', 'error', 'of', 'free', 'energy', 'differences', 'calculated', 'in', 'workbiased', 'fastswitching', 'simulations', 'the', 'optimum', 'bias', 'function', 'is', 'compared', 'to', 'other', 'bias', 'functions', 'using', 'a', 'particle', ... | [-0.09929230707348324, 0.10274777149084002, -0.08774399331014138, 0.11609360475631547, -0.03629845430259593, -0.09753809074027231, 0.0335326227650512, 0.37435102023300715, -0.2768645586220373, -0.3456332204514183, 0.06163466113866889, -0.30375944497063756, -0.10885508658248, 0.2240201955410157, -0.015164233336690813, 0... |
710.153 | Canonical Forms for Unitary Congruence and *Congruence | We use methods of the general theory of congruence and *congruence for
complex matrices--regularization and cosquares-to determine a unitary
congruence canonical form (respectively, a unitary *congruence canonical form)
for complex matrices A such that \bar{A}A (respectively, A^2) is normal.
As special cases of our... | math.RT | we use methods of the general theory of congruence and congruence for complex matricesregularization and cosquaresto determine a unitary congruence canonical form respectively a unitary congruence canonical form for complex matrices a such that baraa respectively a2 is normal as special cases of our canonical forms we ... | [['we', 'use', 'methods', 'of', 'the', 'general', 'theory', 'of', 'congruence', 'and', 'congruence', 'for', 'complex', 'matricesregularization', 'and', 'cosquaresto', 'determine', 'a', 'unitary', 'congruence', 'canonical', 'form', 'respectively', 'a', 'unitary', 'congruence', 'canonical', 'form', 'for', 'complex', 'mat... | [-0.11115855442206045, 0.13525782905401676, -0.07880603622527808, 0.10621120498742996, -0.10753189549436719, -0.1934411169403768, -0.0016476345772962232, 0.4126094484804418, -0.2798784643074307, -0.16983425151740061, 0.07532009556266207, -0.2621738145982216, -0.19787516108875375, 0.20340212334798077, -0.053341888331287... |
710.1531 | Far-Ultraviolet Cooling Features of the Antlia Supernova Remnant | We present far-ultraviolet observations of the Antlia supernova remnant
obtained with Far-ultraviolet IMaging Spectrograph (FIMS, also called SPEAR).
The strongest lines observed are C IV 1548,1551 and C III 977. The C IV
emission of this mixed-morphology supernova remnant shows a clumpy
distribution, and the line in... | astro-ph | we present farultraviolet observations of the antlia supernova remnant obtained with farultraviolet imaging spectrograph fims also called spear the strongest lines observed are c iv 15481551 and c iii 977 the c iv emission of this mixedmorphology supernova remnant shows a clumpy distribution and the line intensity is n... | [['we', 'present', 'farultraviolet', 'observations', 'of', 'the', 'antlia', 'supernova', 'remnant', 'obtained', 'with', 'farultraviolet', 'imaging', 'spectrograph', 'fims', 'also', 'called', 'spear', 'the', 'strongest', 'lines', 'observed', 'are', 'c', 'iv', '15481551', 'and', 'c', 'iii', '977', 'the', 'c', 'iv', 'emis... | [-0.08173904084287642, 0.06537767385816551, -0.005426278790764627, 0.0314710661641584, -0.06391449228249257, -0.18057200073235435, 0.05846948627913662, 0.45236156379178283, -0.20158458928199252, -0.2682901476891857, 0.06738252806280798, -0.29574383223371115, 0.012343002294073813, 0.14935004332801327, 0.0263091360725837... |
710.1532 | A step towards the Analysis of the Influence of an electrical Field on
the Propagation of Light | It is a matter of common knowledge that the field of gravitation influences
the propagation of light, but the question to which extent electromagnetic
fields do something similar is not completely answered. The birefringence
caused by electric and magnetic fields is subject of several articles in
Quantumelectrodynami... | physics.gen-ph | it is a matter of common knowledge that the field of gravitation influences the propagation of light but the question to which extent electromagnetic fields do something similar is not completely answered the birefringence caused by electric and magnetic fields is subject of several articles in quantumelectrodynamics b... | [['it', 'is', 'a', 'matter', 'of', 'common', 'knowledge', 'that', 'the', 'field', 'of', 'gravitation', 'influences', 'the', 'propagation', 'of', 'light', 'but', 'the', 'question', 'to', 'which', 'extent', 'electromagnetic', 'fields', 'do', 'something', 'similar', 'is', 'not', 'completely', 'answered', 'the', 'birefring... | [-0.11220541172143486, 0.16368121618999995, -0.1017807440849504, 0.06837563037837821, -0.12481396042362407, -0.10446181892313891, 0.014126441417330946, 0.41218053756488693, -0.21388997823275901, -0.3627893576743426, 0.08414581907240468, -0.2532165738650494, -0.1468119739692796, 0.2118611399023966, -0.07572441050713813,... |
710.1533 | Determination of the running coupling in pure SU(4) Yang-Mills theory | The Schrodinger functional is used to define a renormalised coupling for pure
SU(4) Yang-Mills theory, with Wilson action and suitably selected boundary
conditions on the link field. The coupling, which runs with the size of the
lattice, is then determined by a finite-size scaling technique through a large
range of m... | hep-lat | the schrodinger functional is used to define a renormalised coupling for pure su4 yangmills theory with wilson action and suitably selected boundary conditions on the link field the coupling which runs with the size of the lattice is then determined by a finitesize scaling technique through a large range of momenta the... | [['the', 'schrodinger', 'functional', 'is', 'used', 'to', 'define', 'a', 'renormalised', 'coupling', 'for', 'pure', 'su4', 'yangmills', 'theory', 'with', 'wilson', 'action', 'and', 'suitably', 'selected', 'boundary', 'conditions', 'on', 'the', 'link', 'field', 'the', 'coupling', 'which', 'runs', 'with', 'the', 'size', ... | [-0.14252890835707197, 0.1801740650433856, -0.0948750284076549, 0.05891742510198711, -0.03765230341098057, -0.11925669006991367, 0.07130686569069393, 0.32489924590127206, -0.23260013835925536, -0.31759809836960184, 0.07293104899909873, -0.2566374267797726, -0.08383860909424794, 0.13062462258713844, 0.053286374419724614... |
710.1534 | Moments of generalized parton distributions and quark angular momentum
of the nucleon | The internal structure of hadrons is important for a variety of topics,
including the hadron form factors, proton spin and spin asymmetry in polarized
proton scattering.
For a systematic study generalized parton distributions (GPDs) encode
important information on hadron structure in the entire impact parameter spa... | hep-lat | the internal structure of hadrons is important for a variety of topics including the hadron form factors proton spin and spin asymmetry in polarized proton scattering for a systematic study generalized parton distributions gpds encode important information on hadron structure in the entire impact parameter space we rep... | [['the', 'internal', 'structure', 'of', 'hadrons', 'is', 'important', 'for', 'a', 'variety', 'of', 'topics', 'including', 'the', 'hadron', 'form', 'factors', 'proton', 'spin', 'and', 'spin', 'asymmetry', 'in', 'polarized', 'proton', 'scattering', 'for', 'a', 'systematic', 'study', 'generalized', 'parton', 'distribution... | [-0.07339978823955688, 0.28194176320814424, -0.14919188065816544, 0.13899804337803895, -0.0985365990601066, -0.006285438629695111, 0.04102607985259965, 0.3638869224737088, -0.14061791553265518, -0.21875421329815353, -0.03639285601934211, -0.2866763323545456, -0.005935854837298393, 0.12263622159759204, 0.100285798275338... |
710.1535 | Charmonium dynamics in heavy ion collisions | Applying the HSD transport approach to charmonium dynamics within the
'hadronic comover model' and the 'QGP melting scenario', we show that the
suppression pattern seen at RHIC cannot be explained by the interaction with
baryons, comoving mesons and/or by color screening mechanism. The interaction
with hadrons in the... | nucl-th hep-ph | applying the hsd transport approach to charmonium dynamics within the hadronic comover model and the qgp melting scenario we show that the suppression pattern seen at rhic cannot be explained by the interaction with baryons comoving mesons andor by color screening mechanism the interaction with hadrons in the late stag... | [['applying', 'the', 'hsd', 'transport', 'approach', 'to', 'charmonium', 'dynamics', 'within', 'the', 'hadronic', 'comover', 'model', 'and', 'the', 'qgp', 'melting', 'scenario', 'we', 'show', 'that', 'the', 'suppression', 'pattern', 'seen', 'at', 'rhic', 'can', 'not', 'be', 'explained', 'by', 'the', 'interaction', 'wit... | [-0.05935458091513838, 0.23444769482751834, -0.15446322205302826, 0.13583631721084496, 0.0014301736639828373, -0.11288310081492793, 0.01980471226655073, 0.33662061959947065, -0.21298398606289745, -0.2757950115601643, -0.0553219688087465, -0.32106321106143926, 0.03227910502058783, 0.06760753750193359, 0.0627808809868391... |
710.1536 | First CNGS events detected by LVD | The CERN Neutrino to Gran Sasso (CNGS) project aims to produce a high energy,
wide band $\nu_{\mu}$ beam at CERN and send it toward the INFN Gran Sasso
National Laboratory (LNGS), 732 km away. Its main goal is the observation of
the $\nu_{\tau}$ appearance, through neutrino flavour oscillation. The beam
started its o... | hep-ex | the cern neutrino to gran sasso cngs project aims to produce a high energy wide band nu_mu beam at cern and send it toward the infn gran sasso national laboratory lngs 732 km away its main goal is the observation of the nu_tau appearance through neutrino flavour oscillation the beam started its operation in august 2006... | [['the', 'cern', 'neutrino', 'to', 'gran', 'sasso', 'cngs', 'project', 'aims', 'to', 'produce', 'a', 'high', 'energy', 'wide', 'band', 'nu_mu', 'beam', 'at', 'cern', 'and', 'send', 'it', 'toward', 'the', 'infn', 'gran', 'sasso', 'national', 'laboratory', 'lngs', '732', 'km', 'away', 'its', 'main', 'goal', 'is', 'the', ... | [-0.09883611028515331, 0.22161081387830062, -0.08429786207787358, 0.07179129227269881, -0.05609796992613105, -0.10715093928587249, 0.06993574355398928, 0.3147623467260942, -0.16447070411930784, -0.3999543650310457, 0.0636545962811719, -0.3711788500879165, 0.07616804305814191, 0.19502686714482179, -0.003507526855417124,... |
710.1537 | Simultaneous H.E.S.S. and Chandra observations of Sgr A* during an X-ray
flare | The rapidly varying non-thermal X-ray emission observed from Sgr A* points to
particle acceleration taking place close to the supermassive black hole. The
TeV gamma-ray source HESS J1745-290 is coincident with Sgr A* and may be
closely related to the X-ray emission. Simultaneous X-ray and TeV observations
are require... | astro-ph | the rapidly varying nonthermal xray emission observed from sgr a points to particle acceleration taking place close to the supermassive black hole the tev gammaray source hess j1745290 is coincident with sgr a and may be closely related to the xray emission simultaneous xray and tev observations are required to elucida... | [['the', 'rapidly', 'varying', 'nonthermal', 'xray', 'emission', 'observed', 'from', 'sgr', 'a', 'points', 'to', 'particle', 'acceleration', 'taking', 'place', 'close', 'to', 'the', 'supermassive', 'black', 'hole', 'the', 'tev', 'gammaray', 'source', 'hess', 'j1745290', 'is', 'coincident', 'with', 'sgr', 'a', 'and', 'm... | [-0.0588957752749723, 0.14504560302791236, -0.029842988768255703, 0.1507464169607764, -0.0994800559378096, -0.08105074732032205, 0.06394130700999605, 0.4372486282805247, -0.1748708741706131, -0.4001276549351003, 0.039448369273616536, -0.3470522143079766, -0.0035528015112504365, 0.23464747638291947, -0.02476205448578444... |
710.1538 | Integrable boundary conditions and modified Lax equations | We consider integrable boundary conditions for both discrete and continuum
classical integrable models. Local integrals of motion generated by the
corresponding transfer matrices give rise to time evolution equations for the
initial Lax operator. We systematically identify the modified Lax pairs for
both discrete and... | hep-th math-ph math.MP math.QA nlin.SI | we consider integrable boundary conditions for both discrete and continuum classical integrable models local integrals of motion generated by the corresponding transfer matrices give rise to time evolution equations for the initial lax operator we systematically identify the modified lax pairs for both discrete and con... | [['we', 'consider', 'integrable', 'boundary', 'conditions', 'for', 'both', 'discrete', 'and', 'continuum', 'classical', 'integrable', 'models', 'local', 'integrals', 'of', 'motion', 'generated', 'by', 'the', 'corresponding', 'transfer', 'matrices', 'give', 'rise', 'to', 'time', 'evolution', 'equations', 'for', 'the', '... | [-0.08919773208567519, 0.08960169708508806, -0.06333967115216214, 0.15374336630940952, -0.0780933401105797, -0.1849991798176077, -0.06496388351159363, 0.34815481835012807, -0.33103790513143455, -0.19799426866791628, 0.13588763931204148, -0.22435887922243825, -0.12265951824695642, 0.12381515751496472, -0.011015035693758... |
710.1539 | Theoretical and experimental \alpha decay half-lives of the heaviest
odd-Z elements and general predictions | Theoretical decay half-lives of the heaviest odd-Z nuclei are calculated
using the experimental Q value. The barriers in the quasimolecular shape path
are determined within a Generalized Liquid Drop Model (GLDM) and the WKB
approximation is used. The results are compared with calculations using the
Density-Dependent ... | nucl-ex | theoretical decay halflives of the heaviest oddz nuclei are calculated using the experimental q value the barriers in the quasimolecular shape path are determined within a generalized liquid drop model gldm and the wkb approximation is used the results are compared with calculations using the densitydependent m3y ddm3y... | [['theoretical', 'decay', 'halflives', 'of', 'the', 'heaviest', 'oddz', 'nuclei', 'are', 'calculated', 'using', 'the', 'experimental', 'q', 'value', 'the', 'barriers', 'in', 'the', 'quasimolecular', 'shape', 'path', 'are', 'determined', 'within', 'a', 'generalized', 'liquid', 'drop', 'model', 'gldm', 'and', 'the', 'wkb... | [-0.015639431818615733, 0.14412570547855158, -0.07693405791119796, 0.10166235197808476, 0.019912235614821666, -0.14235903875990294, 0.07482154326564742, 0.3663716517960814, -0.16592710321186124, -0.30510859903842796, -0.004537965827364856, -0.33294315772556415, -0.006526652903215388, 0.20596825705261856, 0.047066558897... |
710.154 | Jet quenching parameter \hat q in the stochastic QCD vacuum with Landau
damping | We argue that the radiative energy loss of a parton traversing the
quark-gluon plasma is determined by Landau damping of soft modes in the plasma.
Using this idea, we calculate the jet quenching parameter of a gluon. The
calculation is done in SU(3) quenched QCD within the stochastic vacuum model.
At the LHC-relevant... | hep-ph | we argue that the radiative energy loss of a parton traversing the quarkgluon plasma is determined by landau damping of soft modes in the plasma using this idea we calculate the jet quenching parameter of a gluon the calculation is done in su3 quenched qcd within the stochastic vacuum model at the lhcrelevant temperatu... | [['we', 'argue', 'that', 'the', 'radiative', 'energy', 'loss', 'of', 'a', 'parton', 'traversing', 'the', 'quarkgluon', 'plasma', 'is', 'determined', 'by', 'landau', 'damping', 'of', 'soft', 'modes', 'in', 'the', 'plasma', 'using', 'this', 'idea', 'we', 'calculate', 'the', 'jet', 'quenching', 'parameter', 'of', 'a', 'gl... | [-0.062351636383433835, 0.2981069774945601, -0.1455349151262091, 0.10738960032473381, -0.014884500162171887, -0.03772154380793421, 0.042428973447350624, 0.38471609500499027, -0.17919193354697482, -0.2375066966695476, -0.028314784448932928, -0.28808407472826325, 0.0327545025440168, 0.11467143092575727, 0.068853663662629... |
710.1541 | Constraints on Brane Inflation and Cosmic Strings | By considering simple, but representative, models of brane inflation from a
single brane-antibrane pair in the slow roll regime, we provide constraints on
the parameters of the theory imposed by measurements of the CMB anisotropies by
WMAP including a cosmic string component. We find that inclusion of the string
comp... | astro-ph | by considering simple but representative models of brane inflation from a single braneantibrane pair in the slow roll regime we provide constraints on the parameters of the theory imposed by measurements of the cmb anisotropies by wmap including a cosmic string component we find that inclusion of the string component i... | [['by', 'considering', 'simple', 'but', 'representative', 'models', 'of', 'brane', 'inflation', 'from', 'a', 'single', 'braneantibrane', 'pair', 'in', 'the', 'slow', 'roll', 'regime', 'we', 'provide', 'constraints', 'on', 'the', 'parameters', 'of', 'the', 'theory', 'imposed', 'by', 'measurements', 'of', 'the', 'cmb', '... | [-0.11814469187172287, 0.17355697883449975, -0.07244142097481918, 0.1078216579517515, -0.07941806209643554, -0.13764521436086882, 0.025905136197966427, 0.3119158548537955, -0.24087047911843146, -0.32318681666288074, 0.11877347194430828, -0.29346044271940663, -0.07225281566329231, 0.21321040544023512, -0.002442964594201... |
710.1542 | The initial-final mass relationship from white dwarfs in common proper
motion pairs | The initial-final mass relationship of white dwarfs, which is poorly
constrained, is of paramount importance for different aspects in modern
astrophysics. From an observational perspective, most of the studies up to now
have been done using white dwarfs in open clusters. In order to improve the
initial-final mass rel... | astro-ph | the initialfinal mass relationship of white dwarfs which is poorly constrained is of paramount importance for different aspects in modern astrophysics from an observational perspective most of the studies up to now have been done using white dwarfs in open clusters in order to improve the initialfinal mass relationship... | [['the', 'initialfinal', 'mass', 'relationship', 'of', 'white', 'dwarfs', 'which', 'is', 'poorly', 'constrained', 'is', 'of', 'paramount', 'importance', 'for', 'different', 'aspects', 'in', 'modern', 'astrophysics', 'from', 'an', 'observational', 'perspective', 'most', 'of', 'the', 'studies', 'up', 'to', 'now', 'have',... | [-0.054397290465313684, 0.10662517809196712, -0.09398321585166593, 0.11743034837485919, -0.13485202986292194, -0.05016582473072895, 0.10618504237080383, 0.37513716491155846, -0.19730327559559238, -0.3672675556481578, 0.07052475522965367, -0.29008750968374486, -0.062381752866298656, 0.2071194695395439, -0.11356084798137... |
710.1543 | Symmetric bundles and representations of Lie triple systems | We define symmetric bundles as vector bundles in the category of symmetric
spaces; it is shown that this notion is the geometric analog of the one of a
representation of a Lie triple system. We show that such a bundle has an
underlying reflection space, and we investigate the corresponding forgetful
functor both from... | math.DG | we define symmetric bundles as vector bundles in the category of symmetric spaces it is shown that this notion is the geometric analog of the one of a representation of a lie triple system we show that such a bundle has an underlying reflection space and we investigate the corresponding forgetful functor both from the ... | [['we', 'define', 'symmetric', 'bundles', 'as', 'vector', 'bundles', 'in', 'the', 'category', 'of', 'symmetric', 'spaces', 'it', 'is', 'shown', 'that', 'this', 'notion', 'is', 'the', 'geometric', 'analog', 'of', 'the', 'one', 'of', 'a', 'representation', 'of', 'a', 'lie', 'triple', 'system', 'we', 'show', 'that', 'such... | [-0.179674728716592, 0.033097411830607125, -0.11269429296700527, 0.06991721226823637, -0.11412189629070622, -0.09980898381352586, -0.027837942917476936, 0.39414548418110074, -0.373943615583298, -0.17244973449724849, 0.12358141683279941, -0.21218131279696853, -0.24556883265082116, 0.14387369864498792, -0.137960299449648... |
710.1544 | On the projective geometry of the supercircle: a unified construction of
the super cross-ratio and Schwarzian derivative | We consider the standard contact structure on the supercircle, S^{1|1}, and
the supergroups E(1|1), Aff(1|1) and SpO(2|1) of contactomorphisms, defining
the Euclidean, affine and projective geometry respectively. Using the new
notion of (p|q)-transitivity, we construct in synthetic fashion even and odd
invariants cha... | math-ph hep-th math.DG math.MP | we consider the standard contact structure on the supercircle s11 and the supergroups e11 aff11 and spo21 of contactomorphisms defining the euclidean affine and projective geometry respectively using the new notion of pqtransitivity we construct in synthetic fashion even and odd invariants characterizing each geometry ... | [['we', 'consider', 'the', 'standard', 'contact', 'structure', 'on', 'the', 'supercircle', 's11', 'and', 'the', 'supergroups', 'e11', 'aff11', 'and', 'spo21', 'of', 'contactomorphisms', 'defining', 'the', 'euclidean', 'affine', 'and', 'projective', 'geometry', 'respectively', 'using', 'the', 'new', 'notion', 'of', 'pqt... | [-0.1726542245130986, 0.06541050771295832, -0.06756642356306068, 0.06722751182421823, -0.07133125317392543, -0.143262556178824, -0.0350891368374612, 0.31552156868445524, -0.26928698582547334, -0.2502237041535623, 0.1414472224567469, -0.25991149690440474, -0.1777722221415709, 0.1767916002214941, -0.10210026588619632, -0... |
710.1545 | Radiative and isospin-violating decays of Ds mesons in the hadrogenesis
conjecture | The masses and decays of the scalar D_{s0}^*(2317) and axial-vector
D_{s1}^*(2460) charmed strange mesons are calculated consistently in the
hadrogenesis conjecture. These mesons decay either strongly into the
isospin-violating pi^0 D_s and pi^0 D_s^* channels or electromagnetically. They
are generated by coupled-cha... | hep-ph | the masses and decays of the scalar d_s02317 and axialvector d_s12460 charmed strange mesons are calculated consistently in the hadrogenesis conjecture these mesons decay either strongly into the isospinviolating pi0 d_s and pi0 d_s channels or electromagnetically they are generated by coupledchannel dynamics based on ... | [['the', 'masses', 'and', 'decays', 'of', 'the', 'scalar', 'd_s02317', 'and', 'axialvector', 'd_s12460', 'charmed', 'strange', 'mesons', 'are', 'calculated', 'consistently', 'in', 'the', 'hadrogenesis', 'conjecture', 'these', 'mesons', 'decay', 'either', 'strongly', 'into', 'the', 'isospinviolating', 'pi0', 'd_s', 'and... | [-0.15342028631232954, 0.30050526595039306, -0.06995162270648186, 0.14271853777703228, -0.06844663907832, -0.10533204308217939, 0.011944759869263234, 0.30791503736639725, -0.16574914213269948, -0.2018114774104427, -0.07050191867233747, -0.33971384598133975, -0.05640396102852024, 0.04806652006501441, 0.11834784803692909... |
710.1546 | Hydrostatic pressure effects on the electrical transport properties of
Pr0.5Sr0.5MnO3 | We studied single-crystalline Pr0.5Sr0.5MnO3 by means of measurements of
magnetic susceptibility and specific heat at ambient pressure (P), and
electrical resistivity (r) in hydrostatic pressures up to 2 GPa. This material
displays ferromagnetic (FM) order, with Curie temperature TC ~ 255 K. A
crystallographic transf... | cond-mat.str-el | we studied singlecrystalline pr05sr05mno3 by means of measurements of magnetic susceptibility and specific heat at ambient pressure p and electrical resistivity r in hydrostatic pressures up to 2 gpa this material displays ferromagnetic fm order with curie temperature tc 255 k a crystallographic transformation from i4m... | [['we', 'studied', 'singlecrystalline', 'pr05sr05mno3', 'by', 'means', 'of', 'measurements', 'of', 'magnetic', 'susceptibility', 'and', 'specific', 'heat', 'at', 'ambient', 'pressure', 'p', 'and', 'electrical', 'resistivity', 'r', 'in', 'hydrostatic', 'pressures', 'up', 'to', '2', 'gpa', 'this', 'material', 'displays',... | [-0.18289544492749532, 0.27958941814991145, -0.012912821906278482, -0.08268578528390767, -0.034829693803420436, -0.14451363371470227, 0.1867143001837226, 0.3714644441381097, -0.28446962097659706, -0.32914311237669047, 0.03563522153372805, -0.3789426300746317, -0.02486789906039261, 0.13377335398422124, 0.086989058377310... |
710.1547 | Space cowboys odyssey: beyond the Gould Belt | We present our new advanced model for population synthesis of close-by
cooling NSs. Detailed treatment of the initial spatial distribution of NS
progenitors and a detailed ISM structure up to 3 kpc give us an opportunity to
discuss the strategy to look for new isolated cooling NSs. Our main results in
this respect ar... | astro-ph | we present our new advanced model for population synthesis of closeby cooling nss detailed treatment of the initial spatial distribution of ns progenitors and a detailed ism structure up to 3 kpc give us an opportunity to discuss the strategy to look for new isolated cooling nss our main results in this respect are the... | [['we', 'present', 'our', 'new', 'advanced', 'model', 'for', 'population', 'synthesis', 'of', 'closeby', 'cooling', 'nss', 'detailed', 'treatment', 'of', 'the', 'initial', 'spatial', 'distribution', 'of', 'ns', 'progenitors', 'and', 'a', 'detailed', 'ism', 'structure', 'up', 'to', '3', 'kpc', 'give', 'us', 'an', 'oppor... | [-0.03927989803042596, 0.12278504718989001, -0.08476293922356534, 0.1462796168104647, -0.13653049496100927, -0.08737123856033252, 0.11748001055708684, 0.4038014891519537, -0.1980490138133367, -0.3698208935552171, 0.0406815976091865, -0.2793001672858751, 0.006924212938628909, 0.239921355190331, -0.0498734182714602, -0.0... |
710.1548 | Propagation and interaction of chiral states in quantum gravity | We study the stability, propagation and interactions of braid states in
models of quantum gravity in which the states are four-valent spin networks
embedded in a topological three manifold and the evolution moves are given by
the dual Pachner moves. There are results for both the framed and unframed
case. We study si... | hep-th gr-qc math-ph math.MP | we study the stability propagation and interactions of braid states in models of quantum gravity in which the states are fourvalent spin networks embedded in a topological three manifold and the evolution moves are given by the dual pachner moves there are results for both the framed and unframed case we study simple b... | [['we', 'study', 'the', 'stability', 'propagation', 'and', 'interactions', 'of', 'braid', 'states', 'in', 'models', 'of', 'quantum', 'gravity', 'in', 'which', 'the', 'states', 'are', 'fourvalent', 'spin', 'networks', 'embedded', 'in', 'a', 'topological', 'three', 'manifold', 'and', 'the', 'evolution', 'moves', 'are', '... | [-0.2065720129960581, 0.21751719382692777, -0.03177796697317441, 0.08149451905173129, -0.046839510060279914, -0.16620636219664922, -0.0032616930978332202, 0.4210884829416223, -0.2773448049455233, -0.30938476917293406, 0.08677850573187006, -0.3120786603540182, -0.16048734882117613, 0.14196631780688893, -0.02368275271020... |
710.1549 | Phase separation in a polarized Fermi gas at zero temperature | We investigate the phase diagram of asymmetric two-component Fermi gases at
zero temperature as a function of polarization and interaction strength. The
equations of state of the uniform superfluid and normal phase are determined
using quantum Monte Carlo simulations. We find three different mixed states,
where the s... | cond-mat.other | we investigate the phase diagram of asymmetric twocomponent fermi gases at zero temperature as a function of polarization and interaction strength the equations of state of the uniform superfluid and normal phase are determined using quantum monte carlo simulations we find three different mixed states where the superfl... | [['we', 'investigate', 'the', 'phase', 'diagram', 'of', 'asymmetric', 'twocomponent', 'fermi', 'gases', 'at', 'zero', 'temperature', 'as', 'a', 'function', 'of', 'polarization', 'and', 'interaction', 'strength', 'the', 'equations', 'of', 'state', 'of', 'the', 'uniform', 'superfluid', 'and', 'normal', 'phase', 'are', 'd... | [-0.1486503838601133, 0.3061251077163903, -0.10369555934096922, 0.052045317663514355, 0.029869691612055667, -0.13890432974753472, 0.09443130030726585, 0.3681345123101722, -0.29853450023865963, -0.218169916730763, 0.00433070201216941, -0.2908093984351381, -0.01494097202033787, 0.11041010764765215, 0.13044773510933577, 0... |
710.155 | VLT Spectroscopy of Globular Clusters in Low Surface Brightness Dwarf
Galaxies | We present VLT/FORS2 spectroscopic observations of globular clusters (GCs) in
five low surface brightness (LSB) dwarf galaxies: KK211 and KK221, which are
both dwarf spheroidal satellites (dSph) of NGC 5128, dSph KK84 located close to
the isolated S0 galaxy NGC 3115, and two isolated dwarf irregular (dIrr)
galaxies U... | astro-ph | we present vltfors2 spectroscopic observations of globular clusters gcs in five low surface brightness lsb dwarf galaxies kk211 and kk221 which are both dwarf spheroidal satellites dsph of ngc 5128 dsph kk84 located close to the isolated s0 galaxy ngc 3115 and two isolated dwarf irregular dirr galaxies ugc 3755 and eso... | [['we', 'present', 'vltfors2', 'spectroscopic', 'observations', 'of', 'globular', 'clusters', 'gcs', 'in', 'five', 'low', 'surface', 'brightness', 'lsb', 'dwarf', 'galaxies', 'kk211', 'and', 'kk221', 'which', 'are', 'both', 'dwarf', 'spheroidal', 'satellites', 'dsph', 'of', 'ngc', '5128', 'dsph', 'kk84', 'located', 'cl... | [-0.010458909389726295, 0.033964693567535856, -0.11628089801800487, 0.11764147693756968, -0.1040465115357125, -0.06897420857689883, 0.045577580431933724, 0.4863721575931107, -0.06158557329367716, -0.4216540947099004, -0.027792459881554047, -0.33867043796354873, -0.008278690622465914, 0.21925708595152715, -0.06857958250... |
710.1551 | The Inductive Kernels of Graphs | It is well known that kernels in graphs are powerful and useful structures,
for instance in the theory of games. However, a kernel does not always exist
and Chv\'atal proved in 1973 that it is an NP-Complete problem to decide its
existence. We present here an alternative definition of kernels that uses an
inductive m... | math.CO math.OC | it is well known that kernels in graphs are powerful and useful structures for instance in the theory of games however a kernel does not always exist and chvatal proved in 1973 that it is an npcomplete problem to decide its existence we present here an alternative definition of kernels that uses an inductive machinery ... | [['it', 'is', 'well', 'known', 'that', 'kernels', 'in', 'graphs', 'are', 'powerful', 'and', 'useful', 'structures', 'for', 'instance', 'in', 'the', 'theory', 'of', 'games', 'however', 'a', 'kernel', 'does', 'not', 'always', 'exist', 'and', 'chvatal', 'proved', 'in', '1973', 'that', 'it', 'is', 'an', 'npcomplete', 'prob... | [-0.1051794467714468, 0.06474854464008546, -0.09066697874743687, 0.15005821875713177, -0.15253881594705346, -0.18600100334243555, 0.00908874442531286, 0.4178956039347931, -0.29951437005871223, -0.2359030980028604, 0.15394541417297564, -0.2329872862631945, -0.19195004595737708, 0.21396422139123866, -0.11083703493503363,... |
710.1552 | SAX J1808.4-3657 in Quiescence: A Keystone for Neutron Star Science | The accreting millisecond pulsar SAX J1808.4-3658 may be a transition object
between accreting X-ray binaries and millisecond radio pulsars. We have
constrained the thermal radiation from its surface through XMM-Newton X-ray
observations, providing strong evidence for neutrino cooling processes from the
neutron star ... | astro-ph | the accreting millisecond pulsar sax j180843658 may be a transition object between accreting xray binaries and millisecond radio pulsars we have constrained the thermal radiation from its surface through xmmnewton xray observations providing strong evidence for neutrino cooling processes from the neutron star core we h... | [['the', 'accreting', 'millisecond', 'pulsar', 'sax', 'j180843658', 'may', 'be', 'a', 'transition', 'object', 'between', 'accreting', 'xray', 'binaries', 'and', 'millisecond', 'radio', 'pulsars', 'we', 'have', 'constrained', 'the', 'thermal', 'radiation', 'from', 'its', 'surface', 'through', 'xmmnewton', 'xray', 'obser... | [-0.05814118749540614, 0.21254043844360185, -0.10613690210079932, 0.14690111703323536, -0.2705433462712779, -0.10325960202860725, 0.15362118320057103, 0.4805300022105137, -0.18702827682662532, -0.32082807918988077, 0.14086982404044548, -0.3463920654661684, 0.0073736282261873945, 0.32531927242953645, -0.0211954177637775... |
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