id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
706.2514 | Simple proof of gauge invariance for the S-matrix element of
strong-field photoionization | The relationship between the length gauge (LG) and the velocity gauge (VG)
exact forms of the photoionization probability amplitude is considered. Our
motivation for this paper comes from applications of the Keldysh-Faisal-Reiss
(KFR) theory, which describes atoms (or ions) in a strong laser field (in the
nonrelativi... | physics.atom-ph | the relationship between the length gauge lg and the velocity gauge vg exact forms of the photoionization probability amplitude is considered our motivation for this paper comes from applications of the keldyshfaisalreiss kfr theory which describes atoms or ions in a strong laser field in the nonrelativistic approach i... | [['the', 'relationship', 'between', 'the', 'length', 'gauge', 'lg', 'and', 'the', 'velocity', 'gauge', 'vg', 'exact', 'forms', 'of', 'the', 'photoionization', 'probability', 'amplitude', 'is', 'considered', 'our', 'motivation', 'for', 'this', 'paper', 'comes', 'from', 'applications', 'of', 'the', 'keldyshfaisalreiss', ... | [-0.12865980789423562, 0.12160414247513332, -0.07929308918448022, 0.07821777486242354, -0.04176902734996894, -0.10291430558292912, 0.03645414957203544, 0.3416645086012208, -0.21398413876931255, -0.2516381656822677, 0.009789717097121935, -0.23048450996956, -0.11331152115554477, 0.13606647291543106, -0.013074433223272746... |
706.2515 | Canonical Melnikov theory for diffeomorphisms | We study perturbations of diffeomorphisms that have a saddle connection
between a pair of normally hyperbolic invariant manifolds. We develop a
first-order deformation calculus for invariant manifolds and show that a
generalized Melnikov function or Melnikov displacement can be written in a
canonical way. This functi... | nlin.CD math.DS | we study perturbations of diffeomorphisms that have a saddle connection between a pair of normally hyperbolic invariant manifolds we develop a firstorder deformation calculus for invariant manifolds and show that a generalized melnikov function or melnikov displacement can be written in a canonical way this function is... | [['we', 'study', 'perturbations', 'of', 'diffeomorphisms', 'that', 'have', 'a', 'saddle', 'connection', 'between', 'a', 'pair', 'of', 'normally', 'hyperbolic', 'invariant', 'manifolds', 'we', 'develop', 'a', 'firstorder', 'deformation', 'calculus', 'for', 'invariant', 'manifolds', 'and', 'show', 'that', 'a', 'generaliz... | [-0.1857125476217334, 0.03533072723907286, -0.1745051155033122, 0.12211247082346485, -0.08779442737951675, -0.12134614892836128, -0.013292406253250582, 0.3192771365450296, -0.2863523820914062, -0.21062329830601811, 0.06943182570310975, -0.24152444579937896, -0.24094189834223861, 0.16956862730564484, -0.0997078926551954... |
706.2516 | Reconstructing pedigrees: a stochastic perspective | A pedigree is a directed graph that describes how individuals are related
through ancestry in a sexually-reproducing population. In this paper we explore
the question of whether one can reconstruct a pedigree by just observing
sequence data for present day individuals. This is motivated by the increasing
availability... | q-bio.PE | a pedigree is a directed graph that describes how individuals are related through ancestry in a sexuallyreproducing population in this paper we explore the question of whether one can reconstruct a pedigree by just observing sequence data for present day individuals this is motivated by the increasing availability of g... | [['a', 'pedigree', 'is', 'a', 'directed', 'graph', 'that', 'describes', 'how', 'individuals', 'are', 'related', 'through', 'ancestry', 'in', 'a', 'sexuallyreproducing', 'population', 'in', 'this', 'paper', 'we', 'explore', 'the', 'question', 'of', 'whether', 'one', 'can', 'reconstruct', 'a', 'pedigree', 'by', 'just', '... | [-0.07948436589712012, 0.14283501419058742, -0.09922488836743751, 0.10671081296031308, -0.08666167628145267, -0.1496057332955113, 0.07254394418716494, 0.4015902313051604, -0.31932833951608347, -0.31132586732381534, 0.08991853904249068, -0.2563713907377653, -0.20397321166893265, 0.15589331345585714, -0.1451502653590145,... |
706.2517 | Big-Pieces-of-Lipschitz-Images Implies a Sufficient Carleson Estimate in
a Metric Space | This note is intended to be a supplement to the bi-Lipschitz decomposition of
Lipschitz maps shown in [Sch]. We show that in the case of 1-Ahlfors-regular
sets, the condition of having `Big Pieces of bi-Lipschitz Images' (BPBI) is
equivalent to a Carleson condition.
| math.MG math.CA | this note is intended to be a supplement to the bilipschitz decomposition of lipschitz maps shown in sch we show that in the case of 1ahlforsregular sets the condition of having big pieces of bilipschitz images bpbi is equivalent to a carleson condition | [['this', 'note', 'is', 'intended', 'to', 'be', 'a', 'supplement', 'to', 'the', 'bilipschitz', 'decomposition', 'of', 'lipschitz', 'maps', 'shown', 'in', 'sch', 'we', 'show', 'that', 'in', 'the', 'case', 'of', '1ahlforsregular', 'sets', 'the', 'condition', 'of', 'having', 'big', 'pieces', 'of', 'bilipschitz', 'images',... | [-0.12349591227872979, 7.594105923866353e-05, -0.14066395245310737, 0.09372543454136155, -0.0690111002725799, -0.10034431560283028, -0.06133966841848522, 0.40422334197181753, -0.3504063863216377, -0.16281035229018548, 0.13062722054764447, -0.2708407816726987, -0.11138922171440066, 0.16585134726199435, -0.21492629851748... |
706.2518 | Single nitrogen vacancy centers in chemical vapor deposited diamond
nanocrystals | Nanodiamond crystals containing single color centers have been grown by
chemical vapor deposition (CVD). The fluorescence from individual crystallites
was directly correlated with crystallite size using a combined atomic force and
scanning confocal fluorescence microscope. Under the conditions employed, the
optimal s... | cond-mat.mtrl-sci quant-ph | nanodiamond crystals containing single color centers have been grown by chemical vapor deposition cvd the fluorescence from individual crystallites was directly correlated with crystallite size using a combined atomic force and scanning confocal fluorescence microscope under the conditions employed the optimal size for... | [['nanodiamond', 'crystals', 'containing', 'single', 'color', 'centers', 'have', 'been', 'grown', 'by', 'chemical', 'vapor', 'deposition', 'cvd', 'the', 'fluorescence', 'from', 'individual', 'crystallites', 'was', 'directly', 'correlated', 'with', 'crystallite', 'size', 'using', 'a', 'combined', 'atomic', 'force', 'and... | [0.043252203127227815, 0.2148544509553268, -0.009881569921404501, -0.10045426702008972, 0.04462182210888006, -0.17592375094801943, 0.07003101137359155, 0.5444261269478858, -0.22072585457582264, -0.36044727676088295, 0.020923059143397156, -0.36461938213250494, 0.04819451356188783, 0.17484322923553897, -0.017019427746911... |
706.2519 | Chandra Observation of the Cluster Environment of a WAT Radio Source in
Abell 1446 | Wide-angle tail (WAT) radio sources are often found in the centers of galaxy
clusters where intracluster medium (ICM) ram pressure may bend the lobes into
their characteristic C-shape. We examine the low redshift (z=0.1035) cluster
Abell 1446, host to the WAT radio source 1159+583. The cluster exhibits
possible evide... | astro-ph | wideangle tail wat radio sources are often found in the centers of galaxy clusters where intracluster medium icm ram pressure may bend the lobes into their characteristic cshape we examine the low redshift z01035 cluster abell 1446 host to the wat radio source 1159583 the cluster exhibits possible evidence for a smalls... | [['wideangle', 'tail', 'wat', 'radio', 'sources', 'are', 'often', 'found', 'in', 'the', 'centers', 'of', 'galaxy', 'clusters', 'where', 'intracluster', 'medium', 'icm', 'ram', 'pressure', 'may', 'bend', 'the', 'lobes', 'into', 'their', 'characteristic', 'cshape', 'we', 'examine', 'the', 'low', 'redshift', 'z01035', 'cl... | [-0.1227897274990843, 0.12463011139240326, -0.10522291548891347, 0.05302241334541985, -0.13343374616845816, -0.045266640092073616, 0.02388455957607848, 0.4561583001893174, -0.2207000680821787, -0.30314920043396154, 0.06009376989948515, -0.286654942351843, -0.012502020542311145, 0.18356571492140888, 0.015976348614866107... |
706.252 | Analysis of Inter-Domain Traffic Correlations: Random Matrix Theory
Approach | The traffic behavior of University of Louisville network with the
interconnected backbone routers and the number of Virtual Local Area Network
(VLAN) subnets is investigated using the Random Matrix Theory (RMT) approach.
We employ the system of equal interval time series of traffic counts at all
router to router and ... | cs.NI | the traffic behavior of university of louisville network with the interconnected backbone routers and the number of virtual local area network vlan subnets is investigated using the random matrix theory rmt approach we employ the system of equal interval time series of traffic counts at all router to router and router ... | [['the', 'traffic', 'behavior', 'of', 'university', 'of', 'louisville', 'network', 'with', 'the', 'interconnected', 'backbone', 'routers', 'and', 'the', 'number', 'of', 'virtual', 'local', 'area', 'network', 'vlan', 'subnets', 'is', 'investigated', 'using', 'the', 'random', 'matrix', 'theory', 'rmt', 'approach', 'we', ... | [-0.17428965582101616, 0.09711232760136351, -0.08744238145905901, 0.05419196190222682, 0.011475165159474623, -0.15459565866057795, 0.11534155699658458, 0.3559125646816444, -0.2731077068906069, -0.2963939375943755, 0.0786426889005136, -0.3289146873740087, -0.1638408194882275, 0.1290711099045531, -0.007931781441048922, 0... |
706.2521 | Material-Point Simulation to Cavity Collapse Under Shock | The collapse of cavities under shock is a key problem in various fields
ranging from erosion of material, ignition of explosive, to sonoluminescence,
etc. We study such processes using the material-point-method developed recently
in the field of solid physics. The main points of the research include the
relations bet... | cond-mat.mtrl-sci cond-mat.soft | the collapse of cavities under shock is a key problem in various fields ranging from erosion of material ignition of explosive to sonoluminescence etc we study such processes using the materialpointmethod developed recently in the field of solid physics the main points of the research include the relations between symm... | [['the', 'collapse', 'of', 'cavities', 'under', 'shock', 'is', 'a', 'key', 'problem', 'in', 'various', 'fields', 'ranging', 'from', 'erosion', 'of', 'material', 'ignition', 'of', 'explosive', 'to', 'sonoluminescence', 'etc', 'we', 'study', 'such', 'processes', 'using', 'the', 'materialpointmethod', 'developed', 'recent... | [-0.12140183785664184, 0.15188059047396693, -0.09111056473106145, 0.04015711158979684, -0.035406761206686496, -0.0699354720887329, 0.005481508852514838, 0.35208108267347726, -0.27329688704971755, -0.290494400725833, 0.08057934746611864, -0.2379860246314534, -0.08417965606919357, 0.1778541304117867, 0.018060971277632884... |
706.2522 | Grounding Bohmian Mechanics in Weak Values and Bayesianism | Bohmian mechanics (BM) is a popular interpretation of quantum mechanics in
which particles have real positions. The velocity of a point x in configuration
space is defined as the standard probability current j(x) divided by the
probability density P(x). However, this ``standard'' j is in fact only one of
infinitely m... | quant-ph | bohmian mechanics bm is a popular interpretation of quantum mechanics in which particles have real positions the velocity of a point x in configuration space is defined as the standard probability current jx divided by the probability density px however this standard j is in fact only one of infinitely many that transf... | [['bohmian', 'mechanics', 'bm', 'is', 'a', 'popular', 'interpretation', 'of', 'quantum', 'mechanics', 'in', 'which', 'particles', 'have', 'real', 'positions', 'the', 'velocity', 'of', 'a', 'point', 'x', 'in', 'configuration', 'space', 'is', 'defined', 'as', 'the', 'standard', 'probability', 'current', 'jx', 'divided', ... | [-0.09234229467723067, 0.1382682648180537, -0.11245880511890817, 0.08333840339869864, -0.04743392843580832, -0.17297336442202244, 0.05955096382534702, 0.3327775886389992, -0.3031969163916747, -0.26354657202377657, 0.03512182653473819, -0.2323633492574354, -0.1271518729842467, 0.1626426179091193, -0.08562151883927986, 0... |
706.2523 | An in-medium full-folding model approach to quasielastic (p,n)
charge-exchange reactions | A microscopic description of the quasielastic (p,n) charge-exchange reaction
(here, charge-exchange scattering between analogue states) is presented and
discussed. Emphasis is focused on the spin-isospin structure of the
projectile-target coupling. The model is a coupled-channel extension of the
full-folding optical ... | nucl-th | a microscopic description of the quasielastic pn chargeexchange reaction here chargeexchange scattering between analogue states is presented and discussed emphasis is focused on the spinisospin structure of the projectiletarget coupling the model is a coupledchannel extension of the fullfolding optical model approach o... | [['a', 'microscopic', 'description', 'of', 'the', 'quasielastic', 'pn', 'chargeexchange', 'reaction', 'here', 'chargeexchange', 'scattering', 'between', 'analogue', 'states', 'is', 'presented', 'and', 'discussed', 'emphasis', 'is', 'focused', 'on', 'the', 'spinisospin', 'structure', 'of', 'the', 'projectiletarget', 'co... | [-0.09295374420767147, 0.13538041182734545, -0.08010277822904754, 0.15362338602380265, -0.032522145791084596, -0.13277304187067784, 0.015834588978794358, 0.38688258315059576, -0.18576136556276607, -0.24970956086476762, -0.05086377690387298, -0.3261186554880133, -0.05941781879121822, 0.16985707618813548, 0.0928834107139... |
706.2524 | Magnetic Excitations in NpCoGa5 | We report the results of inelastic neutron scattering experiments on
NpCoGa$_{5}$, an isostructural analogue of the PuCoGa$_{5}$ superconductor. Two
energy scales characterize the magnetic response in the antiferromagnetic
phase. One is related to a non-dispersive excitation between two crystal field
levels. The othe... | cond-mat.str-el cond-mat.mtrl-sci | we report the results of inelastic neutron scattering experiments on npcoga_5 an isostructural analogue of the pucoga_5 superconductor two energy scales characterize the magnetic response in the antiferromagnetic phase one is related to a nondispersive excitation between two crystal field levels the other at lower ener... | [['we', 'report', 'the', 'results', 'of', 'inelastic', 'neutron', 'scattering', 'experiments', 'on', 'npcoga_5', 'an', 'isostructural', 'analogue', 'of', 'the', 'pucoga_5', 'superconductor', 'two', 'energy', 'scales', 'characterize', 'the', 'magnetic', 'response', 'in', 'the', 'antiferromagnetic', 'phase', 'one', 'is',... | [-0.21766510114053284, 0.2585564049507381, -0.042998428896560775, 0.07053180129630593, -0.0424738101978469, -0.06784958834504033, 0.051947296932237326, 0.357089715661829, -0.24380851526243183, -0.2660445081950216, -0.011547508988539679, -0.3598062917999514, -0.07027752155049162, 0.17422885071373656, 0.09160044393246318... |
706.2525 | Deconfinement phase transition in holographic QCD with matter | In the framework of a holographic QCD approach we study an influence of
matters on the deconfinement temperature, $T_c$. We first consider quark flavor
number ($N_f$) dependence of $T_c$. We observe that $T_c$ decreases with $N_f$,
which is consistent with a lattice QCD result. We also delve into how the quark
number... | hep-ph hep-th | in the framework of a holographic qcd approach we study an influence of matters on the deconfinement temperature t_c we first consider quark flavor number n_f dependence of t_c we observe that t_c decreases with n_f which is consistent with a lattice qcd result we also delve into how the quark number density rho_q affe... | [['in', 'the', 'framework', 'of', 'a', 'holographic', 'qcd', 'approach', 'we', 'study', 'an', 'influence', 'of', 'matters', 'on', 'the', 'deconfinement', 'temperature', 't_c', 'we', 'first', 'consider', 'quark', 'flavor', 'number', 'n_f', 'dependence', 'of', 't_c', 'we', 'observe', 'that', 't_c', 'decreases', 'with', '... | [-0.08381837203020329, 0.3041329853985716, -0.1168687595740745, 0.03484700368349686, -0.04305543234865916, -0.08611551784469108, 0.12592884612171665, 0.3649432240740249, -0.14372176892173133, -0.24835476067505385, -0.0018303386499419023, -0.36832692807442263, -0.09944250316996324, 0.0989244315087011, 0.0195946868607088... |
706.2526 | Potential inversion with subbarrier fusion data revisited | We invert experimental data for heavy-ion fusion reactions at energies well
below the Coulomb barrier in order to directly determine the internucleus
potential between the colliding nuclei. In contrast to the previous
applications of the inversion formula, we explicitly take into account the
effect of channel couplin... | nucl-th | we invert experimental data for heavyion fusion reactions at energies well below the coulomb barrier in order to directly determine the internucleus potential between the colliding nuclei in contrast to the previous applications of the inversion formula we explicitly take into account the effect of channel couplings on... | [['we', 'invert', 'experimental', 'data', 'for', 'heavyion', 'fusion', 'reactions', 'at', 'energies', 'well', 'below', 'the', 'coulomb', 'barrier', 'in', 'order', 'to', 'directly', 'determine', 'the', 'internucleus', 'potential', 'between', 'the', 'colliding', 'nuclei', 'in', 'contrast', 'to', 'the', 'previous', 'appli... | [0.004161518974148709, 0.1591470792201226, -0.0828191167998897, 0.1768528525110172, 0.0159522476039179, -0.12311788795353926, 0.041781892133471756, 0.40558628187231394, -0.22819415984837257, -0.2782424312693879, -0.09089676283360662, -0.31107496190613704, -0.06159720576125319, 0.15988339695917522, 0.06738768766593674, ... |
706.2527 | Effects of Magnetic Fields on Neutrino-dominated Accretion Model for
Gamma-ray Bursts | Many models of gamma-ray bursts suggest a common central engine: a black hole
of several solar masses accreting matter from a disk at an accretion rate from
0.01 to 10 M_\sun / s. The inner region of the disk is cooled by neutrino
emission and large amounts of its binding energy were liberated, which could
trigger th... | astro-ph | many models of gammaray bursts suggest a common central engine a black hole of several solar masses accreting matter from a disk at an accretion rate from 001 to 10 m_sun s the inner region of the disk is cooled by neutrino emission and large amounts of its binding energy were liberated which could trigger the fireball... | [['many', 'models', 'of', 'gammaray', 'bursts', 'suggest', 'a', 'common', 'central', 'engine', 'a', 'black', 'hole', 'of', 'several', 'solar', 'masses', 'accreting', 'matter', 'from', 'a', 'disk', 'at', 'an', 'accretion', 'rate', 'from', '001', 'to', '10', 'm_sun', 's', 'the', 'inner', 'region', 'of', 'the', 'disk', 'i... | [-0.08762106258480692, 0.21560869786498335, -0.01672743751896088, 0.17514780209912822, -0.10025191231223637, -0.06507604534620653, 0.03144915586527058, 0.39161957324131164, -0.21420095239774306, -0.336543653662244, 0.08413974613628858, -0.30019942973426705, 0.018493162071427142, 0.30244499852763723, 0.01317221139718689... |
706.2528 | Electron-Electron Interactions on the Edge States of Graphene: A Many
Body Configuration Interaction Study | We have studied zigzag and armchair graphene nano ribbons (GNRs), described
by the Hubbard Hamiltonian using quantum many body configuration interaction
methods. Due to finite termination, we find that the bipartite nature of the
graphene lattice gets destroyed at the edges making the ground state of the
zigzag GNRs ... | cond-mat.mtrl-sci cond-mat.str-el | we have studied zigzag and armchair graphene nano ribbons gnrs described by the hubbard hamiltonian using quantum many body configuration interaction methods due to finite termination we find that the bipartite nature of the graphene lattice gets destroyed at the edges making the ground state of the zigzag gnrs a high ... | [['we', 'have', 'studied', 'zigzag', 'and', 'armchair', 'graphene', 'nano', 'ribbons', 'gnrs', 'described', 'by', 'the', 'hubbard', 'hamiltonian', 'using', 'quantum', 'many', 'body', 'configuration', 'interaction', 'methods', 'due', 'to', 'finite', 'termination', 'we', 'find', 'that', 'the', 'bipartite', 'nature', 'of'... | [-0.15809935331937802, 0.21120441502855888, -0.019316977800528524, 0.0027783058181844035, 0.021163578290169002, -0.1739525041798023, 0.08714756773781791, 0.4773047048669712, -0.2532322299459083, -0.2852391178013792, 0.019249068411470505, -0.3166567228651445, -0.08347393213445024, 0.11375745700132457, 0.0721654516457918... |
706.2529 | Compact lattice formulation of Cho-Faddeev-Niemi decomposition: gluon
mass generation and infrared Abelian dominance | This paper complements a new lattice formulation of SU(2) Yang-Mills theory
written in terms of new variables in a compact form proposed in the previous
paper. The new variables used in the formulation were once called the
Cho--Faddeev--Niemi or Cho--Faddeev--Niemi--Shabanov decomposition. Our
formulation enables us ... | hep-lat | this paper complements a new lattice formulation of su2 yangmills theory written in terms of new variables in a compact form proposed in the previous paper the new variables used in the formulation were once called the chofaddeevniemi or chofaddeevniemishabanov decomposition our formulation enables us to explain the in... | [['this', 'paper', 'complements', 'a', 'new', 'lattice', 'formulation', 'of', 'su2', 'yangmills', 'theory', 'written', 'in', 'terms', 'of', 'new', 'variables', 'in', 'a', 'compact', 'form', 'proposed', 'in', 'the', 'previous', 'paper', 'the', 'new', 'variables', 'used', 'in', 'the', 'formulation', 'were', 'once', 'call... | [-0.10871984231571409, 0.14870698672539295, -0.10711678834397252, 0.05618556661085233, -0.12868333810024715, -0.05700694742229055, 0.024541094313187822, 0.3248571754127991, -0.20616299438313776, -0.27232477305253516, 0.05992610057808083, -0.1985597835243249, -0.16164107498431093, 0.11549187398969564, -0.085890890163919... |
706.253 | Newton-Hodge Filtration for Self-Dual F-Crystals | In this paper we study F-crystals with self-dual structure over base schemes
of characteristic p. We generalize Katz's Newton-Hodge Filtration Theorem to
F-crystals with self-dual structure.
| math.AG | in this paper we study fcrystals with selfdual structure over base schemes of characteristic p we generalize katzs newtonhodge filtration theorem to fcrystals with selfdual structure | [['in', 'this', 'paper', 'we', 'study', 'fcrystals', 'with', 'selfdual', 'structure', 'over', 'base', 'schemes', 'of', 'characteristic', 'p', 'we', 'generalize', 'katzs', 'newtonhodge', 'filtration', 'theorem', 'to', 'fcrystals', 'with', 'selfdual', 'structure']] | [-0.23093106474727393, 0.003940437585115432, -0.13133524775505065, 0.019220787710510195, -0.10498014025390148, -0.12583525639027357, -0.014465928780846299, 0.35377232789993285, -0.3730887049436569, -0.1785785300284624, -0.001022497289814055, -0.15188825234770775, -0.24954647202044725, 0.15963722988963128, -0.2030405511... |
706.2531 | R-Parity Violation and Family Symmetry | In this talk, we investigate the implications of R-parity violating (RPV)
operators in a model with family symmetry. Family symmetry can determine the
form of RPV operators as well as the Yukawa matrices. We consider a concrete
model with non-abelian discrete symmetry Q_6, which has only three RPV
trilinear operators... | hep-ph | in this talk we investigate the implications of rparity violating rpv operators in a model with family symmetry family symmetry can determine the form of rpv operators as well as the yukawa matrices we consider a concrete model with nonabelian discrete symmetry q_6 which has only three rpv trilinear operators with no b... | [['in', 'this', 'talk', 'we', 'investigate', 'the', 'implications', 'of', 'rparity', 'violating', 'rpv', 'operators', 'in', 'a', 'model', 'with', 'family', 'symmetry', 'family', 'symmetry', 'can', 'determine', 'the', 'form', 'of', 'rpv', 'operators', 'as', 'well', 'as', 'the', 'yukawa', 'matrices', 'we', 'consider', 'a... | [-0.1588938786455135, 0.2696621750549572, 0.060284641423694246, 0.16110278360926114, -0.1183876182270668, -0.17538096192406444, 0.0726986097757706, 0.2660985172203765, -0.1944877112443309, -0.29777059343461765, 0.08442855427018935, -0.29834410070055506, -0.08467546766396702, 0.06092730957003901, 0.02972612777588571, 0.... |
706.2532 | Neutrino symmetries from high to low scales | Proposed symmetry relations, e.g., quark-lepton complementarity (QLC) or
tribimaximal mixing (TBM), need to be imposed at a high scale $\wedge \sim
10^{12}$ GeV characterising the large masses of right-handed neutrinos required
to implement the seesaw mechanism. RG evolution down to the laboratory scale
$\lambda \sim... | hep-ph | proposed symmetry relations eg quarklepton complementarity qlc or tribimaximal mixing tbm need to be imposed at a high scale wedge sim 1012 gev characterising the large masses of righthanded neutrinos required to implement the seesaw mechanism rg evolution down to the laboratory scale lambda sim 103 gev generically pro... | [['proposed', 'symmetry', 'relations', 'eg', 'quarklepton', 'complementarity', 'qlc', 'or', 'tribimaximal', 'mixing', 'tbm', 'need', 'to', 'be', 'imposed', 'at', 'a', 'high', 'scale', 'wedge', 'sim', '1012', 'gev', 'characterising', 'the', 'large', 'masses', 'of', 'righthanded', 'neutrinos', 'required', 'to', 'implemen... | [-0.13799900465553355, 0.30220047188683963, 0.017964737163458623, 0.1970274277940854, -0.09022261153381222, -0.2185787745178319, 0.05353018779976246, 0.3298759452170796, -0.27877409095899797, -0.3490192203893939, 0.053427682482064344, -0.28305905705126816, -0.02630823411835501, 0.13347235974919403, 0.02180447897567358,... |
706.2533 | Weak phase information from the color suppressed B_d^0 -> D^{*0} K^{*0}
modes | The decay channels $B_d^0 \to D^{*0} K^{*0}$ are investigated for extracting
weak $CKM$ phase information. These channels are described by color-suppressed
tree diagrams only and are free from penguin contributions. The branching
ratios for these channels are found to be $\sim \cal O $ $(10^{-5} - 10^{-6})$
which can... | hep-ph | the decay channels b_d0 to d0 k0 are investigated for extracting weak ckm phase information these channels are described by colorsuppressed tree diagrams only and are free from penguin contributions the branching ratios for these channels are found to be sim cal o 105 106 which can be measured at the currently running ... | [['the', 'decay', 'channels', 'b_d0', 'to', 'd0', 'k0', 'are', 'investigated', 'for', 'extracting', 'weak', 'ckm', 'phase', 'information', 'these', 'channels', 'are', 'described', 'by', 'colorsuppressed', 'tree', 'diagrams', 'only', 'and', 'are', 'free', 'from', 'penguin', 'contributions', 'the', 'branching', 'ratios',... | [-0.11045107355692299, 0.304000476861734, 0.0008851760553557481, 0.11227226268444489, -0.031345091009540346, -0.18505483256903157, 0.07880039123206664, 0.34473785439700777, -0.269110900308214, -0.27990097295381683, 0.08957937673609982, -0.33455405434343355, -0.022137341200749377, 0.18013823618973368, 0.0608942679463149... |
706.2534 | Charged Lepton Mass Formula -- Development and Prospect -- | The recent devolopment on the charged lepton mass forumula
m_e+m_{\mu}+m_{\tau}={2/3}(\sqrt{m_e}+\sqrt{m_\mu}+\sqrt{m_{\tau}})^2 is
reviewed. An S_3 or A_4 model will be promising for the mass relation.
| hep-ph | the recent devolopment on the charged lepton mass forumula m_em_mum_tau23sqrtm_esqrtm_musqrtm_tau2 is reviewed an s_3 or a_4 model will be promising for the mass relation | [['the', 'recent', 'devolopment', 'on', 'the', 'charged', 'lepton', 'mass', 'forumula', 'm_em_mum_tau23sqrtm_esqrtm_musqrtm_tau2', 'is', 'reviewed', 'an', 's_3', 'or', 'a_4', 'model', 'will', 'be', 'promising', 'for', 'the', 'mass', 'relation']] | [-0.07355613145045936, 0.2653795883254913, 0.031225106368462246, 0.143633062854254, -0.07661412088643937, -0.16037690905588015, -0.07843964901708421, 0.351719312724613, -0.19200940146332696, -0.2808138032976006, 0.08812204837089493, -0.3243978080295381, -0.0017718303438630841, 0.1560889558556179, -0.027259725367739088,... |
706.2535 | Optical Marking of Alcohol Induced Hemoglobin Modification | It has been shown that conformational modifications of Hb induced by ethanol
consumption can be visualized in optical spectra studying oxygenation kinetics
of hemoglobin or mixing hemoglobin with Cibacron blue dye. Better dye affinity
of blood proteins extracted from alcoholised rats with respect to those from
non-al... | physics.bio-ph physics.med-ph | it has been shown that conformational modifications of hb induced by ethanol consumption can be visualized in optical spectra studying oxygenation kinetics of hemoglobin or mixing hemoglobin with cibacron blue dye better dye affinity of blood proteins extracted from alcoholised rats with respect to those from nonalcoho... | [['it', 'has', 'been', 'shown', 'that', 'conformational', 'modifications', 'of', 'hb', 'induced', 'by', 'ethanol', 'consumption', 'can', 'be', 'visualized', 'in', 'optical', 'spectra', 'studying', 'oxygenation', 'kinetics', 'of', 'hemoglobin', 'or', 'mixing', 'hemoglobin', 'with', 'cibacron', 'blue', 'dye', 'better', '... | [-0.03453835804481059, 0.16694312839660727, -0.03423725980200938, 0.011124655678203064, 0.004784882693950619, -0.10872467691610967, 0.06866188922032182, 0.3841515808938337, -0.2212307803073366, -0.2895574770086179, 0.07162876871148391, -0.3107071276541267, -0.19642142268829046, 0.17106887218209782, -0.1373647368938795,... |
706.2536 | Exact wave-packet decoherence dynamics in a discrete spectrum
environment | We find an exact analytical solution of the reduced density matrix from the
Feynman-Vernon influence functional theory for a wave packet influenced by an
environment containing a few discrete modes. We obtain two intrinsic energy
scales relating to the time scales of the system and the environment. Different
relation... | quant-ph | we find an exact analytical solution of the reduced density matrix from the feynmanvernon influence functional theory for a wave packet influenced by an environment containing a few discrete modes we obtain two intrinsic energy scales relating to the time scales of the system and the environment different relationship ... | [['we', 'find', 'an', 'exact', 'analytical', 'solution', 'of', 'the', 'reduced', 'density', 'matrix', 'from', 'the', 'feynmanvernon', 'influence', 'functional', 'theory', 'for', 'a', 'wave', 'packet', 'influenced', 'by', 'an', 'environment', 'containing', 'a', 'few', 'discrete', 'modes', 'we', 'obtain', 'two', 'intrins... | [-0.19749381632773558, 0.11934747559080015, -0.102650841249261, 0.0785227441566362, -0.00704336882589142, -0.05984228527581697, 0.037878611080763534, 0.3273138597850566, -0.3075902043585328, -0.24806299217153285, 0.06158611245969634, -0.2918063967043291, -0.16531272350635, 0.1304348170912514, 0.04025141094925989, 0.081... |
706.2537 | One-Range Addition Theorems in Terms of -ETOs for STOs and
Coulomb-Yukawa Like Correlated Interaction Potentials of Integer and
Noninteger Indices | In this study, the one-center expansion formulas in terms of complete
orthonormal sets of -exponential type orbitals (-ETOs,) are established for the
Slater type orbitals (STOs) and Coulomb-Yukawa like correlated interaction
potentials (CIPs) of integer and noninteger indices. These relations are used
in obtaining th... | physics.chem-ph | in this study the onecenter expansion formulas in terms of complete orthonormal sets of exponential type orbitals etos are established for the slater type orbitals stos and coulombyukawa like correlated interaction potentials cips of integer and noninteger indices these relations are used in obtaining the unsymmetrical... | [['in', 'this', 'study', 'the', 'onecenter', 'expansion', 'formulas', 'in', 'terms', 'of', 'complete', 'orthonormal', 'sets', 'of', 'exponential', 'type', 'orbitals', 'etos', 'are', 'established', 'for', 'the', 'slater', 'type', 'orbitals', 'stos', 'and', 'coulombyukawa', 'like', 'correlated', 'interaction', 'potential... | [-0.12962732227918292, 0.114496782566199, 0.013269950103546892, 0.15842514931240917, 0.03890797008283525, -0.14563793791014523, 0.0054663290363913845, 0.33786813591030385, -0.19202018648918187, -0.23312619141679966, 0.04111286195499512, -0.3133477619183915, -0.17160871060609462, 0.20925583338595016, 0.0379895494560991,... |
706.2538 | Bose-Einstein Correlations of Charged and Neutral Kaons in Deep
Inelastic Scattering at HERA | Bose-Einstein correlations of charged and neutral kaons have been measured in
e+-p deep inelastic scattering with an integrated luminosity of 121 pb-1 using
the ZEUS detector at HERA. The two-particle correlation function was studied as
a function of the four-momentum difference of the kaon pairs,
Q_12=sqrt{-(p_1-p_2... | hep-ex | boseeinstein correlations of charged and neutral kaons have been measured in ep deep inelastic scattering with an integrated luminosity of 121 pb1 using the zeus detector at hera the twoparticle correlation function was studied as a function of the fourmomentum difference of the kaon pairs q_12sqrtp_1p_22 assuming a ga... | [['boseeinstein', 'correlations', 'of', 'charged', 'and', 'neutral', 'kaons', 'have', 'been', 'measured', 'in', 'ep', 'deep', 'inelastic', 'scattering', 'with', 'an', 'integrated', 'luminosity', 'of', '121', 'pb1', 'using', 'the', 'zeus', 'detector', 'at', 'hera', 'the', 'twoparticle', 'correlation', 'function', 'was',... | [-0.028111708523864125, 0.21582411000386817, -0.0703855762604941, 0.12907385980670757, 0.06342311666911825, -0.10969564670255963, -0.08320395851834736, 0.3753095696620802, -0.16229908611189495, -0.29805629742034573, -0.04892358793802758, -0.434012747201276, 0.09521193530886098, 0.11743799223381272, 0.15325575917364753,... |
706.2539 | Many body localization in Heisenberg XXZ magnet in a random field | We numerically investigate Heisenberg XXZ spin-1/2 chain in a spatially
random static magnetic field. We find that tDMRG simulations of time evolution
can be performed efficiently, namely the dimension of matrices needed to
efficiently represent the time-evolution increases linearly with time and
entanglement entropi... | quant-ph cond-mat.str-el | we numerically investigate heisenberg xxz spin12 chain in a spatially random static magnetic field we find that tdmrg simulations of time evolution can be performed efficiently namely the dimension of matrices needed to efficiently represent the timeevolution increases linearly with time and entanglement entropies for ... | [['we', 'numerically', 'investigate', 'heisenberg', 'xxz', 'spin12', 'chain', 'in', 'a', 'spatially', 'random', 'static', 'magnetic', 'field', 'we', 'find', 'that', 'tdmrg', 'simulations', 'of', 'time', 'evolution', 'can', 'be', 'performed', 'efficiently', 'namely', 'the', 'dimension', 'of', 'matrices', 'needed', 'to',... | [-0.18704398801284178, 0.2637687113208624, -0.048523152029359494, 0.09916821495908035, 0.01831639822959513, -0.17122864684501252, -0.013928905468095432, 0.41912418468431994, -0.266212242159557, -0.25668352066732747, 0.05754629893276792, -0.2871037982525183, -0.10976376789682485, 0.16005173543552784, 0.0887210981001134,... |
706.254 | Pomeron loop and running coupling effects in high energy QCD evolution | Within the framework of a (1+1)-dimensional model which mimics evolution and
scattering in QCD at high energy, we study the influence of the running of the
coupling on the high-energy dynamics with Pomeron loops. We find that the
particle number fluctuations are strongly suppressed by the running of the
coupling, by ... | hep-ph | within the framework of a 11dimensional model which mimics evolution and scattering in qcd at high energy we study the influence of the running of the coupling on the highenergy dynamics with pomeron loops we find that the particle number fluctuations are strongly suppressed by the running of the coupling by at least o... | [['within', 'the', 'framework', 'of', 'a', '11dimensional', 'model', 'which', 'mimics', 'evolution', 'and', 'scattering', 'in', 'qcd', 'at', 'high', 'energy', 'we', 'study', 'the', 'influence', 'of', 'the', 'running', 'of', 'the', 'coupling', 'on', 'the', 'highenergy', 'dynamics', 'with', 'pomeron', 'loops', 'we', 'fin... | [-0.11217531883092663, 0.1972785200011897, -0.0910822430241306, 0.0810948149382521, -0.013945802227248782, -0.07039433844400557, 0.004678782039823441, 0.3233863351462813, -0.24969598770441187, -0.3251124316699464, 0.05724854824064834, -0.29738380314482676, -0.0681541509148046, 0.14438869945633298, 0.10847247115798764, ... |
706.2541 | Binary Black Holes: Spin Dynamics and Gravitational Recoil | We present a study of spinning black hole binaries focusing on the spin
dynamics of the individual black holes as well as on the gravitational recoil
acquired by the black hole produced by the merger. We consider two series of
initial spin orientations away from the binary orbital plane. In one of the
series, the spi... | gr-qc astro-ph | we present a study of spinning black hole binaries focusing on the spin dynamics of the individual black holes as well as on the gravitational recoil acquired by the black hole produced by the merger we consider two series of initial spin orientations away from the binary orbital plane in one of the series the spins ar... | [['we', 'present', 'a', 'study', 'of', 'spinning', 'black', 'hole', 'binaries', 'focusing', 'on', 'the', 'spin', 'dynamics', 'of', 'the', 'individual', 'black', 'holes', 'as', 'well', 'as', 'on', 'the', 'gravitational', 'recoil', 'acquired', 'by', 'the', 'black', 'hole', 'produced', 'by', 'the', 'merger', 'we', 'consid... | [-0.17915565200787495, 0.12727341738175899, -0.030840302132727468, 0.07578318949382912, -0.05536897368679311, -0.07655945550500948, 0.008939069755534755, 0.3518281529538015, -0.21152123383291185, -0.3000942176994793, 0.05605597541179448, -0.3464664788767297, -0.018670909566167283, 0.2327640267726492, 0.0419858493842184... |
706.2542 | Understanding of complex periodic transformations of moving domain walls
in magnetic nanostripes | The magnetic field (or electric current) driven domain-wall motion in
magnetic nanostripes is of considerable interest because it is essential to the
performance of information storage and logic devices. One of the currently key
problems is to unveil the complex behaviors of oscillatory domain-wall motions
under appl... | cond-mat.other cond-mat.soft | the magnetic field or electric current driven domainwall motion in magnetic nanostripes is of considerable interest because it is essential to the performance of information storage and logic devices one of the currently key problems is to unveil the complex behaviors of oscillatory domainwall motions under applied mag... | [['the', 'magnetic', 'field', 'or', 'electric', 'current', 'driven', 'domainwall', 'motion', 'in', 'magnetic', 'nanostripes', 'is', 'of', 'considerable', 'interest', 'because', 'it', 'is', 'essential', 'to', 'the', 'performance', 'of', 'information', 'storage', 'and', 'logic', 'devices', 'one', 'of', 'the', 'currently'... | [-0.1714322789997927, 0.19683891972260817, -0.05621082731655666, 0.033371313572196026, -0.13339405700564386, -0.11037733606029568, 0.020405658924386703, 0.39653710448316165, -0.30417368969480907, -0.31309320565845283, 0.10001752006555242, -0.18624188898746588, -0.11660917962369109, 0.22516074650388743, -0.0280786027958... |
706.2543 | Dirac Equation in the Background of the Nutku Helicoid Metric | We study the solutions of the Dirac equation in the background of the Nutku
helicoid metric. This metric has curvature singularities, which necessitates
imposing a boundary to exclude this point. We use the Atiyah-Patodi-Singer non
local spectral boundary conditions for both the four and the five dimensional
manifold... | gr-qc math-ph math.MP | we study the solutions of the dirac equation in the background of the nutku helicoid metric this metric has curvature singularities which necessitates imposing a boundary to exclude this point we use the atiyahpatodisinger non local spectral boundary conditions for both the four and the five dimensional manifolds | [['we', 'study', 'the', 'solutions', 'of', 'the', 'dirac', 'equation', 'in', 'the', 'background', 'of', 'the', 'nutku', 'helicoid', 'metric', 'this', 'metric', 'has', 'curvature', 'singularities', 'which', 'necessitates', 'imposing', 'a', 'boundary', 'to', 'exclude', 'this', 'point', 'we', 'use', 'the', 'atiyahpatodisi... | [-0.20854971709195524, 0.03848521541901088, -0.1339974419097416, 0.07865751594363246, -0.114510990519193, -0.13087141617628126, -0.011822742507016907, 0.3140884458941097, -0.19843578268773854, -0.22413093829527497, 0.1615604723992874, -0.2971102598433693, -0.142125382903032, 0.09435929575314124, -0.08465269279743855, 0... |
706.2544 | Abstract machines for dialogue games | The notion of abstract Boehm tree has arisen as an operationally-oriented
distillation of works on game semantics, and has been investigated in two
papers. This paper revisits the notion, providing more syntactic support and
more examples (like call-by-value evaluation) illustrating the generality of
the underlying c... | cs.LO | the notion of abstract boehm tree has arisen as an operationallyoriented distillation of works on game semantics and has been investigated in two papers this paper revisits the notion providing more syntactic support and more examples like callbyvalue evaluation illustrating the generality of the underlying computing d... | [['the', 'notion', 'of', 'abstract', 'boehm', 'tree', 'has', 'arisen', 'as', 'an', 'operationallyoriented', 'distillation', 'of', 'works', 'on', 'game', 'semantics', 'and', 'has', 'been', 'investigated', 'in', 'two', 'papers', 'this', 'paper', 'revisits', 'the', 'notion', 'providing', 'more', 'syntactic', 'support', 'a... | [-0.11822409501497741, 0.02188054527386023, -0.0967674748361355, 0.12935429358602973, -0.14382389272166202, -0.13992997970370974, 0.059291930810059804, 0.3788155737470408, -0.25156718649000664, -0.3101995199552325, 0.07185870516457457, -0.24915580640806526, -0.17287808339126776, 0.19083456618741887, -0.1647683944492066... |
706.2545 | Factorization and Gauge Invariance of Twist-3 Cross Section for Single
Spin Asymmetry | We prove factorization and gauge invariance of the twist-3
single-spin-dependent cross section in the leading order perturbative QCD,
which was missing in the previous literature. We emphasize that the consistency
relation from the Ward identities for color gauge invariance is crucial to
guarantee the cancelation amo... | hep-ph | we prove factorization and gauge invariance of the twist3 singlespindependent cross section in the leading order perturbative qcd which was missing in the previous literature we emphasize that the consistency relation from the ward identities for color gauge invariance is crucial to guarantee the cancelation among the ... | [['we', 'prove', 'factorization', 'and', 'gauge', 'invariance', 'of', 'the', 'twist3', 'singlespindependent', 'cross', 'section', 'in', 'the', 'leading', 'order', 'perturbative', 'qcd', 'which', 'was', 'missing', 'in', 'the', 'previous', 'literature', 'we', 'emphasize', 'that', 'the', 'consistency', 'relation', 'from',... | [-0.10116565785370767, 0.09302576654939912, -0.12788395324139856, 0.16025113997980953, -0.054059404446743425, -0.0036917663738131523, -0.02330709925852716, 0.3460394487623125, -0.20806941331364215, -0.20268873358145356, -0.042985199484974146, -0.3408815648779273, -0.08050729165785014, 0.08592236646916718, 0.01014120429... |
706.2546 | Kink Confinement and Supersymmetry | We analyze non-integrable deformations of two-dimensional N=1 supersymmetric
quantum field theories with kink excitations. As example, we consider the
multi-frequency Super Sine Gordon model. At weak coupling, this model is robust
with respect to kink confinement phenomena, in contrast to the purely bosonic
case. If ... | hep-th cond-mat.stat-mech hep-lat | we analyze nonintegrable deformations of twodimensional n1 supersymmetric quantum field theories with kink excitations as example we consider the multifrequency super sine gordon model at weak coupling this model is robust with respect to kink confinement phenomena in contrast to the purely bosonic case if we vary the ... | [['we', 'analyze', 'nonintegrable', 'deformations', 'of', 'twodimensional', 'n1', 'supersymmetric', 'quantum', 'field', 'theories', 'with', 'kink', 'excitations', 'as', 'example', 'we', 'consider', 'the', 'multifrequency', 'super', 'sine', 'gordon', 'model', 'at', 'weak', 'coupling', 'this', 'model', 'is', 'robust', 'w... | [-0.16433189042387591, 0.2324079584092802, -0.032601126810323275, 0.08488363757160736, -0.03204805007666949, -0.18507424575095408, 0.032271629898658886, 0.30988898508300716, -0.21114567959143613, -0.24854045455858123, 0.0630647139178414, -0.296053227224706, -0.1488865430548087, 0.08570065602016379, 0.028404395814810024... |
706.2547 | Swift-XRT observation of 34 new INTEGRAL/IBIS AGNs: discovery of Compton
thick and other peculiar sources | For a significant number of the sources detected at high energies (>10 keV)
by the INTEGRAL/IBIS and Swift/BAT instruments there is either a lack
information about them in the 2-10 keV range or they are totally unidentified.
Herein, we report on a sample of 34 IBIS AGN or AGN candidate objects for which
there is X-ra... | astro-ph | for a significant number of the sources detected at high energies 10 kev by the integralibis and swiftbat instruments there is either a lack information about them in the 210 kev range or they are totally unidentified herein we report on a sample of 34 ibis agn or agn candidate objects for which there is xray data in t... | [['for', 'a', 'significant', 'number', 'of', 'the', 'sources', 'detected', 'at', 'high', 'energies', '10', 'kev', 'by', 'the', 'integralibis', 'and', 'swiftbat', 'instruments', 'there', 'is', 'either', 'a', 'lack', 'information', 'about', 'them', 'in', 'the', '210', 'kev', 'range', 'or', 'they', 'are', 'totally', 'unid... | [-0.03582318474429176, 0.11172862775120605, -0.03388171692101939, 0.11231326799512513, -0.05899276067664609, -0.11860473549647911, 0.08200209751063563, 0.4821774747625396, -0.1283797641144526, -0.4113426076816431, 0.09810366677830507, -0.36629857966302387, 0.025988590605125463, 0.20909607960144957, -0.01962078521594506... |
706.2548 | WSRT Faraday tomography of the Galactic ISM at \lambda \sim 0.86 m | We investigate the distribution and properties of Faraday rotating and
synchrotron emitting regions in the Galactic ISM in the direction of the
Galactic anti-centre. We apply Faraday tomography to a radio polarization
dataset that we obtained with the WSRT. We developed a new method to calculate
a linear fit to perio... | astro-ph | we investigate the distribution and properties of faraday rotating and synchrotron emitting regions in the galactic ism in the direction of the galactic anticentre we apply faraday tomography to a radio polarization dataset that we obtained with the wsrt we developed a new method to calculate a linear fit to periodic d... | [['we', 'investigate', 'the', 'distribution', 'and', 'properties', 'of', 'faraday', 'rotating', 'and', 'synchrotron', 'emitting', 'regions', 'in', 'the', 'galactic', 'ism', 'in', 'the', 'direction', 'of', 'the', 'galactic', 'anticentre', 'we', 'apply', 'faraday', 'tomography', 'to', 'a', 'radio', 'polarization', 'datas... | [-0.09330327646737849, 0.09772829876811658, -0.0901122617897474, 0.06316255658037133, -0.10839799876428313, -0.03822219121373362, 0.018148060199908084, 0.46009969242193083, -0.2670073999850838, -0.2827535575773153, 0.06983492763764743, -0.28432589510662687, -0.04124233388790378, 0.24602540836290077, -0.0327844272559525... |
706.2549 | A statistical mechanics approach to reverse engineering: sparsity and
biological priors on gene regulatory networks | The important task of determining the connectivity of gene networks, and at a
more detailed level even the kind of interaction existing between genes, can
nowadays be tackled by microarraylike technologies. Yet, there is still a large
amount of unknowns with respect to the amount of data provided by a single
microarr... | q-bio.MN q-bio.QM | the important task of determining the connectivity of gene networks and at a more detailed level even the kind of interaction existing between genes can nowadays be tackled by microarraylike technologies yet there is still a large amount of unknowns with respect to the amount of data provided by a single microarray exp... | [['the', 'important', 'task', 'of', 'determining', 'the', 'connectivity', 'of', 'gene', 'networks', 'and', 'at', 'a', 'more', 'detailed', 'level', 'even', 'the', 'kind', 'of', 'interaction', 'existing', 'between', 'genes', 'can', 'nowadays', 'be', 'tackled', 'by', 'microarraylike', 'technologies', 'yet', 'there', 'is',... | [-0.07723095233206512, 0.0331093475856271, -0.02883138587535119, 0.08095968938036582, -0.09482676477097071, -0.12114817778983143, 0.08829691213346806, 0.3822646431004408, -0.2751589744140576, -0.3299409935323488, 0.07926529598513561, -0.25914234307368966, -0.21387363961278508, 0.21413126354917078, -0.055813780030446875... |
706.255 | Entanglement swapping in a Franson interferometer setup | We propose a simple scheme to swap the non local correlations, characteristic
of a Franson interferometric setup, between pairs of frequency entangled
photons emitted by distinct non linear crystals in a parametric down conversion
process. Our scheme consists of two distinct sources of frequency entangled
photons. On... | quant-ph | we propose a simple scheme to swap the non local correlations characteristic of a franson interferometric setup between pairs of frequency entangled photons emitted by distinct non linear crystals in a parametric down conversion process our scheme consists of two distinct sources of frequency entangled photons one phot... | [['we', 'propose', 'a', 'simple', 'scheme', 'to', 'swap', 'the', 'non', 'local', 'correlations', 'characteristic', 'of', 'a', 'franson', 'interferometric', 'setup', 'between', 'pairs', 'of', 'frequency', 'entangled', 'photons', 'emitted', 'by', 'distinct', 'non', 'linear', 'crystals', 'in', 'a', 'parametric', 'down', '... | [-0.18111646644527388, 0.22285658798058666, -0.1076303582124969, 0.02914812306421779, 0.009147795097832786, -0.20454798761111137, 0.06492754091969996, 0.377073399235155, -0.23085132647723516, -0.283948386027086, -0.03412941564527279, -0.29541482647584977, 0.008221776346528084, 0.2281867549450041, -0.0005965489702664804... |
706.2551 | The Dependence of Galaxy Formation on Cosmological Parameters: Can we
distinguish the WMAP1 and WMAP3 Parameter Sets? | We combine N-body simulations of structure growth with physical modelling of
galaxy evolution to investigate whether the shift in cosmological parameters
between the 1-year and 3-year results from the Wilkinson Microwave Anisotropy
Probe affects predictions for the galaxy population. Structure formation is
significan... | astro-ph | we combine nbody simulations of structure growth with physical modelling of galaxy evolution to investigate whether the shift in cosmological parameters between the 1year and 3year results from the wilkinson microwave anisotropy probe affects predictions for the galaxy population structure formation is significantly de... | [['we', 'combine', 'nbody', 'simulations', 'of', 'structure', 'growth', 'with', 'physical', 'modelling', 'of', 'galaxy', 'evolution', 'to', 'investigate', 'whether', 'the', 'shift', 'in', 'cosmological', 'parameters', 'between', 'the', '1year', 'and', '3year', 'results', 'from', 'the', 'wilkinson', 'microwave', 'anisot... | [-0.047489695761424415, 0.10657918371416353, -0.09056163908349038, 0.15984653812154656, -0.1346240805238654, -0.09315966282827923, -0.014874467961764073, 0.3871712853006884, -0.18727588115525495, -0.39027878216876566, 0.03359159818277336, -0.29574871727747937, -0.004603303112285855, 0.22001959327545134, 0.0258216002989... |
706.2552 | The noncommutative residue and canonical trace in the light of Stokes'
and continuity properties | We show that the noncommutative residue density, resp. the cut-off
regularised integral are the only closed linear, resp. continuous closed linear
forms on certain classes of symbols. This leads to alternative proofs of the
uniqueness of the noncommutative residue, resp. the canonical trace as linear,
resp. continuou... | math.OA math.AP | we show that the noncommutative residue density resp the cutoff regularised integral are the only closed linear resp continuous closed linear forms on certain classes of symbols this leads to alternative proofs of the uniqueness of the noncommutative residue resp the canonical trace as linear resp continuous linear for... | [['we', 'show', 'that', 'the', 'noncommutative', 'residue', 'density', 'resp', 'the', 'cutoff', 'regularised', 'integral', 'are', 'the', 'only', 'closed', 'linear', 'resp', 'continuous', 'closed', 'linear', 'forms', 'on', 'certain', 'classes', 'of', 'symbols', 'this', 'leads', 'to', 'alternative', 'proofs', 'of', 'the'... | [-0.18274750337941045, 0.09796951157314006, -0.04364632390628474, 0.12487453130492265, -0.05381360642638975, -0.14514785828541263, -0.04438924021678099, 0.26991469086404296, -0.28347376303112914, -0.1803870252671017, 0.11801209127651932, -0.29318682664492424, -0.12110124848634544, 0.15708428795408944, -0.05682464134946... |
706.2553 | Asymptotic freedom and quarks confinement treated through Thompson's
approach | In this work, we first use Thompson's renormalization group method to treat
QCD-vacuum behavior close to the regime of asymptotic freedom. QCD-vacuum
behaves effectively like a "paramagnetic system" of a classical theory in the
sense that virtual color charges (gluons) emerge in it as spin effect of a
paramagnetic ma... | hep-ph | in this work we first use thompsons renormalization group method to treat qcdvacuum behavior close to the regime of asymptotic freedom qcdvacuum behaves effectively like a paramagnetic system of a classical theory in the sense that virtual color charges gluons emerge in it as spin effect of a paramagnetic material when... | [['in', 'this', 'work', 'we', 'first', 'use', 'thompsons', 'renormalization', 'group', 'method', 'to', 'treat', 'qcdvacuum', 'behavior', 'close', 'to', 'the', 'regime', 'of', 'asymptotic', 'freedom', 'qcdvacuum', 'behaves', 'effectively', 'like', 'a', 'paramagnetic', 'system', 'of', 'a', 'classical', 'theory', 'in', 't... | [-0.12046360293821748, 0.19454557159907873, -0.1211083397937996, 0.06878294607692106, -0.11644929531748337, -0.12548371605341227, 0.05979035463400025, 0.334144085735936, -0.2167130122822812, -0.30174500125743414, 0.020118518313495565, -0.2748855799385926, -0.1232261400719046, 0.13137402748668542, -0.010923956032629054,... |
706.2554 | Chern-Weil calculus extended to a class of infinite dimensional
manifolds | We discuss possible extensions of the classical Chern-Weil formalism to an
infinite dimensional setup. This is based on joint work with Steven
Rosenberg, joint work with Simon Scott and joint work with Jouko Mickelsson.
| math.DG math.OA | we discuss possible extensions of the classical chernweil formalism to an infinite dimensional setup this is based on joint work with steven rosenberg joint work with simon scott and joint work with jouko mickelsson | [['we', 'discuss', 'possible', 'extensions', 'of', 'the', 'classical', 'chernweil', 'formalism', 'to', 'an', 'infinite', 'dimensional', 'setup', 'this', 'is', 'based', 'on', 'joint', 'work', 'with', 'steven', 'rosenberg', 'joint', 'work', 'with', 'simon', 'scott', 'and', 'joint', 'work', 'with', 'jouko', 'mickelsson']] | [-0.05442282754708739, 0.03261292898070464, -0.10999971896629124, -0.003952593816553845, -0.175253711092998, -0.13100117198465502, 0.024201594346189213, 0.3143033517853302, -0.19644791705479078, -0.29096445238546415, 0.020011190378093433, -0.21076504866976073, -0.2192739914445316, 0.14561363424325144, -0.22261682037702... |
706.2555 | The AMIGA sample of isolated galaxies. V. Quantification of the
isolation | The AMIGA project aims to build a well defined and statistically significant
reference sample of isolated galaxies in order to estimate the environmental
effects on the formation and evolution of galaxies. The goal of this paper is
to provide a measure of the environment of the isolated galaxies in the AMIGA
sample, ... | astro-ph | the amiga project aims to build a well defined and statistically significant reference sample of isolated galaxies in order to estimate the environmental effects on the formation and evolution of galaxies the goal of this paper is to provide a measure of the environment of the isolated galaxies in the amiga sample quan... | [['the', 'amiga', 'project', 'aims', 'to', 'build', 'a', 'well', 'defined', 'and', 'statistically', 'significant', 'reference', 'sample', 'of', 'isolated', 'galaxies', 'in', 'order', 'to', 'estimate', 'the', 'environmental', 'effects', 'on', 'the', 'formation', 'and', 'evolution', 'of', 'galaxies', 'the', 'goal', 'of',... | [-0.09067605377891831, 0.040036203879059006, -0.08431558321538321, 0.08367166448118192, -0.04188152922907, 0.013442444052252409, 0.05599753677205031, 0.3971322420582497, -0.13113744748434264, -0.37845324234460753, 0.03275659726011373, -0.2959883255857251, -0.05509620826425895, 0.1575160783626769, 0.01369983565209688, -... |
706.2556 | Inhomogeneous High Frequency Expansion-Free Gravitational Waves | We describe a natural inhomogeneous generalization of high frequency plane
gravitational waves. The waves are high frequency waves of the Kundt type whose
null propagation direction in space-time has vanishing expansion, twist and
shear but is not covariantly constant. The introduction of a cosmological
constant is d... | gr-qc | we describe a natural inhomogeneous generalization of high frequency plane gravitational waves the waves are high frequency waves of the kundt type whose null propagation direction in spacetime has vanishing expansion twist and shear but is not covariantly constant the introduction of a cosmological constant is discuss... | [['we', 'describe', 'a', 'natural', 'inhomogeneous', 'generalization', 'of', 'high', 'frequency', 'plane', 'gravitational', 'waves', 'the', 'waves', 'are', 'high', 'frequency', 'waves', 'of', 'the', 'kundt', 'type', 'whose', 'null', 'propagation', 'direction', 'in', 'spacetime', 'has', 'vanishing', 'expansion', 'twist'... | [-0.28392130669530935, 0.1993754847031651, -0.02311219478900911, 0.06834719727824752, -0.20054239233617077, -0.11069173916863899, -0.06203730159375647, 0.3687063653134938, -0.22530507924260967, -0.18082816049343708, 0.11809362086933106, -0.25658783049915324, -0.1254031311607722, 0.1605185352435166, -0.00311912691011622... |
706.2557 | Heavy Flavor Production at HERA | Studies of charm and beauty production in ep collisions with a center-of-mass
energy of 318 GeV are reported from the two HERA collaborations, H1 and ZEUS.
The analyses make use of both the HERA-I data sample recorded between 1996 and
2000 and a sample from HERA-II, which started in 2003. The cross sections
measured ... | hep-ex | studies of charm and beauty production in ep collisions with a centerofmass energy of 318 gev are reported from the two hera collaborations h1 and zeus the analyses make use of both the herai data sample recorded between 1996 and 2000 and a sample from heraii which started in 2003 the cross sections measured by both h1... | [['studies', 'of', 'charm', 'and', 'beauty', 'production', 'in', 'ep', 'collisions', 'with', 'a', 'centerofmass', 'energy', 'of', '318', 'gev', 'are', 'reported', 'from', 'the', 'two', 'hera', 'collaborations', 'h1', 'and', 'zeus', 'the', 'analyses', 'make', 'use', 'of', 'both', 'the', 'herai', 'data', 'sample', 'recor... | [-0.004502934207649608, 0.10684201335044284, -0.11636523238236182, 0.1190486307917653, 0.004970577770942136, -0.008264309683152915, 0.023280616053134986, 0.36553975590749793, -0.14316682580270265, -0.3315895330651026, 0.0014779951827796666, -0.4556494631069271, 0.06768756492161437, 0.1437620815624924, 0.116804373859869... |
706.2558 | A phenomenological model of galaxy clusters | We present a simple model to describe the dark matter density, the gas
density, and the gas temperature profiles of galaxy clusters. Analytical
expressions for these quantities are given in terms of only five free
parameters with a clear physical meaning: the mass M of the dark matter halo
(or the characteristic temp... | astro-ph | we present a simple model to describe the dark matter density the gas density and the gas temperature profiles of galaxy clusters analytical expressions for these quantities are given in terms of only five free parameters with a clear physical meaning the mass m of the dark matter halo or the characteristic temperature... | [['we', 'present', 'a', 'simple', 'model', 'to', 'describe', 'the', 'dark', 'matter', 'density', 'the', 'gas', 'density', 'and', 'the', 'gas', 'temperature', 'profiles', 'of', 'galaxy', 'clusters', 'analytical', 'expressions', 'for', 'these', 'quantities', 'are', 'given', 'in', 'terms', 'of', 'only', 'five', 'free', 'p... | [-0.1114234824271989, 0.15243841075425735, -0.06874269799482136, 0.07691371138389513, -0.021341646326618502, -0.041943139336581226, 0.02767917932033015, 0.35863599681761116, -0.20320509509360818, -0.3451488357386552, 0.04673020264817751, -0.2870852995692985, -0.027888889286089125, 0.2019868957795552, 0.0237860801262286... |
706.2559 | The physics and chemistry of circumstellar envelopes of S-stars on the
AGB | The S-stars have been suggested to be a brief transitional phase as stars
evolve from oxygen-rich M-type stars into carbon stars, through the dredge up
of carbon from He-shell burning. As possible transition objects, S-stars might
help achieve a deeper understanding of the chemical evolution as a star ascends
the AGB... | astro-ph | the sstars have been suggested to be a brief transitional phase as stars evolve from oxygenrich mtype stars into carbon stars through the dredge up of carbon from heshell burning as possible transition objects sstars might help achieve a deeper understanding of the chemical evolution as a star ascends the agb as well a... | [['the', 'sstars', 'have', 'been', 'suggested', 'to', 'be', 'a', 'brief', 'transitional', 'phase', 'as', 'stars', 'evolve', 'from', 'oxygenrich', 'mtype', 'stars', 'into', 'carbon', 'stars', 'through', 'the', 'dredge', 'up', 'of', 'carbon', 'from', 'heshell', 'burning', 'as', 'possible', 'transition', 'objects', 'sstar... | [0.003010652443793203, 0.11778710943933829, -0.04242942020773215, 0.07493848099173712, -0.10530198555915876, -0.052160280215715, 0.11717765162965017, 0.45206291045069247, -0.13869058922689437, -0.3270646447413846, 0.04699675448823552, -0.2784745441784704, -0.01758201051804524, 0.1533776358456204, -0.02531653331348743, ... |
706.256 | Sparticle Mass Spectrum in Grand Unified Theories | We carry out a detailed analysis of sparticle mass spectrum in supersymmetric
grand unified theories. We consider the spectroscopy of the squarks and
sleptons in SU(5) and SO(10) grand unified theories, and show how the
underlying supersymmetry breaking parameters of these theories can be
determined from a measuremen... | hep-ph | we carry out a detailed analysis of sparticle mass spectrum in supersymmetric grand unified theories we consider the spectroscopy of the squarks and sleptons in su5 and so10 grand unified theories and show how the underlying supersymmetry breaking parameters of these theories can be determined from a measurement of dif... | [['we', 'carry', 'out', 'a', 'detailed', 'analysis', 'of', 'sparticle', 'mass', 'spectrum', 'in', 'supersymmetric', 'grand', 'unified', 'theories', 'we', 'consider', 'the', 'spectroscopy', 'of', 'the', 'squarks', 'and', 'sleptons', 'in', 'su5', 'and', 'so10', 'grand', 'unified', 'theories', 'and', 'show', 'how', 'the',... | [-0.10317151467001602, 0.24378559162177466, -0.08039016733117448, 0.22706107946649834, -0.0693063969649603, -0.13821613386936166, 0.04613272380655163, 0.3512960930406316, -0.191709758548146, -0.3262501444519023, 0.04727244098239401, -0.2081437406374393, -0.10596381043843879, 0.09519799296427062, -0.009299872175253288, ... |
706.2561 | Study of multi-muon bundles in cosmic ray showers detected with the
DELPHI detector at LEP | The DELPHI detector at LEP has been used to measure multi-muon bundles
originating from cosmic ray interactions with air. The cosmic events were
recorded in ``parasitic mode'' between individual e+e- interactions and the
total live time of this data taking is equivalent to 1.6x10^6 seconds. The
DELPHI apparatus is lo... | astro-ph hep-ex | the delphi detector at lep has been used to measure multimuon bundles originating from cosmic ray interactions with air the cosmic events were recorded in parasitic mode between individual ee interactions and the total live time of this data taking is equivalent to 16x106 seconds the delphi apparatus is located about 1... | [['the', 'delphi', 'detector', 'at', 'lep', 'has', 'been', 'used', 'to', 'measure', 'multimuon', 'bundles', 'originating', 'from', 'cosmic', 'ray', 'interactions', 'with', 'air', 'the', 'cosmic', 'events', 'were', 'recorded', 'in', 'parasitic', 'mode', 'between', 'individual', 'ee', 'interactions', 'and', 'the', 'total... | [-0.058301731011157445, 0.2013137260480329, -0.07584329855382647, 0.1311709947992248, -0.026791081687721506, -0.04870144846504481, -0.007733535663202757, 0.32994231842751576, -0.18463410748036826, -0.403387112414655, 0.044373378329947005, -0.4093389457209021, 0.0769309645709325, 0.1816825498863468, 0.013594635586276299... |
706.2562 | X-ray observations of ultraluminous X-ray sources | Ultraluminous X-ray sources (ULXs) are amongst the most intriguing of X-ray
source classes. Their extreme luminosities - greater than 10^39 erg/s in the
0.3 - 10 keV band alone - suggest either the presence of black holes larger
than those regularly encountered in our own Galaxy (the Galactic centre
excepted), or sou... | astro-ph | ultraluminous xray sources ulxs are amongst the most intriguing of xray source classes their extreme luminosities greater than 1039 ergs in the 03 10 kev band alone suggest either the presence of black holes larger than those regularly encountered in our own galaxy the galactic centre excepted or sources apparently rad... | [['ultraluminous', 'xray', 'sources', 'ulxs', 'are', 'amongst', 'the', 'most', 'intriguing', 'of', 'xray', 'source', 'classes', 'their', 'extreme', 'luminosities', 'greater', 'than', '1039', 'ergs', 'in', 'the', '03', '10', 'kev', 'band', 'alone', 'suggest', 'either', 'the', 'presence', 'of', 'black', 'holes', 'larger'... | [-0.03513182219036895, 0.10062188114464769, -0.032688321869658386, 0.18662922223220052, -0.12812131608471922, -0.08700389534882877, 0.08801844794222194, 0.46968297801263953, -0.13597397468680436, -0.395567337051034, 0.10319695382115796, -0.3847263003537512, -0.020997858422038995, 0.26411082912641376, -0.045316483930725... |
706.2563 | On Poincare Polynomials of Hyperbolic Lie Algebras | We have general frameworks to obtain Poincare polynomials for Finite and also
Affine types of Kac-Moody Lie algebras. Very little is known however beyond
Affine ones, though we have a constructive theorem which can be applied both
for finite and infinite cases. One can conclusively said that theorem gives the
Poincar... | math-ph hep-th math.GR math.MP math.RT | we have general frameworks to obtain poincare polynomials for finite and also affine types of kacmoody lie algebras very little is known however beyond affine ones though we have a constructive theorem which can be applied both for finite and infinite cases one can conclusively said that theorem gives the poincare poly... | [['we', 'have', 'general', 'frameworks', 'to', 'obtain', 'poincare', 'polynomials', 'for', 'finite', 'and', 'also', 'affine', 'types', 'of', 'kacmoody', 'lie', 'algebras', 'very', 'little', 'is', 'known', 'however', 'beyond', 'affine', 'ones', 'though', 'we', 'have', 'a', 'constructive', 'theorem', 'which', 'can', 'be'... | [-0.1239226395733493, 0.06637842647978687, -0.14450242125894874, 0.06919061070681093, -0.13219190066993922, -0.1793416607578532, 0.0006834860007297628, 0.3630322685930878, -0.29856143081759706, -0.21986699003574192, 0.13035592460608092, -0.22246279152186246, -0.16467212763619704, 0.23713679287383066, -0.099596079811928... |
706.2564 | Hubble Space Telescope far-ultraviolet imaging of the jet in 3C273: a
common emission component from optical to X-rays | We present far-ultraviolet (UV) observations at 150 nm of the jet of the
quasar 3C 273 obtained with the Advanced Camera for Survey's Solar Blind
Channel (ACS/SBC) on board the Hubble Space Telescope. While the jet morphology
is very similar to that in the optical and near-ultraviolet, the spectral
energy distributio... | astro-ph | we present farultraviolet uv observations at 150 nm of the jet of the quasar 3c 273 obtained with the advanced camera for surveys solar blind channel acssbc on board the hubble space telescope while the jet morphology is very similar to that in the optical and nearultraviolet the spectral energy distributions seds of t... | [['we', 'present', 'farultraviolet', 'uv', 'observations', 'at', '150', 'nm', 'of', 'the', 'jet', 'of', 'the', 'quasar', '3c', '273', 'obtained', 'with', 'the', 'advanced', 'camera', 'for', 'surveys', 'solar', 'blind', 'channel', 'acssbc', 'on', 'board', 'the', 'hubble', 'space', 'telescope', 'while', 'the', 'jet', 'mo... | [-0.03406927493516598, 0.1312206343234656, -0.09028516446664576, 0.08870636874302869, -0.09797601072674275, -0.07755033079446597, 0.027081091148426106, 0.48884231566324743, -0.17964268002945644, -0.3417344694384016, 0.07888648007753905, -0.3069115528098401, 0.008024064549134725, 0.2191264873512431, -0.0099048754711809,... |
706.2565 | Zgamma* production in e+e- interactions at sqrt{s} = 183 - 209 GeV | Measurements of Zgamma* production are presented using data collected by the
DELPHI detector at centre-of-mass energies ranging from 183 to 209 GeV,
corresponding to an integrated luminosity of about 667 pb^{-1}. The
measurements cover a wide range of the possible final state four-fermion
configurations: hadronic and... | hep-ex | measurements of zgamma production are presented using data collected by the delphi detector at centreofmass energies ranging from 183 to 209 gev corresponding to an integrated luminosity of about 667 pb1 the measurements cover a wide range of the possible final state fourfermion configurations hadronic and leptonic e e... | [['measurements', 'of', 'zgamma', 'production', 'are', 'presented', 'using', 'data', 'collected', 'by', 'the', 'delphi', 'detector', 'at', 'centreofmass', 'energies', 'ranging', 'from', '183', 'to', '209', 'gev', 'corresponding', 'to', 'an', 'integrated', 'luminosity', 'of', 'about', '667', 'pb1', 'the', 'measurements'... | [-0.06388396252188142, 0.2116608453363706, -0.03840552320772851, 0.07408135964241983, -0.01631867696048209, -0.16406244267192152, 0.052396322400481615, 0.31717825220483875, -0.18498522822779637, -0.33623611281315485, -0.07670423782568563, -0.3587019950082457, 0.1339778154881464, 0.13849119488322348, 0.08474259944115248... |
706.2566 | An anomaly detector with immediate feedback to hunt for planets of Earth
mass and below by microlensing | (abridged) The discovery of OGLE 2005-BLG-390Lb, the first cool rocky/icy
exoplanet, impressively demonstrated the sensitivity of the microlensing
technique to extra-solar planets below 10 M_earth. A planet of 1 M_earth in the
same spot would have provided a detectable deviation with an amplitude of ~ 3 %
and a durat... | astro-ph | abridged the discovery of ogle 2005blg390lb the first cool rockyicy exoplanet impressively demonstrated the sensitivity of the microlensing technique to extrasolar planets below 10 m_earth a planet of 1 m_earth in the same spot would have provided a detectable deviation with an amplitude of 3 and a duration of 12 h an ... | [['abridged', 'the', 'discovery', 'of', 'ogle', '2005blg390lb', 'the', 'first', 'cool', 'rockyicy', 'exoplanet', 'impressively', 'demonstrated', 'the', 'sensitivity', 'of', 'the', 'microlensing', 'technique', 'to', 'extrasolar', 'planets', 'below', '10', 'm_earth', 'a', 'planet', 'of', '1', 'm_earth', 'in', 'the', 'sam... | [-0.12671290675527416, 0.14799906848501201, -0.05865998755272647, 0.05338545306903225, -0.12542170188305052, -0.09934695159339092, 0.08665010428437117, 0.33354628590401264, -0.17533754354893144, -0.38375841386277565, 0.14042284812312572, -0.31054631914604797, -0.091130554638803, 0.2357555394077843, -0.09021968301808969... |
706.2567 | The hyperyoung HII region in G24.78+0.08 A1 | Context. G24.78+0.08 A1 is a 20 Msun star surrounded by a hypercompact (HC)
HII region, driving a CO bipolar outflow, and located at the center of a
massive rotating toroid undergoing infall towards the HC region. Recent water
maser observations suggest that the HC region is expanding and accretion onto
the star is h... | astro-ph | context g2478008 a1 is a 20 msun star surrounded by a hypercompact hc hii region driving a co bipolar outflow and located at the center of a massive rotating toroid undergoing infall towards the hc region recent water maser observations suggest that the hc region is expanding and accretion onto the star is halted aims ... | [['context', 'g2478008', 'a1', 'is', 'a', '20', 'msun', 'star', 'surrounded', 'by', 'a', 'hypercompact', 'hc', 'hii', 'region', 'driving', 'a', 'co', 'bipolar', 'outflow', 'and', 'located', 'at', 'the', 'center', 'of', 'a', 'massive', 'rotating', 'toroid', 'undergoing', 'infall', 'towards', 'the', 'hc', 'region', 'rece... | [-0.08603373393328544, 0.06478182707533223, -0.044784904132544434, 0.020079682737957898, -0.0301081005237856, -0.07089958604038606, 0.041286726583252255, 0.42690655055614013, -0.17191333092995129, -0.2613487206399441, 0.10633703934968854, -0.23562215097107977, 0.0035899180374196113, 0.11926335099632061, 0.0169469235642... |
706.2568 | Effect of Hetrovalent substitution at Mn site on the Magnetic and
Transport Properties of La$_{0.67}$Sr$_{0.33}$MnO$_3$ | Magnetic and transport properties of Ti substituted
La$_{0.67}$Sr$_{0.33}$MnO$_3$ are drastically affected with a change in
preparation conditions. Low temperature infra-red absorption measurements
reveal that this is perhaps due to inhomogeniety in substitution of Ti$^{4+}$
on Mn sites. It is found that, in the high... | cond-mat.str-el | magnetic and transport properties of ti substituted la_067sr_033mno_3 are drastically affected with a change in preparation conditions low temperature infrared absorption measurements reveal that this is perhaps due to inhomogeniety in substitution of ti4 on mn sites it is found that in the high temperature annealed sa... | [['magnetic', 'and', 'transport', 'properties', 'of', 'ti', 'substituted', 'la_067sr_033mno_3', 'are', 'drastically', 'affected', 'with', 'a', 'change', 'in', 'preparation', 'conditions', 'low', 'temperature', 'infrared', 'absorption', 'measurements', 'reveal', 'that', 'this', 'is', 'perhaps', 'due', 'to', 'inhomogenie... | [-0.14021356522095052, 0.2263790073338896, 0.024799996203827588, 0.01937419533152768, 0.03209459035530348, -0.17097080491525543, 0.1332904340656982, 0.3958005026533184, -0.2796238691715354, -0.30506827342535625, 0.007746763056440448, -0.3457960427463563, -0.034746785637583925, 0.11973891990121709, 0.017665165577041494,... |
706.2569 | Comparative study of various algorithms for the merging of parton
showers and matrix elements in hadronic collisions | We compare different procedures for combining fixed-order tree-level
matrix-element generators with parton showers. We use the case of W-production
at the Tevatron and the LHC to compare different implementations of the
so-called CKKW and MLM schemes using different matrix-element generators and
different parton casc... | hep-ph | we compare different procedures for combining fixedorder treelevel matrixelement generators with parton showers we use the case of wproduction at the tevatron and the lhc to compare different implementations of the socalled ckkw and mlm schemes using different matrixelement generators and different parton cascades we f... | [['we', 'compare', 'different', 'procedures', 'for', 'combining', 'fixedorder', 'treelevel', 'matrixelement', 'generators', 'with', 'parton', 'showers', 'we', 'use', 'the', 'case', 'of', 'wproduction', 'at', 'the', 'tevatron', 'and', 'the', 'lhc', 'to', 'compare', 'different', 'implementations', 'of', 'the', 'socalled'... | [-0.04290518336692604, 0.1615884928900938, -0.08243882499035385, 0.197945024202562, -0.00845431575898902, -0.08542572040016115, -0.04522125086731325, 0.46433947702585643, -0.13988901853908675, -0.2593357590484922, 0.018172775203819876, -0.33886525843103055, -0.05608909286684909, 0.21805250121406833, 0.02730089325015828... |
706.257 | Gray Curvature Identities for Almost Contact Metric Manifolds | The aim of this research is the study of Gray curvature identities,
introduced by Alfred Gray in \cite{kn:Gra76} for the class of almost hermitian
manifolds. As known till now, there is no equivalent for the class of almost
contact manifolds. For this purpose we use the Boohby-Wang fibration and the
warped manifolds ... | math.DG | the aim of this research is the study of gray curvature identities introduced by alfred gray in citekngra76 for the class of almost hermitian manifolds as known till now there is no equivalent for the class of almost contact manifolds for this purpose we use the boohbywang fibration and the warped manifolds constructio... | [['the', 'aim', 'of', 'this', 'research', 'is', 'the', 'study', 'of', 'gray', 'curvature', 'identities', 'introduced', 'by', 'alfred', 'gray', 'in', 'citekngra76', 'for', 'the', 'class', 'of', 'almost', 'hermitian', 'manifolds', 'as', 'known', 'till', 'now', 'there', 'is', 'no', 'equivalent', 'for', 'the', 'class', 'of... | [-0.15696387844016918, 0.06767864137946163, -0.0370492834597826, 0.10869889568824034, -0.06200792035804345, -0.1437679013953759, -0.05278619410326848, 0.36313147072035534, -0.24507966757966923, -0.2825026518235413, 0.16762795286038173, -0.24527117718870822, -0.20711304565461783, 0.19098457407492858, -0.1391114458728295... |
706.2571 | The contribution of Oxygen-Neon white dwarfs to the MACHO content of the
Galactic Halo | The interpretation of microlensing results towards the Large
Magellanic Cloud (LMC) still remains controversial. White dwarfs have been
proposed to explain these results and, hence, to contribute significantly to
the mass budget of our Galaxy. However, several constraints on the role played
by regular carbon-oxygen... | astro-ph | the interpretation of microlensing results towards the large magellanic cloud lmc still remains controversial white dwarfs have been proposed to explain these results and hence to contribute significantly to the mass budget of our galaxy however several constraints on the role played by regular carbonoxygen white dwarf... | [['the', 'interpretation', 'of', 'microlensing', 'results', 'towards', 'the', 'large', 'magellanic', 'cloud', 'lmc', 'still', 'remains', 'controversial', 'white', 'dwarfs', 'have', 'been', 'proposed', 'to', 'explain', 'these', 'results', 'and', 'hence', 'to', 'contribute', 'significantly', 'to', 'the', 'mass', 'budget'... | [-0.053102313610982374, 0.1554649975922638, -0.07561223401600567, 0.14599264062328768, -0.11416484907659244, -0.06178450433393292, 0.10407484638201103, 0.37470826078515024, -0.14172348875529261, -0.3591160098018732, 0.053216258775267894, -0.2989136104430818, -0.058475169939765946, 0.24647615485675428, -0.11275512107850... |
706.2572 | The Blackholic energy and the canonical Gamma-Ray Burst | We outline the main results of our GRB model, based on the three
interpretation paradigms we proposed in July 2001, comparing and contrasting
them with the ones in the current literature. Thanks to the observations by
Swift and by VLT, this analysis points to a "canonical GRB" originating from
markedly different astr... | astro-ph | we outline the main results of our grb model based on the three interpretation paradigms we proposed in july 2001 comparing and contrasting them with the ones in the current literature thanks to the observations by swift and by vlt this analysis points to a canonical grb originating from markedly different astrophysica... | [['we', 'outline', 'the', 'main', 'results', 'of', 'our', 'grb', 'model', 'based', 'on', 'the', 'three', 'interpretation', 'paradigms', 'we', 'proposed', 'in', 'july', '2001', 'comparing', 'and', 'contrasting', 'them', 'with', 'the', 'ones', 'in', 'the', 'current', 'literature', 'thanks', 'to', 'the', 'observations', '... | [-0.08045429583662786, 0.17324653204712562, -0.06718671595295653, 0.10276690893870881, -0.06630681834589594, -0.028121306066616225, 0.023243054548481433, 0.39813972775561685, -0.20902289600135424, -0.3027492296547653, 0.004096299323898095, -0.2870159711557417, 0.034776415937365246, 0.1806858419201886, 0.002074798086705... |
706.2573 | VLT/NACO observations of the High-Magnetic field radio pulsar PSR
J1119-6127 | Recent radio observations have unveiled the existence of a number of radio
pulsars with spin-down derived magnetic fields in the magnetar range. However,
their observational properties appears to be more similar to classical radio
pulsars than to magnetars. To shed light on this puzzle we first have to
determine whet... | astro-ph | recent radio observations have unveiled the existence of a number of radio pulsars with spindown derived magnetic fields in the magnetar range however their observational properties appears to be more similar to classical radio pulsars than to magnetars to shed light on this puzzle we first have to determine whether th... | [['recent', 'radio', 'observations', 'have', 'unveiled', 'the', 'existence', 'of', 'a', 'number', 'of', 'radio', 'pulsars', 'with', 'spindown', 'derived', 'magnetic', 'fields', 'in', 'the', 'magnetar', 'range', 'however', 'their', 'observational', 'properties', 'appears', 'to', 'be', 'more', 'similar', 'to', 'classical... | [-0.11249443794112289, 0.13238075761260784, -0.056055665549981155, 0.09600205407477916, -0.16549843846161555, -0.09607802436846058, 0.08512271231653669, 0.4083948243454826, -0.2086316980171676, -0.3667613983472309, 0.09223799808405159, -0.25421340866241515, -0.018645638194525752, 0.2688827919944121, -0.0138281542694241... |
706.2574 | The narrow-line region of narrow-line and broad-line type 1 AGN I. A
zone of avoidance in density | The properties of narrow-line Seyfert 1 (NLS1) galaxies, the links and
correlations between them, and the physics behind them, are still not well
understood. Apart from accretion rates and black hole masses, density and
outflows were speculated to be among the main drivers of the NLS1 phenomenon.
Here, we utilize the... | astro-ph | the properties of narrowline seyfert 1 nls1 galaxies the links and correlations between them and the physics behind them are still not well understood apart from accretion rates and black hole masses density and outflows were speculated to be among the main drivers of the nls1 phenomenon here we utilize the diagnostic ... | [['the', 'properties', 'of', 'narrowline', 'seyfert', '1', 'nls1', 'galaxies', 'the', 'links', 'and', 'correlations', 'between', 'them', 'and', 'the', 'physics', 'behind', 'them', 'are', 'still', 'not', 'well', 'understood', 'apart', 'from', 'accretion', 'rates', 'and', 'black', 'hole', 'masses', 'density', 'and', 'out... | [-0.06144971690992726, 0.07663150330054316, -0.028641165010234778, 0.1600945038760596, -0.06697683413810235, -0.09452328188939298, 0.07082253553993763, 0.4793557335642424, -0.0875404309996582, -0.32817034390259614, 0.015078517460224634, -0.295924014376199, -0.019846214393668987, 0.15253356825337408, -0.0325604490044110... |
706.2575 | A new lower bound on the independence number of a graph | For a given connected graph G on n vertices and m edges, we prove that its
independence number is at least (2m+n+2-sqrt(sqr(2m+n+2)-16sqr(n)))/8.
| cs.DM | for a given connected graph g on n vertices and m edges we prove that its independence number is at least 2mn2sqrtsqr2mn216sqrn8 | [['for', 'a', 'given', 'connected', 'graph', 'g', 'on', 'n', 'vertices', 'and', 'm', 'edges', 'we', 'prove', 'that', 'its', 'independence', 'number', 'is', 'at', 'least', '2mn2sqrtsqr2mn216sqrn8']] | [-0.2753657395286219, 0.13849923639957393, -0.02128304871508763, -0.028165505461705227, -0.1143964741024233, -0.17875527594948099, 0.06924949496862523, 0.40835259340348695, -0.208010532671497, -0.36105866277856485, 0.04248273317214279, -0.39746456415880294, -0.12106265492426853, 0.04388896906970158, -0.0762468159110063... |
706.2576 | First performance studies of a prototype for the CASTOR forward
calorimeter at the CMS experiment | We present results on the performance of the first prototype of the CASTOR
quartz-tungsten sampling calorimeter, to be installed in the very forward
region of the CMS experiment at the LHC. This study includes GEANT Monte Carlo
simulations of the Cherenkov light transmission efficiency of different types
of air-core ... | physics.ins-det nucl-ex | we present results on the performance of the first prototype of the castor quartztungsten sampling calorimeter to be installed in the very forward region of the cms experiment at the lhc this study includes geant monte carlo simulations of the cherenkov light transmission efficiency of different types of aircore light ... | [['we', 'present', 'results', 'on', 'the', 'performance', 'of', 'the', 'first', 'prototype', 'of', 'the', 'castor', 'quartztungsten', 'sampling', 'calorimeter', 'to', 'be', 'installed', 'in', 'the', 'very', 'forward', 'region', 'of', 'the', 'cms', 'experiment', 'at', 'the', 'lhc', 'this', 'study', 'includes', 'geant', ... | [-0.040148218024949556, 0.15084116191786454, -0.07621149932698454, 0.0063066143937576865, 0.0021261648975358515, -0.15774770946333522, -0.007138652615840776, 0.4401750853476038, -0.16896595843288986, -0.3782637938093699, 0.08693249319817443, -0.3448869257737867, -0.015561486659266177, 0.2427809358208028, 0.009958142725... |
706.2577 | A Groshev Theorem for Small Linear Forms | In this paper the absolute value or distance from the origin analogue of the
classical Khintchine-Groshev theorem is established for a single linear form
with a `slowly decreasing' error function.
| math.NT | in this paper the absolute value or distance from the origin analogue of the classical khintchinegroshev theorem is established for a single linear form with a slowly decreasing error function | [['in', 'this', 'paper', 'the', 'absolute', 'value', 'or', 'distance', 'from', 'the', 'origin', 'analogue', 'of', 'the', 'classical', 'khintchinegroshev', 'theorem', 'is', 'established', 'for', 'a', 'single', 'linear', 'form', 'with', 'a', 'slowly', 'decreasing', 'error', 'function']] | [-0.10439621868232886, 0.06816721921786666, -0.1208586849582692, 0.07747811923424403, -0.05103997178375721, -0.11295222866659363, 0.10259638345257069, 0.28277944078048073, -0.33384193405508994, -0.259104768683513, 0.1271260582221051, -0.271354699259003, -0.12653895443460594, 0.2080418984638527, -0.08963991242150465, 0.... |
706.2578 | Using the $e^\pm \mu^\mp + E^{miss}_T$ and $l^+l^- + E^{miss}_T$
Signatures in the Search for Supersymmetry and Constraining the MSSM model at
LHC | We study the $e^{\pm}\mu^{\mp} + E^{miss}_T$ and $l^+l^- + E^{miss}_T$
signatures $(l = e, \mu)$ for different values of $\tan\beta$ in the mSUGRA
model. With $\tan\beta$ rising, we observe a characteristic change in the shape
of dilepton mass spectra in $l^+l^- + E^{miss}_T $ versus $e^{\pm}\mu^{\mp}$
final states r... | hep-ph | we study the epmmump emiss_t and ll emiss_t signatures l e mu for different values of tanbeta in the msugra model with tanbeta rising we observe a characteristic change in the shape of dilepton mass spectra in ll emiss_t versus epmmump final states reflecting the decrease of tildechi0_2 to ll tildechi0_1 branching rati... | [['we', 'study', 'the', 'epmmump', 'emiss_t', 'and', 'll', 'emiss_t', 'signatures', 'l', 'e', 'mu', 'for', 'different', 'values', 'of', 'tanbeta', 'in', 'the', 'msugra', 'model', 'with', 'tanbeta', 'rising', 'we', 'observe', 'a', 'characteristic', 'change', 'in', 'the', 'shape', 'of', 'dilepton', 'mass', 'spectra', 'in... | [-0.11663887950134517, 0.2637256753337367, -0.01708011815081472, 0.18058429229194703, -0.06318296699960163, -0.21139034339685694, 0.05732095011584191, 0.3012272621356491, -0.16222335461635087, -0.3308829368105617, 0.0009332103722229384, -0.31782417121491785, 0.027723434770925214, 0.13107784967650188, 0.0106483081834849... |
706.2579 | Prescribing the behaviour of geodesics in negative curvature | Given a family of (almost) disjoint strictly convex subsets of a complete
negatively curved Riemannian manifold M, such as balls, horoballs, tubular
neighborhoods of totally geodesic submanifolds, etc, the aim of this paper is
to construct geodesic rays or lines in M which have exactly once an exactly
prescribed (big... | math.DG math.MG math.NT | given a family of almost disjoint strictly convex subsets of a complete negatively curved riemannian manifold m such as balls horoballs tubular neighborhoods of totally geodesic submanifolds etc the aim of this paper is to construct geodesic rays or lines in m which have exactly once an exactly prescribed big enough pe... | [['given', 'a', 'family', 'of', 'almost', 'disjoint', 'strictly', 'convex', 'subsets', 'of', 'a', 'complete', 'negatively', 'curved', 'riemannian', 'manifold', 'm', 'such', 'as', 'balls', 'horoballs', 'tubular', 'neighborhoods', 'of', 'totally', 'geodesic', 'submanifolds', 'etc', 'the', 'aim', 'of', 'this', 'paper', 'i... | [-0.17967874605083534, 0.15254182114586, -0.049032647531034784, 0.09014401974507483, -0.0825404276751649, -0.14720519408305635, 0.009132541237405933, 0.3651729422454625, -0.2673639448554213, -0.24380310738820637, 0.09424118946546188, -0.30917269080606247, -0.11983000621574917, 0.20891940870944328, -0.13674915892266626,... |
706.258 | Planar maps whose second iterate has a unique fixed point | Let a>0, F: R^2 -> R^2 be a differentiable (not necessarily C^1) map and
Spec(F) be the set of (complex) eigenvalues of the derivative F'(p) when p
varies in R^2.
(a) If Spec(F) is disjoint of the interval [1,1+a[, then Fix(F) has at most
one element, where Fix(F) denotes the set of fixed points of F.
(b) If Spec... | math.DS math.CA | let a0 f r2 r2 be a differentiable not necessarily c1 map and specf be the set of complex eigenvalues of the derivative fp when p varies in r2 a if specf is disjoint of the interval 11a then fixf has at most one element where fixf denotes the set of fixed points of f b if specf is disjoint of the real line r then fixf2... | [['let', 'a0', 'f', 'r2', 'r2', 'be', 'a', 'differentiable', 'not', 'necessarily', 'c1', 'map', 'and', 'specf', 'be', 'the', 'set', 'of', 'complex', 'eigenvalues', 'of', 'the', 'derivative', 'fp', 'when', 'p', 'varies', 'in', 'r2', 'a', 'if', 'specf', 'is', 'disjoint', 'of', 'the', 'interval', '11a', 'then', 'fixf', 'h... | [-0.16538263966237576, 0.10601935519928664, -0.04113759687268766, -0.03826808635781611, -0.04249086974411678, -0.22441875773259032, -0.013769515904820931, 0.3474983969886958, -0.27379745103641817, -0.16199685871260058, 0.13271744074677053, -0.35129668143935316, -0.03060259477687921, 0.14774685619156283, -0.038166197003... |
706.2581 | Internal labelling operators and contractions of Lie algebras | We analyze under which conditions the missing label problem associated to a
reduction chain $\frak{s}^{\prime}\subset \frak{s}$ of (simple) Lie algebras
can be completely solved by means of an In\"on\"u-Wigner contraction $\frak{g}$
naturally related to the embedding. This provides a new interpretation of the
missing... | hep-th | we analyze under which conditions the missing label problem associated to a reduction chain fraksprimesubset fraks of simple lie algebras can be completely solved by means of an inonuwigner contraction frakg naturally related to the embedding this provides a new interpretation of the missing label operators in terms of... | [['we', 'analyze', 'under', 'which', 'conditions', 'the', 'missing', 'label', 'problem', 'associated', 'to', 'a', 'reduction', 'chain', 'fraksprimesubset', 'fraks', 'of', 'simple', 'lie', 'algebras', 'can', 'be', 'completely', 'solved', 'by', 'means', 'of', 'an', 'inonuwigner', 'contraction', 'frakg', 'naturally', 'rel... | [-0.14846909705762906, 0.09939207867864752, -0.06557415529257721, 0.09432028647150016, -0.1433727957877434, -0.1394616929296818, 0.0002690633526071906, 0.3366888348452954, -0.3677634823032551, -0.24087949350165824, 0.14312018899945542, -0.21698824142416318, -0.1422955913262235, 0.18997862717757621, -0.14318498300595417... |
706.2582 | Diagrammatic content of the DMFT for the Holstein polaron problem in
finite dimensions | In the context of the Holstein polaron problem it is shown that the dynamical
mean field theory (DMFT) corresponds to the summation of a special class of
local diagrams in the skeleton expansion of the self-energy. In the real space
representation, these local diagrams are characterized by the absence of vertex
corre... | cond-mat.str-el | in the context of the holstein polaron problem it is shown that the dynamical mean field theory dmft corresponds to the summation of a special class of local diagrams in the skeleton expansion of the selfenergy in the real space representation these local diagrams are characterized by the absence of vertex corrections ... | [['in', 'the', 'context', 'of', 'the', 'holstein', 'polaron', 'problem', 'it', 'is', 'shown', 'that', 'the', 'dynamical', 'mean', 'field', 'theory', 'dmft', 'corresponds', 'to', 'the', 'summation', 'of', 'a', 'special', 'class', 'of', 'local', 'diagrams', 'in', 'the', 'skeleton', 'expansion', 'of', 'the', 'selfenergy',... | [-0.12732706640659372, 0.1428138092577235, -0.05862967358943798, 0.12146115523533646, -0.025396274013528182, -0.110109469798609, 0.056437042396717166, 0.3379120863557084, -0.2653266287325367, -0.20801447810771972, 0.03486157984754293, -0.3017202635285264, -0.11605661987229737, 0.14119943495450624, 0.027317627951669605,... |
706.2583 | Hindered Coulomb explosion of embedded Na clusters -- stopping, shape
dynamics and energy transport | We investigate the dynamical evolution of a Na$_8$ cluster embedded in Ar
matrices of various sizes from N=30 to 1048. The system is excited by an
intense short laser pulse leading to high ionization stages. We analyze the
subsequent highly non-linear motion of cluster and Ar environment in terms of
trajectories, sha... | cond-mat.other | we investigate the dynamical evolution of a na_8 cluster embedded in ar matrices of various sizes from n30 to 1048 the system is excited by an intense short laser pulse leading to high ionization stages we analyze the subsequent highly nonlinear motion of cluster and ar environment in terms of trajectories shapes and e... | [['we', 'investigate', 'the', 'dynamical', 'evolution', 'of', 'a', 'na_8', 'cluster', 'embedded', 'in', 'ar', 'matrices', 'of', 'various', 'sizes', 'from', 'n30', 'to', '1048', 'the', 'system', 'is', 'excited', 'by', 'an', 'intense', 'short', 'laser', 'pulse', 'leading', 'to', 'high', 'ionization', 'stages', 'we', 'ana... | [-0.10159249837823098, 0.2191394833754126, -0.03724631280389451, 0.07282824748469417, 0.05360080784129846, -0.09582497682226893, -0.003154326272943548, 0.4155562049247154, -0.2936213586651827, -0.3155910722690969, 0.0751492970655068, -0.27366732453522163, -0.014762885193162748, 0.14696282962379792, 0.02440269552313417,... |
706.2584 | Vortex States Induced by Proximity Effect in Hybrid
Ferromagnet-Superconductor Systems | We consider superconductivity nucleation in multiply connected mesoscopic
samples such as thin-walled cylinders or rings placed in electrical contact
with a ferromagnet. The superconducting critical temperature and order
parameter structure are studied on the basis of linearized Usadel equations. We
suggest a mechani... | cond-mat.supr-con | we consider superconductivity nucleation in multiply connected mesoscopic samples such as thinwalled cylinders or rings placed in electrical contact with a ferromagnet the superconducting critical temperature and order parameter structure are studied on the basis of linearized usadel equations we suggest a mechanism of... | [['we', 'consider', 'superconductivity', 'nucleation', 'in', 'multiply', 'connected', 'mesoscopic', 'samples', 'such', 'as', 'thinwalled', 'cylinders', 'or', 'rings', 'placed', 'in', 'electrical', 'contact', 'with', 'a', 'ferromagnet', 'the', 'superconducting', 'critical', 'temperature', 'and', 'order', 'parameter', 's... | [-0.2736228964317383, 0.2068656815810957, -0.014386897027078602, 0.007641445754820274, -0.0533858902409621, -0.14529181611336148, 0.05110026789932615, 0.35595557611021733, -0.24943354808621937, -0.2450000428297143, 0.010404826596236995, -0.3245051889939027, -0.1109845565224532, 0.16650520226620655, 0.09792374987025848,... |
706.2585 | Decisive Markov Chains | We consider qualitative and quantitative verification problems for
infinite-state Markov chains. We call a Markov chain decisive w.r.t. a given
set of target states F if it almost certainly eventually reaches either F or a
state from which F can no longer be reached. While all finite Markov chains are
trivially decis... | cs.LO cs.DM | we consider qualitative and quantitative verification problems for infinitestate markov chains we call a markov chain decisive wrt a given set of target states f if it almost certainly eventually reaches either f or a state from which f can no longer be reached while all finite markov chains are trivially decisive for ... | [['we', 'consider', 'qualitative', 'and', 'quantitative', 'verification', 'problems', 'for', 'infinitestate', 'markov', 'chains', 'we', 'call', 'a', 'markov', 'chain', 'decisive', 'wrt', 'a', 'given', 'set', 'of', 'target', 'states', 'f', 'if', 'it', 'almost', 'certainly', 'eventually', 'reaches', 'either', 'f', 'or', ... | [-0.13522362806500263, 0.1283440206614092, -0.04665931495042117, 0.11577391408173611, -0.03907345037097858, -0.20446103611638777, 0.07916326419242072, 0.40805171358591646, -0.30619248525015536, -0.22470489831028295, 0.13773403705082016, -0.22669215155333156, -0.0720044969991714, 0.19186679800512577, -0.0376033481050337... |
706.2586 | Nuclear Cosmic Rays propagation in the Atmosphere | The transport of the nuclear cosmic ray flux in the atmosphere is studied and
the atmospheric corrections to be applied to the measurements are calculated.
The contribution of the calculated corrections to the accuracy of the
experimental results are discussed and evaluated over the kinetic energy range
10-10$^{3}$ G... | astro-ph | the transport of the nuclear cosmic ray flux in the atmosphere is studied and the atmospheric corrections to be applied to the measurements are calculated the contribution of the calculated corrections to the accuracy of the experimental results are discussed and evaluated over the kinetic energy range 10103 gevn the b... | [['the', 'transport', 'of', 'the', 'nuclear', 'cosmic', 'ray', 'flux', 'in', 'the', 'atmosphere', 'is', 'studied', 'and', 'the', 'atmospheric', 'corrections', 'to', 'be', 'applied', 'to', 'the', 'measurements', 'are', 'calculated', 'the', 'contribution', 'of', 'the', 'calculated', 'corrections', 'to', 'the', 'accuracy'... | [-0.0778604096934631, 0.15522908068421046, -0.014965129948062142, 0.12784311550004954, 0.05191825028145459, -0.05636335300031777, -0.007879186183123327, 0.37333909867376813, -0.23550474149084127, -0.3143928596727187, 0.06386553508331771, -0.3250361361268272, -0.014064368417077675, 0.24077692637560752, 0.039711851569846... |
706.2587 | Electroproduction of longitudinally polarized vector mesons | It is reported on an analysis of electroproduction of light vector mesons at
small Bjorken-x within the handbag approach. The partonic subprocesses, meson
electroproduction off quarks or gluons, are calculated within the modified
perturbative approach in which quark transverse momenta are retained. The soft
hadronic ... | hep-ph | it is reported on an analysis of electroproduction of light vector mesons at small bjorkenx within the handbag approach the partonic subprocesses meson electroproduction off quarks or gluons are calculated within the modified perturbative approach in which quark transverse momenta are retained the soft hadronic matrix ... | [['it', 'is', 'reported', 'on', 'an', 'analysis', 'of', 'electroproduction', 'of', 'light', 'vector', 'mesons', 'at', 'small', 'bjorkenx', 'within', 'the', 'handbag', 'approach', 'the', 'partonic', 'subprocesses', 'meson', 'electroproduction', 'off', 'quarks', 'or', 'gluons', 'are', 'calculated', 'within', 'the', 'modi... | [-0.020343093977518087, 0.2719290896381656, -0.16863671423573243, 0.15683219379402305, -0.013774429947922105, -0.05454178118686143, 0.0020671093493307893, 0.4061265498987938, -0.15681481546673334, -0.22354321510187888, -0.11979344511576193, -0.32777178013011027, 0.03291886026088737, 0.13668766640077687, 0.0881824014120... |
706.2588 | Betti numbers for fat point ideals in the plane: a geometric approach | We consider the open problem of determining the graded Betti numbers for fat
point subschemes supported at general points of the projective plane. We relate
this problem to the open geometric problem of determining the splitting type of
the pullback of the cotangent bundle on the plane to the normalization of
certain... | math.AG math.AC | we consider the open problem of determining the graded betti numbers for fat point subschemes supported at general points of the projective plane we relate this problem to the open geometric problem of determining the splitting type of the pullback of the cotangent bundle on the plane to the normalization of certain ra... | [['we', 'consider', 'the', 'open', 'problem', 'of', 'determining', 'the', 'graded', 'betti', 'numbers', 'for', 'fat', 'point', 'subschemes', 'supported', 'at', 'general', 'points', 'of', 'the', 'projective', 'plane', 'we', 'relate', 'this', 'problem', 'to', 'the', 'open', 'geometric', 'problem', 'of', 'determining', 't... | [-0.21648761999755595, 0.028014604195050197, -0.0689444827683572, 0.10209834001678345, -0.08832155124951355, -0.12603465248390125, 0.049735076848190986, 0.300927046346604, -0.3183707645826822, -0.25475349350253473, 0.07612855640881871, -0.2176973327752077, -0.14185756502824054, 0.2623197239889713, -0.12415092311975723,... |
706.2589 | The aligned nuclear targets for investigation of time reversal
invariance violation: thermal heating and optimization of target dimension | The thermal heating of aligned nuclear targets of HIO_3, LiIO_3 ans Sb target
materials under neutron irradiation at JSNS is considered. It is shown that
presently the targets of large volumes (several tens of cm^3) can be used in
experiment. The optimal target dimensions are recommended for investigation
with resona... | nucl-ex | the thermal heating of aligned nuclear targets of hio_3 liio_3 ans sb target materials under neutron irradiation at jsns is considered it is shown that presently the targets of large volumes several tens of cm3 can be used in experiment the optimal target dimensions are recommended for investigation with resonance neut... | [['the', 'thermal', 'heating', 'of', 'aligned', 'nuclear', 'targets', 'of', 'hio_3', 'liio_3', 'ans', 'sb', 'target', 'materials', 'under', 'neutron', 'irradiation', 'at', 'jsns', 'is', 'considered', 'it', 'is', 'shown', 'that', 'presently', 'the', 'targets', 'of', 'large', 'volumes', 'several', 'tens', 'of', 'cm3', 'c... | [-0.06971534481678202, 0.214561399115726, -0.01327287472058954, 0.10241167079982195, -0.041642544249635795, -0.10893150750374378, 0.04070014960868934, 0.3629135359403526, -0.2039522199869849, -0.3562689511495274, 0.05761375107537132, -0.3254616990425559, 0.013651202939082544, 0.18934395272273916, 0.026675030691982356, ... |
706.259 | Extreme Value Theory and the Solar Cycle | We investigate the statistical properties of the extreme events of the solar
cycle as measured by the sunspot number. The recent advances in the methodology
of the theory of extreme values is applied to the maximal extremes of the time
series of sunspots. We focus on the extreme events that exceed a carefully
chosen ... | astro-ph | we investigate the statistical properties of the extreme events of the solar cycle as measured by the sunspot number the recent advances in the methodology of the theory of extreme values is applied to the maximal extremes of the time series of sunspots we focus on the extreme events that exceed a carefully chosen thre... | [['we', 'investigate', 'the', 'statistical', 'properties', 'of', 'the', 'extreme', 'events', 'of', 'the', 'solar', 'cycle', 'as', 'measured', 'by', 'the', 'sunspot', 'number', 'the', 'recent', 'advances', 'in', 'the', 'methodology', 'of', 'the', 'theory', 'of', 'extreme', 'values', 'is', 'applied', 'to', 'the', 'maxima... | [-0.07026294673905795, 0.12156406064471716, -0.07158981537407574, 0.10185470686168022, -0.043351615365827455, -0.04023082864975246, 0.10613030896007937, 0.3359118808953402, -0.22584290732872128, -0.3619524513060848, 0.12830601281505855, -0.29522129593339436, -0.08996967059647432, 0.22570543919379513, -0.061504478320906... |
706.2591 | Self-assembled Pt nanowires on Ge(001): Relaxation effects | Absorption of Pt on the Ge(001) surface results in stable self-organized Pt
nanowires, extending over some hundred nanometers. Based on band structure
calculations within density functional theory and the generalized gradient
approximation, the structural relaxation of the Ge--Pt surface is investigated.
The surface ... | cond-mat.mes-hall | absorption of pt on the ge001 surface results in stable selforganized pt nanowires extending over some hundred nanometers based on band structure calculations within density functional theory and the generalized gradient approximation the structural relaxation of the gept surface is investigated the surface reconstruct... | [['absorption', 'of', 'pt', 'on', 'the', 'ge001', 'surface', 'results', 'in', 'stable', 'selforganized', 'pt', 'nanowires', 'extending', 'over', 'some', 'hundred', 'nanometers', 'based', 'on', 'band', 'structure', 'calculations', 'within', 'density', 'functional', 'theory', 'and', 'the', 'generalized', 'gradient', 'app... | [-0.12916895191683764, 0.14855053876479618, -0.04588409458202394, 0.027190949155177658, 0.014158993263286774, -0.1289247999983755, 0.05400213437223092, 0.4145637439996606, -0.28400333145765044, -0.30457361915496867, -0.008230292381756384, -0.33521054951342366, -0.16610738615307843, 0.16292894904200703, 0.02593458180775... |
706.2592 | Inhomogeneous and self-organised temperature in Schelling-Ising model | The Schelling model of 1971 is a complicated version of a square-lattice
Ising model at zero temperature, to explain urban segregation, based on the
neighbour preferences of the residents, without external reasons. Various
versions between Ising and Schelling models give about the same results.
Inhomogeneous "tempera... | physics.soc-ph | the schelling model of 1971 is a complicated version of a squarelattice ising model at zero temperature to explain urban segregation based on the neighbour preferences of the residents without external reasons various versions between ising and schelling models give about the same results inhomogeneous temperatures t d... | [['the', 'schelling', 'model', 'of', '1971', 'is', 'a', 'complicated', 'version', 'of', 'a', 'squarelattice', 'ising', 'model', 'at', 'zero', 'temperature', 'to', 'explain', 'urban', 'segregation', 'based', 'on', 'the', 'neighbour', 'preferences', 'of', 'the', 'residents', 'without', 'external', 'reasons', 'various', '... | [-0.09714281796614695, 0.1464690183486656, -0.09548992041142329, 0.11995689044466845, -0.07544275778619682, -0.17245013206539786, 0.10269770889905938, 0.36580127261250334, -0.19513048798612811, -0.3555695593685788, 0.04399135810158709, -0.2654097552329083, -0.11623903747086468, 0.11696645452021211, -0.03371776204884929... |
706.2593 | Using the Zeldovich dynamics to test expansion schemes | We apply various expansion schemes that may be used to study gravitational
clustering to the simple case of the Zeldovich dynamics. Using the well-known
exact solution of the Zeldovich dynamics we can compare the predictions of
these various perturbative methods with the exact nonlinear result and study
their converg... | astro-ph | we apply various expansion schemes that may be used to study gravitational clustering to the simple case of the zeldovich dynamics using the wellknown exact solution of the zeldovich dynamics we can compare the predictions of these various perturbative methods with the exact nonlinear result and study their convergence... | [['we', 'apply', 'various', 'expansion', 'schemes', 'that', 'may', 'be', 'used', 'to', 'study', 'gravitational', 'clustering', 'to', 'the', 'simple', 'case', 'of', 'the', 'zeldovich', 'dynamics', 'using', 'the', 'wellknown', 'exact', 'solution', 'of', 'the', 'zeldovich', 'dynamics', 'we', 'can', 'compare', 'the', 'pred... | [-0.09556653353635736, 0.0811302310367244, -0.13099576399559584, 0.12737828460949813, -0.08286271026759497, -0.10382489467618901, -0.02566486289732935, 0.34429515658486176, -0.25843883712953714, -0.26490854086064775, 0.10400499137675442, -0.2681773063486488, -0.1440642263275514, 0.21395491378286413, 0.01954923410547811... |
706.2594 | Baryogenesis from the amplification of vacuum fluctuations during
inflation | We propose that the baryon asymmetry of the Universe may originate from the
amplification of quantum fluctuations of a light complex scalar field during
inflation. CP-violation is sourced by complex mass terms, which are smaller
than the Hubble rate, as well as non-standard kinetic terms. We find that, when
assuming ... | astro-ph | we propose that the baryon asymmetry of the universe may originate from the amplification of quantum fluctuations of a light complex scalar field during inflation cpviolation is sourced by complex mass terms which are smaller than the hubble rate as well as nonstandard kinetic terms we find that when assuming 60 efolds... | [['we', 'propose', 'that', 'the', 'baryon', 'asymmetry', 'of', 'the', 'universe', 'may', 'originate', 'from', 'the', 'amplification', 'of', 'quantum', 'fluctuations', 'of', 'a', 'light', 'complex', 'scalar', 'field', 'during', 'inflation', 'cpviolation', 'is', 'sourced', 'by', 'complex', 'mass', 'terms', 'which', 'are'... | [-0.14160431162297224, 0.2871110989057179, -0.046099624999411656, 0.12027392234245127, -0.05550902391773429, -0.07433267124258819, -0.0369847723821785, 0.2532698071948933, -0.21136959403585853, -0.38943626723262703, 0.07678818805509488, -0.2214347799936456, -0.04597035703364383, 0.21033463367585387, -0.0144294167690899... |
706.2595 | The Kashiwara-Vergne conjecture | This is a Bourbaki's seminar text. We introduce the combinatorial
Kashiwara-Vergne conjecture on the Baker-Campbell-Hausdorff serie. After
recalling previous results and consequences, we explain the
Alekseev-Meinrenken's proof [math.QA/0506499]
| math.QA math.RT | this is a bourbakis seminar text we introduce the combinatorial kashiwaravergne conjecture on the bakercampbellhausdorff serie after recalling previous results and consequences we explain the alekseevmeinrenkens proof mathqa0506499 | [['this', 'is', 'a', 'bourbakis', 'seminar', 'text', 'we', 'introduce', 'the', 'combinatorial', 'kashiwaravergne', 'conjecture', 'on', 'the', 'bakercampbellhausdorff', 'serie', 'after', 'recalling', 'previous', 'results', 'and', 'consequences', 'we', 'explain', 'the', 'alekseevmeinrenkens', 'proof', 'mathqa0506499']] | [-0.12462844900213756, -0.010651030058327775, -0.18417517024164015, 0.0905394025433522, -0.17198399937926576, -0.07400906515809205, 0.017501589770500477, 0.28174156007858425, -0.2468366357856072, -0.23857644429573646, 0.13100492938135105, -0.2588971372102745, -0.24166884158666319, 0.1878724547389608, -0.237098212532985... |
706.2596 | Is the Interpretation of Delayed-Choice Experiments Misleading? | The interpretation of an experimental realization of Wheeler's delayed-choice
gedanken experiment is discussed and called into question.
| physics.pop-ph physics.hist-ph quant-ph | the interpretation of an experimental realization of wheelers delayedchoice gedanken experiment is discussed and called into question | [['the', 'interpretation', 'of', 'an', 'experimental', 'realization', 'of', 'wheelers', 'delayedchoice', 'gedanken', 'experiment', 'is', 'discussed', 'and', 'called', 'into', 'question']] | [-0.10569724152960322, 0.15843875046822872, -0.15047661291764064, 0.07219974963021848, -0.12368397885823951, -0.2516087260754669, -0.007136341458296075, 0.28248517861699357, -0.17502930102979436, -0.29320684853283796, 0.018166289774372298, -0.2767651266801883, -0.18654129007721648, 0.31025531011469226, -0.1602842676288... |
706.2597 | Propagation of UHE protons through a magnetized large scale structure | The propagation of UHECRs is affected by the intergalactic magnetic fields
that were produced during the course of the large scale structure formation of
the universe. We adopt a novel model where the large scale extragalactic
magnetic fields (EGMF) are estimated from local dynamic properties of the gas
flows in hydr... | astro-ph | the propagation of uhecrs is affected by the intergalactic magnetic fields that were produced during the course of the large scale structure formation of the universe we adopt a novel model where the large scale extragalactic magnetic fields egmf are estimated from local dynamic properties of the gas flows in hydrodyna... | [['the', 'propagation', 'of', 'uhecrs', 'is', 'affected', 'by', 'the', 'intergalactic', 'magnetic', 'fields', 'that', 'were', 'produced', 'during', 'the', 'course', 'of', 'the', 'large', 'scale', 'structure', 'formation', 'of', 'the', 'universe', 'we', 'adopt', 'a', 'novel', 'model', 'where', 'the', 'large', 'scale', '... | [-0.1437203960824543, 0.2242248165858989, -0.04753177587398622, 0.1242332607985307, -0.052354808470918834, 0.006884905881781736, -0.03212840923975803, 0.3693756869174222, -0.2683462497069795, -0.3750730668170712, 0.01572544703908806, -0.26736081787186045, -0.0107271357670299, 0.1701621125714901, 0.08827839865006952, -0... |
706.2598 | Practical wavelet design on the sphere | We address the question of designing isotropic analysis functions on the
sphere which are perfectly limited in the spectral domain and optimally
localized in the spatial domain. This work is motivated by the need of
localized analysis tools in domains where the data is lying on the sphere,
e.g.{} the science of the C... | math.NA astro-ph math.CA math.ST stat.TH | we address the question of designing isotropic analysis functions on the sphere which are perfectly limited in the spectral domain and optimally localized in the spatial domain this work is motivated by the need of localized analysis tools in domains where the data is lying on the sphere eg the science of the cosmic mi... | [['we', 'address', 'the', 'question', 'of', 'designing', 'isotropic', 'analysis', 'functions', 'on', 'the', 'sphere', 'which', 'are', 'perfectly', 'limited', 'in', 'the', 'spectral', 'domain', 'and', 'optimally', 'localized', 'in', 'the', 'spatial', 'domain', 'this', 'work', 'is', 'motivated', 'by', 'the', 'need', 'of'... | [-0.08234924705521691, 0.07380709468409241, -0.05005157888600869, 0.0695452852371437, -0.05451741217569049, -0.07868403987959027, 0.007916166036877604, 0.37547488756743924, -0.24006814721533806, -0.3024195143065992, 0.16070638329672096, -0.2680316505277352, -0.14629188336298934, 0.2153496813428189, -0.06670686848727721... |
706.2599 | Black hole in the West Nucleus of Arp 220 | We present new observations with the IRAM Interferometer, in its
longest-baseline configuration, of the CO(2-1) line and the 1.3mm dust
radiation from the Arp 220 nuclear region. The dust source in the West nucleus
has a size of 0.19 x 0.13 arcsec and a 1.3mm brightness temperature of 90K.
This implies that the dust ... | astro-ph | we present new observations with the iram interferometer in its longestbaseline configuration of the co21 line and the 13mm dust radiation from the arp 220 nuclear region the dust source in the west nucleus has a size of 019 x 013 arcsec and a 13mm brightness temperature of 90k this implies that the dust ring in the we... | [['we', 'present', 'new', 'observations', 'with', 'the', 'iram', 'interferometer', 'in', 'its', 'longestbaseline', 'configuration', 'of', 'the', 'co21', 'line', 'and', 'the', '13mm', 'dust', 'radiation', 'from', 'the', 'arp', '220', 'nuclear', 'region', 'the', 'dust', 'source', 'in', 'the', 'west', 'nucleus', 'has', 'a... | [-0.04296692522309188, 0.11032739097891386, -0.060194923334001074, 0.045799450829092946, -0.0399429130390109, -0.09517702871567703, -0.01813930949817101, 0.47877468419305624, -0.1587568221491113, -0.240872468180134, 0.0955429121652352, -0.2942592405403654, 0.06190610101801299, 0.14272679284747158, -0.039229363869526426... |
706.26 | Deformations of M-theory Killing superalgebras | We classify the Lie superalgebra deformations of the Killing superalgebras of
some M-theory backgrounds. We show that the Killing superalgebras of the
Minkowski, Freund--Rubin and M5-brane backgrounds are rigid, whereas the ones
for the M-wave, the Kaluza--Klein monopole and the M2-brane admit deformations,
which we ... | hep-th math.RT | we classify the lie superalgebra deformations of the killing superalgebras of some mtheory backgrounds we show that the killing superalgebras of the minkowski freundrubin and m5brane backgrounds are rigid whereas the ones for the mwave the kaluzaklein monopole and the m2brane admit deformations which we give explicitly | [['we', 'classify', 'the', 'lie', 'superalgebra', 'deformations', 'of', 'the', 'killing', 'superalgebras', 'of', 'some', 'mtheory', 'backgrounds', 'we', 'show', 'that', 'the', 'killing', 'superalgebras', 'of', 'the', 'minkowski', 'freundrubin', 'and', 'm5brane', 'backgrounds', 'are', 'rigid', 'whereas', 'the', 'ones', ... | [-0.194818003578706, 0.0838069208560789, -0.0008357813423301311, 0.11138939981081306, -0.19677088849563548, -0.15274961601863515, -0.11241920538088108, 0.31471555549255076, -0.1460811874056433, -0.19337809488098037, 0.12285663607465896, -0.29132504903889717, -0.23070195860209616, 0.08668599035987194, -0.143238620713670... |
706.2601 | Change of Optical Properties of Space under Gravitation Field | It is shown that, in the model of a flat 3D space, the time (i.e., the Hubble
or the gravitation constant) plays a role of a spatial property. Gravitation
field of spherical central mass does not lead to a lowering of symmetry of the
space and appearance of anisotropy. In particular, the relations that describe
the c... | physics.optics | it is shown that in the model of a flat 3d space the time ie the hubble or the gravitation constant plays a role of a spatial property gravitation field of spherical central mass does not lead to a lowering of symmetry of the space and appearance of anisotropy in particular the relations that describe the changes in th... | [['it', 'is', 'shown', 'that', 'in', 'the', 'model', 'of', 'a', 'flat', '3d', 'space', 'the', 'time', 'ie', 'the', 'hubble', 'or', 'the', 'gravitation', 'constant', 'plays', 'a', 'role', 'of', 'a', 'spatial', 'property', 'gravitation', 'field', 'of', 'spherical', 'central', 'mass', 'does', 'not', 'lead', 'to', 'a', 'lo... | [-0.1456224868791954, 0.13776143276222033, -0.10653674983738949, 0.044426651434540484, -0.06628003042923021, -0.04996823889779903, -0.04480550184546571, 0.3499176051783642, -0.2345295752664762, -0.30023963842956747, 0.08043898478943101, -0.20069690040933588, -0.148503778959691, 0.16286426523653236, -0.04772303367610134... |
706.2602 | Effects of Hebbian learning on the dynamics and structure of random
networks with inhibitory and excitatory neurons | The aim of the present paper is to study the effects of Hebbian learning in
random recurrent neural networks with biological connectivity, i.e. sparse
connections and separate populations of excitatory and inhibitory neurons. We
furthermore consider that the neuron dynamics may occur at a (shorter) time
scale than sy... | q-bio.NC | the aim of the present paper is to study the effects of hebbian learning in random recurrent neural networks with biological connectivity ie sparse connections and separate populations of excitatory and inhibitory neurons we furthermore consider that the neuron dynamics may occur at a shorter time scale than synaptic p... | [['the', 'aim', 'of', 'the', 'present', 'paper', 'is', 'to', 'study', 'the', 'effects', 'of', 'hebbian', 'learning', 'in', 'random', 'recurrent', 'neural', 'networks', 'with', 'biological', 'connectivity', 'ie', 'sparse', 'connections', 'and', 'separate', 'populations', 'of', 'excitatory', 'and', 'inhibitory', 'neurons... | [-0.11944756664273043, 0.13549599863248518, -0.0663519928651882, 0.042366821556732666, -0.05525994031072164, -0.14946121959935857, 0.07925180643696177, 0.38611781855489913, -0.32738829750227383, -0.23614476718536864, 0.05107463984425591, -0.24546582067761427, -0.27897113098207715, 0.10737764512920805, -0.05372132059990... |
706.2603 | All quantum expectation values as classical statistical mean values | Given a physical quantum system described by a Hilbert H, for any bounded
quantum observable (a bounded self-adjoint operator) T it is possible to define
several ''hidden observable'' functions f:H->R associated to T and for any
quantum mixed state (a density matrix) D it is possible to define several
''hidden mixed ... | quant-ph | given a physical quantum system described by a hilbert h for any bounded quantum observable a bounded selfadjoint operator t it is possible to define several hidden observable functions fhr associated to t and for any quantum mixed state a density matrix d it is possible to define several hidden mixed states probabilit... | [['given', 'a', 'physical', 'quantum', 'system', 'described', 'by', 'a', 'hilbert', 'h', 'for', 'any', 'bounded', 'quantum', 'observable', 'a', 'bounded', 'selfadjoint', 'operator', 't', 'it', 'is', 'possible', 'to', 'define', 'several', 'hidden', 'observable', 'functions', 'fhr', 'associated', 'to', 't', 'and', 'for',... | [-0.13929844294942104, 0.18517989033630283, -0.11347044238101432, 0.10797897286339672, -0.06395951472222805, -0.19894496939320228, 0.05247336240960193, 0.3078714934279128, -0.3201075842117633, -0.228521170527997, 0.0717969577157833, -0.2464447712622546, -0.11235450731940788, 0.14751075921663184, -0.05327817773225137, 0... |
706.2604 | Electrically and magnetically induced optical rotation in Pb5Ge3O11:Cr
crystals at the phase transition. 2. Faraday effect in pure and Cr-doped lead
germanate in the presence of electric field and spontaneous polarization | This work presents the results for the Faraday rotation in pure and Cr-doped
lead germanate crystals studied in the course of proper ferroelectric phase
transition. We show that the increment of the Faraday rotation appearing at the
phase transition is caused by a combined magneto-electrooptic effect induced by
spont... | cond-mat.mtrl-sci | this work presents the results for the faraday rotation in pure and crdoped lead germanate crystals studied in the course of proper ferroelectric phase transition we show that the increment of the faraday rotation appearing at the phase transition is caused by a combined magnetoelectrooptic effect induced by spontaneou... | [['this', 'work', 'presents', 'the', 'results', 'for', 'the', 'faraday', 'rotation', 'in', 'pure', 'and', 'crdoped', 'lead', 'germanate', 'crystals', 'studied', 'in', 'the', 'course', 'of', 'proper', 'ferroelectric', 'phase', 'transition', 'we', 'show', 'that', 'the', 'increment', 'of', 'the', 'faraday', 'rotation', 'a... | [-0.12583011246722522, 0.21580301283540415, -0.06778056811706364, -0.017197769811624495, -0.06879928182291833, -0.05175380328009966, 0.05512312888698299, 0.38474947093879874, -0.28002780162481755, -0.28328226303941084, 0.06847761940104957, -0.23898186171545258, -0.15597278268748446, 0.17289260193658404, -0.036268040195... |
706.2605 | On the genealogy on conditioned stable L\'evy forest | We give a realization of the stable L\'evy forest of a given size conditioned
by its mass from the path of the unconditioned forest. Then, we prove an
invariance principle for this conditioned forest by considering $k$ independent
Galton-Watson trees whose offspring distribution is in the domain of attraction
of any ... | math.PR | we give a realization of the stable levy forest of a given size conditioned by its mass from the path of the unconditioned forest then we prove an invariance principle for this conditioned forest by considering k independent galtonwatson trees whose offspring distribution is in the domain of attraction of any stable la... | [['we', 'give', 'a', 'realization', 'of', 'the', 'stable', 'levy', 'forest', 'of', 'a', 'given', 'size', 'conditioned', 'by', 'its', 'mass', 'from', 'the', 'path', 'of', 'the', 'unconditioned', 'forest', 'then', 'we', 'prove', 'an', 'invariance', 'principle', 'for', 'this', 'conditioned', 'forest', 'by', 'considering',... | [-0.0745716537348926, 0.21311949105035768, -0.10072134703763627, 0.034893568519074894, -0.03416943279028471, -0.136084658837977, 0.1398858092735671, 0.3980784994367111, -0.305777436795844, -0.18769107744862726, 0.10775607758010405, -0.2769731974985916, -0.0971876146525444, 0.14042643490081122, -0.09098757146411376, 0.0... |
706.2606 | Randomness Extraction via Delta-Biased Masking in the Presence of a
Quantum Attacker | Randomness extraction is of fundamental importance for information-theoretic
cryptography. It allows to transform a raw key about which an attacker has some
limited knowledge into a fully secure random key, on which the attacker has
essentially no information. Up to date, only very few randomness-extraction
technique... | quant-ph cs.CR | randomness extraction is of fundamental importance for informationtheoretic cryptography it allows to transform a raw key about which an attacker has some limited knowledge into a fully secure random key on which the attacker has essentially no information up to date only very few randomnessextraction techniques are kn... | [['randomness', 'extraction', 'is', 'of', 'fundamental', 'importance', 'for', 'informationtheoretic', 'cryptography', 'it', 'allows', 'to', 'transform', 'a', 'raw', 'key', 'about', 'which', 'an', 'attacker', 'has', 'some', 'limited', 'knowledge', 'into', 'a', 'fully', 'secure', 'random', 'key', 'on', 'which', 'the', 'a... | [-0.09736703488533004, 0.03491549280896252, -0.12299679742637472, 0.10348134000402051, -0.09287073875116146, -0.23880428751571806, 0.0894620645377159, 0.3292130402873316, -0.30676082931229937, -0.2956588106180043, 0.13104668238603884, -0.25734305510225375, -0.14508226303265384, 0.237085366276423, -0.18574462596853797, ... |
706.2607 | Kinematic effect in gravitational lensing by clusters of galaxies | Gravitational lensing provides an efficient tool for the investigation of
matter structures, independent of the dynamical or hydrostatic equilibrium
properties of the deflecting system. However, it depends on the kinematic
status. In fact, either a translational motion or a coherent rotation of the
mass distribution ... | astro-ph | gravitational lensing provides an efficient tool for the investigation of matter structures independent of the dynamical or hydrostatic equilibrium properties of the deflecting system however it depends on the kinematic status in fact either a translational motion or a coherent rotation of the mass distribution can aff... | [['gravitational', 'lensing', 'provides', 'an', 'efficient', 'tool', 'for', 'the', 'investigation', 'of', 'matter', 'structures', 'independent', 'of', 'the', 'dynamical', 'or', 'hydrostatic', 'equilibrium', 'properties', 'of', 'the', 'deflecting', 'system', 'however', 'it', 'depends', 'on', 'the', 'kinematic', 'status'... | [-0.1545230468242701, 0.1291496334314089, -0.10180074498380431, 0.09464858891386717, -0.1031467381855874, -0.034481563080106664, 0.0032889641616404342, 0.32961782404894463, -0.24725158772827907, -0.3356028741270718, 0.0694934150580602, -0.268774875615719, -0.027701605502660855, 0.2224321258744519, -0.010714197034488598... |
706.2608 | A refinement of multi-dimensional persistence | We study the multi-dimensional persistence of Carlsson and Zomorodian and
obtain a finer classification based upon the higher tor-modules of a
persistence module. We propose a variety structure on the set of isomorphism
classes of these modules, and present several examples. We also provide a
geometric interpretation... | math.AT | we study the multidimensional persistence of carlsson and zomorodian and obtain a finer classification based upon the higher tormodules of a persistence module we propose a variety structure on the set of isomorphism classes of these modules and present several examples we also provide a geometric interpretation for th... | [['we', 'study', 'the', 'multidimensional', 'persistence', 'of', 'carlsson', 'and', 'zomorodian', 'and', 'obtain', 'a', 'finer', 'classification', 'based', 'upon', 'the', 'higher', 'tormodules', 'of', 'a', 'persistence', 'module', 'we', 'propose', 'a', 'variety', 'structure', 'on', 'the', 'set', 'of', 'isomorphism', 'c... | [-0.15527571329911208, 0.005771309342074754, -0.09999876014952516, 0.11855956141290994, -0.06032697361861837, -0.0856340513885792, 0.019150173592638094, 0.3644588191447587, -0.3165854385186886, -0.2554082425375437, 0.13781102436819467, -0.15823200219792538, -0.20467260479927063, 0.20575726289173651, -0.1240779248804881... |
706.2609 | A Global Fit to Scattering Data with NLL BFKL Resummations | We perform a global parton fit to DIS and related data, including
next-to-leading logarithmic (NLL) BFKL resummations in both the massless and
massive sectors. The resummed fit improves over a standard next-to-leading
order (NLO) DGLAP fit, with a positive definite gluon at the input scale as
opposed to the negative ... | hep-ph | we perform a global parton fit to dis and related data including nexttoleading logarithmic nll bfkl resummations in both the massless and massive sectors the resummed fit improves over a standard nexttoleading order nlo dglap fit with a positive definite gluon at the input scale as opposed to the negative gluon seen at... | [['we', 'perform', 'a', 'global', 'parton', 'fit', 'to', 'dis', 'and', 'related', 'data', 'including', 'nexttoleading', 'logarithmic', 'nll', 'bfkl', 'resummations', 'in', 'both', 'the', 'massless', 'and', 'massive', 'sectors', 'the', 'resummed', 'fit', 'improves', 'over', 'a', 'standard', 'nexttoleading', 'order', 'nl... | [-0.03212608182167804, 0.0893118377584456, -0.14958302479300817, 0.20162258575146552, -0.038534816330700945, -0.07839624195846474, -0.02343671660260456, 0.3570578743449666, -0.16993780360049146, -0.24072714763778177, -0.017423244423381137, -0.36212041855535726, 0.04888647541255606, 0.06861479782541706, 0.08105121007445... |
706.261 | Optical properties of SiC nanotubes: A systematic $\textit{ab initio}$
study | The band structure and optical dielectric function $\epsilon$ of
single-walled zigzag
[(3,0),(4,0),(5,0),(6,0),(8,0),(9,0),(12,0),(16,0),(20,0),(24,0)], armchair
[(3,3),(4,4),(5,5),(8,8),(12,12),(15,15)], and chiral
[(4,2),(6,2),(8,4),(10,4)] SiC-NTs as well as the single honeycomb SiC sheet
have been calculated with... | cond-mat.mtrl-sci | the band structure and optical dielectric function epsilon of singlewalled zigzag 304050608090120160200240 armchair 3344558812121515 and chiral 426284104 sicnts as well as the single honeycomb sic sheet have been calculated within dft with the lda it is found that all the sic nanotubes are semiconductors except the ult... | [['the', 'band', 'structure', 'and', 'optical', 'dielectric', 'function', 'epsilon', 'of', 'singlewalled', 'zigzag', '304050608090120160200240', 'armchair', '3344558812121515', 'and', 'chiral', '426284104', 'sicnts', 'as', 'well', 'as', 'the', 'single', 'honeycomb', 'sic', 'sheet', 'have', 'been', 'calculated', 'within... | [-0.13171197081772754, 0.15770773714287387, 0.035987019972302595, -0.00480614434569501, 0.03138063515227539, -0.14663027081763946, 0.05489868302650463, 0.4484627415640996, -0.23520190442392888, -0.34557325966474867, 0.03592002778235698, -0.3297454999186672, -0.040040242269885944, 0.15027755856728897, 0.0575455735585329... |
706.2611 | Rosenbluth Nonlinearity from Two-Photon Exchange | We calculate, using a generalized parton distribution based formalism, the
nonlinearity of the Rosenbluth plots that arise from hard two-photon exchange
corrections that are not included in the classic calculations of the radiative
corrections to electron-proton elastic scattering.
| hep-ph | we calculate using a generalized parton distribution based formalism the nonlinearity of the rosenbluth plots that arise from hard twophoton exchange corrections that are not included in the classic calculations of the radiative corrections to electronproton elastic scattering | [['we', 'calculate', 'using', 'a', 'generalized', 'parton', 'distribution', 'based', 'formalism', 'the', 'nonlinearity', 'of', 'the', 'rosenbluth', 'plots', 'that', 'arise', 'from', 'hard', 'twophoton', 'exchange', 'corrections', 'that', 'are', 'not', 'included', 'in', 'the', 'classic', 'calculations', 'of', 'the', 'ra... | [-0.026893676503708486, 0.15337708673292869, -0.151283194654082, 0.20886433395361037, -0.04327825449505135, -0.07796379373604923, 0.017861922565651566, 0.35923891436112554, -0.24841458727850727, -0.21656701743210616, -0.06606464799015636, -0.36327565914804216, -0.10885506005663621, 0.17660628800206868, 0.10730420165744... |
706.2612 | Fermi Edge Singularities in the Mesoscopic Regime: II. Photo-absorption
Spectra | We study Fermi edge singularities in photo-absorption spectra of generic
mesoscopic systems such as quantum dots or nanoparticles. We predict deviations
from macroscopic-metallic behavior and propose experimental setups for the
observation of these effects. The theory is based on the model of a localized,
or rank one... | cond-mat.mes-hall | we study fermi edge singularities in photoabsorption spectra of generic mesoscopic systems such as quantum dots or nanoparticles we predict deviations from macroscopicmetallic behavior and propose experimental setups for the observation of these effects the theory is based on the model of a localized or rank one pertur... | [['we', 'study', 'fermi', 'edge', 'singularities', 'in', 'photoabsorption', 'spectra', 'of', 'generic', 'mesoscopic', 'systems', 'such', 'as', 'quantum', 'dots', 'or', 'nanoparticles', 'we', 'predict', 'deviations', 'from', 'macroscopicmetallic', 'behavior', 'and', 'propose', 'experimental', 'setups', 'for', 'the', 'ob... | [-0.10985513707207327, 0.16755650343479886, -0.09136298091940676, 0.07315514362608731, 0.02334819317064425, -0.1250367897527316, 0.058799739176248304, 0.32132991535966343, -0.2623545617201142, -0.27913145984145754, 0.04359534667816626, -0.3378602208973415, -0.13225773471124658, 0.17147698018941557, 0.020041009817932602... |
706.2613 | Probing micro-arcsec astrometry with NACO | Relative astrometric measurements with a precision far better than 1 mas
(milli-arcsec) are commonly regarded as the domain of interferometry.
Pioneering work by Pravdo & Shaklan (1996), made in the optical, reached a
precision of 150 micro-arcsec in direct imaging but is ultimately limited by
atmospheric turbulence ... | astro-ph | relative astrometric measurements with a precision far better than 1 mas milliarcsec are commonly regarded as the domain of interferometry pioneering work by pravdo shaklan 1996 made in the optical reached a precision of 150 microarcsec in direct imaging but is ultimately limited by atmospheric turbulence and different... | [['relative', 'astrometric', 'measurements', 'with', 'a', 'precision', 'far', 'better', 'than', '1', 'mas', 'milliarcsec', 'are', 'commonly', 'regarded', 'as', 'the', 'domain', 'of', 'interferometry', 'pioneering', 'work', 'by', 'pravdo', 'shaklan', '1996', 'made', 'in', 'the', 'optical', 'reached', 'a', 'precision', '... | [-0.06615344356157679, 0.1446857456171305, -0.03923152499358918, 0.00549435822415303, -0.11239924484942124, -0.12733151187254765, 0.09183812711090154, 0.3826198492993097, -0.20366925758511958, -0.4343587807417832, 0.13515260282161523, -0.26804200902230063, -0.05657949078862448, 0.23132422333583236, -0.12193401476757632... |
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