id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
710.2053 | Fokker-Planck Equation for Fractional Systems | The normalization condition, average values and reduced distribution
functions can be generalized by fractional integrals. The interpretation of the
fractional analog of phase space as a space with noninteger dimension is
discussed. A fractional (power) system is described by the fractional powers of
coordinates and ... | cond-mat.stat-mech | the normalization condition average values and reduced distribution functions can be generalized by fractional integrals the interpretation of the fractional analog of phase space as a space with noninteger dimension is discussed a fractional power system is described by the fractional powers of coordinates and momenta... | [['the', 'normalization', 'condition', 'average', 'values', 'and', 'reduced', 'distribution', 'functions', 'can', 'be', 'generalized', 'by', 'fractional', 'integrals', 'the', 'interpretation', 'of', 'the', 'fractional', 'analog', 'of', 'phase', 'space', 'as', 'a', 'space', 'with', 'noninteger', 'dimension', 'is', 'disc... | [-0.16257838705288513, 0.13884051023688654, -0.09339033040617194, 0.08770764483709909, -0.06472702893162412, -0.097841733135283, -0.029779406652475398, 0.2463552098072666, -0.3006393903023785, -0.2758276002658975, 0.1298217183752318, -0.26737202762714807, -0.14480025158818102, 0.2248682448851122, -0.04239376379354369, ... |
710.2054 | Non-gapped Fermi surfaces, quasiparticles and the anomalous temperature
dependence of the near-$E_F$ electronic states in the CMR oxide
La$_{2-2x}$Sr$_{1+2x}$Mn$_2$O$_7$ with $x=0.36$ | After years of research into colossal magnetoresistant (CMR) manganites using
bulk techniques, there has been a recent upsurge in experiments directly
probing the electronic states at or near the surface of the bilayer CMR
materials La$_{2-2x}$Sr$_{1+2x}$Mn$_2$O$_7$ using angle-resolved photoemission
or scanning prob... | cond-mat.str-el | after years of research into colossal magnetoresistant cmr manganites using bulk techniques there has been a recent upsurge in experiments directly probing the electronic states at or near the surface of the bilayer cmr materials la_22xsr_12xmn_2o_7 using angleresolved photoemission or scanning probe microscopy here we... | [['after', 'years', 'of', 'research', 'into', 'colossal', 'magnetoresistant', 'cmr', 'manganites', 'using', 'bulk', 'techniques', 'there', 'has', 'been', 'a', 'recent', 'upsurge', 'in', 'experiments', 'directly', 'probing', 'the', 'electronic', 'states', 'at', 'or', 'near', 'the', 'surface', 'of', 'the', 'bilayer', 'cm... | [-0.13453888725796406, 0.1947208640440994, -0.08712209701783709, 0.0010549804032012656, -0.01657959377869022, -0.11966583984750477, 0.12189068402845546, 0.38331245034830747, -0.2732712326335956, -0.29144574040649357, 0.030064770497079774, -0.3424942375334737, -0.11003200846128064, 0.20089376199086054, -0.01402400924240... |
710.2055 | Anatomy of nuclear matrix elements for neutrinoless double-beta decay | We show that, within the Quasiparticle Random Phase Approximation (QRPA) and
the renormalized QRPA (RQRPA) based on the Bonn CD nucleon-nucleon interaction,
the competition between the pairing and the neutron-proton particle-particle
and particle-hole interactions causes contributions to the neutrinoless
double-beta ... | nucl-th | we show that within the quasiparticle random phase approximation qrpa and the renormalized qrpa rqrpa based on the bonn cd nucleonnucleon interaction the competition between the pairing and the neutronproton particleparticle and particlehole interactions causes contributions to the neutrinoless doublebeta decay matrix ... | [['we', 'show', 'that', 'within', 'the', 'quasiparticle', 'random', 'phase', 'approximation', 'qrpa', 'and', 'the', 'renormalized', 'qrpa', 'rqrpa', 'based', 'on', 'the', 'bonn', 'cd', 'nucleonnucleon', 'interaction', 'the', 'competition', 'between', 'the', 'pairing', 'and', 'the', 'neutronproton', 'particleparticle', ... | [-0.07407834726473084, 0.21058575741092986, -0.10549100285485717, 0.1578989869922225, 0.0009916890170037125, -0.14044403967272956, 0.04719738448087204, 0.32824466174618766, -0.23182636642983803, -0.23740539551363327, -0.062039042360993335, -0.38095620544239256, -0.11599290574425443, 0.10251471269051156, 0.1070891669927... |
710.2056 | Rotating Radio Transients: X-ray observations | Rotating Radio Transients (RRATs) are a new class of neutron stars discovered
through the emission of radio bursts. Eleven sources are known up to now, but
population studies predict these objects to be more numerous than the normal
radio pulsar population. Multiwavelength observations of these peculiar objects
are i... | astro-ph | rotating radio transients rrats are a new class of neutron stars discovered through the emission of radio bursts eleven sources are known up to now but population studies predict these objects to be more numerous than the normal radio pulsar population multiwavelength observations of these peculiar objects are in progr... | [['rotating', 'radio', 'transients', 'rrats', 'are', 'a', 'new', 'class', 'of', 'neutron', 'stars', 'discovered', 'through', 'the', 'emission', 'of', 'radio', 'bursts', 'eleven', 'sources', 'are', 'known', 'up', 'to', 'now', 'but', 'population', 'studies', 'predict', 'these', 'objects', 'to', 'be', 'more', 'numerous', ... | [-0.059832146752424625, 0.1239093019341288, -0.039020271056374026, 0.11531502497779332, -0.1681071972178126, -0.050560327791820535, 0.0755144096487625, 0.4596696093847806, -0.18465371497652747, -0.3530673165699806, 0.12432684733754616, -0.3024106881877577, -0.07444935702634128, 0.27305495514619077, -0.03737278594847091... |
710.2057 | Optical saturation driven by exciton confinement in molecular-chains: a
TDDFT study | We have identified excitonic confinement in one-dimensional molecular chains
(i.e. polyacetylene and H$_2$) as the main driving force for the saturation of
the chain polarizability as a function of the number of molecular units. This
conclusion is based on first principles time--dependent density functional
theory ca... | cond-mat.mtrl-sci | we have identified excitonic confinement in onedimensional molecular chains ie polyacetylene and h_2 as the main driving force for the saturation of the chain polarizability as a function of the number of molecular units this conclusion is based on first principles timedependent density functional theory calculations p... | [['we', 'have', 'identified', 'excitonic', 'confinement', 'in', 'onedimensional', 'molecular', 'chains', 'ie', 'polyacetylene', 'and', 'h_2', 'as', 'the', 'main', 'driving', 'force', 'for', 'the', 'saturation', 'of', 'the', 'chain', 'polarizability', 'as', 'a', 'function', 'of', 'the', 'number', 'of', 'molecular', 'uni... | [-0.10274494387037218, 0.0727627775061895, -0.08839886162119608, 0.1058437843566935, -0.0052953138171384735, -0.09902326198061928, 0.03159801182846422, 0.3634555733200007, -0.26005633695361513, -0.2977007583055335, 0.030157772622866712, -0.2532696701431026, -0.1426677085304012, 0.14460396085511698, 0.019360585896113964... |
710.2058 | Non-universal gaugino masses and implications on the dark matter and
Higgs searches | Non-universal boundary conditions in grand unified theories can lead to
non-universal gaugino masses at the unification scale. In R-parity preserving
theories the lightest supersymmetric particle is a natural candidate for the
dark matter. We have studied the composition of the lightest neutralino in
non-universal ga... | hep-ph | nonuniversal boundary conditions in grand unified theories can lead to nonuniversal gaugino masses at the unification scale in rparity preserving theories the lightest supersymmetric particle is a natural candidate for the dark matter we have studied the composition of the lightest neutralino in nonuniversal gaugino ma... | [['nonuniversal', 'boundary', 'conditions', 'in', 'grand', 'unified', 'theories', 'can', 'lead', 'to', 'nonuniversal', 'gaugino', 'masses', 'at', 'the', 'unification', 'scale', 'in', 'rparity', 'preserving', 'theories', 'the', 'lightest', 'supersymmetric', 'particle', 'is', 'a', 'natural', 'candidate', 'for', 'the', 'd... | [-0.09832180220247158, 0.30949645036972073, -0.08295196108080728, 0.26529409367490103, -0.09730777524648902, -0.16741178913771193, -0.02661541085419814, 0.29854508139465424, -0.17350408886471447, -0.3515321616575403, -0.005768171808120074, -0.24083538213305455, 0.03764210191537749, 0.08202286272854456, 0.01964821629852... |
710.2059 | Covariance, Dynamics and Symmetries, and Hadron Form Factors | We summarise applications of Dyson-Schwinger equations to the theory and
phenomenology of hadrons. Some exact results for pseudoscalar mesons are
highlighted with details relating to the U_A(1) problem. We describe inferences
from the gap equation relating to the radius of convergence for expansions of
observables in... | nucl-th hep-lat hep-ph nucl-ex | we summarise applications of dysonschwinger equations to the theory and phenomenology of hadrons some exact results for pseudoscalar mesons are highlighted with details relating to the u_a1 problem we describe inferences from the gap equation relating to the radius of convergence for expansions of observables in the cu... | [['we', 'summarise', 'applications', 'of', 'dysonschwinger', 'equations', 'to', 'the', 'theory', 'and', 'phenomenology', 'of', 'hadrons', 'some', 'exact', 'results', 'for', 'pseudoscalar', 'mesons', 'are', 'highlighted', 'with', 'details', 'relating', 'to', 'the', 'u_a1', 'problem', 'we', 'describe', 'inferences', 'fro... | [-0.1034665606978039, 0.164043829026632, -0.09942451829711596, 0.1248720903073748, -0.10761070514718692, -0.02873790288809687, 0.06900229979616901, 0.3076460756113132, -0.16750898975878953, -0.25517229075854025, 0.010404307952461143, -0.3408387390524149, -0.08495979696512222, 0.1529673336694638, 0.0383902911717693, 0.0... |
710.206 | Polariton laser using single micropillar GaAs-GaAlAs semiconductor
cavities | Polariton lasing is demonstrated on the zero dimensional states of single
GaAs/GaAlAs micropillar cavities. Under non resonant excitation, the measured
polariton ground state occupancy is found to be as large as $10^{4}$. Changing
the spatial excitation conditions, competition between several polariton lasing
modes i... | cond-mat.mtrl-sci | polariton lasing is demonstrated on the zero dimensional states of single gaasgaalas micropillar cavities under non resonant excitation the measured polariton ground state occupancy is found to be as large as 104 changing the spatial excitation conditions competition between several polariton lasing modes is observed r... | [['polariton', 'lasing', 'is', 'demonstrated', 'on', 'the', 'zero', 'dimensional', 'states', 'of', 'single', 'gaasgaalas', 'micropillar', 'cavities', 'under', 'non', 'resonant', 'excitation', 'the', 'measured', 'polariton', 'ground', 'state', 'occupancy', 'is', 'found', 'to', 'be', 'as', 'large', 'as', '104', 'changing... | [-0.14445566900872758, 0.29365620355986594, -0.03980076524562069, 0.03642931511359555, 0.01625160071000989, -0.16928558010341865, 0.06283647121329393, 0.4201669840541269, -0.16374893239034075, -0.24946343377232552, -0.03381041440713618, -0.29875625510300907, -0.011727579882634537, 0.17903751412273516, 0.060520515728941... |
710.2061 | Nonlinear Dynamical Equation for Irreversible, Steepest-Entropy-Ascent
Relaxation to Stable Equilibrium | We discuss the structure and main features of the nonlinear evolution
equation proposed by this author as the fundamental dynamical law within the
framework of Quantum Thermodynamics. The nonlinear equation generates a
dynamical group providing a unique deterministic description of irreversible,
conservative relaxati... | quant-ph | we discuss the structure and main features of the nonlinear evolution equation proposed by this author as the fundamental dynamical law within the framework of quantum thermodynamics the nonlinear equation generates a dynamical group providing a unique deterministic description of irreversible conservative relaxation t... | [['we', 'discuss', 'the', 'structure', 'and', 'main', 'features', 'of', 'the', 'nonlinear', 'evolution', 'equation', 'proposed', 'by', 'this', 'author', 'as', 'the', 'fundamental', 'dynamical', 'law', 'within', 'the', 'framework', 'of', 'quantum', 'thermodynamics', 'the', 'nonlinear', 'equation', 'generates', 'a', 'dyn... | [-0.08120690091957593, 0.07462719461711292, -0.1608804117316719, 0.08022316140837078, -0.08565951688003472, -0.1397427545452956, 0.06490517858368218, 0.2529253943860319, -0.3361101001871496, -0.26998660288518295, 0.07993425005075881, -0.24780505782374265, -0.17478011743250219, 0.15727436510761353, -0.034419895818432036... |
710.2062 | Indirect Searches For Dark Matter: Signals, Hints and Otherwise | For the SUSY 2007 conference, I was asked to review the topic of indirect
searches for dark matter. As part of that talk, I summarized several
observations which have been interpreted as the product of dark matter
annihilations. In my contribution to the proceedings, I have decided to focus
on this aspect of my talk.... | hep-ph astro-ph | for the susy 2007 conference i was asked to review the topic of indirect searches for dark matter as part of that talk i summarized several observations which have been interpreted as the product of dark matter annihilations in my contribution to the proceedings i have decided to focus on this aspect of my talk in part... | [['for', 'the', 'susy', '2007', 'conference', 'i', 'was', 'asked', 'to', 'review', 'the', 'topic', 'of', 'indirect', 'searches', 'for', 'dark', 'matter', 'as', 'part', 'of', 'that', 'talk', 'i', 'summarized', 'several', 'observations', 'which', 'have', 'been', 'interpreted', 'as', 'the', 'product', 'of', 'dark', 'matte... | [-0.013447505757212638, 0.14606369979213923, -0.06662986849434674, 0.12558299186988733, -0.13879604315385222, -0.0592172502912581, -0.004647394884377718, 0.35462296431243884, -0.2025632517784834, -0.3860781975556165, 0.01905482871225104, -0.3532181068789214, 0.013389729000627994, 0.19426438551570754, -0.012220707419328... |
710.2063 | Distance matrices and isometric embeddings | We review the relations between distance matrices and isometric embeddings
and give simple proofs that distance matrices defined on euclidean and
spherical spaces have all eigenvalues except one non-negative. Several
generalizations are discussed.
| nlin.CD | we review the relations between distance matrices and isometric embeddings and give simple proofs that distance matrices defined on euclidean and spherical spaces have all eigenvalues except one nonnegative several generalizations are discussed | [['we', 'review', 'the', 'relations', 'between', 'distance', 'matrices', 'and', 'isometric', 'embeddings', 'and', 'give', 'simple', 'proofs', 'that', 'distance', 'matrices', 'defined', 'on', 'euclidean', 'and', 'spherical', 'spaces', 'have', 'all', 'eigenvalues', 'except', 'one', 'nonnegative', 'several', 'generalizati... | [-0.10899324234483312, 0.10295140317104982, -0.008638908719700394, 0.17768243042695703, -0.08356755332682621, -0.18599573339363842, -0.053204871149677216, 0.4454089936546304, -0.24197952028815495, -0.2007935569536957, 0.15096851244963932, -0.36685983043615567, -0.1981983876815348, 0.18910036399734742, -0.07778799284256... |
710.2064 | Reduction of structure for torsors over semilocal rings | Let G be a reductive affine group scheme defined over a semilocal ring k.
Assume that either G is semisimple or k is normal and noetherian. We show that
G has a finite k-subgroup S such that the natural map H^1(R, S) --> H^1(R, G)
is surjective for every semilocal ring R containing k. In other words,
G-torsors over S... | math.AG math.GR | let g be a reductive affine group scheme defined over a semilocal ring k assume that either g is semisimple or k is normal and noetherian we show that g has a finite ksubgroup s such that the natural map h1r s h1r g is surjective for every semilocal ring r containing k in other words gtorsors over specr admit reduction... | [['let', 'g', 'be', 'a', 'reductive', 'affine', 'group', 'scheme', 'defined', 'over', 'a', 'semilocal', 'ring', 'k', 'assume', 'that', 'either', 'g', 'is', 'semisimple', 'or', 'k', 'is', 'normal', 'and', 'noetherian', 'we', 'show', 'that', 'g', 'has', 'a', 'finite', 'ksubgroup', 's', 'such', 'that', 'the', 'natural', '... | [-0.23769351696022428, 0.04700939263073871, -0.1117150713582165, 0.01367931393100522, -0.1020274092998499, -0.2055755059270618, -0.024512392385468748, 0.41150319093408494, -0.35901179349479767, -0.18246491490146863, 0.07420496079587163, -0.2445578596053215, -0.10677118515774894, 0.2146099584521905, -0.101722283478683, ... |
710.2065 | Commensurate magnetic structures ofRMn2O5 (R=Y, Ho, Bi) determined by
Single-crystal Neutron Diffraction | Precise magnetic structures of RMn2O5, with R= Y, Ho, Bi in the
commensurate/ferroelectric regime, have been determined by single-crystal
neutron diffraction. For each system, the integrated intensities of a large
number of independent magnetic Bragg reflections have been measured, allowing
unconstrained least-square... | cond-mat.mtrl-sci | precise magnetic structures of rmn2o5 with r y ho bi in the commensurateferroelectric regime have been determined by singlecrystal neutron diffraction for each system the integrated intensities of a large number of independent magnetic bragg reflections have been measured allowing unconstrained leastsquares refinement ... | [['precise', 'magnetic', 'structures', 'of', 'rmn2o5', 'with', 'r', 'y', 'ho', 'bi', 'in', 'the', 'commensurateferroelectric', 'regime', 'have', 'been', 'determined', 'by', 'singlecrystal', 'neutron', 'diffraction', 'for', 'each', 'system', 'the', 'integrated', 'intensities', 'of', 'a', 'large', 'number', 'of', 'indepe... | [-0.22336878226449092, 0.20794837326277046, -0.0016522697561110059, 0.0046675810202335315, -0.06010274810522484, -0.12140474590472877, 0.06002290412938843, 0.43004730297873417, -0.269164633040006, -0.2867180710658431, 0.02968458173330873, -0.30053742408752443, -0.06539760681490103, 0.1404864786705002, 0.097964783000449... |
710.2066 | A Unified Spiral Chain Coloring Algorithm for Planar Graphs | In this paper we have given a unified graph coloring algorithm for planar
graphs. The problems that have been considered in this context respectively,
are vertex, edge, total and entire colorings of the planar graphs. The main
tool in the coloring algorithm is the use of spiral chain which has been used
in the non-co... | math.CO | in this paper we have given a unified graph coloring algorithm for planar graphs the problems that have been considered in this context respectively are vertex edge total and entire colorings of the planar graphs the main tool in the coloring algorithm is the use of spiral chain which has been used in the noncomputer p... | [['in', 'this', 'paper', 'we', 'have', 'given', 'a', 'unified', 'graph', 'coloring', 'algorithm', 'for', 'planar', 'graphs', 'the', 'problems', 'that', 'have', 'been', 'considered', 'in', 'this', 'context', 'respectively', 'are', 'vertex', 'edge', 'total', 'and', 'entire', 'colorings', 'of', 'the', 'planar', 'graphs', ... | [-0.166364223059107, 0.053698099734342225, -0.09887452874768018, 0.022493515764335555, -0.11273708066644048, -0.1117534881110507, 0.023628230181180997, 0.39400136461977425, -0.230108904613722, -0.3400192156533253, 0.10821575364070399, -0.27460851337479636, -0.16734663372826294, 0.1350234473666959, -0.12947681453767834,... |
710.2067 | SuperIso: A program for calculating the isospin asymmetry of B -> K*
gamma in the MSSM | We present a program for calculating the isospin symmetry breaking of the B
-> K* gamma decay in the MSSM with minimal flavor violation. This program
calculates the NLO supersymmetric contributions to the isospin asymmetry, using
the effective Hamiltonian approach and within the QCD factorization method. We
show that... | hep-ph | we present a program for calculating the isospin symmetry breaking of the b k gamma decay in the mssm with minimal flavor violation this program calculates the nlo supersymmetric contributions to the isospin asymmetry using the effective hamiltonian approach and within the qcd factorization method we show that isospin ... | [['we', 'present', 'a', 'program', 'for', 'calculating', 'the', 'isospin', 'symmetry', 'breaking', 'of', 'the', 'b', 'k', 'gamma', 'decay', 'in', 'the', 'mssm', 'with', 'minimal', 'flavor', 'violation', 'this', 'program', 'calculates', 'the', 'nlo', 'supersymmetric', 'contributions', 'to', 'the', 'isospin', 'asymmetry'... | [-0.1227686005842266, 0.18706943518874874, -0.09995002595214061, 0.1364487536596583, -0.07767380845272936, -0.15533372053472572, 0.09286250929763339, 0.3225809662737491, -0.217181671321033, -0.25976707970342006, 0.009453934742171452, -0.25260789744578394, -0.02522924259103027, 0.041222369747169044, 0.06917767989426761,... |
710.2068 | Analytic continuation of the critical line in 2-color QCD at nonzero
temperature and density | We determine the pseudo-critical line in the temperature - chemical potential
plane of 2-color QCD by direct Monte Carlo simulations and by analytic
continuation from imaginary chemical potential.
| hep-lat | we determine the pseudocritical line in the temperature chemical potential plane of 2color qcd by direct monte carlo simulations and by analytic continuation from imaginary chemical potential | [['we', 'determine', 'the', 'pseudocritical', 'line', 'in', 'the', 'temperature', 'chemical', 'potential', 'plane', 'of', '2color', 'qcd', 'by', 'direct', 'monte', 'carlo', 'simulations', 'and', 'by', 'analytic', 'continuation', 'from', 'imaginary', 'chemical', 'potential']] | [-0.10828067403700617, 0.1039297855976555, -0.12087496804694335, 0.029494850861805456, -0.0584269541281241, -0.027402450020114582, 0.20033393717474407, 0.4216041330386091, -0.19513842908458578, -0.25195275702410275, 0.028024635721791397, -0.2989404906553251, -0.09889367191741864, 0.16423270768589443, 0.2169086090806457... |
710.2069 | The Quest for the Ideal Scintillator for Hybrid Phototubes | In this paper we present the results of extensive studies of scintillators
for hybrid phototubes with luminescent screens. The results of the developments
of such phototubes with a variety of scintillators are presented. New
scintillator materials for such kind of application are discussed. The
requirements for scint... | physics.optics astro-ph nucl-ex physics.ins-det | in this paper we present the results of extensive studies of scintillators for hybrid phototubes with luminescent screens the results of the developments of such phototubes with a variety of scintillators are presented new scintillator materials for such kind of application are discussed the requirements for scintillat... | [['in', 'this', 'paper', 'we', 'present', 'the', 'results', 'of', 'extensive', 'studies', 'of', 'scintillators', 'for', 'hybrid', 'phototubes', 'with', 'luminescent', 'screens', 'the', 'results', 'of', 'the', 'developments', 'of', 'such', 'phototubes', 'with', 'a', 'variety', 'of', 'scintillators', 'are', 'presented', ... | [-0.059625461236452806, 0.13963037613150361, -0.02249073860078276, 0.011218767840711569, -0.04570448417942245, -0.14527252549305558, -0.053596113005640926, 0.4670656689188697, -0.20502502906632114, -0.3000771590061002, 0.16467979311181064, -0.33356515113748125, -0.15345502581882786, 0.30431238382861214, -0.078971620764... |
710.207 | The sh-Lie algebra perturbation Lemma | Let R be a commutative ring which contains the rationals as a subring and let
g be a chain complex. Suppose given an sh-Lie algebra structure on g, that is,
a coalgebra perturbation of the coalgebra differential on the cofree
coaugmented differential graded cocommutative coalgebra T' on the suspension of
g and write ... | math.AG math.AC | let r be a commutative ring which contains the rationals as a subring and let g be a chain complex suppose given an shlie algebra structure on g that is a coalgebra perturbation of the coalgebra differential on the cofree coaugmented differential graded cocommutative coalgebra t on the suspension of g and write the per... | [['let', 'r', 'be', 'a', 'commutative', 'ring', 'which', 'contains', 'the', 'rationals', 'as', 'a', 'subring', 'and', 'let', 'g', 'be', 'a', 'chain', 'complex', 'suppose', 'given', 'an', 'shlie', 'algebra', 'structure', 'on', 'g', 'that', 'is', 'a', 'coalgebra', 'perturbation', 'of', 'the', 'coalgebra', 'differential',... | [-0.21878210063778647, 0.04448319292377595, -0.07726766181080356, 0.010696874191911008, -0.16096033778678823, -0.1375728526936942, -0.061230775410015335, 0.3484242338607529, -0.44912310530872723, -0.1705618304935725, 0.10207925799094435, -0.23165683527109457, -0.11131786353592026, 0.16478555967394065, -0.11460213978578... |
710.2071 | Generalized multiresolution analyses with given multiplicity functions | Generalized multiresolution analyses are increasing sequences of subspaces of
a Hilbert space $\H$ that fail to be multiresolution analyses in the sense of
wavelet theory because the core subspace does not have an orthonormal basis
generated by a fixed scaling function. Previous authors have studied a
multiplicity fu... | math.FA math.CA | generalized multiresolution analyses are increasing sequences of subspaces of a hilbert space h that fail to be multiresolution analyses in the sense of wavelet theory because the core subspace does not have an orthonormal basis generated by a fixed scaling function previous authors have studied a multiplicity function... | [['generalized', 'multiresolution', 'analyses', 'are', 'increasing', 'sequences', 'of', 'subspaces', 'of', 'a', 'hilbert', 'space', 'h', 'that', 'fail', 'to', 'be', 'multiresolution', 'analyses', 'in', 'the', 'sense', 'of', 'wavelet', 'theory', 'because', 'the', 'core', 'subspace', 'does', 'not', 'have', 'an', 'orthono... | [-0.12137167312797498, 0.12223065842977535, -0.14790321451357819, 0.07257604801561683, -0.06530481750695881, -0.09186601935547184, -0.03778106649088758, 0.35366072480312805, -0.2848615913736549, -0.21689963484690947, 0.10615296594332904, -0.23795410186390986, -0.1413787383670834, 0.15511472663122483, -0.095934282950210... |
710.2072 | On numerical averaging of the conductivity coefficient using two-scale
extensions | In this article we compare solutions to elliptic problems having rapidly
oscillated conductivity (permeability, etc) coefficient with solutions to
corresponding homogenized problems obtained from two-scale extensions of the
initial coefficient. The comparison is done numerically on several one and two
dimensional tes... | math.AP math.NA | in this article we compare solutions to elliptic problems having rapidly oscillated conductivity permeability etc coefficient with solutions to corresponding homogenized problems obtained from twoscale extensions of the initial coefficient the comparison is done numerically on several one and two dimensional test probl... | [['in', 'this', 'article', 'we', 'compare', 'solutions', 'to', 'elliptic', 'problems', 'having', 'rapidly', 'oscillated', 'conductivity', 'permeability', 'etc', 'coefficient', 'with', 'solutions', 'to', 'corresponding', 'homogenized', 'problems', 'obtained', 'from', 'twoscale', 'extensions', 'of', 'the', 'initial', 'co... | [-0.08302015651447268, 0.07953989236937979, -0.027066592367079395, 0.03427992819342762, -0.04121329861048322, -0.10998255434231116, -0.012798239964132126, 0.3668671683623241, -0.30351845636390723, -0.25262566592830876, 0.1502661696402356, -0.32825440764427183, -0.08793416129281888, 0.24138196966109368, -0.0211363337217... |
710.2073 | On coincidence of Alday-Maldacena-regularized $\sigma$-model and
Nambu-Goto areas of minimal surfaces | For the $\sigma$-model and Nambu-Goto actions, values of the
Alday-Maldacena-regularized actions are calculated on solutions of the
equations of motion with constant non-regularized Lagrangian. It turns out that
these values coincide up to a factor, independent of boundary conditions.
| hep-th | for the sigmamodel and nambugoto actions values of the aldaymaldacenaregularized actions are calculated on solutions of the equations of motion with constant nonregularized lagrangian it turns out that these values coincide up to a factor independent of boundary conditions | [['for', 'the', 'sigmamodel', 'and', 'nambugoto', 'actions', 'values', 'of', 'the', 'aldaymaldacenaregularized', 'actions', 'are', 'calculated', 'on', 'solutions', 'of', 'the', 'equations', 'of', 'motion', 'with', 'constant', 'nonregularized', 'lagrangian', 'it', 'turns', 'out', 'that', 'these', 'values', 'coincide', '... | [-0.15437910833248966, 0.13039818327677877, -0.06504393023389735, 0.003941535680113654, -0.06407063056739341, -0.12438347962635912, 0.03857377137204534, 0.33436337829028306, -0.21834033943320574, -0.27594374830981616, 0.12264720539219286, -0.2914373300185329, -0.1008231827106915, 0.19535682669007465, -0.026485474461591... |
710.2074 | Noncommutative Solitons | Solitonic objects play a central role in gauge and string theory (as, e.g.,
monopoles, black holes, D-branes, etc.). Certain string backgrounds produce a
noncommutative deformation of the low-energy effective field theory, which
allows for new types of solitonic solutions. I present the construction, moduli
spaces an... | hep-th | solitonic objects play a central role in gauge and string theory as eg monopoles black holes dbranes etc certain string backgrounds produce a noncommutative deformation of the lowenergy effective field theory which allows for new types of solitonic solutions i present the construction moduli spaces and dynamics of moya... | [['solitonic', 'objects', 'play', 'a', 'central', 'role', 'in', 'gauge', 'and', 'string', 'theory', 'as', 'eg', 'monopoles', 'black', 'holes', 'dbranes', 'etc', 'certain', 'string', 'backgrounds', 'produce', 'a', 'noncommutative', 'deformation', 'of', 'the', 'lowenergy', 'effective', 'field', 'theory', 'which', 'allows... | [-0.138038362340224, 0.16759915475960194, -0.06670112665109698, 0.20426871394851578, -0.08623410062412325, -0.18649158626342716, -0.07913619623230138, 0.27760884755300086, -0.20172070661216107, -0.25225813648871426, 0.12032624134043395, -0.25018981701563886, -0.20758169839267157, 0.13315439582305047, -0.079650064546036... |
710.2075 | Corrections to Schwarzschild Solution in Noncommutative Gauge Theory of
Gravity | A deformed Schwarzschild solution in noncommutative gauge theory of
gravitation is obtained. The gauge potentials (tetrad fields) are determined up
to the second order in the noncommutativity parameters $\Theta^{\mu\nu}$. A
deformed real metric is defined and its components are obtained. The
noncommutativity correcti... | hep-th gr-qc | a deformed schwarzschild solution in noncommutative gauge theory of gravitation is obtained the gauge potentials tetrad fields are determined up to the second order in the noncommutativity parameters thetamunu a deformed real metric is defined and its components are obtained the noncommutativity correction to the red s... | [['a', 'deformed', 'schwarzschild', 'solution', 'in', 'noncommutative', 'gauge', 'theory', 'of', 'gravitation', 'is', 'obtained', 'the', 'gauge', 'potentials', 'tetrad', 'fields', 'are', 'determined', 'up', 'to', 'the', 'second', 'order', 'in', 'the', 'noncommutativity', 'parameters', 'thetamunu', 'a', 'deformed', 'rea... | [-0.15409659235677742, 0.17093084159295086, -0.10495694544069566, 0.14177543161340156, -0.12177465111017227, -0.14317767320853936, -0.08219818757127294, 0.3414386847637013, -0.21686590262144417, -0.2721848737648023, 0.03939444946983902, -0.27600438101821906, -0.14021450652462708, 0.1539572397513049, -0.0984696750891963... |
710.2076 | Asymmetric weak-pinning superconducting channels: vortex ratchets | The controlled motion of objects through narrow channels is important in many
fields. We have fabricated asymmetric weak-pinning channels in a
superconducting thin-film strip for controlling the dynamics of vortices. The
lack of pinning allows the vortices to move through the channels with the
dominant interaction de... | cond-mat.supr-con | the controlled motion of objects through narrow channels is important in many fields we have fabricated asymmetric weakpinning channels in a superconducting thinfilm strip for controlling the dynamics of vortices the lack of pinning allows the vortices to move through the channels with the dominant interaction determin... | [['the', 'controlled', 'motion', 'of', 'objects', 'through', 'narrow', 'channels', 'is', 'important', 'in', 'many', 'fields', 'we', 'have', 'fabricated', 'asymmetric', 'weakpinning', 'channels', 'in', 'a', 'superconducting', 'thinfilm', 'strip', 'for', 'controlling', 'the', 'dynamics', 'of', 'vortices', 'the', 'lack', ... | [-0.22285890927718532, 0.174873199595529, -0.07147783226513814, -0.003699698882560516, -0.03870149971466632, -0.14667984952158744, 0.05034843764846183, 0.40827903397861987, -0.25642262648550734, -0.26622002978899306, 0.06993347096196827, -0.242614004349889, -0.0878149370527676, 0.19374029028920398, 0.023360034627389285... |
710.2077 | Towards Phonon Spectrum of Graphene | It is shown that the nearest neighbor coupling between the carbon atoms is
not enough to reproduce the phonon spectrum as observed in graphene, the second
neighbor force constant is essential. For completeness we have rederived the
phonon spectrum of one dimensional chains and two dimensional lattices like
square lat... | cond-mat.mtrl-sci | it is shown that the nearest neighbor coupling between the carbon atoms is not enough to reproduce the phonon spectrum as observed in graphene the second neighbor force constant is essential for completeness we have rederived the phonon spectrum of one dimensional chains and two dimensional lattices like square lattice... | [['it', 'is', 'shown', 'that', 'the', 'nearest', 'neighbor', 'coupling', 'between', 'the', 'carbon', 'atoms', 'is', 'not', 'enough', 'to', 'reproduce', 'the', 'phonon', 'spectrum', 'as', 'observed', 'in', 'graphene', 'the', 'second', 'neighbor', 'force', 'constant', 'is', 'essential', 'for', 'completeness', 'we', 'have... | [-0.11535628584090449, 0.13636007592039873, 0.01345950121263406, 0.036064543342485426, -0.052142404041242325, -0.1790318746171924, 0.05955361436795572, 0.4325733735365258, -0.25857815527539146, -0.2225129762985583, 0.061239229171301354, -0.33949993441587895, -0.11484754685522927, 0.14142187205196796, 0.0947561710323581... |
710.2078 | On Direct Verification of Warped Hierarchy-and-Flavor Models | We consider direct experimental verification of warped models, based on the
Randall-Sundrum (RS) scenario, that explain gauge and flavor hierarchies,
assuming that the gauge fields and fermions of the Standard Model (SM)
propagate in the 5D bulk. Most studies have focused on the bosonic Kaluza Klein
(KK) signatures a... | hep-ph | we consider direct experimental verification of warped models based on the randallsundrum rs scenario that explain gauge and flavor hierarchies assuming that the gauge fields and fermions of the standard model sm propagate in the 5d bulk most studies have focused on the bosonic kaluza klein kk signatures and indicate t... | [['we', 'consider', 'direct', 'experimental', 'verification', 'of', 'warped', 'models', 'based', 'on', 'the', 'randallsundrum', 'rs', 'scenario', 'that', 'explain', 'gauge', 'and', 'flavor', 'hierarchies', 'assuming', 'that', 'the', 'gauge', 'fields', 'and', 'fermions', 'of', 'the', 'standard', 'model', 'sm', 'propagat... | [-0.09496137846087781, 0.25682851362480685, -0.061336058436199, 0.14944496291732945, -0.11717376663638752, -0.20002742482842328, 0.0095618350668719, 0.31640778996013835, -0.15776317592769606, -0.2986071975673458, 0.040390981307627596, -0.30247694977522627, -0.025566483500833605, 0.132637203125484, 0.08055445653621528, ... |
710.2079 | The yoga of the Cassels-Tate pairing | Cassels has described a pairing on the 2-Selmer group of an elliptic curve
which shares some properties with the Cassels-Tate pairing. In this article, we
prove that the two pairings are the same.
| math.NT | cassels has described a pairing on the 2selmer group of an elliptic curve which shares some properties with the casselstate pairing in this article we prove that the two pairings are the same | [['cassels', 'has', 'described', 'a', 'pairing', 'on', 'the', '2selmer', 'group', 'of', 'an', 'elliptic', 'curve', 'which', 'shares', 'some', 'properties', 'with', 'the', 'casselstate', 'pairing', 'in', 'this', 'article', 'we', 'prove', 'that', 'the', 'two', 'pairings', 'are', 'the', 'same']] | [-0.2812453314774867, 0.09421824674152021, -0.22062085719186475, 0.08935990050138737, -0.06756791195860415, -0.10975769400653063, -0.04040489024059339, 0.3233420086855238, -0.31632365354082803, -0.20890891032688547, 0.0367506843476528, -0.31710497097987117, -0.1346127609298988, 0.2211078634542046, -0.11744056543278875,... |
710.208 | The classification of simple Jacobi--Ricci commuting algebraic curvature
tensors | We classify algebraic curvature tensors such that the Ricci operator is
simple (i.e. the Ricci operator is complex diagonalizable and either the
complex spectrum consists of a single real eigenvalue or the complex spectrum
consists of a pair of eigenvalues which are complex conjugates of each other)
and which are Jac... | math.DG | we classify algebraic curvature tensors such that the ricci operator is simple ie the ricci operator is complex diagonalizable and either the complex spectrum consists of a single real eigenvalue or the complex spectrum consists of a pair of eigenvalues which are complex conjugates of each other and which are jacobiric... | [['we', 'classify', 'algebraic', 'curvature', 'tensors', 'such', 'that', 'the', 'ricci', 'operator', 'is', 'simple', 'ie', 'the', 'ricci', 'operator', 'is', 'complex', 'diagonalizable', 'and', 'either', 'the', 'complex', 'spectrum', 'consists', 'of', 'a', 'single', 'real', 'eigenvalue', 'or', 'the', 'complex', 'spectru... | [-0.22916221494476, 0.13250313245410483, -0.012032027637201643, 0.01719828389422406, -0.16726282687251648, -0.186211418463952, -0.16417798501927228, 0.34419587987755973, -0.2980579087244613, -0.1470490698185232, 0.11847560993942713, -0.3684572199034312, -0.17332131775199539, 0.1011148171225888, -0.012516872177550953, 0... |
710.2081 | A semigroup approach to wreath-product extensions of Solomon's descent
algebras | There is a well-known combinatorial definition, based on ordered set
partitions, of the semigroup of faces of the braid arrangement. We generalize
this definition to obtain a semigroup Sigma_n^G associated with G wr S_n, the
wreath product of the symmetric group S_n with an arbitrary group G. Techniques
of Bidigare a... | math.RA math.CO | there is a wellknown combinatorial definition based on ordered set partitions of the semigroup of faces of the braid arrangement we generalize this definition to obtain a semigroup sigma_ng associated with g wr s_n the wreath product of the symmetric group s_n with an arbitrary group g techniques of bidigare and brown ... | [['there', 'is', 'a', 'wellknown', 'combinatorial', 'definition', 'based', 'on', 'ordered', 'set', 'partitions', 'of', 'the', 'semigroup', 'of', 'faces', 'of', 'the', 'braid', 'arrangement', 'we', 'generalize', 'this', 'definition', 'to', 'obtain', 'a', 'semigroup', 'sigma_ng', 'associated', 'with', 'g', 'wr', 's_n', '... | [-0.143920766769184, 0.09232992372870083, -0.11406341066790951, 0.02265064132322247, -0.15591094403838118, -0.10455869669094682, 0.005351475729710526, 0.3743108297387759, -0.3526614466475116, -0.22242748257186679, 0.12179864268336031, -0.26026711640879513, -0.08550667002693646, 0.18226052549564176, -0.17772610138894784... |
710.2082 | Exponential stability of non-autonomous stochastic partial differential
equations with finite memory | The exponential stability, in both mean square and almost sure senses, for
energy solutions to a class of nonlinear and non-autonomous stochastic PDEs
with finite memory is investigated. Various criteria for stability are
obtained. An example is presented to demonstrate the main results.
| math.DS math.PR | the exponential stability in both mean square and almost sure senses for energy solutions to a class of nonlinear and nonautonomous stochastic pdes with finite memory is investigated various criteria for stability are obtained an example is presented to demonstrate the main results | [['the', 'exponential', 'stability', 'in', 'both', 'mean', 'square', 'and', 'almost', 'sure', 'senses', 'for', 'energy', 'solutions', 'to', 'a', 'class', 'of', 'nonlinear', 'and', 'nonautonomous', 'stochastic', 'pdes', 'with', 'finite', 'memory', 'is', 'investigated', 'various', 'criteria', 'for', 'stability', 'are', '... | [-0.12770365354020236, 0.046279734740003964, -0.03256562827588167, 0.10485331758553552, -0.024002506722544514, -0.12708535676735433, -0.05035002690978175, 0.37192335560224776, -0.2949522393214148, -0.2468972886630962, 0.20459794251215752, -0.27485453709959984, -0.1502099721584209, 0.2482816736148887, -0.080154115832302... |
710.2083 | Association Rules in the Relational Calculus | One of the most utilized data mining tasks is the search for association
rules. Association rules represent significant relationships between items in
transactions. We extend the concept of association rule to represent a much
broader class of associations, which we refer to as \emph{entity-relationship
rules.} Seman... | cs.DB cs.LG cs.LO | one of the most utilized data mining tasks is the search for association rules association rules represent significant relationships between items in transactions we extend the concept of association rule to represent a much broader class of associations which we refer to as emphentityrelationship rules semantically en... | [['one', 'of', 'the', 'most', 'utilized', 'data', 'mining', 'tasks', 'is', 'the', 'search', 'for', 'association', 'rules', 'association', 'rules', 'represent', 'significant', 'relationships', 'between', 'items', 'in', 'transactions', 'we', 'extend', 'the', 'concept', 'of', 'association', 'rule', 'to', 'represent', 'a',... | [-0.10998967720322239, 0.024200942584322493, -0.08864688471375594, 0.16832634625454587, -0.23588448039536336, -0.145523848206492, 0.23168603574983704, 0.41586822007999763, -0.28929938290616297, -0.2896330798840494, 0.04545002865709039, -0.2564032010517074, -0.11966937993544614, 0.14147173269489074, -0.09122116351952252... |
710.2084 | Supersymmetry Breaking and Radius Stabilization by Constant Boundary
Superpotentials in Warped Space | Supersymmetry breaking and radius stabilization by constant superpotentials
localized at boundaries is studied in a supersymmetric warped space model where
a hypermultiplet, a compensator and a radion multiplet are taken into account.
Soft mass induced by the anomaly mediation can be of the order of 100GeV and
can be... | hep-th hep-ph | supersymmetry breaking and radius stabilization by constant superpotentials localized at boundaries is studied in a supersymmetric warped space model where a hypermultiplet a compensator and a radion multiplet are taken into account soft mass induced by the anomaly mediation can be of the order of 100gev and can be dom... | [['supersymmetry', 'breaking', 'and', 'radius', 'stabilization', 'by', 'constant', 'superpotentials', 'localized', 'at', 'boundaries', 'is', 'studied', 'in', 'a', 'supersymmetric', 'warped', 'space', 'model', 'where', 'a', 'hypermultiplet', 'a', 'compensator', 'and', 'a', 'radion', 'multiplet', 'are', 'taken', 'into', ... | [-0.15891449541737468, 0.2694493947617001, -0.030462779005559288, 0.09749398362562377, -0.08924368482824983, -0.12169847191485056, -0.023610377826301727, 0.3305033306764849, -0.20058691164210313, -0.3332814375664723, 0.10550924881965205, -0.22806340007711265, -0.06274981552071995, 0.11620248756095199, -0.00930375234871... |
710.2085 | Screening masses in the SU(3) pure gauge theory and universality | We determine from Polyakov loop correlators the screening masses in th e
deconfined phase of the (3+1)d SU(3) pure gauge theory at finite temperature
near transition, for two different channels of angular momentum and parity.
Their ratio is compared with that of the massive excitations with the same
quantum numbers i... | hep-lat | we determine from polyakov loop correlators the screening masses in th e deconfined phase of the 31d su3 pure gauge theory at finite temperature near transition for two different channels of angular momentum and parity their ratio is compared with that of the massive excitations with the same quantum numbers in the 3d ... | [['we', 'determine', 'from', 'polyakov', 'loop', 'correlators', 'the', 'screening', 'masses', 'in', 'th', 'e', 'deconfined', 'phase', 'of', 'the', '31d', 'su3', 'pure', 'gauge', 'theory', 'at', 'finite', 'temperature', 'near', 'transition', 'for', 'two', 'different', 'channels', 'of', 'angular', 'momentum', 'and', 'par... | [-0.1309513401328808, 0.2673083590920128, -0.07883269298777339, 0.08087220341521537, 0.024519068397404184, -0.12055914601133692, 0.03591026260650584, 0.3431287544469039, -0.19708577568775842, -0.2537799795646043, 0.020913271041631345, -0.3309983506443955, -0.08937063830062038, 0.07489020699147313, 0.09434551577128115, ... |
710.2086 | Strings on conifolds from strong coupling dynamics, part I | A method to solve various aspects of the strong coupling expansion of the
superconformal field theory duals of AdS_5 x X geometries from first principles
is proposed. The main idea is that at strong coupling the configurations that
dominate the low energy dynamics of the field theory compactified on a three
sphere ar... | hep-th | a method to solve various aspects of the strong coupling expansion of the superconformal field theory duals of ads_5 x x geometries from first principles is proposed the main idea is that at strong coupling the configurations that dominate the low energy dynamics of the field theory compactified on a three sphere are g... | [['a', 'method', 'to', 'solve', 'various', 'aspects', 'of', 'the', 'strong', 'coupling', 'expansion', 'of', 'the', 'superconformal', 'field', 'theory', 'duals', 'of', 'ads_5', 'x', 'x', 'geometries', 'from', 'first', 'principles', 'is', 'proposed', 'the', 'main', 'idea', 'is', 'that', 'at', 'strong', 'coupling', 'the',... | [-0.14870411095204006, 0.14657395250148067, -0.12163689226415658, 0.07503134092020933, -0.03673869833691305, -0.08491842557952284, -0.021466695283252617, 0.31268777867080644, -0.2283024734575139, -0.2675465273042751, 0.056518412498367386, -0.25875589551761485, -0.18965716898809512, 0.14206076246012153, -0.0330847536110... |
710.2087 | Impact of slepton generation mixing on the search for sneutrinos -
Lepton flavour violation in sneutrino production and decays in the general
MSSM | We perform a systematic study of sneutrino production and decays in the
Minimal Supersymmetric Standard Model (MSSM) with slepton generation mixing. We
study bosonic decays like sneutrino \to slepton^- + W^+/H^+ as well as
fermionic ones. We show that the effect of slepton generation mixing on the
sneutrino productio... | hep-ph hep-ex | we perform a systematic study of sneutrino production and decays in the minimal supersymmetric standard model mssm with slepton generation mixing we study bosonic decays like sneutrino to slepton wh as well as fermionic ones we show that the effect of slepton generation mixing on the sneutrino production and decays can... | [['we', 'perform', 'a', 'systematic', 'study', 'of', 'sneutrino', 'production', 'and', 'decays', 'in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'with', 'slepton', 'generation', 'mixing', 'we', 'study', 'bosonic', 'decays', 'like', 'sneutrino', 'to', 'slepton', 'wh', 'as', 'well', 'as', 'fermioni... | [-0.06917356125540236, 0.28424018249494926, 0.01453708501496506, 0.2123564131573765, -0.09387222874584128, -0.1822963904462827, 0.03203633814955185, 0.30112803957506434, -0.212983496939239, -0.26927611796474715, 0.04966731607751215, -0.31507881753851924, 0.028103350191512732, 0.17318649983793064, 0.0595955132581384, 0.... |
710.2088 | Multiplicative function instead of logarithm (an elementary approach) | V.I. Arnold has recently defined the complexity of finite sequences of zeroes
and ones in terms of periods and preperiods of attractors of a dynamic system
of the operator of finite differentiation. Arnold has set up a hypothesis that
the sequence of the values of the logarithm is most complicated or almost most
comp... | math.NT math.AC | vi arnold has recently defined the complexity of finite sequences of zeroes and ones in terms of periods and preperiods of attractors of a dynamic system of the operator of finite differentiation arnold has set up a hypothesis that the sequence of the values of the logarithm is most complicated or almost most complicat... | [['vi', 'arnold', 'has', 'recently', 'defined', 'the', 'complexity', 'of', 'finite', 'sequences', 'of', 'zeroes', 'and', 'ones', 'in', 'terms', 'of', 'periods', 'and', 'preperiods', 'of', 'attractors', 'of', 'a', 'dynamic', 'system', 'of', 'the', 'operator', 'of', 'finite', 'differentiation', 'arnold', 'has', 'set', 'u... | [-0.1592260351128996, 0.11138245897418862, -0.08565134391906339, 0.07544841325132672, -0.06768660249034746, -0.10160014543195314, 0.038204437162334084, 0.3088018150162806, -0.2585593622803705, -0.23728252389818566, 0.13638766367018326, -0.22531440732877814, -0.18039217807882285, 0.21172214502366174, -0.0747840015063865... |
710.2089 | Tailoring polarization entanglement in anisotropy-compensated SPDC | We show that the angular spectrum of type-II SPDC contains a continuum of
maximally entangled states. For the realization of a bright source of entangled
two-photon states, a standard technique is to compensate for the transverse
walk-off in the production crystal. We demonstrate that polarization entangled
states ca... | quant-ph | we show that the angular spectrum of typeii spdc contains a continuum of maximally entangled states for the realization of a bright source of entangled twophoton states a standard technique is to compensate for the transverse walkoff in the production crystal we demonstrate that polarization entangled states can be eff... | [['we', 'show', 'that', 'the', 'angular', 'spectrum', 'of', 'typeii', 'spdc', 'contains', 'a', 'continuum', 'of', 'maximally', 'entangled', 'states', 'for', 'the', 'realization', 'of', 'a', 'bright', 'source', 'of', 'entangled', 'twophoton', 'states', 'a', 'standard', 'technique', 'is', 'to', 'compensate', 'for', 'the'... | [-0.09784449674771167, 0.24690791728062322, -0.09297979099210352, 0.019293374894510232, -0.02130480943661597, -0.16783858235511515, 0.05876477713981229, 0.42590178466505474, -0.25734988576732576, -0.25959369263404775, -0.007440305930989173, -0.2656557426511831, -0.0486053452671816, 0.211140829537827, 0.0020788596302736... |
710.209 | Dynamical systems with double recursion are undecidable | A primitive type of two-dimensional dynamic system is introduced. It is shown
that there is no decision procedure able to answer if such a dynamical system
is ultimately zero.
| math.DS math.AC | a primitive type of twodimensional dynamic system is introduced it is shown that there is no decision procedure able to answer if such a dynamical system is ultimately zero | [['a', 'primitive', 'type', 'of', 'twodimensional', 'dynamic', 'system', 'is', 'introduced', 'it', 'is', 'shown', 'that', 'there', 'is', 'no', 'decision', 'procedure', 'able', 'to', 'answer', 'if', 'such', 'a', 'dynamical', 'system', 'is', 'ultimately', 'zero']] | [-0.15811637244267582, 0.12690697889775038, -0.12167624223591952, 0.09106562416679387, -0.0992539047167219, -0.21566205230995145, 0.042429715138057184, 0.3479690880611025, -0.3077411502599716, -0.20872564093563065, 0.12923667944389686, -0.2460974359820629, -0.2823152508715103, 0.2022580111335064, -0.09198034655880825, ... |
710.2091 | Slow and fast micro-field components in warm and dense hydrogen plasmas | The aim of this work is the investigation of the statistical properties of
local electric fields in an ion-electron two component plasmas for coupled
conditions. The stochastic fields at a charged or at a neutral point in plasmas
involve both slow and fast fluctuation characteristics. The statistical study
of these l... | physics.plasm-ph | the aim of this work is the investigation of the statistical properties of local electric fields in an ionelectron two component plasmas for coupled conditions the stochastic fields at a charged or at a neutral point in plasmas involve both slow and fast fluctuation characteristics the statistical study of these local ... | [['the', 'aim', 'of', 'this', 'work', 'is', 'the', 'investigation', 'of', 'the', 'statistical', 'properties', 'of', 'local', 'electric', 'fields', 'in', 'an', 'ionelectron', 'two', 'component', 'plasmas', 'for', 'coupled', 'conditions', 'the', 'stochastic', 'fields', 'at', 'a', 'charged', 'or', 'at', 'a', 'neutral', 'p... | [-0.13375352247211034, 0.160981985548836, -0.07069211360624807, 0.05497799348643797, 0.014590438773219814, -0.06153573126191954, 0.015260149719204731, 0.38731857957485727, -0.21745597522616564, -0.28813888811824206, 0.05483044213601416, -0.23891782002578613, -0.0754901366182854, 0.20958199124214447, 0.06755480501510783... |
710.2092 | Self-similarity of complex networks and hidden metric spaces | We demonstrate that the self-similarity of some scale-free networks with
respect to a simple degree-thresholding renormalization scheme finds a natural
interpretation in the assumption that network nodes exist in hidden metric
spaces. Clustering, i.e., cycles of length three, plays a crucial role in this
framework as... | cond-mat.dis-nn cs.NI physics.soc-ph | we demonstrate that the selfsimilarity of some scalefree networks with respect to a simple degreethresholding renormalization scheme finds a natural interpretation in the assumption that network nodes exist in hidden metric spaces clustering ie cycles of length three plays a crucial role in this framework as a topologi... | [['we', 'demonstrate', 'that', 'the', 'selfsimilarity', 'of', 'some', 'scalefree', 'networks', 'with', 'respect', 'to', 'a', 'simple', 'degreethresholding', 'renormalization', 'scheme', 'finds', 'a', 'natural', 'interpretation', 'in', 'the', 'assumption', 'that', 'network', 'nodes', 'exist', 'in', 'hidden', 'metric', '... | [-0.13669034648327189, 0.0849758058627087, -0.1021725856494812, 0.13889729753116212, -0.07071714807432472, -0.12665995886639217, 0.022482430807461862, 0.42735379999666884, -0.28072717559131743, -0.2909505961170796, 0.06443694324984231, -0.24655897340230776, -0.25576389862793514, 0.15289361758582426, -0.0447078590891977... |
710.2093 | Boundary action of the H3+ model | We find the boundary action for Euclidean AdS2 D-branes in H3+. This action
is consistent with the D-branes' symmetries and with the H3+-Liouville relation
for disc correlators. It can be used for performing free-field calculations in
the H3+ model with boundaries. We explicitly perform the Coulomb-like integrals
whi... | hep-th | we find the boundary action for euclidean ads2 dbranes in h3 this action is consistent with the dbranes symmetries and with the h3liouville relation for disc correlators it can be used for performing freefield calculations in the h3 model with boundaries we explicitly perform the coulomblike integrals which appear in t... | [['we', 'find', 'the', 'boundary', 'action', 'for', 'euclidean', 'ads2', 'dbranes', 'in', 'h3', 'this', 'action', 'is', 'consistent', 'with', 'the', 'dbranes', 'symmetries', 'and', 'with', 'the', 'h3liouville', 'relation', 'for', 'disc', 'correlators', 'it', 'can', 'be', 'used', 'for', 'performing', 'freefield', 'calcu... | [-0.09094004222953861, 0.10853610450938118, -0.08587054050329959, 0.11755422677026328, -0.02632668044305209, -0.0999905898828398, -0.024967505046251146, 0.38809236799451435, -0.1557317910200888, -0.2511589336632328, 0.06890468072379008, -0.27824405885555525, -0.16223853956696324, 0.13356090725794662, -0.022990451166124... |
710.2094 | Improving Guess Geminals for the Geminal Mean Field Configuration
Interaction Method | The purpose of this letter is to show that a rotation of Hartree-Fock
canonical orbitals which minimizes the lowest eigenvalues of a configuration
interaction calculation limited to the mono-excitated configurations from a
given orbital allows one to construct a better starting guess for the geminal
mean field config... | physics.chem-ph quant-ph | the purpose of this letter is to show that a rotation of hartreefock canonical orbitals which minimizes the lowest eigenvalues of a configuration interaction calculation limited to the monoexcitated configurations from a given orbital allows one to construct a better starting guess for the geminal mean field configurat... | [['the', 'purpose', 'of', 'this', 'letter', 'is', 'to', 'show', 'that', 'a', 'rotation', 'of', 'hartreefock', 'canonical', 'orbitals', 'which', 'minimizes', 'the', 'lowest', 'eigenvalues', 'of', 'a', 'configuration', 'interaction', 'calculation', 'limited', 'to', 'the', 'monoexcitated', 'configurations', 'from', 'a', '... | [-0.14793071960460166, 0.07647865657143448, -0.12024646728983795, 0.08329676208561476, -0.05691858601509309, -0.09500956476418948, 0.06169682052176522, 0.3268332377228202, -0.22629764461319665, -0.31524408053682773, -0.04925674093621118, -0.2540226368170008, -0.11384770091699094, 0.11396372620472495, 0.0085251085764291... |
710.2095 | Entanglement in spatially inhomogeneous many-fermion systems | We investigate entanglement of strongly interacting fermions in spatially
inhomogeneous environments. To quantify entanglement in the presence of spatial
inhomogeneity, we propose a local-density approximation (LDA) to the
entanglement entropy, and a nested LDA scheme to evaluate the entanglement
entropy on inhomogen... | cond-mat.str-el cond-mat.stat-mech quant-ph | we investigate entanglement of strongly interacting fermions in spatially inhomogeneous environments to quantify entanglement in the presence of spatial inhomogeneity we propose a localdensity approximation lda to the entanglement entropy and a nested lda scheme to evaluate the entanglement entropy on inhomogeneous den... | [['we', 'investigate', 'entanglement', 'of', 'strongly', 'interacting', 'fermions', 'in', 'spatially', 'inhomogeneous', 'environments', 'to', 'quantify', 'entanglement', 'in', 'the', 'presence', 'of', 'spatial', 'inhomogeneity', 'we', 'propose', 'a', 'localdensity', 'approximation', 'lda', 'to', 'the', 'entanglement', ... | [-0.15819312949620543, 0.21930239683992805, -0.0719053513547849, 0.08287896708740543, 0.09942174571832375, -0.18383086799599585, 0.03400778061532903, 0.41147301956301646, -0.24486845934852247, -0.24344408930323663, -0.03545899631987725, -0.3285831352518428, -0.0986417927823606, 0.10184182136186531, 0.008061903799396185... |
710.2096 | A geometric approach to full Colombeau algebras | We present a geometric approach to diffeomorphism invariant full Colombeau
algebras which allows a particularly clear view on the construction of the
intrinsically defined algebra $\hat{\mathcal G}(M)$ on the manifold $M$ given
in (Grosser et al., Adv. Math. 166 (2002), 179--206).
| math.FA | we present a geometric approach to diffeomorphism invariant full colombeau algebras which allows a particularly clear view on the construction of the intrinsically defined algebra hatmathcal gm on the manifold m given in grosser et al adv math 166 2002 179206 | [['we', 'present', 'a', 'geometric', 'approach', 'to', 'diffeomorphism', 'invariant', 'full', 'colombeau', 'algebras', 'which', 'allows', 'a', 'particularly', 'clear', 'view', 'on', 'the', 'construction', 'of', 'the', 'intrinsically', 'defined', 'algebra', 'hatmathcal', 'gm', 'on', 'the', 'manifold', 'm', 'given', 'in'... | [-0.1549286655616015, -0.012211160827428102, -0.11257055213209241, 0.02917536291060969, -0.15781795184593647, -0.08188500909600407, 0.004052754753502086, 0.33102178368717433, -0.2296138327445078, -0.3511037455871701, 0.04957044941256754, -0.17887440330268872, -0.24078264068812133, 0.16057543801725843, -0.24930261513218... |
710.2097 | The algebra of Wilson-'t Hooft operators | We study the Operator Product Expansion of Wilson-'t Hooft operators in a
twisted N=4 super-Yang-Mills theory with gauge group G. The Montonen-Olive
duality puts strong constraints on the OPE and in the case G=SU(2) completely
determines it. From the mathematical point of view, the Montonen-Olive duality
predicts the... | hep-th math.AG | we study the operator product expansion of wilsont hooft operators in a twisted n4 superyangmills theory with gauge group g the montonenolive duality puts strong constraints on the ope and in the case gsu2 completely determines it from the mathematical point of view the montonenolive duality predicts the l2 dolbeault c... | [['we', 'study', 'the', 'operator', 'product', 'expansion', 'of', 'wilsont', 'hooft', 'operators', 'in', 'a', 'twisted', 'n4', 'superyangmills', 'theory', 'with', 'gauge', 'group', 'g', 'the', 'montonenolive', 'duality', 'puts', 'strong', 'constraints', 'on', 'the', 'ope', 'and', 'in', 'the', 'case', 'gsu2', 'completel... | [-0.19513404440589338, 0.09213908498072886, -0.07336547174989912, 0.10625481319480709, -0.10359639763399693, -0.14097204055481902, 0.03209930411512254, 0.33631675274643513, -0.25014728037196965, -0.1784244685744246, 0.10025877089702546, -0.2450510191542673, -0.21656128845643252, 0.08841626622181918, -0.1495222868065216... |
710.2098 | Propositional systems, Hilbert lattices and generalized Hilbert spaces | With this chapter we provide a compact yet complete survey of two most
remarkable "representation theorems": every arguesian projective geometry is
represented by an essentially unique vector space, and every arguesian Hilbert
geometry is represented by an essentially unique generalized Hilbert space. C.
Piron's orig... | quant-ph | with this chapter we provide a compact yet complete survey of two most remarkable representation theorems every arguesian projective geometry is represented by an essentially unique vector space and every arguesian hilbert geometry is represented by an essentially unique generalized hilbert space c pirons original repr... | [['with', 'this', 'chapter', 'we', 'provide', 'a', 'compact', 'yet', 'complete', 'survey', 'of', 'two', 'most', 'remarkable', 'representation', 'theorems', 'every', 'arguesian', 'projective', 'geometry', 'is', 'represented', 'by', 'an', 'essentially', 'unique', 'vector', 'space', 'and', 'every', 'arguesian', 'hilbert',... | [-0.14066732665208778, 0.08269055679217734, -0.11538372086221002, 0.062083725726907665, -0.09366051212681416, -0.15181767672328347, -0.015537514038825114, 0.36234372406077564, -0.3572997317546138, -0.1474905169421905, 0.08647133213690222, -0.23196188091099984, -0.1574585734922579, 0.1704395442686387, -0.142782762464612... |
710.2099 | The structure and properties of vacancies in Si nano-crystals calculated
by real-space pseudopotential methods | The structure and properties of vacancies in a 2 nm Si nano-crystal are
studied using a real space density functional theory/pseudopotential method. It
is observed that a vacancy's electronic properties and energy of formation are
directly related to the local symmetry of the vacancy site. The formation
energy for va... | cond-mat.mtrl-sci | the structure and properties of vacancies in a 2 nm si nanocrystal are studied using a real space density functional theorypseudopotential method it is observed that a vacancys electronic properties and energy of formation are directly related to the local symmetry of the vacancy site the formation energy for vacancies... | [['the', 'structure', 'and', 'properties', 'of', 'vacancies', 'in', 'a', '2', 'nm', 'si', 'nanocrystal', 'are', 'studied', 'using', 'a', 'real', 'space', 'density', 'functional', 'theorypseudopotential', 'method', 'it', 'is', 'observed', 'that', 'a', 'vacancys', 'electronic', 'properties', 'and', 'energy', 'of', 'forma... | [-0.07919847644882759, 0.16270702635800396, -0.008832058110446841, 0.10465460689630601, 0.02811439560847012, -0.10667628015357035, 0.0555844631873899, 0.4583701512741822, -0.24768974500302984, -0.33604785051472763, -0.002848405105329153, -0.3334666277644121, -0.0715386983593581, 0.12713956438367152, 0.07766975811682642... |
710.21 | Kaon semileptonic decay form factors from N_f = 2 non-perturbatively
O(a)-improved Wilson fermions | We present first results from the QCDSF collaboration for the kaon
semileptonic decay form factors at zero momentum transfer, using two flavours
of non-perturbatively O(a)-improved Wilson quarks. A lattice determination of
these form factors is of particular interest to improve the accuracy on the CKM
matrix element ... | hep-lat | we present first results from the qcdsf collaboration for the kaon semileptonic decay form factors at zero momentum transfer using two flavours of nonperturbatively oaimproved wilson quarks a lattice determination of these form factors is of particular interest to improve the accuracy on the ckm matrix element v_us cal... | [['we', 'present', 'first', 'results', 'from', 'the', 'qcdsf', 'collaboration', 'for', 'the', 'kaon', 'semileptonic', 'decay', 'form', 'factors', 'at', 'zero', 'momentum', 'transfer', 'using', 'two', 'flavours', 'of', 'nonperturbatively', 'oaimproved', 'wilson', 'quarks', 'a', 'lattice', 'determination', 'of', 'these',... | [-0.05040086050036499, 0.259665068882528, -0.08248166107373793, 0.05136365720379595, -0.05859073627154144, -0.10666236733975873, 0.14903197285007644, 0.3766162300042892, -0.15255558176824216, -0.251323902798984, 0.027289125730880024, -0.34040025358230236, 0.008575333392226629, 0.14730654950149022, 0.041009834072856084,... |
710.2101 | Order one invariants of spherical curves | We give a complete description of all order 1 invariants of spherical curves.
We also identify the subspaces of all J-invariants and S-invariants, and
present two equalities satisfied by any spherical curve.
| math.GT | we give a complete description of all order 1 invariants of spherical curves we also identify the subspaces of all jinvariants and sinvariants and present two equalities satisfied by any spherical curve | [['we', 'give', 'a', 'complete', 'description', 'of', 'all', 'order', '1', 'invariants', 'of', 'spherical', 'curves', 'we', 'also', 'identify', 'the', 'subspaces', 'of', 'all', 'jinvariants', 'and', 'sinvariants', 'and', 'present', 'two', 'equalities', 'satisfied', 'by', 'any', 'spherical', 'curve']] | [-0.22346461561392061, 0.08801242834306322, -0.11424296710174531, 0.09683132154168561, -0.050802701560314745, -0.13447881197498646, 0.0003350149418110959, 0.29726571298670024, -0.22169886996562127, -0.24972253490705043, 0.09761904401239008, -0.27074728603474796, -0.15140815658378415, 0.2403853974537924, -0.075531465528... |
710.2102 | Molecular Hydrogen and Global Star Formation Relations in Galaxies | (ABRIDGED) We use hydrodynamical simulations of disk galaxies to study
relations between star formation and properties of the molecular interstellar
medium (ISM). We implement a model for the ISM that includes low-temperature
(T<10^4K) cooling, directly ties the star formation rate to the molecular gas
density, and a... | astro-ph | abridged we use hydrodynamical simulations of disk galaxies to study relations between star formation and properties of the molecular interstellar medium ism we implement a model for the ism that includes lowtemperature t104k cooling directly ties the star formation rate to the molecular gas density and accounts for th... | [['abridged', 'we', 'use', 'hydrodynamical', 'simulations', 'of', 'disk', 'galaxies', 'to', 'study', 'relations', 'between', 'star', 'formation', 'and', 'properties', 'of', 'the', 'molecular', 'interstellar', 'medium', 'ism', 'we', 'implement', 'a', 'model', 'for', 'the', 'ism', 'that', 'includes', 'lowtemperature', 't... | [-0.049421101579597844, 0.1096878752897222, -0.09645164025792231, 0.1372124401666224, -0.04530949087658276, -0.010115449062238137, 0.05952559155994095, 0.3953826684875336, -0.1821556208531062, -0.32937026551614207, -0.06368220791608716, -0.2749057577798764, -0.061460952355215946, 0.1565859444408367, 0.00566176043202479... |
710.2103 | X-ray enabled MOCASSIN: a 3D code for photoionized media | We present a new version of the fully 3D photoionization and dust radiative
transfer code, MOCASSIN, that uses a Monte Carlo approach for the transfer of
radiation. The X-ray enabled MOCASSIN allows a fully geometry independent
description of low-density gaseous environments strongly photoionized by a
radiation field... | astro-ph | we present a new version of the fully 3d photoionization and dust radiative transfer code mocassin that uses a monte carlo approach for the transfer of radiation the xray enabled mocassin allows a fully geometry independent description of lowdensity gaseous environments strongly photoionized by a radiation field extend... | [['we', 'present', 'a', 'new', 'version', 'of', 'the', 'fully', '3d', 'photoionization', 'and', 'dust', 'radiative', 'transfer', 'code', 'mocassin', 'that', 'uses', 'a', 'monte', 'carlo', 'approach', 'for', 'the', 'transfer', 'of', 'radiation', 'the', 'xray', 'enabled', 'mocassin', 'allows', 'a', 'fully', 'geometry', '... | [-0.013389298866968602, 0.03181225565451853, -0.07242467450150461, 0.09237260806494979, -0.06123192511990459, -0.13303771935817268, 0.005748646060022077, 0.4298604503618898, -0.222296143541354, -0.31177327966886675, 0.08690379872267065, -0.21175285747408956, -0.06665373417652315, 0.285289893961615, 0.001075738264868656... |
710.2104 | Scalar Bilepton Dark Matter | In this work we show that 3-3-1 model with right-handed neutrinos has a
natural weakly interacting massive particle (WIMP) dark mater candidate. It is
a complex scalar with mass of order of some hundreds of GeV which carries two
units of lepton number, a scalar bilepton. This makes it a very peculiar WIMP,
very disti... | hep-ph astro-ph hep-th | in this work we show that 331 model with righthanded neutrinos has a natural weakly interacting massive particle wimp dark mater candidate it is a complex scalar with mass of order of some hundreds of gev which carries two units of lepton number a scalar bilepton this makes it a very peculiar wimp very distinct from su... | [['in', 'this', 'work', 'we', 'show', 'that', '331', 'model', 'with', 'righthanded', 'neutrinos', 'has', 'a', 'natural', 'weakly', 'interacting', 'massive', 'particle', 'wimp', 'dark', 'mater', 'candidate', 'it', 'is', 'a', 'complex', 'scalar', 'with', 'mass', 'of', 'order', 'of', 'some', 'hundreds', 'of', 'gev', 'whic... | [-0.09534134184536727, 0.21248760065468758, -0.060440775918085936, 0.13289976686077273, -0.12618556126000602, -0.16072043455813242, 0.020114249331147773, 0.34462271086547686, -0.1625805644966338, -0.392805945776079, 0.004662437248043716, -0.2951624784618616, -0.05680502162962828, 0.15199820256650287, 0.0424693961627781... |
710.2105 | AEGIS: New Evidence Linking Active Galactic Nuclei to the Quenching of
Star Formation | Utilizing Chandra X-ray observations in the All-wavelength Extended Groth
Strip International Survey (AEGIS) we identify 241 X-ray selected Active
Galactic Nuclei (AGNs, L > 10^{42} ergs/s) and study the properties of their
host galaxies in the range 0.4 < z < 1.4. By making use of infrared photometry
from Palomar Ob... | astro-ph | utilizing chandra xray observations in the allwavelength extended groth strip international survey aegis we identify 241 xray selected active galactic nuclei agns l 1042 ergss and study the properties of their host galaxies in the range 04 z 14 by making use of infrared photometry from palomar observatory and bri imagi... | [['utilizing', 'chandra', 'xray', 'observations', 'in', 'the', 'allwavelength', 'extended', 'groth', 'strip', 'international', 'survey', 'aegis', 'we', 'identify', '241', 'xray', 'selected', 'active', 'galactic', 'nuclei', 'agns', 'l', '1042', 'ergss', 'and', 'study', 'the', 'properties', 'of', 'their', 'host', 'galaxi... | [-0.02457711451931338, 0.11210078481854492, -0.03199654026378401, 0.16456304888011322, -0.12512714886822954, -0.03707528448499301, 0.09422482682783916, 0.4581890491456872, -0.11722067936388902, -0.3876208098604222, 0.07929350512641654, -0.32624874481029503, -0.0142049929098125, 0.2297558494858292, -0.008066314541233273... |
710.2106 | Large nearly regular induced subgraphs | For a real c \geq 1 and an integer n, let f(n,c) denote the maximum integer f
so that every graph on n vertices contains an induced subgraph on at least f
vertices in which the maximum degree is at most c times the minimum degree.
Thus, in particular, every graph on n vertices contains a regular induced
subgraph on a... | math.CO | for a real c geq 1 and an integer n let fnc denote the maximum integer f so that every graph on n vertices contains an induced subgraph on at least f vertices in which the maximum degree is at most c times the minimum degree thus in particular every graph on n vertices contains a regular induced subgraph on at least fn... | [['for', 'a', 'real', 'c', 'geq', '1', 'and', 'an', 'integer', 'n', 'let', 'fnc', 'denote', 'the', 'maximum', 'integer', 'f', 'so', 'that', 'every', 'graph', 'on', 'n', 'vertices', 'contains', 'an', 'induced', 'subgraph', 'on', 'at', 'least', 'f', 'vertices', 'in', 'which', 'the', 'maximum', 'degree', 'is', 'at', 'most... | [-0.22794036295237965, 0.1681436265187559, 0.04637235112528762, -0.007266466690571574, -0.023830428068269637, -0.24114648975512903, 0.05275292844052656, 0.3390743264209722, -0.2530428785940403, -0.2961331293580757, 0.07458193786779715, -0.38255850011077913, -0.0938250886046908, 0.09580491026239199, -0.06667765587622272... |
710.2107 | Whitehead moves for G-trees | We generalize the familiar notion of a Whitehead move from Culler and
Vogtmann's Outer space to the setting of deformation spaces of G-trees.
Specifically, we show that there are two moves, each of which transforms a
reduced G-tree into another reduced G-tree, that suffice to relate any two
reduced trees in the same ... | math.GR | we generalize the familiar notion of a whitehead move from culler and vogtmanns outer space to the setting of deformation spaces of gtrees specifically we show that there are two moves each of which transforms a reduced gtree into another reduced gtree that suffice to relate any two reduced trees in the same deformatio... | [['we', 'generalize', 'the', 'familiar', 'notion', 'of', 'a', 'whitehead', 'move', 'from', 'culler', 'and', 'vogtmanns', 'outer', 'space', 'to', 'the', 'setting', 'of', 'deformation', 'spaces', 'of', 'gtrees', 'specifically', 'we', 'show', 'that', 'there', 'are', 'two', 'moves', 'each', 'of', 'which', 'transforms', 'a'... | [-0.11406067431111026, 0.16444233226601357, -0.1083837601436693, 0.05513641407661554, -0.07506337106503823, -0.1173822505020157, 0.03151400132035768, 0.3628403289404548, -0.31642709941499764, -0.26039387722626145, 0.07564495561678929, -0.24366544690672998, -0.15984216999308562, 0.19111472268784305, -0.11782243047599439... |
710.2108 | On the isomorphism problem for generalized Baumslag-Solitar groups | Generalized Baumslag-Solitar groups (GBS groups) are groups that act on trees
with infinite cyclic edge and vertex stabilizers. Such an action is described
by a labeled graph (essentially, the quotient graph of groups). This paper
addresses the problem of determining whether two given labeled graphs define
isomorphic... | math.GR | generalized baumslagsolitar groups gbs groups are groups that act on trees with infinite cyclic edge and vertex stabilizers such an action is described by a labeled graph essentially the quotient graph of groups this paper addresses the problem of determining whether two given labeled graphs define isomorphic groups th... | [['generalized', 'baumslagsolitar', 'groups', 'gbs', 'groups', 'are', 'groups', 'that', 'act', 'on', 'trees', 'with', 'infinite', 'cyclic', 'edge', 'and', 'vertex', 'stabilizers', 'such', 'an', 'action', 'is', 'described', 'by', 'a', 'labeled', 'graph', 'essentially', 'the', 'quotient', 'graph', 'of', 'groups', 'this',... | [-0.16279272174733317, 0.13581815662977392, -0.017914954226655073, 0.06496056587520875, -0.11150531672562163, -0.1470839918201041, 0.026628689927996226, 0.4444381272436207, -0.3594448801386767, -0.32355046142529476, 0.1481183517214834, -0.2622519744814843, -0.16632410634356815, 0.20356776667997623, -0.1442085059825331,... |
710.2109 | A new proof of the Erd\H{o}s-Ko-Rado theorem for intersecting families
of permutations | Let S(n) be the symmetric group on n points. A subset S of S(n) is
intersecting if for any pair of permutations \pi, \sigma in S there is a point
i in {1,...,n} such that \pi(i)=\sigma(i). Deza and Frankl \cite{MR0439648}
proved that if S a subset of S(n) is intersecting then |S| \leq (n-1)!.
Further, Cameron and Ku ... | math.CO | let sn be the symmetric group on n points a subset s of sn is intersecting if for any pair of permutations pi sigma in s there is a point i in 1n such that piisigmai deza and frankl citemr0439648 proved that if s a subset of sn is intersecting then s leq n1 further cameron and ku citemr2009400 show that the only sets t... | [['let', 'sn', 'be', 'the', 'symmetric', 'group', 'on', 'n', 'points', 'a', 'subset', 's', 'of', 'sn', 'is', 'intersecting', 'if', 'for', 'any', 'pair', 'of', 'permutations', 'pi', 'sigma', 'in', 's', 'there', 'is', 'a', 'point', 'i', 'in', '1n', 'such', 'that', 'piisigmai', 'deza', 'and', 'frankl', 'citemr0439648', 'p... | [-0.171511758482833, 0.14044733697698378, -0.06828574722782633, 0.00832343275990637, -0.022832255620487976, -0.20164731694064264, 0.10993184085169957, 0.32853195906199256, -0.2474111660287298, -0.19065753013516465, 0.06575099995557818, -0.33501557521950237, -0.11388175099841907, 0.14678438837056573, -0.0978534527219318... |
710.211 | Stability and Adsorption Properties of Electrostatic Complexes : Design
of Hybrid Nanostructures for Coating Applications | We report the presence of a correlation between the bulk and interfacial
properties of electrostatic coacervate complexes. Complexes were obtained by
co-assembly between cationic-neutral diblocks and oppositely charged surfactant
micelles or 7 nm cerium oxide nanoparticles. Light scattering and reflectometry
measurem... | cond-mat.soft cond-mat.mtrl-sci | we report the presence of a correlation between the bulk and interfacial properties of electrostatic coacervate complexes complexes were obtained by coassembly between cationicneutral diblocks and oppositely charged surfactant micelles or 7 nm cerium oxide nanoparticles light scattering and reflectometry measurements r... | [['we', 'report', 'the', 'presence', 'of', 'a', 'correlation', 'between', 'the', 'bulk', 'and', 'interfacial', 'properties', 'of', 'electrostatic', 'coacervate', 'complexes', 'complexes', 'were', 'obtained', 'by', 'coassembly', 'between', 'cationicneutral', 'diblocks', 'and', 'oppositely', 'charged', 'surfactant', 'mic... | [-0.1234953915966047, 0.22138976549689213, -0.07005381661102823, 0.004752946469006533, 0.06064025509049711, -0.15499014280857923, 0.05403768285886263, 0.4538972130774156, -0.23530532439927693, -0.31736104004085064, 0.030811999300646636, -0.3672074625349563, -0.11479619580432368, 0.13178917772703522, 0.04056992341318856... |
710.2111 | R-Hadron and long lived particle searches at the LHC | If long lived charged particles exist, and produced at the LHC, they may
travel with velocity significantly slower than the speed of light. This unique
signature was not considered during the design of the LHC experiments, ATLAS
and CMS. As a result, hardware and trigger capabilities need to be evaluated.
Model indep... | hep-ex | if long lived charged particles exist and produced at the lhc they may travel with velocity significantly slower than the speed of light this unique signature was not considered during the design of the lhc experiments atlas and cms as a result hardware and trigger capabilities need to be evaluated model independent ap... | [['if', 'long', 'lived', 'charged', 'particles', 'exist', 'and', 'produced', 'at', 'the', 'lhc', 'they', 'may', 'travel', 'with', 'velocity', 'significantly', 'slower', 'than', 'the', 'speed', 'of', 'light', 'this', 'unique', 'signature', 'was', 'not', 'considered', 'during', 'the', 'design', 'of', 'the', 'lhc', 'exper... | [-0.04931363949146946, 0.20473890670553874, -0.09275641419946123, 0.08025072150746403, -0.04942479862596925, -0.21312903579082768, -0.051859503156924974, 0.3881068123888423, -0.19901691183789086, -0.35590677285382083, 0.1344209181021309, -0.2817798515938166, -0.028136257870026816, 0.23983422386502662, -0.00635833642623... |
710.2112 | Ab initio calculations of BaTiO3 and PbTiO3 (001) and (011) surface
structure | We present and discuss the results of calculations of surface relaxations and
rumplings for the (001) and (011) surfaces of BaTiO3 and PbTiO3, using a hybrid
B3PW description of exchange and correlation. On the (001) surfaces, we
consider both AO (A = Ba or Pb) and TiO2 terminations. In the former case, the
surface A... | cond-mat.mtrl-sci | we present and discuss the results of calculations of surface relaxations and rumplings for the 001 and 011 surfaces of batio3 and pbtio3 using a hybrid b3pw description of exchange and correlation on the 001 surfaces we consider both ao a ba or pb and tio2 terminations in the former case the surface ao layer is found ... | [['we', 'present', 'and', 'discuss', 'the', 'results', 'of', 'calculations', 'of', 'surface', 'relaxations', 'and', 'rumplings', 'for', 'the', '001', 'and', '011', 'surfaces', 'of', 'batio3', 'and', 'pbtio3', 'using', 'a', 'hybrid', 'b3pw', 'description', 'of', 'exchange', 'and', 'correlation', 'on', 'the', '001', 'sur... | [-0.08585381180605979, 0.15117071004357874, 0.011982858124799255, 0.04110620181381819, 0.020562422807039373, -0.13940512129820176, 0.0797608103071227, 0.4318536045310762, -0.23872609131423564, -0.3188542602362978, 0.0640371381310176, -0.33588766981847584, -0.08681260226274326, 0.20339622144920527, 0.0036153827195762305... |
710.2113 | Periodic automorphisms of Takiff algebras, contractions, and
$\theta$-groups | Let $q$ be an algebraic Lie algebra and $q<m>$ a (generalised) Takiff
algebra. Any finite order automorphism $\theta$ of $q$ induces an automorphisms
of $q<m>$ of the same order, denoted $\Theta$. We study invariant-theoretic
properties of representations of the fixed point subalgebra of $\Theta$ on
other eigenspaces... | math.RT math.AG | let q be an algebraic lie algebra and qm a generalised takiff algebra any finite order automorphism theta of q induces an automorphisms of qm of the same order denoted theta we study invarianttheoretic properties of representations of the fixed point subalgebra of theta on other eigenspaces of theta in qm | [['let', 'q', 'be', 'an', 'algebraic', 'lie', 'algebra', 'and', 'qm', 'a', 'generalised', 'takiff', 'algebra', 'any', 'finite', 'order', 'automorphism', 'theta', 'of', 'q', 'induces', 'an', 'automorphisms', 'of', 'qm', 'of', 'the', 'same', 'order', 'denoted', 'theta', 'we', 'study', 'invarianttheoretic', 'properties', ... | [-0.26397538838871554, 0.11588875946244133, -0.11089936318789043, -0.026213974180613078, -0.14630813929982775, -0.1157670084149668, -0.03171474809813149, 0.28756754582419114, -0.38957964070141315, -0.19179534634538725, 0.043084690637210855, -0.2698079286252751, -0.12448571090285174, 0.11764469339201848, -0.105410002372... |
710.2114 | Birth rates of SGRs and AXPs: delayed amplification of magnetic field | We present new determination of the birth rate of AXPs and SGRS and their
associated SNRs. We find a high birth rate of 1/(500 yr) for AXPs/SGRs and
1/(1700 yr) for associated SNRs. These high rates suggest that all massive
stars (greater than ~ 25 M_sun) give rise to remnants with magnetar-like
fields. Recent observ... | astro-ph | we present new determination of the birth rate of axps and sgrs and their associated snrs we find a high birth rate of 1500 yr for axpssgrs and 11700 yr for associated snrs these high rates suggest that all massive stars greater than 25 m_sun give rise to remnants with magnetarlike fields recent observations indicate t... | [['we', 'present', 'new', 'determination', 'of', 'the', 'birth', 'rate', 'of', 'axps', 'and', 'sgrs', 'and', 'their', 'associated', 'snrs', 'we', 'find', 'a', 'high', 'birth', 'rate', 'of', '1500', 'yr', 'for', 'axpssgrs', 'and', '11700', 'yr', 'for', 'associated', 'snrs', 'these', 'high', 'rates', 'suggest', 'that', '... | [-0.12731962940100325, 0.23782937885811611, 0.0013855004029475755, 0.13749934381155315, -0.12643962818261537, -0.06226558948039823, 0.09074766550759744, 0.38725666589572194, -0.17960171739900518, -0.35826728658993606, 0.08428347275898972, -0.25231876315676277, -0.028199399283852844, 0.2531895832699486, -0.0396502989616... |
710.2115 | Formaldehyde Densitometry of Starburst Galaxies | With a goal toward deriving the physical conditions in external galaxies, we
present a survey of the formaldehyde emission in a sample of starburst systems.
By extending a technique used to derive the spatial density in star formation
regions in our own Galaxy, we show how the relative intensity of the
1(10)-1(11) an... | astro-ph | with a goal toward deriving the physical conditions in external galaxies we present a survey of the formaldehyde emission in a sample of starburst systems by extending a technique used to derive the spatial density in star formation regions in our own galaxy we show how the relative intensity of the 110111 and 211212 k... | [['with', 'a', 'goal', 'toward', 'deriving', 'the', 'physical', 'conditions', 'in', 'external', 'galaxies', 'we', 'present', 'a', 'survey', 'of', 'the', 'formaldehyde', 'emission', 'in', 'a', 'sample', 'of', 'starburst', 'systems', 'by', 'extending', 'a', 'technique', 'used', 'to', 'derive', 'the', 'spatial', 'density'... | [-0.0305103957477069, 0.07425189914173706, -0.06832335150778987, 0.08870026357959263, -0.014746570077096654, -0.039570065498958494, 0.03367572122600016, 0.4739702892857929, -0.1058804992120713, -0.3192329951973502, 0.03683775177355422, -0.2592426970341178, -0.04318443420586761, 0.1577531044761282, -0.009177860952264002... |
710.2116 | Atom detection and photon production in a scalable, open, optical
microcavity | A microfabricated Fabry-Perot optical resonator has been used for atom
detection and photon production with less than 1 atom on average in the cavity
mode. Our cavity design combines the intrinsic scalability of microfabrication
processes with direct coupling of the cavity field to single-mode optical
waveguides or f... | quant-ph | a microfabricated fabryperot optical resonator has been used for atom detection and photon production with less than 1 atom on average in the cavity mode our cavity design combines the intrinsic scalability of microfabrication processes with direct coupling of the cavity field to singlemode optical waveguides or fibers... | [['a', 'microfabricated', 'fabryperot', 'optical', 'resonator', 'has', 'been', 'used', 'for', 'atom', 'detection', 'and', 'photon', 'production', 'with', 'less', 'than', '1', 'atom', 'on', 'average', 'in', 'the', 'cavity', 'mode', 'our', 'cavity', 'design', 'combines', 'the', 'intrinsic', 'scalability', 'of', 'microfab... | [-0.12422110346226913, 0.15081514607565782, -0.03932813214867011, -0.09047192597012643, -0.005619645588423895, -0.20608757219641752, 0.01917727109976113, 0.490527639861988, -0.22110413962813175, -0.2573009314096492, 0.03148163059908573, -0.3025999734097201, -0.039365529213303135, 0.26680673162614843, -0.011022758581526... |
710.2117 | Gravitation in 4D Euclidean Space-Time Geometry | The Euclidean interpretation of special relativity which has been suggested
by the author is a formulation of special relativity in ordinary 4D Euclidean
space-time geometry. The natural and geometrically intuitive generalization of
this view involves variations of the speed of light (depending on location and
direct... | physics.gen-ph | the euclidean interpretation of special relativity which has been suggested by the author is a formulation of special relativity in ordinary 4d euclidean spacetime geometry the natural and geometrically intuitive generalization of this view involves variations of the speed of light depending on location and direction a... | [['the', 'euclidean', 'interpretation', 'of', 'special', 'relativity', 'which', 'has', 'been', 'suggested', 'by', 'the', 'author', 'is', 'a', 'formulation', 'of', 'special', 'relativity', 'in', 'ordinary', '4d', 'euclidean', 'spacetime', 'geometry', 'the', 'natural', 'and', 'geometrically', 'intuitive', 'generalization... | [-0.09051676728931553, 0.06604782710568903, -0.14811193639320414, 0.08620854820749098, -0.1216717960292494, -0.11593309472632277, -0.01285574331004582, 0.2848533526277886, -0.2365629175104774, -0.31062840400161323, 0.06693382094650027, -0.20562459078648096, -0.2146201151996278, 0.16872829427574199, -0.1565177480198934,... |
710.2118 | Tri-bimaximal Neutrino Mixing and CKM Matrix in a SU(5)x(d)T Model | In this talk, we present a model based on SU(5)x(d)T which successfully gives
rise to near tri-bimaximal leptonic mixing as well as realistic CKM matrix
elements for the quarks. The Georgi-Jarlskog relations for three generations
are also obtained. Due to the (d)T transformation property of the matter
fields, the b-q... | hep-ph | in this talk we present a model based on su5xdt which successfully gives rise to near tribimaximal leptonic mixing as well as realistic ckm matrix elements for the quarks the georgijarlskog relations for three generations are also obtained due to the dt transformation property of the matter fields the bquark mass can b... | [['in', 'this', 'talk', 'we', 'present', 'a', 'model', 'based', 'on', 'su5xdt', 'which', 'successfully', 'gives', 'rise', 'to', 'near', 'tribimaximal', 'leptonic', 'mixing', 'as', 'well', 'as', 'realistic', 'ckm', 'matrix', 'elements', 'for', 'the', 'quarks', 'the', 'georgijarlskog', 'relations', 'for', 'three', 'gener... | [-0.07981776106423019, 0.22537524512712528, -0.04854613496116488, 0.1186025853224753, -0.0688168952644274, -0.1295289122364232, 0.08280128742870245, 0.3200187618089085, -0.24792423553362086, -0.33119241644099756, 0.0781548524663211, -0.2882870791077211, -0.06864948894929242, 0.14243194571494855, 0.01743153411190252, 0.... |
710.2119 | On quantum vs. classical probability | Quantum theory shares with classical probability theory many important
properties. I show that this common core regards at least the following six
areas, and I provide details on each of these: the logic of propositions,
symmetry, probabilities, composition of systems, state preparation and
reductionism. The essentia... | quant-ph | quantum theory shares with classical probability theory many important properties i show that this common core regards at least the following six areas and i provide details on each of these the logic of propositions symmetry probabilities composition of systems state preparation and reductionism the essential distinct... | [['quantum', 'theory', 'shares', 'with', 'classical', 'probability', 'theory', 'many', 'important', 'properties', 'i', 'show', 'that', 'this', 'common', 'core', 'regards', 'at', 'least', 'the', 'following', 'six', 'areas', 'and', 'i', 'provide', 'details', 'on', 'each', 'of', 'these', 'the', 'logic', 'of', 'proposition... | [-0.07096546792430065, 0.11375439011802276, -0.08610981369565707, 0.11503795024812764, -0.04739422269631177, -0.20729760293215804, 0.036593254622857785, 0.3349043720615252, -0.27831294864881784, -0.25504127983003855, 0.08290993904665811, -0.28141080141843605, -0.175882968508328, 0.18544803680561017, -0.0949860917874805... |
710.212 | A Note on the a-numbers and p-ranks of Kummer Covers | We study the a-numbers and p-ranks of Kummer covers of the projective line,
and we give bounds for these numbers.
| math.AG | we study the anumbers and pranks of kummer covers of the projective line and we give bounds for these numbers | [['we', 'study', 'the', 'anumbers', 'and', 'pranks', 'of', 'kummer', 'covers', 'of', 'the', 'projective', 'line', 'and', 'we', 'give', 'bounds', 'for', 'these', 'numbers']] | [-0.2126559130847454, 0.048510970920324324, -0.051691836304962636, 0.08684643357992172, -0.040854363422840836, -0.09254176612012088, 0.05663133100606501, 0.34072918388992546, -0.21064590476453304, -0.26809715330600736, 0.10726564932847396, -0.2320603467989713, -0.11720641748979688, 0.3018011625856161, -0.10626009255647... |
710.2121 | Micromaser line broadening without photon exchange | We perform a calculation of the linewidth of a micromaser, using the master
equation and the quantum regression approach. A `dephasing' contribution is
identified from pumping processes that conserve the photon number and do not
appear in the photon statistics. We work out examples for a single-atom maser
with a prec... | quant-ph | we perform a calculation of the linewidth of a micromaser using the master equation and the quantum regression approach a dephasing contribution is identified from pumping processes that conserve the photon number and do not appear in the photon statistics we work out examples for a singleatom maser with a precisely co... | [['we', 'perform', 'a', 'calculation', 'of', 'the', 'linewidth', 'of', 'a', 'micromaser', 'using', 'the', 'master', 'equation', 'and', 'the', 'quantum', 'regression', 'approach', 'a', 'dephasing', 'contribution', 'is', 'identified', 'from', 'pumping', 'processes', 'that', 'conserve', 'the', 'photon', 'number', 'and', '... | [-0.10715174751186912, 0.12313141526696696, -0.10783263526602903, 0.06968142328101253, -0.03079267527209595, -0.14633094583405182, 0.0746698917963923, 0.3686200911179185, -0.23905484916229564, -0.26417567803450354, 0.044278973176419226, -0.2592059512072327, -0.11225272832565349, 0.21940467482438014, -0.0044454845747995... |
710.2122 | The Hawking temperature of expanding cosmological black holes | In the context of a debate on the correct expression of the Hawking
temperature of an expanding cosmological black hole, we show that the correct
expression in terms of the Hawking-Hayward quasi-local energy m of the hole is
T=1/(8\pi m(t)). This expression holds for comoving black holes and agrees with
a recent prop... | gr-qc | in the context of a debate on the correct expression of the hawking temperature of an expanding cosmological black hole we show that the correct expression in terms of the hawkinghayward quasilocal energy m of the hole is t18pi mt this expression holds for comoving black holes and agrees with a recent proposal by saida... | [['in', 'the', 'context', 'of', 'a', 'debate', 'on', 'the', 'correct', 'expression', 'of', 'the', 'hawking', 'temperature', 'of', 'an', 'expanding', 'cosmological', 'black', 'hole', 'we', 'show', 'that', 'the', 'correct', 'expression', 'in', 'terms', 'of', 'the', 'hawkinghayward', 'quasilocal', 'energy', 'm', 'of', 'th... | [-0.17608045557114696, 0.06606293826631113, -0.07697687267292556, 0.11921674011474741, -0.017460065611105944, -0.0845445939506005, 0.029883925004729202, 0.26191802063424674, -0.07605520376403417, -0.3131164679569857, 0.029792248641440113, -0.2895436932864998, -0.10457649071966964, 0.23645386578365496, -0.10151091637089... |
710.2123 | Are There Infinitely Many Primes? | This paper is based on a talk given to motivated high school (and younger)
students at a BAMA (Bay Area Math Adventure) event. Some of the methods used to
study primes and twin primes are introduced.
| math.NT | this paper is based on a talk given to motivated high school and younger students at a bama bay area math adventure event some of the methods used to study primes and twin primes are introduced | [['this', 'paper', 'is', 'based', 'on', 'a', 'talk', 'given', 'to', 'motivated', 'high', 'school', 'and', 'younger', 'students', 'at', 'a', 'bama', 'bay', 'area', 'math', 'adventure', 'event', 'some', 'of', 'the', 'methods', 'used', 'to', 'study', 'primes', 'and', 'twin', 'primes', 'are', 'introduced']] | [-0.06192558729607198, 0.10061406390741467, -0.14180622168350965, 0.12934065594648322, -0.1325118826288316, -0.13778891934392354, 0.056360296804794215, 0.3083451787630717, -0.1750909744037522, -0.37530309706926346, 0.08120729021094222, -0.31105805754972, -0.140703945627643, 0.22560461574337548, -0.24898244600950015, 0.... |
710.2124 | The Singular Locus of the Theta Divisor and Quadrics through a Canonical
Curve | A section K on a genus g canonical curve C is identified as the key tool to
prove new results on the geometry of the singular locus Theta_s of the theta
divisor. The K divisor is characterized by the condition of linear dependence
of a set of quadrics containing C and naturally associated to a degree g
effective divi... | math.AG hep-th math.CO | a section k on a genus g canonical curve c is identified as the key tool to prove new results on the geometry of the singular locus theta_s of the theta divisor the k divisor is characterized by the condition of linear dependence of a set of quadrics containing c and naturally associated to a degree g effective divisor... | [['a', 'section', 'k', 'on', 'a', 'genus', 'g', 'canonical', 'curve', 'c', 'is', 'identified', 'as', 'the', 'key', 'tool', 'to', 'prove', 'new', 'results', 'on', 'the', 'geometry', 'of', 'the', 'singular', 'locus', 'theta_s', 'of', 'the', 'theta', 'divisor', 'the', 'k', 'divisor', 'is', 'characterized', 'by', 'the', 'c... | [-0.19579912482796813, 0.03921793956509261, -0.08087953217596154, 0.0776224238249072, -0.0906147973439694, -0.10747192774679724, 0.03058204721239191, 0.2755310165599307, -0.2973763623740524, -0.23333123614595128, 0.06228505111452309, -0.22817599320522985, -0.19327916175399612, 0.24287876347842963, -0.11217984773797869,... |
710.2125 | Chasing Lambda | Recent astronomical observations of SNIa, CMB, as well as BAO in the Sloan
Digital Sky Survey, suggest that the current Universe has entered a stage of an
accelerated expansion with the transition redshift at $z \simeq 0.5$. While the
simplest candidates to explain this fact is cosmological constant/vacuum
energy, th... | astro-ph | recent astronomical observations of snia cmb as well as bao in the sloan digital sky survey suggest that the current universe has entered a stage of an accelerated expansion with the transition redshift at z simeq 05 while the simplest candidates to explain this fact is cosmological constantvacuum energy there exists a... | [['recent', 'astronomical', 'observations', 'of', 'snia', 'cmb', 'as', 'well', 'as', 'bao', 'in', 'the', 'sloan', 'digital', 'sky', 'survey', 'suggest', 'that', 'the', 'current', 'universe', 'has', 'entered', 'a', 'stage', 'of', 'an', 'accelerated', 'expansion', 'with', 'the', 'transition', 'redshift', 'at', 'z', 'sime... | [-0.07952930013153205, 0.049083775749102346, -0.08992514351051148, 0.08807976476844936, -0.11488371337955333, -0.09390534388143824, 0.04170991369357256, 0.3278373881268685, -0.24894957839230664, -0.3276185510386649, 0.06866040664776037, -0.2815600292221324, -0.07080451402596313, 0.20527232890750907, -0.0327641317582599... |
710.2126 | Masses, Luminosities, and Orbital Coplanarities of the mu Orionis
Quadruple Star System from PHASES Differential Astrometry | mu Orionis was identified by spectroscopic studies as a quadruple star
system. Seventeen high precision differential astrometry measurements of mu Ori
have been collected by the Palomar High-precision Astrometric Search for
Exoplanet Systems (PHASES). These show both the motion of the long period
binary orbit and sho... | astro-ph | mu orionis was identified by spectroscopic studies as a quadruple star system seventeen high precision differential astrometry measurements of mu ori have been collected by the palomar highprecision astrometric search for exoplanet systems phases these show both the motion of the long period binary orbit and short peri... | [['mu', 'orionis', 'was', 'identified', 'by', 'spectroscopic', 'studies', 'as', 'a', 'quadruple', 'star', 'system', 'seventeen', 'high', 'precision', 'differential', 'astrometry', 'measurements', 'of', 'mu', 'ori', 'have', 'been', 'collected', 'by', 'the', 'palomar', 'highprecision', 'astrometric', 'search', 'for', 'ex... | [-0.18895209602643875, 0.13043855258829237, -0.06222885455576455, 0.012223446106662086, -0.04105474265460165, -0.10051491071396136, 0.058375257181299475, 0.37034425626672773, -0.2376606505376171, -0.36255042278307764, 0.10202667684006493, -0.29573193069771253, -0.03393702503781398, 0.21174229142983553, -0.0325767567057... |
710.2127 | The orbits of the quadruple star system 88 Tau A from PHASES
differential astrometry and radial velocity | We have used high precision differential astrometry from the Palomar
High-precision Astrometric Search for Exoplanet Systems (PHASES) project and
radial velocity measurements covering a time-span of 20 years to determine the
orbital parameters of the 88 Tau A system. 88 Tau is a complex hierarchical
multiple system c... | astro-ph | we have used high precision differential astrometry from the palomar highprecision astrometric search for exoplanet systems phases project and radial velocity measurements covering a timespan of 20 years to determine the orbital parameters of the 88 tau a system 88 tau is a complex hierarchical multiple system comprisi... | [['we', 'have', 'used', 'high', 'precision', 'differential', 'astrometry', 'from', 'the', 'palomar', 'highprecision', 'astrometric', 'search', 'for', 'exoplanet', 'systems', 'phases', 'project', 'and', 'radial', 'velocity', 'measurements', 'covering', 'a', 'timespan', 'of', '20', 'years', 'to', 'determine', 'the', 'orb... | [-0.18835960571877947, 0.09316087900870751, -0.06590039220949014, 0.0064579717239162835, -0.06423163199219709, -0.07717773034201228, 0.06740840664313918, 0.33551485757812743, -0.20725722779888053, -0.3770810028812451, 0.09222044159799035, -0.31514830184133014, -0.03387590375766808, 0.22134698973968625, -0.0198459960700... |
710.2128 | Interferometric Observations of V1663 Aquilae (Nova Aql 2005) | We have resolved the classical nova V1663 Aql using long-baseline near-IR
interferometry covering the period from 5--18 days after peak brightness. We
directly measure the shape and size of the fireball, which we find to be
asymmetric. In addition we measure an apparent expansion rate of 0.21 +/- 0.03
mas/day. Assumi... | astro-ph | we have resolved the classical nova v1663 aql using longbaseline nearir interferometry covering the period from 518 days after peak brightness we directly measure the shape and size of the fireball which we find to be asymmetric in addition we measure an apparent expansion rate of 021 003 masday assuming a linear expan... | [['we', 'have', 'resolved', 'the', 'classical', 'nova', 'v1663', 'aql', 'using', 'longbaseline', 'nearir', 'interferometry', 'covering', 'the', 'period', 'from', '518', 'days', 'after', 'peak', 'brightness', 'we', 'directly', 'measure', 'the', 'shape', 'and', 'size', 'of', 'the', 'fireball', 'which', 'we', 'find', 'to'... | [-0.052215798116555814, 0.10122228718096575, -0.142698019661588, 0.04165998950105576, -0.06923660998983146, -0.10875508808123979, 0.09161044428468619, 0.4383565291256002, -0.23232455049795145, -0.32509458585398143, 0.1082040515674043, -0.3089379667602841, 0.021478745145994484, 0.1971187267336063, -0.05576394587411609, ... |
710.2129 | Partition Functions of Three-Dimensional Pure Gravity | The three-dimensional pure quantum gravity with a negative cosmological
constant has been conjectured to be dual to an extremal conformal field theory
(ECFT), of central charge c=24k for some positive integer k. We compute the
partition function of the dual ECFT by summing over gravitational instanton
contributions. ... | hep-th | the threedimensional pure quantum gravity with a negative cosmological constant has been conjectured to be dual to an extremal conformal field theory ecft of central charge c24k for some positive integer k we compute the partition function of the dual ecft by summing over gravitational instanton contributions in partic... | [['the', 'threedimensional', 'pure', 'quantum', 'gravity', 'with', 'a', 'negative', 'cosmological', 'constant', 'has', 'been', 'conjectured', 'to', 'be', 'dual', 'to', 'an', 'extremal', 'conformal', 'field', 'theory', 'ecft', 'of', 'central', 'charge', 'c24k', 'for', 'some', 'positive', 'integer', 'k', 'we', 'compute',... | [-0.1491828319835074, 0.12091853015195222, -0.08414792348228303, 0.06261519328863532, -0.04783699819013292, -0.13747554377618212, -0.02482446069099055, 0.28131462323168915, -0.21426546190474413, -0.26313737717767555, 0.028199437692370495, -0.30325047075633466, -0.1560937279122479, 0.16982156475201066, -0.00607303471338... |
710.213 | Externally Dispersed Interferometry for Precision Radial Velocimetry | Externally Dispersed Interferometry (EDI) is the series combination of a
fixed-delay field-widened Michelson interferometer with a dispersive
spectrograph. This combination boosts the spectrograph performance for both
Doppler velocimetry and high resolution spectroscopy. The interferometer
creates a periodic spectral... | astro-ph | externally dispersed interferometry edi is the series combination of a fixeddelay fieldwidened michelson interferometer with a dispersive spectrograph this combination boosts the spectrograph performance for both doppler velocimetry and high resolution spectroscopy the interferometer creates a periodic spectral comb th... | [['externally', 'dispersed', 'interferometry', 'edi', 'is', 'the', 'series', 'combination', 'of', 'a', 'fixeddelay', 'fieldwidened', 'michelson', 'interferometer', 'with', 'a', 'dispersive', 'spectrograph', 'this', 'combination', 'boosts', 'the', 'spectrograph', 'performance', 'for', 'both', 'doppler', 'velocimetry', '... | [-0.14760434022735797, 0.16936185585820124, -0.1502112661676184, 0.026581640338658223, -0.1327272395509444, -0.1894426487949716, -0.002146894235492629, 0.4763071754900347, -0.2711355732206036, -0.34174666478603827, 0.07836467494988548, -0.2571528765605029, -0.08897026640777829, 0.22182126687213527, -0.09427757790906965... |
710.2131 | Spontaneously Broken Gauge Symmetry in SUSY Yang-Mills Theories with
Matter | The analysis of spontaneous gauge symmetry breaking of N=1 supersymmetric
SU(N_c) Yang-Mills theory with matter is performed. The supersymmetric
$R_\xi$-gauge is used and its non-local effects investigated. Superpropagators
and vertices are computed, and it is shown that the non-local terms introduced
by the $R_\xi$-... | hep-th | the analysis of spontaneous gauge symmetry breaking of n1 supersymmetric sun_c yangmills theory with matter is performed the supersymmetric r_xigauge is used and its nonlocal effects investigated superpropagators and vertices are computed and it is shown that the nonlocal terms introduced by the r_xigaugefixing are wel... | [['the', 'analysis', 'of', 'spontaneous', 'gauge', 'symmetry', 'breaking', 'of', 'n1', 'supersymmetric', 'sun_c', 'yangmills', 'theory', 'with', 'matter', 'is', 'performed', 'the', 'supersymmetric', 'r_xigauge', 'is', 'used', 'and', 'its', 'nonlocal', 'effects', 'investigated', 'superpropagators', 'and', 'vertices', 'a... | [-0.11067146300920286, 0.22184084605736037, -0.06701658621896059, 0.14140989314570712, -0.0666820694381992, -0.16699278990272431, -0.08675986707094126, 0.34808619708443683, -0.14858325604194153, -0.2517655641771853, 0.056189341693728544, -0.28228735650579134, -0.19817700342585642, 0.05638678741330902, -0.01628429636669... |
710.2132 | TEDI: the TripleSpec Exoplanet Discovery Instrument | The TEDI (TripleSpec - Exoplanet Discovery Instrument) will be the first
instrument fielded specifically for finding low-mass stellar companions. The
instrument is a near infra-red interferometric spectrometer used as a radial
velocimeter. TEDI joins Externally Dispersed Interferometery (EDI) with an
efficient, mediu... | astro-ph | the tedi triplespec exoplanet discovery instrument will be the first instrument fielded specifically for finding lowmass stellar companions the instrument is a near infrared interferometric spectrometer used as a radial velocimeter tedi joins externally dispersed interferometery edi with an efficient mediumresolution n... | [['the', 'tedi', 'triplespec', 'exoplanet', 'discovery', 'instrument', 'will', 'be', 'the', 'first', 'instrument', 'fielded', 'specifically', 'for', 'finding', 'lowmass', 'stellar', 'companions', 'the', 'instrument', 'is', 'a', 'near', 'infrared', 'interferometric', 'spectrometer', 'used', 'as', 'a', 'radial', 'velocim... | [-0.06189640798017054, 0.15582202918170984, -0.17707953636315377, 0.019409037778934685, -0.17731525022399558, -0.13292908773291856, -0.003619206709759858, 0.4622009079903364, -0.12058109560765683, -0.40212897448252666, 0.12667533965534805, -0.32142209606793, -0.014397869050941047, 0.265672151105451, -0.0663482271270100... |
710.2133 | Resolving the Outer Disks and Halos of Nearby Galaxies | In a hierarchical merging scenario, the outer parts of a galaxy are a fossil
record of the galaxy's early history. Observations of the outer disks and halos
of galaxies thus provide a tool to study individual galaxy histories and test
formation theories. Locally, an impressive effort has been made to understand
the h... | astro-ph | in a hierarchical merging scenario the outer parts of a galaxy are a fossil record of the galaxys early history observations of the outer disks and halos of galaxies thus provide a tool to study individual galaxy histories and test formation theories locally an impressive effort has been made to understand the halo of ... | [['in', 'a', 'hierarchical', 'merging', 'scenario', 'the', 'outer', 'parts', 'of', 'a', 'galaxy', 'are', 'a', 'fossil', 'record', 'of', 'the', 'galaxys', 'early', 'history', 'observations', 'of', 'the', 'outer', 'disks', 'and', 'halos', 'of', 'galaxies', 'thus', 'provide', 'a', 'tool', 'to', 'study', 'individual', 'gal... | [-0.08496900603308209, 0.029252317172878455, -0.1466251112919833, 0.10294153079787845, -0.1703581802680024, 0.038042340853384565, 0.005257487290405802, 0.38350534832903316, -0.1352202575922482, -0.37801641703450256, 0.022957169028398183, -0.2418211686092296, -0.03885543857343562, 0.1727296774608216, -0.0274693105735683... |
710.2134 | Discrete entropies of orthogonal polynomials | Let $p_n$ be the $n$-th orthonormal polynomial on the real line, whose zeros
are $\lambda_j^{(n)}$, $j=1, ..., n$. Then for each $j=1, ..., n$, $$ \vec
\Psi_j^2 = (\Psi_{1j}^2, ..., \Psi_{nj}^2) $$ with $$ \Psi_{ij}^2= p_{i-1}^2
(\lambda_j^{(n)}) (\sum_{k=0}^{n-1} p_k^2(\lambda_j^{(n)}))^{-1}, \quad i=1,
>..., n, $$ ... | math.CA cs.IT math-ph math.IT math.MP | let p_n be the nth orthonormal polynomial on the real line whose zeros are lambda_jn j1 n then for each j1 n vec psi_j2 psi_1j2 psi_nj2 with psi_ij2 p_i12 lambda_jn sum_k0n1 p_k2lambda_jn1 quad i1 n defines a discrete probability distribution the shannon entropy of the sequence p_n is consequently defined as mathcal s_... | [['let', 'p_n', 'be', 'the', 'nth', 'orthonormal', 'polynomial', 'on', 'the', 'real', 'line', 'whose', 'zeros', 'are', 'lambda_jn', 'j1', 'n', 'then', 'for', 'each', 'j1', 'n', 'vec', 'psi_j2', 'psi_1j2', 'psi_nj2', 'with', 'psi_ij2', 'p_i12', 'lambda_jn', 'sum_k0n1', 'p_k2lambda_jn1', 'quad', 'i1', 'n', 'defines', 'a'... | [-0.20312269590314977, 0.1173518386289307, -0.011884921969673069, 0.002687417141152258, -0.027335212000684103, -0.17761319376931517, -0.019140740384866205, 0.29701975265460223, -0.28186278876076815, -0.18555005929269588, 0.06062859270275215, -0.353638925224773, -0.13486025553225472, 0.18897019629126666, -0.017484073892... |
710.2135 | IC 4406: a radio-infrared view | IC 4406 is a large (about 100'' x 30'') southern bipolar planetary nebula,
composed of two elongated lobes extending from a bright central region, where
there is evidence for the presence of a large torus of gas and dust. We show
new observations of this source performed with IRAC (Spitzer Space Telescope)
and the Au... | astro-ph | ic 4406 is a large about 100 x 30 southern bipolar planetary nebula composed of two elongated lobes extending from a bright central region where there is evidence for the presence of a large torus of gas and dust we show new observations of this source performed with irac spitzer space telescope and the australia teles... | [['ic', '4406', 'is', 'a', 'large', 'about', '100', 'x', '30', 'southern', 'bipolar', 'planetary', 'nebula', 'composed', 'of', 'two', 'elongated', 'lobes', 'extending', 'from', 'a', 'bright', 'central', 'region', 'where', 'there', 'is', 'evidence', 'for', 'the', 'presence', 'of', 'a', 'large', 'torus', 'of', 'gas', 'an... | [-0.09203888566671162, 0.0779322536943096, -0.04240086092244065, 0.06889479457112473, -0.06482170564529027, -0.038586361422425226, -0.017808343820636056, 0.4619457077767168, -0.15694209152004784, -0.2859835879108499, 0.09795853975118093, -0.2586476669964632, -0.056984302772593406, 0.18253553342739387, -0.02511882075613... |
710.2136 | Twisted equivariant K-theory for proper actions of discrete groups | We give a construction for twisted equivariant K-theory in the case of a
proper action of a discrete group using twisted bundles. Our construction uses
results of Lueck and Oliver to extend a construction of Adem and Ruan. We also
show the existence of a Chern character to twisted Bredon cohomology. This
gives a part... | math.KT | we give a construction for twisted equivariant ktheory in the case of a proper action of a discrete group using twisted bundles our construction uses results of lueck and oliver to extend a construction of adem and ruan we also show the existence of a chern character to twisted bredon cohomology this gives a partial an... | [['we', 'give', 'a', 'construction', 'for', 'twisted', 'equivariant', 'ktheory', 'in', 'the', 'case', 'of', 'a', 'proper', 'action', 'of', 'a', 'discrete', 'group', 'using', 'twisted', 'bundles', 'our', 'construction', 'uses', 'results', 'of', 'lueck', 'and', 'oliver', 'to', 'extend', 'a', 'construction', 'of', 'adem',... | [-0.22576525786968127, 0.06140502376883763, -0.14159278265417438, 0.09016197739800515, -0.14033063255531125, -0.12472110865510082, 0.03285775499494925, 0.33844995649199777, -0.2992014020222099, -0.20859827805463582, 0.09708682528524723, -0.16369487363239113, -0.18982771209964197, 0.19265693562003236, -0.228019440597663... |
710.2137 | The heat operator in infinite dimensions | Let (H,B) be an abstract Wiener space and let \mu_{s} be the Gaussian measure
on B with variance s. Let \Delta be the Laplacian (*not* the number operator),
that is, a sum of squares of derivatives associated to an orthonormal basis of
H. I will show that the heat operator \exp(t\Delta/2) is a contraction operator
fr... | math-ph math.FA math.MP | let hb be an abstract wiener space and let mu_s be the gaussian measure on b with variance s let delta be the laplacian not the number operator that is a sum of squares of derivatives associated to an orthonormal basis of h i will show that the heat operator exptdelta2 is a contraction operator from l2bmu_s to l2bmu_st... | [['let', 'hb', 'be', 'an', 'abstract', 'wiener', 'space', 'and', 'let', 'mu_s', 'be', 'the', 'gaussian', 'measure', 'on', 'b', 'with', 'variance', 's', 'let', 'delta', 'be', 'the', 'laplacian', 'not', 'the', 'number', 'operator', 'that', 'is', 'a', 'sum', 'of', 'squares', 'of', 'derivatives', 'associated', 'to', 'an', ... | [-0.10738948541240663, 0.16662391391356424, -0.09544024410554104, 0.022726882913977734, -0.11789054393043949, -0.14330405099834834, 0.009468188937494739, 0.3357284883658091, -0.30881083470562265, -0.18896956400324902, 0.11274458813584513, -0.31461280757147403, -0.08543934029488204, 0.19994527267602583, -0.0761186309081... |
710.2138 | Hysteretic Optimization For Spin Glasses | The recently proposed Hysteretic Optimization (HO) procedure is applied to
the 1D Ising spin chain with long range interactions. To study its
effectiveness, the quality of ground state energies found as a function of the
distance dependence exponent, $\sigma$, is assessed. It is found that the
transition from an infi... | cond-mat.soft | the recently proposed hysteretic optimization ho procedure is applied to the 1d ising spin chain with long range interactions to study its effectiveness the quality of ground state energies found as a function of the distance dependence exponent sigma is assessed it is found that the transition from an infiniterange to... | [['the', 'recently', 'proposed', 'hysteretic', 'optimization', 'ho', 'procedure', 'is', 'applied', 'to', 'the', '1d', 'ising', 'spin', 'chain', 'with', 'long', 'range', 'interactions', 'to', 'study', 'its', 'effectiveness', 'the', 'quality', 'of', 'ground', 'state', 'energies', 'found', 'as', 'a', 'function', 'of', 'th... | [-0.11326561259920709, 0.13774808637415326, -0.07746375533386267, 0.06947657832315599, -0.044509134938208655, -0.12908230570277998, 0.05401789236813784, 0.38842332298202176, -0.25459182317501733, -0.32438329385859627, 0.0856294215570337, -0.2737830446341208, -0.14604861765434698, 0.1614037868739771, -0.0092385866546205... |
710.2139 | Approximation algorithms and hardness for domination with propagation | The power dominating set (PDS) problem is the following extension of the
well-known dominating set problem: find a smallest-size set of nodes $S$ that
power dominates all the nodes, where a node $v$ is power dominated if (1) $v$
is in $S$ or $v$ has a neighbor in $S$, or (2) $v$ has a neighbor $w$ such that
$w$ and a... | cs.CC cs.DM | the power dominating set pds problem is the following extension of the wellknown dominating set problem find a smallestsize set of nodes s that power dominates all the nodes where a node v is power dominated if 1 v is in s or v has a neighbor in s or 2 v has a neighbor w such that w and all of its neighbors except v ar... | [['the', 'power', 'dominating', 'set', 'pds', 'problem', 'is', 'the', 'following', 'extension', 'of', 'the', 'wellknown', 'dominating', 'set', 'problem', 'find', 'a', 'smallestsize', 'set', 'of', 'nodes', 's', 'that', 'power', 'dominates', 'all', 'the', 'nodes', 'where', 'a', 'node', 'v', 'is', 'power', 'dominated', 'i... | [-0.15174922236398636, 0.08126565764815767, -0.01372493849462503, 0.03464484597743767, -0.07736319260272596, -0.1518711230669219, 0.09320717217954777, 0.4161219164825879, -0.3277398346100825, -0.28599750421118814, 0.05415164456436677, -0.31940564423702755, -0.12924908525189505, 0.1365435949599298, -0.03750098025269032,... |
710.214 | Noncommutative field theories from a deformation point of view | In this review we discuss the global geometry of noncommutative field
theories from a deformation point of view: The space-times under consideration
are deformations of classical space-time manifolds using star products. Then
matter fields are encoded in deformation quantizations of vector bundles over
the classical ... | math.QA math-ph math.MP | in this review we discuss the global geometry of noncommutative field theories from a deformation point of view the spacetimes under consideration are deformations of classical spacetime manifolds using star products then matter fields are encoded in deformation quantizations of vector bundles over the classical spacet... | [['in', 'this', 'review', 'we', 'discuss', 'the', 'global', 'geometry', 'of', 'noncommutative', 'field', 'theories', 'from', 'a', 'deformation', 'point', 'of', 'view', 'the', 'spacetimes', 'under', 'consideration', 'are', 'deformations', 'of', 'classical', 'spacetime', 'manifolds', 'using', 'star', 'products', 'then', ... | [-0.21056239813413113, 0.12696886648685504, -0.12069393742880592, 0.0645611405879744, -0.08055102608281456, -0.1053706376736805, -0.07655189803814234, 0.36556167742365026, -0.2972869645446947, -0.17331951536391288, 0.10902392712408958, -0.18158403303982906, -0.22199571576632865, 0.1491991909195299, -0.14949862054255728... |
710.2141 | Intersecting Brane Models and Cosmology | We discuss the application of general features of intersecting brane model
constructions in cosmology. In particular, we describe a scenario for D-term
inflation which arises straightforwardly in IBM constructions wherein open
non-vectorlike strings play the role of the inflaton. We also show that
baryogenesis driven... | hep-th | we discuss the application of general features of intersecting brane model constructions in cosmology in particular we describe a scenario for dterm inflation which arises straightforwardly in ibm constructions wherein open nonvectorlike strings play the role of the inflaton we also show that baryogenesis driven by hid... | [['we', 'discuss', 'the', 'application', 'of', 'general', 'features', 'of', 'intersecting', 'brane', 'model', 'constructions', 'in', 'cosmology', 'in', 'particular', 'we', 'describe', 'a', 'scenario', 'for', 'dterm', 'inflation', 'which', 'arises', 'straightforwardly', 'in', 'ibm', 'constructions', 'wherein', 'open', '... | [-0.1760287497748147, 0.20113884747485844, -0.06871086490552938, 0.17436560073442625, -0.07782709428615738, -0.21656294104136659, -0.037198619631102735, 0.28513859410508813, -0.2547004051637231, -0.2750138931237815, 0.09461479066675038, -0.21530100956493825, -0.1967786845113886, 0.12625934591663904, -0.1114208069875052... |
710.2142 | Quarks in the universe | Matter in its present form was formed when our
Universe emerged from the quark-gluon phase (QGP) at about 30mus into its
evolution. To explore this early period in the laboratory, we study highly
excited matter formed in relativistic heavy ion collision experiments: heavy
nuclei crash into each other, and form comp... | nucl-th | matter in its present form was formed when our universe emerged from the quarkgluon phase qgp at about 30mus into its evolution to explore this early period in the laboratory we study highly excited matter formed in relativistic heavy ion collision experiments heavy nuclei crash into each other and form compressed and ... | [['matter', 'in', 'its', 'present', 'form', 'was', 'formed', 'when', 'our', 'universe', 'emerged', 'from', 'the', 'quarkgluon', 'phase', 'qgp', 'at', 'about', '30mus', 'into', 'its', 'evolution', 'to', 'explore', 'this', 'early', 'period', 'in', 'the', 'laboratory', 'we', 'study', 'highly', 'excited', 'matter', 'formed... | [-0.09390548369781186, 0.2830463571090859, -0.11195986268316158, 0.09397226386185048, -0.0037262273410744702, -0.12123424925095012, -0.03883968592135909, 0.32102362409643564, -0.22552026372323644, -0.2745402506073765, 0.002738174431666679, -0.2984161937596105, -0.010843479064630067, 0.11122516698884309, 0.0838073797751... |
710.2143 | Right coideal subalgebras in $U_q(\frak{sl}_{n+1}).$ | We offer a complete classification of right coideal subalgebras which contain
all group-like elements for the multiparameter version of the quantum group
$U_q(\mathfrak{sl}_{n+1})$ provided that the main parameter $q$ is not a root
of 1. As a consequence, we determine that for each subgroup $\Sigma $ of the
group $G$... | math.QA math.RA | we offer a complete classification of right coideal subalgebras which contain all grouplike elements for the multiparameter version of the quantum group u_qmathfraksl_n1 provided that the main parameter q is not a root of 1 as a consequence we determine that for each subgroup sigma of the group g of all grouplike eleme... | [['we', 'offer', 'a', 'complete', 'classification', 'of', 'right', 'coideal', 'subalgebras', 'which', 'contain', 'all', 'grouplike', 'elements', 'for', 'the', 'multiparameter', 'version', 'of', 'the', 'quantum', 'group', 'u_qmathfraksl_n1', 'provided', 'that', 'the', 'main', 'parameter', 'q', 'is', 'not', 'a', 'root', ... | [-0.17311381783656543, 0.08834577784728026, -0.03497135831639753, 0.015448766655936197, -0.1352771741730976, -0.17312106661483995, 0.0026309734194001066, 0.3370400509738829, -0.35705133847659454, -0.12444270317791961, 0.1270117299809499, -0.265505672301515, -0.08839332779825781, 0.1776749400087283, -0.15482277301271097... |
710.2144 | Convexity properties of solutions to the free Schr\"odinger equation
with Gaussian decay | We study convexity properties of solutions to the free Schrodinger equation
with Gaussian decay.
| math.AP math-ph math.MP | we study convexity properties of solutions to the free schrodinger equation with gaussian decay | [['we', 'study', 'convexity', 'properties', 'of', 'solutions', 'to', 'the', 'free', 'schrodinger', 'equation', 'with', 'gaussian', 'decay']] | [-0.08177132425563675, 0.061831396272672076, -0.14496904787873582, 0.08046799851581454, -0.14379427562068617, -0.15611308493784495, -0.06464008374937943, 0.3529075056846653, -0.33423373848199844, -0.1674661485677851, 0.07775016373489052, -0.3911445574568851, -0.09160584104912621, 0.11517775351447719, 0.0491561811151249... |
710.2145 | Are the compact star clusters in M82 evolving towards globular clusters? | Recent HST/ACS images of M82 covering the entire galaxy have been used to
detect star clusters. The galaxy is known to contain a young population (age <
10 Myr) in its starburst nucleus, surrounded by a post-starburst disk of age <
1 Gyr. We detect more than 650 star clusters in this galaxy, nearly 400 of them
in the... | astro-ph | recent hstacs images of m82 covering the entire galaxy have been used to detect star clusters the galaxy is known to contain a young population age 10 myr in its starburst nucleus surrounded by a poststarburst disk of age 1 gyr we detect more than 650 star clusters in this galaxy nearly 400 of them in the poststarburst... | [['recent', 'hstacs', 'images', 'of', 'm82', 'covering', 'the', 'entire', 'galaxy', 'have', 'been', 'used', 'to', 'detect', 'star', 'clusters', 'the', 'galaxy', 'is', 'known', 'to', 'contain', 'a', 'young', 'population', 'age', '10', 'myr', 'in', 'its', 'starburst', 'nucleus', 'surrounded', 'by', 'a', 'poststarburst', ... | [-0.005711668218316284, 0.08664567228928904, -0.10405980297538374, 0.16457497888510159, -0.09107120750498061, -0.0009414931741830345, 0.0471581863674605, 0.4910522638776592, -0.14825744834450014, -0.38172751142008005, 0.05509013958083831, -0.2834200790145426, 0.025209419699124644, 0.16951279425950042, -0.04991257078423... |
710.2146 | Electron-phonon interaction alone does not explain the photoemission
kink in cuprate superconductors | Despite over two decades of intense research efforts, the origin of
high-temperature superconductivity in the copper oxides remains elusive.
Angle-resolved photoemission experiments (ARPES) revealed a kink in the
dispersion relations (energy vs. wavevector) of electronic states in the
cuprates at binding energies of ... | cond-mat.supr-con | despite over two decades of intense research efforts the origin of hightemperature superconductivity in the copper oxides remains elusive angleresolved photoemission experiments arpes revealed a kink in the dispersion relations energy vs wavevector of electronic states in the cuprates at binding energies of 5080 mev an... | [['despite', 'over', 'two', 'decades', 'of', 'intense', 'research', 'efforts', 'the', 'origin', 'of', 'hightemperature', 'superconductivity', 'in', 'the', 'copper', 'oxides', 'remains', 'elusive', 'angleresolved', 'photoemission', 'experiments', 'arpes', 'revealed', 'a', 'kink', 'in', 'the', 'dispersion', 'relations', ... | [-0.16191130263730882, 0.20218321235617623, -0.06930288246949204, 0.0899915210402105, -0.05514910881596734, -0.1045638507953845, 0.10590296788956038, 0.39211132273077964, -0.22831537153106182, -0.29631531378254294, -0.02699977874115575, -0.37433696023887025, -0.10597622572735417, 0.18441512917517686, 0.0618217997881583... |
710.2147 | Superspecies and their representations | Superspecies are introduced to provide the nice constructions of all
finite-dimensional superalgebras. All acyclic superspecies, or equivalently all
finite-dimensional (gr-basic) gr-hereditary superalgebras, are classified
according to their graded representation types. To this end, graded
equivalence, graded represe... | math.RA math.RT | superspecies are introduced to provide the nice constructions of all finitedimensional superalgebras all acyclic superspecies or equivalently all finitedimensional grbasic grhereditary superalgebras are classified according to their graded representation types to this end graded equivalence graded representation type a... | [['superspecies', 'are', 'introduced', 'to', 'provide', 'the', 'nice', 'constructions', 'of', 'all', 'finitedimensional', 'superalgebras', 'all', 'acyclic', 'superspecies', 'or', 'equivalently', 'all', 'finitedimensional', 'grbasic', 'grhereditary', 'superalgebras', 'are', 'classified', 'according', 'to', 'their', 'gra... | [-0.13125960332002828, 0.10075343848968094, 0.016761249481615694, 0.07212334469923834, -0.24904088283338668, -0.2514350095086477, -0.1242609611151486, 0.4166699380359866, -0.4489019397561523, -0.2045674237676642, 0.10676441282372583, -0.1854173390364105, -0.14003095566824247, 0.1117681662118147, -0.21192743934013628, -... |
710.2148 | Deep inelastic scattering at strong coupling from gauge/string duality :
the saturation line | For gauge theories which admit a dual string description, we analyze deep
inelastic scattering at strong 't Hooft coupling and high energy, in the
vicinity of the unitarity limit. We discuss the onset of unitarity corrections
and determine the saturation line which separates weak scattering from strong
scattering in ... | hep-th hep-ph | for gauge theories which admit a dual string description we analyze deep inelastic scattering at strong t hooft coupling and high energy in the vicinity of the unitarity limit we discuss the onset of unitarity corrections and determine the saturation line which separates weak scattering from strong scattering in the pa... | [['for', 'gauge', 'theories', 'which', 'admit', 'a', 'dual', 'string', 'description', 'we', 'analyze', 'deep', 'inelastic', 'scattering', 'at', 'strong', 't', 'hooft', 'coupling', 'and', 'high', 'energy', 'in', 'the', 'vicinity', 'of', 'the', 'unitarity', 'limit', 'we', 'discuss', 'the', 'onset', 'of', 'unitarity', 'co... | [-0.14009780632896404, 0.28200075735874247, -0.09001105670309202, 0.14247997427204004, -0.03913928360932253, -0.09643682237065425, 0.06704956387649431, 0.33449703421105037, -0.2139174860238916, -0.2585499480218542, -0.038223487563134935, -0.30231738966099464, 0.0031159231121736493, 0.11519177926520845, 0.07676773908892... |
710.2149 | On (Co-)morphisms of Lie Pseudoalgebras and Groupoids | We give a unified description of morphisms and comorphisms of Lie
pseudoalgebras, showing that the both types of morphisms can be regarded as
subalgebras of a Lie pseudoalgebra, called the $\psi$-sum. We also provide
similar descriptions for morphisms and comorphisms of Lie algebroids and
groupoids.
| math.RA math.AC | we give a unified description of morphisms and comorphisms of lie pseudoalgebras showing that the both types of morphisms can be regarded as subalgebras of a lie pseudoalgebra called the psisum we also provide similar descriptions for morphisms and comorphisms of lie algebroids and groupoids | [['we', 'give', 'a', 'unified', 'description', 'of', 'morphisms', 'and', 'comorphisms', 'of', 'lie', 'pseudoalgebras', 'showing', 'that', 'the', 'both', 'types', 'of', 'morphisms', 'can', 'be', 'regarded', 'as', 'subalgebras', 'of', 'a', 'lie', 'pseudoalgebra', 'called', 'the', 'psisum', 'we', 'also', 'provide', 'simil... | [-0.16497338537804104, 0.011049165411598304, -0.09535234453241256, 0.15673645976295864, -0.18013244647194038, -0.1372458424884826, -0.002510813297703862, 0.4115303282371976, -0.3626006984003735, -0.21685168506916275, 0.07997135389384559, -0.17725654124197635, -0.16314877171746708, 0.2257997782223604, -0.208983805580911... |
710.215 | Effect of disorder on a graphene p-n junction | We propose the theory of transport in a gate-tunable graphene p-n junction,
in which the gradient of the carrier density is controlled by the gate voltage.
Depending on this gradient and on the density of charged impurities, the
junction resistance is dominated by either diffusive or ballistic contribution.
We find t... | cond-mat.mes-hall cond-mat.mtrl-sci | we propose the theory of transport in a gatetunable graphene pn junction in which the gradient of the carrier density is controlled by the gate voltage depending on this gradient and on the density of charged impurities the junction resistance is dominated by either diffusive or ballistic contribution we find the condi... | [['we', 'propose', 'the', 'theory', 'of', 'transport', 'in', 'a', 'gatetunable', 'graphene', 'pn', 'junction', 'in', 'which', 'the', 'gradient', 'of', 'the', 'carrier', 'density', 'is', 'controlled', 'by', 'the', 'gate', 'voltage', 'depending', 'on', 'this', 'gradient', 'and', 'on', 'the', 'density', 'of', 'charged', '... | [-0.20574747098824323, 0.1622589784831311, -0.06631478964445296, 0.021303537161759194, 0.021795633031850618, -0.1836121057767128, 0.060817806022712605, 0.38039756124692686, -0.2748844509609462, -0.2724210031205014, 0.010083473062540373, -0.301644352463524, -0.16728463835407342, 0.22877433890571003, -0.04188402594077620... |
710.2151 | Analytical investigation of magnetic field distributions around
superconducting strips on ferromagnetic substrates | The complex-field approach is developed to derive analytical expressions of
the magnetic field distributions around superconducting strips on ferromagnetic
substrates (SC/FM strips). We consider the ferromagnetic substrates as ideal
soft magnets with an infinite magnetic permeability, neglecting the
ferromagnetic hys... | cond-mat.supr-con | the complexfield approach is developed to derive analytical expressions of the magnetic field distributions around superconducting strips on ferromagnetic substrates scfm strips we consider the ferromagnetic substrates as ideal soft magnets with an infinite magnetic permeability neglecting the ferromagnetic hysteresis ... | [['the', 'complexfield', 'approach', 'is', 'developed', 'to', 'derive', 'analytical', 'expressions', 'of', 'the', 'magnetic', 'field', 'distributions', 'around', 'superconducting', 'strips', 'on', 'ferromagnetic', 'substrates', 'scfm', 'strips', 'we', 'consider', 'the', 'ferromagnetic', 'substrates', 'as', 'ideal', 'so... | [-0.22190780795794743, 0.1880220200830549, 0.02097025391651176, -0.009839130895027118, -0.0668528348953621, -0.14366721772801197, 0.05294583677668233, 0.3705257864462005, -0.18540818161843073, -0.24709039085615447, 0.07615282985365443, -0.321373842765539, -0.04536895037013275, 0.24267990818813617, 0.06147282026920533, ... |
710.2152 | Consequences of a Lambda_c/D enhancement effect on the non-photonic
electron nuclear modification factor in central heavy ion collisions at RHIC
energy | The RHIC experiments have measured the nuclear modification factor R_AA of
non-photonic electrons in Au+Au collisions at sqrt(s) = 200 GeV. This R_AA
exhibits a large suppression for pt > 2 GeV/c which is commonly attributed to
heavy-quark energy loss. It is expected that the heavy-quark radiative energy
loss is smal... | hep-ph | the rhic experiments have measured the nuclear modification factor r_aa of nonphotonic electrons in auau collisions at sqrts 200 gev this r_aa exhibits a large suppression for pt 2 gevc which is commonly attributed to heavyquark energy loss it is expected that the heavyquark radiative energy loss is smaller than the li... | [['the', 'rhic', 'experiments', 'have', 'measured', 'the', 'nuclear', 'modification', 'factor', 'r_aa', 'of', 'nonphotonic', 'electrons', 'in', 'auau', 'collisions', 'at', 'sqrts', '200', 'gev', 'this', 'r_aa', 'exhibits', 'a', 'large', 'suppression', 'for', 'pt', '2', 'gevc', 'which', 'is', 'commonly', 'attributed', '... | [-0.038362708693667015, 0.24983241688276214, -0.15456218863223362, 0.1655982578899916, -0.009156052069226792, -0.10612091181830473, -0.002284103475516191, 0.33698014043537633, -0.18590537235294316, -0.31102942774528997, -0.09627951224268015, -0.3585386572835537, 0.07009520268344044, 0.16388562526860898, 0.0125127188697... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.