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 |
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709.0235 | Flavors and Phases in Unparticle Physics | Inspired by the recent Georgi's unparticle proposal, we study the flavor
structures of the standard model (SM) particles when they couple to
unparticles. At a very high energy scale, we introduce $\BZ$ charges for the SM
particles, which are universal for each generation and allow $\BZ$ fields to
distinguish flavor g... | hep-ph | inspired by the recent georgis unparticle proposal we study the flavor structures of the standard model sm particles when they couple to unparticles at a very high energy scale we introduce bz charges for the sm particles which are universal for each generation and allow bz fields to distinguish flavor generations at t... | [['inspired', 'by', 'the', 'recent', 'georgis', 'unparticle', 'proposal', 'we', 'study', 'the', 'flavor', 'structures', 'of', 'the', 'standard', 'model', 'sm', 'particles', 'when', 'they', 'couple', 'to', 'unparticles', 'at', 'a', 'very', 'high', 'energy', 'scale', 'we', 'introduce', 'bz', 'charges', 'for', 'the', 'sm'... | [-0.10764419335385629, 0.28744360735461294, -0.005575167701070385, 0.13946639359963076, -0.08183073118017078, -0.14976523527181637, 0.059730348552879994, 0.32142896956667816, -0.24283769112476034, -0.2688533771172937, 0.024842554114109794, -0.2898848761088706, -0.09520264553924647, 0.09330465020342349, 0.02252360018481... |
709.0236 | The hierarchical build-up of bulges in CDM | We investigate the hierarchical build-up of stars in bulges within the
standard $\Lambda$-cold dark matter scenario. By separating the population into
stars born during starbursts that accompany the formation of spheroids in major
mergers ({\it starburst} component), and stars that are previously formed in
discs of p... | astro-ph | we investigate the hierarchical buildup of stars in bulges within the standard lambdacold dark matter scenario by separating the population into stars born during starbursts that accompany the formation of spheroids in major mergers it starburst component and stars that are previously formed in discs of progenitor gala... | [['we', 'investigate', 'the', 'hierarchical', 'buildup', 'of', 'stars', 'in', 'bulges', 'within', 'the', 'standard', 'lambdacold', 'dark', 'matter', 'scenario', 'by', 'separating', 'the', 'population', 'into', 'stars', 'born', 'during', 'starbursts', 'that', 'accompany', 'the', 'formation', 'of', 'spheroids', 'in', 'ma... | [-0.08335358740494973, 0.16353133252012161, -0.07516666135856716, 0.15224031597561377, -0.060954844193888934, 0.006432447888665053, -0.02399944522743666, 0.4113321015687008, -0.07908608119535389, -0.36659506325561714, 0.026621667760030585, -0.28335334441995597, -0.013202424392073862, 0.18524593702797604, -0.04002616834... |
709.0237 | Interqubit coupling mediated by a high-excitation-energy quantum object | We consider a system composed of two qubits and a high-excitation-energy
quantum object used to mediate coupling between the qubits. We treat the entire
system quantum mechanically and analyze the properties of the eigenvalues and
eigenstates of the total Hamiltonian. After reproducing well-known results
concerning t... | cond-mat.supr-con | we consider a system composed of two qubits and a highexcitationenergy quantum object used to mediate coupling between the qubits we treat the entire system quantum mechanically and analyze the properties of the eigenvalues and eigenstates of the total hamiltonian after reproducing wellknown results concerning the lead... | [['we', 'consider', 'a', 'system', 'composed', 'of', 'two', 'qubits', 'and', 'a', 'highexcitationenergy', 'quantum', 'object', 'used', 'to', 'mediate', 'coupling', 'between', 'the', 'qubits', 'we', 'treat', 'the', 'entire', 'system', 'quantum', 'mechanically', 'and', 'analyze', 'the', 'properties', 'of', 'the', 'eigenv... | [-0.19177955016493797, 0.1538924644298283, 0.0026158458778165836, 0.03370377484813561, 0.05032796104799728, -0.1785023287223766, 0.03952830206748529, 0.3823056120526831, -0.19777574336320972, -0.2836438745298252, 0.0520110196452968, -0.30743250526728577, -0.155940860180425, 0.23232343202760938, -0.005328687784566107, 0... |
709.0238 | Large deviation for return times in open sets for axiom A
diffeomorphisms | For axiom A diffeomorphisms and equilibrium state, we prove a Large deviation
result for the sequence of successive return times into a fixed open set, under
some assumption on the boundary. Our result relies on and extends the work by
Chazottes and Leplaideur who where considering cylinder sets of a Markov
partition... | math.DS | for axiom a diffeomorphisms and equilibrium state we prove a large deviation result for the sequence of successive return times into a fixed open set under some assumption on the boundary our result relies on and extends the work by chazottes and leplaideur who where considering cylinder sets of a markov partition | [['for', 'axiom', 'a', 'diffeomorphisms', 'and', 'equilibrium', 'state', 'we', 'prove', 'a', 'large', 'deviation', 'result', 'for', 'the', 'sequence', 'of', 'successive', 'return', 'times', 'into', 'a', 'fixed', 'open', 'set', 'under', 'some', 'assumption', 'on', 'the', 'boundary', 'our', 'result', 'relies', 'on', 'and... | [-0.1318638753862335, 0.09995981693142451, -0.09717519961010951, 0.025174534225908037, -0.017788653884333774, -0.10130206848351428, 0.14069774983531366, 0.29343192275756824, -0.24198470392730087, -0.2430136256510965, 0.15898359357379377, -0.24786860076710582, -0.07033030086985001, 0.2013852892873379, -0.104417476623963... |
709.0239 | Percolation sur le syst\`eme \`a trois points | The three dot system is an action by homeomorphisms of $\mathbb Z^2$ on a
compact space, which invariant measures are supposed to satisfy rigidity
properties analoguous to the ones of invariant measures of angle doubling and
tripling on the circle. For such measures, we establish a dichotomy which is
related to perco... | math.DS | the three dot system is an action by homeomorphisms of mathbb z2 on a compact space which invariant measures are supposed to satisfy rigidity properties analoguous to the ones of invariant measures of angle doubling and tripling on the circle for such measures we establish a dichotomy which is related to percolation pr... | [['the', 'three', 'dot', 'system', 'is', 'an', 'action', 'by', 'homeomorphisms', 'of', 'mathbb', 'z2', 'on', 'a', 'compact', 'space', 'which', 'invariant', 'measures', 'are', 'supposed', 'to', 'satisfy', 'rigidity', 'properties', 'analoguous', 'to', 'the', 'ones', 'of', 'invariant', 'measures', 'of', 'angle', 'doubling... | [-0.20757829433061042, 0.13906046585866277, -0.09949978648351049, 0.107285713342036, -0.047510166670072754, -0.12041711991758279, 0.03463209420442581, 0.370980108262233, -0.26281330803022634, -0.21348479912036433, 0.16154404967707, -0.323101409464934, -0.13119101513809753, 0.2209907035466354, -0.1380296410940025, 0.087... |
709.024 | Analyse harmonique sur le graphe de Pascal | We prove a spectral decomposition theorem for a well-known self-similar
graph, for some finite graphs which are quotients of this graph and for a
compactification of it.
| math.DS math.SP | we prove a spectral decomposition theorem for a wellknown selfsimilar graph for some finite graphs which are quotients of this graph and for a compactification of it | [['we', 'prove', 'a', 'spectral', 'decomposition', 'theorem', 'for', 'a', 'wellknown', 'selfsimilar', 'graph', 'for', 'some', 'finite', 'graphs', 'which', 'are', 'quotients', 'of', 'this', 'graph', 'and', 'for', 'a', 'compactification', 'of', 'it']] | [-0.11702904367336521, 0.06807329964444593, -0.18512627792855105, 0.13609689527139482, -0.1414535444367815, -0.09443375069854988, 0.03179099862636239, 0.3590222217694477, -0.31266686844604985, -0.20042651149237323, 0.19987991574668773, -0.23769172550075585, -0.14012015502279004, 0.20861557170886685, -0.1320284172823583... |
709.0241 | Scalar Emission in the Bulk in a Rotating Black Hole Background | We study the emission of scalars into the bulk from a higher-dimensional
rotating black hole. We obtain an analytic solution to the field equation by
employing matching techniques on expressions valid in the near-horizon and
far-field regimes. Both analytic and numerical results for the absorption
probability, in the... | hep-th astro-ph gr-qc hep-ph | we study the emission of scalars into the bulk from a higherdimensional rotating black hole we obtain an analytic solution to the field equation by employing matching techniques on expressions valid in the nearhorizon and farfield regimes both analytic and numerical results for the absorption probability in the lowener... | [['we', 'study', 'the', 'emission', 'of', 'scalars', 'into', 'the', 'bulk', 'from', 'a', 'higherdimensional', 'rotating', 'black', 'hole', 'we', 'obtain', 'an', 'analytic', 'solution', 'to', 'the', 'field', 'equation', 'by', 'employing', 'matching', 'techniques', 'on', 'expressions', 'valid', 'in', 'the', 'nearhorizon'... | [-0.10956871620905788, 0.08481927365510669, -0.051022012535806585, 0.12414203953180138, -0.00677130650728941, -0.09426237733113459, 0.02851862900728441, 0.3520093840020506, -0.17867734340910355, -0.26225171103547124, 0.0682664398893552, -0.2830314488129933, -0.07681802565323027, 0.2523416314051365, 0.014887203265022, 0... |
709.0242 | The Poisson bracket compatible with the classical reflection equation
algebra | We introduce a family of compatible Poisson brackets on the space of $2\times
2$ polynomial matrices, which contains the reflection equation algebra bracket.
Then we use it to derive a multi-Hamiltonian structure for a set of integrable
systems that includes the $XXX$ Heisenberg magnet with boundary conditions, the
g... | nlin.SI | we introduce a family of compatible poisson brackets on the space of 2times 2 polynomial matrices which contains the reflection equation algebra bracket then we use it to derive a multihamiltonian structure for a set of integrable systems that includes the xxx heisenberg magnet with boundary conditions the generalized ... | [['we', 'introduce', 'a', 'family', 'of', 'compatible', 'poisson', 'brackets', 'on', 'the', 'space', 'of', '2times', '2', 'polynomial', 'matrices', 'which', 'contains', 'the', 'reflection', 'equation', 'algebra', 'bracket', 'then', 'we', 'use', 'it', 'to', 'derive', 'a', 'multihamiltonian', 'structure', 'for', 'a', 'se... | [-0.19787108532407066, 0.07718569488497451, -0.00912775078957731, 0.06993599054826931, -0.13859705873765052, -0.1570406328971413, -0.042858730967749246, 0.31080060614780947, -0.3182658170794391, -0.1781005123630166, 0.11583043277178975, -0.23124111301519654, -0.15985712505961683, 0.1876881883945316, -0.0199173658578233... |
709.0243 | The sharp $A_p$ constant for weights in a reverse-H\"older class | In a recent paper V. Vasyunin presented a proof of the reverse H\"older
inequality with sharp constants for the weights satisfying the usual
Muckenhoupt condition. In this paper we present the inverse, that is, we use
the Bellman function technique to find the sharp $A_p$ constants for weights in
a reverse-H\"older c... | math.CA math.AP | in a recent paper v vasyunin presented a proof of the reverse holder inequality with sharp constants for the weights satisfying the usual muckenhoupt condition in this paper we present the inverse that is we use the bellman function technique to find the sharp a_p constants for weights in a reverseholder class on an in... | [['in', 'a', 'recent', 'paper', 'v', 'vasyunin', 'presented', 'a', 'proof', 'of', 'the', 'reverse', 'holder', 'inequality', 'with', 'sharp', 'constants', 'for', 'the', 'weights', 'satisfying', 'the', 'usual', 'muckenhoupt', 'condition', 'in', 'this', 'paper', 'we', 'present', 'the', 'inverse', 'that', 'is', 'we', 'use'... | [-0.09715604034581167, 0.06946376224257299, -0.024755950830876828, 0.05250961053020814, -0.07240513968555366, -0.11850341635701411, 0.07480885316343869, 0.4028437639860546, -0.31583499130519, -0.20537047076367718, 0.08757397885543897, -0.25061794955502537, -0.13943691817112266, 0.2142760266056832, -0.09719362725668093,... |
709.0244 | Neutrino Interactions with Nuclei | We investigate neutrino-nucleus collisions at intermediate energies
incorporating quasi-elastic scattering and the excitation of 13 resonances as
elementary processes, taking into account medium effects such as Fermi motion,
Pauli blocking, mean-field potentials and in-medium spectral functions. A
coupled-channel tre... | nucl-ex hep-ph nucl-th | we investigate neutrinonucleus collisions at intermediate energies incorporating quasielastic scattering and the excitation of 13 resonances as elementary processes taking into account medium effects such as fermi motion pauli blocking meanfield potentials and inmedium spectral functions a coupledchannel treatment of f... | [['we', 'investigate', 'neutrinonucleus', 'collisions', 'at', 'intermediate', 'energies', 'incorporating', 'quasielastic', 'scattering', 'and', 'the', 'excitation', 'of', '13', 'resonances', 'as', 'elementary', 'processes', 'taking', 'into', 'account', 'medium', 'effects', 'such', 'as', 'fermi', 'motion', 'pauli', 'blo... | [-0.039919394092387796, 0.2619166543967474, -0.08629382983524599, 0.21572650347404895, 0.009470132700003246, -0.10523529934888597, 0.05903756674653029, 0.3509113489759757, -0.1974357886116623, -0.24549462057321386, -0.10595674281392027, -0.37985335723223057, 0.006939864716567921, 0.10106879220385213, 0.1796064898577135... |
709.0245 | Instanton effects in N=1 brane models and the Kahler metric of twisted
matter | We consider locally consistent systems of magnetized D9 branes on an
orbifolded six-torus which support N=1 gauge theories. In such realizations,
the matter multiplets arise from "twisted" strings connecting different stacks
of branes. The introduction of Euclidean 5 branes (E5) wrapped on the
six-dimensional compact... | hep-th | we consider locally consistent systems of magnetized d9 branes on an orbifolded sixtorus which support n1 gauge theories in such realizations the matter multiplets arise from twisted strings connecting different stacks of branes the introduction of euclidean 5 branes e5 wrapped on the sixdimensional compact space leads... | [['we', 'consider', 'locally', 'consistent', 'systems', 'of', 'magnetized', 'd9', 'branes', 'on', 'an', 'orbifolded', 'sixtorus', 'which', 'support', 'n1', 'gauge', 'theories', 'in', 'such', 'realizations', 'the', 'matter', 'multiplets', 'arise', 'from', 'twisted', 'strings', 'connecting', 'different', 'stacks', 'of', ... | [-0.19818929682701272, 0.1882143203356238, -0.06899072266807241, 0.12791118384935424, -0.0861377663360062, -0.14448565743817401, -0.013860008902539892, 0.31538979146506424, -0.18522065550796996, -0.2698938206746435, 0.07479878546177479, -0.2903593914442136, -0.12610847463692762, 0.10372848938842696, -0.0863369976416661... |
709.0246 | Mesh update techniques for free-surface flow solvers using spectral
element method | This paper presents a novel mesh-update technique for unsteady free-surface
Newtonian flows using spectral element method and relying on the arbitrary
Lagrangian--Eulerian kinematic description for moving the grid. Selected
results showing compatibility of this mesh-update technique with spectral
element method are g... | cond-mat.soft | this paper presents a novel meshupdate technique for unsteady freesurface newtonian flows using spectral element method and relying on the arbitrary lagrangianeulerian kinematic description for moving the grid selected results showing compatibility of this meshupdate technique with spectral element method are given | [['this', 'paper', 'presents', 'a', 'novel', 'meshupdate', 'technique', 'for', 'unsteady', 'freesurface', 'newtonian', 'flows', 'using', 'spectral', 'element', 'method', 'and', 'relying', 'on', 'the', 'arbitrary', 'lagrangianeulerian', 'kinematic', 'description', 'for', 'moving', 'the', 'grid', 'selected', 'results', '... | [-0.09085725578479469, 0.002149253443349153, -0.16560842827893793, -0.043653348000952975, -0.0827884771861136, -0.1378421893226914, -0.010651232506643283, 0.42049647551029923, -0.24117976307170466, -0.33285302128642796, 0.084052570926724, -0.1685892013134435, -0.11248452317668126, 0.24923719873913797, -0.08640270717442... |
709.0247 | Decay of the Mixed States | We study the classical escape from local minima for 2d multi-well Hamiltonian
systems, realizing the mixed state. We show that escape from such local minima
has a diversity of principally new features, representing an interesting topic
for conceptual understanding of chaotic dynamics and applications.
| nlin.CD | we study the classical escape from local minima for 2d multiwell hamiltonian systems realizing the mixed state we show that escape from such local minima has a diversity of principally new features representing an interesting topic for conceptual understanding of chaotic dynamics and applications | [['we', 'study', 'the', 'classical', 'escape', 'from', 'local', 'minima', 'for', '2d', 'multiwell', 'hamiltonian', 'systems', 'realizing', 'the', 'mixed', 'state', 'we', 'show', 'that', 'escape', 'from', 'such', 'local', 'minima', 'has', 'a', 'diversity', 'of', 'principally', 'new', 'features', 'representing', 'an', 'i... | [-0.1162899812175469, 0.09750208941543613, -0.1140610403381288, 0.0977713058871979, -0.012965282382951542, -0.1449310305337845, 0.009827897926284508, 0.30316124483942986, -0.3325572979255495, -0.26517343262887816, 0.049175443172729996, -0.2651441452326253, -0.24108082276176324, 0.2203885594128885, -0.05887162231374532,... |
709.0248 | Homotopy theoretic models of identity types | This paper presents a novel connection between homotopical algebra and
mathematical logic. It is shown that a form of intensional type theory is valid
in any Quillen model category, generalizing the Hofmann-Streicher groupoid
model of Martin-Loef type theory.
| math.LO math.AT math.CT | this paper presents a novel connection between homotopical algebra and mathematical logic it is shown that a form of intensional type theory is valid in any quillen model category generalizing the hofmannstreicher groupoid model of martinloef type theory | [['this', 'paper', 'presents', 'a', 'novel', 'connection', 'between', 'homotopical', 'algebra', 'and', 'mathematical', 'logic', 'it', 'is', 'shown', 'that', 'a', 'form', 'of', 'intensional', 'type', 'theory', 'is', 'valid', 'in', 'any', 'quillen', 'model', 'category', 'generalizing', 'the', 'hofmannstreicher', 'groupoi... | [-0.1269084057059592, -0.0023588942414199984, -0.11713829452826365, 0.1424126484261423, -0.19071893605428772, -0.22856115300611063, 0.009605427722547305, 0.3038588830999829, -0.373936166584089, -0.19959000042463476, 0.005295369280124637, -0.1906242915177466, -0.2531551616014661, 0.12472364801057689, -0.2482628853035134... |
709.0249 | First-order phase transitions in two-dimensional off-lattice liquid
crystals | We consider an off-lattice liquid crystal pair potential in strictly two
dimensions. The potential is purely repulsive and short-ranged. Nevertheless,
by means of a single parameter in the potential, the system is shown to undergo
a first-order phase transition. The transition is studied using mean-field
density func... | cond-mat.soft cond-mat.stat-mech | we consider an offlattice liquid crystal pair potential in strictly two dimensions the potential is purely repulsive and shortranged nevertheless by means of a single parameter in the potential the system is shown to undergo a firstorder phase transition the transition is studied using meanfield density functional theo... | [['we', 'consider', 'an', 'offlattice', 'liquid', 'crystal', 'pair', 'potential', 'in', 'strictly', 'two', 'dimensions', 'the', 'potential', 'is', 'purely', 'repulsive', 'and', 'shortranged', 'nevertheless', 'by', 'means', 'of', 'a', 'single', 'parameter', 'in', 'the', 'potential', 'the', 'system', 'is', 'shown', 'to',... | [-0.15821718685037922, 0.14962719623885773, -0.10459555961530317, 0.03882319941714575, 0.00683097635099495, -0.12072074889544059, 0.04027356244411997, 0.33846366339447825, -0.2640291608192704, -0.29164720179343767, 0.05633640656649897, -0.30559662787074393, -0.19174244960939343, 0.11971183988604356, 0.05536897640505975... |
709.025 | Large-eddy simulation of the lid-driven cubic cavity flow by the
spectral element method | This paper presents the large-eddy simulation of the lid-driven cubic cavity
flow by the spectral element method (SEM) using the dynamic model. Two spectral
filtering techniques suitable for these simulations have been implemented.
Numerical results for Reynolds number $\text{Re}=12'000$ are showing very good
agreeme... | physics.flu-dyn physics.comp-ph | this paper presents the largeeddy simulation of the liddriven cubic cavity flow by the spectral element method sem using the dynamic model two spectral filtering techniques suitable for these simulations have been implemented numerical results for reynolds number textre12000 are showing very good agreement with other e... | [['this', 'paper', 'presents', 'the', 'largeeddy', 'simulation', 'of', 'the', 'liddriven', 'cubic', 'cavity', 'flow', 'by', 'the', 'spectral', 'element', 'method', 'sem', 'using', 'the', 'dynamic', 'model', 'two', 'spectral', 'filtering', 'techniques', 'suitable', 'for', 'these', 'simulations', 'have', 'been', 'impleme... | [-0.10968894579113936, 0.014799177172189613, -0.09900572460215047, -0.004634228001243241, -0.028255024257133592, -0.1260183889348552, -0.057521649746153994, 0.43581098648455907, -0.21556181142563527, -0.37020529437599314, 0.11914450586290222, -0.2622871366593073, -0.12953716892538206, 0.3160475580294107, -0.00784647513... |
709.0251 | Femtosecond Photoionization of Atoms under Noise | We investigate the effect of incoherent perturbations on atomic
photoionization due to a femtosecond mid-infrared laser pulse by solving the
time-dependent stochastic Schr\"odinger equation. For a weak laser pulse which
causes almost no ionization, an addition of a Gaussian white noise to the pulse
leads to a signifi... | quant-ph | we investigate the effect of incoherent perturbations on atomic photoionization due to a femtosecond midinfrared laser pulse by solving the timedependent stochastic schrodinger equation for a weak laser pulse which causes almost no ionization an addition of a gaussian white noise to the pulse leads to a significantly e... | [['we', 'investigate', 'the', 'effect', 'of', 'incoherent', 'perturbations', 'on', 'atomic', 'photoionization', 'due', 'to', 'a', 'femtosecond', 'midinfrared', 'laser', 'pulse', 'by', 'solving', 'the', 'timedependent', 'stochastic', 'schrodinger', 'equation', 'for', 'a', 'weak', 'laser', 'pulse', 'which', 'causes', 'al... | [-0.12055926374313945, 0.14681147744964704, -0.0989112320991344, 0.09103475700191142, -0.013886929976920419, -0.13208186607006073, 0.06734071978111905, 0.44334467288896146, -0.27078167140015114, -0.2938024013099686, 0.0380376949459191, -0.23087963139767825, -0.1386063206595498, 0.2572739898560211, -0.06145011408821933,... |
709.0252 | Asymptotic analysis of the Bell polynomials by the ray method | We analyze the Bell polynomials $B_{n}(x)$ asymptotically as $n\to\infty$. We
obtain asymptotic approximations from the differential-difference equation
which they satisfy, using a discrete version of the ray method. We give some
examples showing the accuracy of our formulas.
| math.CA | we analyze the bell polynomials b_nx asymptotically as ntoinfty we obtain asymptotic approximations from the differentialdifference equation which they satisfy using a discrete version of the ray method we give some examples showing the accuracy of our formulas | [['we', 'analyze', 'the', 'bell', 'polynomials', 'b_nx', 'asymptotically', 'as', 'ntoinfty', 'we', 'obtain', 'asymptotic', 'approximations', 'from', 'the', 'differentialdifference', 'equation', 'which', 'they', 'satisfy', 'using', 'a', 'discrete', 'version', 'of', 'the', 'ray', 'method', 'we', 'give', 'some', 'examples... | [-0.09592497365941342, 0.007566594494212615, -0.14463812899530717, 0.1469746576499586, -0.049365084324228134, -0.12828503462093832, 0.06694026823204599, 0.33263771052129176, -0.24553460133239768, -0.2523432974948695, 0.12594321297824776, -0.3030755655153802, -0.19046555905553855, 0.23055664153377475, -0.089484894854601... |
709.0253 | Neutrino Mass, Dark Energy, and the Linear Growth Factor | We study the degeneracies between neutrino mass and dark energy as they
manifest themselves in cosmological observations. In contradiction to a popular
formula in the literature, the suppression of the matter power spectrum caused
by massive neutrinos is not just a function of the ratio of neutrino to total
mass dens... | astro-ph | we study the degeneracies between neutrino mass and dark energy as they manifest themselves in cosmological observations in contradiction to a popular formula in the literature the suppression of the matter power spectrum caused by massive neutrinos is not just a function of the ratio of neutrino to total mass densitie... | [['we', 'study', 'the', 'degeneracies', 'between', 'neutrino', 'mass', 'and', 'dark', 'energy', 'as', 'they', 'manifest', 'themselves', 'in', 'cosmological', 'observations', 'in', 'contradiction', 'to', 'a', 'popular', 'formula', 'in', 'the', 'literature', 'the', 'suppression', 'of', 'the', 'matter', 'power', 'spectrum... | [-0.14127617316674998, 0.131331206688574, -0.08951009929513754, 0.13057765348400893, -0.07672947559700306, -0.09062318024642543, 0.030256496411583164, 0.2992296695271368, -0.22968837017985755, -0.3360628122559387, 0.027722833802360597, -0.27096913635397135, -0.06251062939652423, 0.16220079237289392, 0.00519426362658503... |
709.0254 | Tidal waves as yrast states in transitional nuclei | The yrast states of transitional nuclei are described as quadrupole waves
running over the nuclear surface, which we call tidal waves. In contrast to a
rotor, which generates angular momentum by increasing the angular velocity at
approximately constant deformation, a tidal wave generates angular momentum by
increasin... | nucl-th | the yrast states of transitional nuclei are described as quadrupole waves running over the nuclear surface which we call tidal waves in contrast to a rotor which generates angular momentum by increasing the angular velocity at approximately constant deformation a tidal wave generates angular momentum by increasing the ... | [['the', 'yrast', 'states', 'of', 'transitional', 'nuclei', 'are', 'described', 'as', 'quadrupole', 'waves', 'running', 'over', 'the', 'nuclear', 'surface', 'which', 'we', 'call', 'tidal', 'waves', 'in', 'contrast', 'to', 'a', 'rotor', 'which', 'generates', 'angular', 'momentum', 'by', 'increasing', 'the', 'angular', '... | [-0.14293759820760565, 0.23237847173124676, -0.028075906990696328, 0.0628732588730968, -0.008786652960683688, -0.05629373426464471, 0.015086722423607283, 0.33205298469825223, -0.21406637062511044, -0.3301446317456478, -0.048059675976858195, -0.2956687287496757, -0.05077161351855015, 0.14722555689802316, 0.0826640326976... |
709.0255 | Exclusive J/psi and Upsilon hadroproduction as a probe of the QCD
Odderon | We study the exclusive production of J/psi or Upsilon in pp and bar pp
collisions, where the meson emerges from the pomeron--odderon and the
pomeron--photon fusion. We estimate the cross sections for these processes for
the kinematical conditions of the Tevatron and of the LHC.
| hep-ph | we study the exclusive production of jpsi or upsilon in pp and bar pp collisions where the meson emerges from the pomeronodderon and the pomeronphoton fusion we estimate the cross sections for these processes for the kinematical conditions of the tevatron and of the lhc | [['we', 'study', 'the', 'exclusive', 'production', 'of', 'jpsi', 'or', 'upsilon', 'in', 'pp', 'and', 'bar', 'pp', 'collisions', 'where', 'the', 'meson', 'emerges', 'from', 'the', 'pomeronodderon', 'and', 'the', 'pomeronphoton', 'fusion', 'we', 'estimate', 'the', 'cross', 'sections', 'for', 'these', 'processes', 'for', ... | [-0.017366628773096533, 0.1904891699138615, -0.1623586906120181, 0.13732820629245704, 0.037829966051504016, -0.04969649975084596, 0.0102945478943487, 0.2738360855624907, -0.21960303179091878, -0.1502610017442041, -0.07195103678904059, -0.3520665365995632, 0.057357985235285014, 0.11689448298162056, 0.11668033744725916, ... |
709.0256 | Magnetic fields in massive star forming regions | We present the largest sample of high-mass star-forming regions observed
using submillimetre imaging polarimetry. The data were taken using SCUBA in
conjunction with the polarimeter on the JCMT in Hawaii. In total, 16 star
forming regions were observed, although some of these contain multiple cores.
The polarimetry i... | astro-ph | we present the largest sample of highmass starforming regions observed using submillimetre imaging polarimetry the data were taken using scuba in conjunction with the polarimeter on the jcmt in hawaii in total 16 star forming regions were observed although some of these contain multiple cores the polarimetry implies a ... | [['we', 'present', 'the', 'largest', 'sample', 'of', 'highmass', 'starforming', 'regions', 'observed', 'using', 'submillimetre', 'imaging', 'polarimetry', 'the', 'data', 'were', 'taken', 'using', 'scuba', 'in', 'conjunction', 'with', 'the', 'polarimeter', 'on', 'the', 'jcmt', 'in', 'hawaii', 'in', 'total', '16', 'star'... | [-0.11701349794066378, 0.09189688376949302, -0.002830565594402807, 0.05887587231716939, -0.03928000112729413, -0.04052428974104779, 0.00964830227861447, 0.4477059923325266, -0.18124930818698237, -0.3953032291574138, 0.07050019216657218, -0.27859390452504157, -0.008672245453510965, 0.21142753431839603, 0.044410681538283... |
709.0257 | D-branes in T-fold conformal field theory | We investigate boundary dynamics of orbifold conformal field theory involving
T-duality twists. Such models typically appear in contexts of non-geometric
string compactifications that are called monodrofolds or T-folds in recent
literature. We use the framework of boundary conformal field theory to analyse
the models... | hep-th | we investigate boundary dynamics of orbifold conformal field theory involving tduality twists such models typically appear in contexts of nongeometric string compactifications that are called monodrofolds or tfolds in recent literature we use the framework of boundary conformal field theory to analyse the models from a... | [['we', 'investigate', 'boundary', 'dynamics', 'of', 'orbifold', 'conformal', 'field', 'theory', 'involving', 'tduality', 'twists', 'such', 'models', 'typically', 'appear', 'in', 'contexts', 'of', 'nongeometric', 'string', 'compactifications', 'that', 'are', 'called', 'monodrofolds', 'or', 'tfolds', 'in', 'recent', 'li... | [-0.1262137013776131, 0.15765816539108832, -0.09769337109901244, 0.1493631401838987, -0.10998558089704602, -0.16611223320796853, -0.010218488718237495, 0.3486179963135025, -0.19433653715774804, -0.2770121618474756, 0.1061118453102002, -0.2722000137049084, -0.15705693789520106, 0.15509526460785614, -0.10741974434010142,... |
709.0258 | Networks of Polynomial Pieces with Application to the Analysis of Point
Clouds and Images | We consider Holder smoothness classes of surfaces for which we construct
piecewise polynomial approximation networks, which are graphs with polynomial
pieces as nodes and edges between polynomial pieces that are in `good
continuation' of each other. Little known to the community, a similar
construction was used by Ko... | stat.ME | we consider holder smoothness classes of surfaces for which we construct piecewise polynomial approximation networks which are graphs with polynomial pieces as nodes and edges between polynomial pieces that are in good continuation of each other little known to the community a similar construction was used by kolmogoro... | [['we', 'consider', 'holder', 'smoothness', 'classes', 'of', 'surfaces', 'for', 'which', 'we', 'construct', 'piecewise', 'polynomial', 'approximation', 'networks', 'which', 'are', 'graphs', 'with', 'polynomial', 'pieces', 'as', 'nodes', 'and', 'edges', 'between', 'polynomial', 'pieces', 'that', 'are', 'in', 'good', 'co... | [-0.10787205052229443, 0.008286321835226512, -0.08419690390782697, 0.10679097878613643, -0.08604392382183246, -0.1358377144858241, 0.027427141442894935, 0.4000864229457719, -0.2954215556383133, -0.28608224648716196, 0.0935000379383564, -0.2521531859372875, -0.19247832483478955, 0.22447557563228265, -0.1157411334477365,... |
709.0259 | Spectrum Sensing in Wideband OFDM Cognitive Radios | In this paper, detection of the primary user (PU) signal in an orthogonal
frequency division multiplexing (OFDM) based cognitive radio (CR) system is
addressed. According to the prior knowledge of the PU signal known to the
detector, three detection algorithms based on the Neyman-Pearson philosophy are
proposed. In t... | cs.IT math.IT | in this paper detection of the primary user pu signal in an orthogonal frequency division multiplexing ofdm based cognitive radio cr system is addressed according to the prior knowledge of the pu signal known to the detector three detection algorithms based on the neymanpearson philosophy are proposed in the first case... | [['in', 'this', 'paper', 'detection', 'of', 'the', 'primary', 'user', 'pu', 'signal', 'in', 'an', 'orthogonal', 'frequency', 'division', 'multiplexing', 'ofdm', 'based', 'cognitive', 'radio', 'cr', 'system', 'is', 'addressed', 'according', 'to', 'the', 'prior', 'knowledge', 'of', 'the', 'pu', 'signal', 'known', 'to', '... | [-0.18798125201916968, 0.044720984462264336, -0.030819232962394673, 0.005034225223641041, -0.1012774265461391, -0.20834729129383442, 0.0855837532986326, 0.40173424747321873, -0.2710347555487627, -0.2611521491430379, 0.08222971879063494, -0.2935989718053049, -0.16007660078986358, 0.11688098512334569, -0.0747932558829185... |
709.026 | Mixing of shear Alfven wave packets | The propagation of shear Alfven wave packets in inhomogeneous magnetic
fields, at the origin of their distortion, regardless of the occurrence of
non-linear coupling, is considered. It is shown that the distortion mechanism
can be regarded as mixing process and hence, standard "phase mixing"
corresponds to the effect... | astro-ph | the propagation of shear alfven wave packets in inhomogeneous magnetic fields at the origin of their distortion regardless of the occurrence of nonlinear coupling is considered it is shown that the distortion mechanism can be regarded as mixing process and hence standard phase mixing corresponds to the effect of an alf... | [['the', 'propagation', 'of', 'shear', 'alfven', 'wave', 'packets', 'in', 'inhomogeneous', 'magnetic', 'fields', 'at', 'the', 'origin', 'of', 'their', 'distortion', 'regardless', 'of', 'the', 'occurrence', 'of', 'nonlinear', 'coupling', 'is', 'considered', 'it', 'is', 'shown', 'that', 'the', 'distortion', 'mechanism', ... | [-0.22848917234899715, 0.24663281306979187, -0.056216078061173416, 0.08070531270355817, -0.06096160178613854, -0.041026382082709055, -0.011280258898961478, 0.3095600604425658, -0.3339153986772803, -0.24212229737814245, 0.048103037718865586, -0.23129653508837372, -0.1009322725621432, 0.1804523273116217, 0.06826600260179... |
709.0261 | No resonant tunneling in standard scalar quantum field theory | We investigate the nature of resonant tunneling in Quantum Field Theory.
Following the pioneering work of Banks, Bender and Wu, we describe quantum
field theory in terms of infinite dimensional quantum mechanics and utilize the
``Most probable escape path'' (MPEP) as the class of paths which dominate the
path integra... | hep-th | we investigate the nature of resonant tunneling in quantum field theory following the pioneering work of banks bender and wu we describe quantum field theory in terms of infinite dimensional quantum mechanics and utilize the most probable escape path mpep as the class of paths which dominate the path integral in the cl... | [['we', 'investigate', 'the', 'nature', 'of', 'resonant', 'tunneling', 'in', 'quantum', 'field', 'theory', 'following', 'the', 'pioneering', 'work', 'of', 'banks', 'bender', 'and', 'wu', 'we', 'describe', 'quantum', 'field', 'theory', 'in', 'terms', 'of', 'infinite', 'dimensional', 'quantum', 'mechanics', 'and', 'utili... | [-0.1421225319415313, 0.18250894343968735, -0.053764117280364905, 0.08416952720156066, -0.04873016945005042, -0.1503043143865336, 0.03541265432022114, 0.36014069027258355, -0.2511238421333809, -0.25893358408826067, 0.06303782455478478, -0.2591380215457921, -0.19724430724327424, 0.18880343753663661, -0.04865024493412721... |
709.0262 | Discovery of multiple Lorentzian components in the X-ray timing
properties of the Narrow Line Seyfert 1 Ark 564 | We present a power spectral analysis of a 100 ksec XMM-Newton observation of
the narrow line Seyfert 1 galaxy Ark~564. When combined with earlier RXTE and
ASCA observations, these data produce a power spectrum covering seven decades
of frequency which is well described by a power law with two very clear breaks.
This ... | astro-ph | we present a power spectral analysis of a 100 ksec xmmnewton observation of the narrow line seyfert 1 galaxy ark564 when combined with earlier rxte and asca observations these data produce a power spectrum covering seven decades of frequency which is well described by a power law with two very clear breaks this shape i... | [['we', 'present', 'a', 'power', 'spectral', 'analysis', 'of', 'a', '100', 'ksec', 'xmmnewton', 'observation', 'of', 'the', 'narrow', 'line', 'seyfert', '1', 'galaxy', 'ark564', 'when', 'combined', 'with', 'earlier', 'rxte', 'and', 'asca', 'observations', 'these', 'data', 'produce', 'a', 'power', 'spectrum', 'covering'... | [-0.09395788516169482, 0.10529099947715137, -0.07746270083631966, 0.09895708263396238, -0.08383602873816488, -0.1398644268149034, 0.04070188618098542, 0.4293826515140542, -0.21144089314491354, -0.3322734217920823, 0.10545027522874968, -0.3099336876078461, -0.050687891832233344, 0.21928503507676866, -0.01003336216396155... |
709.0263 | Violation of the Luttinger sum rule within the Hubbard model on a
triangular lattice | The frequency-moment expansion method is developed to analyze the validity of
the Luttinger sum rule within the Mott-Hubbard insulator, as represented by the
generalized Hubbard model at half filling and large $U$. For the particular
case of the Hubbard model with nearest-neighbor hopping on a triangular lattice
lack... | cond-mat.str-el cond-mat.stat-mech | the frequencymoment expansion method is developed to analyze the validity of the luttinger sum rule within the motthubbard insulator as represented by the generalized hubbard model at half filling and large u for the particular case of the hubbard model with nearestneighbor hopping on a triangular lattice lacking the p... | [['the', 'frequencymoment', 'expansion', 'method', 'is', 'developed', 'to', 'analyze', 'the', 'validity', 'of', 'the', 'luttinger', 'sum', 'rule', 'within', 'the', 'motthubbard', 'insulator', 'as', 'represented', 'by', 'the', 'generalized', 'hubbard', 'model', 'at', 'half', 'filling', 'and', 'large', 'u', 'for', 'the',... | [-0.14236356055661073, 0.11351591449808972, 0.01645541496992368, 0.07937502207692135, -0.03949389038286332, -0.19281628813819382, 0.15790664070639118, 0.32161675725967204, -0.25339365842077755, -0.21183050215115834, 0.042659942992031574, -0.2984451185751321, -0.11294464567868874, 0.08386172385533051, 0.1060927109993544... |
709.0264 | A search for electron cyclotron maser emission from compact binaries | Unipolar induction (UI) is a fundamental physical process, which occurs when
a conducting body transverses a magnetic field. It has been suggested that UI
is operating in RX J0806+15 and RX J1914+24, which are believed to be
ultra-compact binaries with orbital periods of 5.4 min and 9.6 min
respectively. The UI model... | astro-ph | unipolar induction ui is a fundamental physical process which occurs when a conducting body transverses a magnetic field it has been suggested that ui is operating in rx j080615 and rx j191424 which are believed to be ultracompact binaries with orbital periods of 54 min and 96 min respectively the ui model predicts tha... | [['unipolar', 'induction', 'ui', 'is', 'a', 'fundamental', 'physical', 'process', 'which', 'occurs', 'when', 'a', 'conducting', 'body', 'transverses', 'a', 'magnetic', 'field', 'it', 'has', 'been', 'suggested', 'that', 'ui', 'is', 'operating', 'in', 'rx', 'j080615', 'and', 'rx', 'j191424', 'which', 'are', 'believed', '... | [-0.1420825213031996, 0.11999840810454285, -0.059241114891236006, 0.06882380476990838, -0.1120189211184257, -0.16816436103639393, 0.04731432088228463, 0.46700350464008716, -0.2008502299497696, -0.29428364655666567, 0.10282348216226633, -0.2828861297159371, -0.07960054139335176, 0.2304217101353775, -0.019478520299289148... |
709.0265 | How far can you go ? Surprises and pitfalls in three-flavour chiral
extrapolations | The presence of strange sea quark pairs may have a significant impact of the
pattern of chiral symmetry breaking : in particular large differences can occur
between the chiral limits of two and three massless flavours (i.e., whether
$m_s$ is kept at its physical value or sent to zero). We recall some
indications of s... | hep-lat | the presence of strange sea quark pairs may have a significant impact of the pattern of chiral symmetry breaking in particular large differences can occur between the chiral limits of two and three massless flavours ie whether m_s is kept at its physical value or sent to zero we recall some indications of such a scenar... | [['the', 'presence', 'of', 'strange', 'sea', 'quark', 'pairs', 'may', 'have', 'a', 'significant', 'impact', 'of', 'the', 'pattern', 'of', 'chiral', 'symmetry', 'breaking', 'in', 'particular', 'large', 'differences', 'can', 'occur', 'between', 'the', 'chiral', 'limits', 'of', 'two', 'and', 'three', 'massless', 'flavours... | [-0.14580497973720016, 0.2592217865613866, -0.12289866421614652, 0.09267316112375777, -0.06345700885614623, -0.07552250226979833, 0.0770471350249389, 0.3506280873719927, -0.21061188403678976, -0.28287359374048915, 0.07231628479658747, -0.307001832905023, -0.11424071153261416, 0.12024663517697026, 0.03188743694057769, 0... |
709.0266 | Investigation of Bioglass-Electrode Interfaces after Thermal Poling | Electrical and electrochemical processes in a bioactive soda-lime
phosphosilicate glasses and in a bioabsorbable soda-lime phosphate glass during
thermal poling were studied by means of thermally stimulated depolarization
current measurements, ac impedance spectroscopy, and SEM/EDX analyses. The
thermal poling was do... | cond-mat.mtrl-sci cond-mat.other | electrical and electrochemical processes in a bioactive sodalime phosphosilicate glasses and in a bioabsorbable sodalime phosphate glass during thermal poling were studied by means of thermally stimulated depolarization current measurements ac impedance spectroscopy and semedx analyses the thermal poling was done by sp... | [['electrical', 'and', 'electrochemical', 'processes', 'in', 'a', 'bioactive', 'sodalime', 'phosphosilicate', 'glasses', 'and', 'in', 'a', 'bioabsorbable', 'sodalime', 'phosphate', 'glass', 'during', 'thermal', 'poling', 'were', 'studied', 'by', 'means', 'of', 'thermally', 'stimulated', 'depolarization', 'current', 'me... | [-0.0802096658297113, 0.23021562006518556, -0.002536571707586961, -0.06650879499144279, 0.03317200057417489, -0.17117889803380537, 0.09520361229974347, 0.4439887535304595, -0.23222387609525752, -0.28161005564750385, 0.050422195699819636, -0.31423727388326556, -0.06055742235949788, 0.18212590527195388, -0.00662783863476... |
709.0267 | Quadratic supersymmetric transformations of the Dirac Green functions | We consider the quadratic supersymmetric aspect of the Darboux transformation
for the Green functions of the one-dimensional Dirac equation with a
generalized form of the potential. We obtain the relation between the initial
and the transformed Green functions on the whole real line. We also construct
the formula for... | hep-th | we consider the quadratic supersymmetric aspect of the darboux transformation for the green functions of the onedimensional dirac equation with a generalized form of the potential we obtain the relation between the initial and the transformed green functions on the whole real line we also construct the formula for the ... | [['we', 'consider', 'the', 'quadratic', 'supersymmetric', 'aspect', 'of', 'the', 'darboux', 'transformation', 'for', 'the', 'green', 'functions', 'of', 'the', 'onedimensional', 'dirac', 'equation', 'with', 'a', 'generalized', 'form', 'of', 'the', 'potential', 'we', 'obtain', 'the', 'relation', 'between', 'the', 'initia... | [-0.12549006940113216, 0.011749994170541074, -0.07693680752469581, 0.08278738792184033, -0.04178376590444034, -0.048661042676790604, 0.0276666692534721, 0.33269070258623434, -0.2515778342096866, -0.2198542561617833, 0.11611185976469159, -0.2588186519739183, -0.20753852070509632, 0.20968867720493786, 0.04050644544908140... |
709.0268 | Exchange between deep donors in semiconductors: a quantum defect
approach | Exchange interactions among defects in semiconductors are commonly treated
within effective-mass theory using a scaled hydrogenic wave-function. However
such a wave-function is only applicable to shallow impurities; here we present
a simple but robust generalization to treat deep donors, in which we treat the
long-ra... | cond-mat.mtrl-sci | exchange interactions among defects in semiconductors are commonly treated within effectivemass theory using a scaled hydrogenic wavefunction however such a wavefunction is only applicable to shallow impurities here we present a simple but robust generalization to treat deep donors in which we treat the longrange part ... | [['exchange', 'interactions', 'among', 'defects', 'in', 'semiconductors', 'are', 'commonly', 'treated', 'within', 'effectivemass', 'theory', 'using', 'a', 'scaled', 'hydrogenic', 'wavefunction', 'however', 'such', 'a', 'wavefunction', 'is', 'only', 'applicable', 'to', 'shallow', 'impurities', 'here', 'we', 'present', '... | [-0.07675895392366046, 0.12772938111740037, -0.022966873123387778, 0.1443201680728702, 0.004926411402472763, -0.1755134026747701, 0.06712769174553844, 0.38169686554821297, -0.2518382022995095, -0.32719958184376424, -0.02007982721420078, -0.3475604670206273, -0.08228931576359888, 0.14058370198180095, 0.02167801690230951... |
709.0269 | Strange non-chaotic attractors in quasiperiodically forced circle maps | The occurrence of strange non-chaotic attractors (SNA) in quasiperiodically
forced systems has attracted considerable interest over the last two decades,
in particular since it provides a rich class of examples for the possibility of
complicated dynamics in the absence of chaos. Their existence was discovered in
the ... | math.DS | the occurrence of strange nonchaotic attractors sna in quasiperiodically forced systems has attracted considerable interest over the last two decades in particular since it provides a rich class of examples for the possibility of complicated dynamics in the absence of chaos their existence was discovered in the early 1... | [['the', 'occurrence', 'of', 'strange', 'nonchaotic', 'attractors', 'sna', 'in', 'quasiperiodically', 'forced', 'systems', 'has', 'attracted', 'considerable', 'interest', 'over', 'the', 'last', 'two', 'decades', 'in', 'particular', 'since', 'it', 'provides', 'a', 'rich', 'class', 'of', 'examples', 'for', 'the', 'possib... | [-0.16016442755547664, 0.13979108220619132, -0.06937741928770408, 0.08135967096427967, -0.04790531816166442, -0.11738364434088855, 0.05047017298684474, 0.27821230969857424, -0.2600907482362042, -0.2313126528849049, 0.14461089125731685, -0.2532859346509783, -0.21325484710727252, 0.25319153195310967, -0.09829555811159604... |
709.027 | X-ray reflection in accreting stellar-mass black hole systems | The X-ray spectra of accreting stellar-mass black hole systems exhibit
spectral features due to reflection, especially broad iron K alpha emission
lines. We investigate the reflection by the accretion disc that can be expected
in the high/soft state of such a system. First, we perform a self-consistent
calculation of... | astro-ph | the xray spectra of accreting stellarmass black hole systems exhibit spectral features due to reflection especially broad iron k alpha emission lines we investigate the reflection by the accretion disc that can be expected in the highsoft state of such a system first we perform a selfconsistent calculation of the refle... | [['the', 'xray', 'spectra', 'of', 'accreting', 'stellarmass', 'black', 'hole', 'systems', 'exhibit', 'spectral', 'features', 'due', 'to', 'reflection', 'especially', 'broad', 'iron', 'k', 'alpha', 'emission', 'lines', 'we', 'investigate', 'the', 'reflection', 'by', 'the', 'accretion', 'disc', 'that', 'can', 'be', 'expe... | [-0.07424429057824329, 0.11134410550497204, -0.09661821245440635, 0.0703106284872147, -0.06668065819319273, -0.07467316149669731, 0.04364549177337502, 0.42480050590981183, -0.2115948938218684, -0.31754469734231205, 0.07542731552906655, -0.266342881529046, -0.02413924136560346, 0.21304539403203746, -0.04523967287567412,... |
709.0271 | Quantum Critical Phenomena, Entanglement Entropy and Hubbard Model in 1d
with the Boundary Site with a Negative Chemical Potential -p and the Hubbard
Coupling U Positive | Recently the ground state and some excited states of the half-filled case of
the 1d Hubbard model were discussed for an open chain with L sites. Authors
considered the case when the boundary site has a negative chemical potential -p
and the Hubbard coupling U is positive. They have shown by an analytic method
that wh... | cond-mat.str-el cond-mat.other | recently the ground state and some excited states of the halffilled case of the 1d hubbard model were discussed for an open chain with l sites authors considered the case when the boundary site has a negative chemical potential p and the hubbard coupling u is positive they have shown by an analytic method that when p i... | [['recently', 'the', 'ground', 'state', 'and', 'some', 'excited', 'states', 'of', 'the', 'halffilled', 'case', 'of', 'the', '1d', 'hubbard', 'model', 'were', 'discussed', 'for', 'an', 'open', 'chain', 'with', 'l', 'sites', 'authors', 'considered', 'the', 'case', 'when', 'the', 'boundary', 'site', 'has', 'a', 'negative'... | [-0.15686889722196434, 0.17797721042120135, -0.06470119577527118, 0.05742253614256957, -0.007232273345232591, -0.1656695017318979, 0.05867512919032922, 0.34596974065817604, -0.22830797886693632, -0.2301191623117049, 0.08761180578368147, -0.3495813015933064, -0.1254747448770281, 0.11079959618230048, 0.06851954285853676,... |
709.0272 | Strong Law of Large Numbers for branching diffusions | Let $X$ be the branching particle diffusion corresponding to the operator
$Lu+\beta (u^{2}-u)$ on $D\subseteq \mathbb{R}^{d}$
(where $\beta \geq 0$ and $\beta\not\equiv 0$). Let $\lambda_{c}$ denote the
generalized principal eigenvalue for the operator $L+\beta $ on $D$ and assume
that it is finite. When $\lambda... | math.PR | let x be the branching particle diffusion corresponding to the operator lubeta u2u on dsubseteq mathbbrd where beta geq 0 and betanotequiv 0 let lambda_c denote the generalized principal eigenvalue for the operator lbeta on d and assume that it is finite when lambda_c0 and lbetalambda_c satisfies certain spectral theor... | [['let', 'x', 'be', 'the', 'branching', 'particle', 'diffusion', 'corresponding', 'to', 'the', 'operator', 'lubeta', 'u2u', 'on', 'dsubseteq', 'mathbbrd', 'where', 'beta', 'geq', '0', 'and', 'betanotequiv', '0', 'let', 'lambda_c', 'denote', 'the', 'generalized', 'principal', 'eigenvalue', 'for', 'the', 'operator', 'lbe... | [-0.053347959222392764, 0.13567067028316496, -0.06912439041943462, 0.05438693441517696, -0.06205422893959891, -0.15341621860516844, 0.03780915676529899, 0.32125993354970384, -0.28664340997390725, -0.20605533414140895, 0.13270864407704383, -0.33884527336254167, -0.11875159991042758, 0.17787314041483182, -0.1057041803236... |
709.0273 | Chemical evolution of Seyfert galaxies | We computed the chemical evolution of Seyfert galaxies, residing in spiral
bulges, based on an updated model for the Milky Way bulge with updated
calculations of the Galactic potential and of the feedback from the central
supermassive black hole (BH) in a spherical approximation. We followed the
evolution of bulges o... | astro-ph | we computed the chemical evolution of seyfert galaxies residing in spiral bulges based on an updated model for the milky way bulge with updated calculations of the galactic potential and of the feedback from the central supermassive black hole bh in a spherical approximation we followed the evolution of bulges of masse... | [['we', 'computed', 'the', 'chemical', 'evolution', 'of', 'seyfert', 'galaxies', 'residing', 'in', 'spiral', 'bulges', 'based', 'on', 'an', 'updated', 'model', 'for', 'the', 'milky', 'way', 'bulge', 'with', 'updated', 'calculations', 'of', 'the', 'galactic', 'potential', 'and', 'of', 'the', 'feedback', 'from', 'the', '... | [-0.02230671457433646, 0.04202134058868978, -0.060013952639398224, 0.14585780140456803, -0.035734226038559865, -0.040373067888473974, 0.056460796530708804, 0.41388682113669883, -0.12433162370884637, -0.37281205265893846, 0.002292041740499847, -0.2791444384108443, -0.008294962839983882, 0.20998361193651863, 0.0012387415... |
709.0274 | Extrinsic Isoperimetric Analysis on Submanifolds with Curvatures Bounded
from Below | We obtain upper bounds for the isoperimetric quotients of extrinsic balls of
submanifolds in ambient spaces which have a lower bound on their radial
sectional curvatures. The submanifolds are themselves only assumed to have
lower bounds on the radial part of the mean curvature vector field and on the
radial part of t... | math.DG math.AP | we obtain upper bounds for the isoperimetric quotients of extrinsic balls of submanifolds in ambient spaces which have a lower bound on their radial sectional curvatures the submanifolds are themselves only assumed to have lower bounds on the radial part of the mean curvature vector field and on the radial part of the ... | [['we', 'obtain', 'upper', 'bounds', 'for', 'the', 'isoperimetric', 'quotients', 'of', 'extrinsic', 'balls', 'of', 'submanifolds', 'in', 'ambient', 'spaces', 'which', 'have', 'a', 'lower', 'bound', 'on', 'their', 'radial', 'sectional', 'curvatures', 'the', 'submanifolds', 'are', 'themselves', 'only', 'assumed', 'to', '... | [-0.1175601802445868, 0.10397308327943608, -0.09859979633987952, 0.06440127488558671, -0.07145131861300318, -0.100802219267534, 0.03799566463504728, 0.3625685327225715, -0.23852733330411827, -0.2667905287998628, 0.13486353969714673, -0.28091175883247327, -0.11355826055746206, 0.18878670253412877, -0.13550669500561713, ... |
709.0275 | R-matrix propagation with adiabatic bases for the photoionization
spectra of atoms in magnetic fields | The photoionization spectrum of an atom in a magnetic field is calculated by
combining R-matrix propagation with local adiabatic basis expansions. This
approach considerably increases the speed and the energy range over which
calculations can be performed compared to previous methods, allowing one to
obtain accurate ... | physics.atom-ph physics.comp-ph | the photoionization spectrum of an atom in a magnetic field is calculated by combining rmatrix propagation with local adiabatic basis expansions this approach considerably increases the speed and the energy range over which calculations can be performed compared to previous methods allowing one to obtain accurate parti... | [['the', 'photoionization', 'spectrum', 'of', 'an', 'atom', 'in', 'a', 'magnetic', 'field', 'is', 'calculated', 'by', 'combining', 'rmatrix', 'propagation', 'with', 'local', 'adiabatic', 'basis', 'expansions', 'this', 'approach', 'considerably', 'increases', 'the', 'speed', 'and', 'the', 'energy', 'range', 'over', 'whi... | [-0.07760252408112556, 0.10726483530440652, -0.03027663248038925, 0.05333627097770176, 0.012151975312426818, -0.06524246510744622, 0.007374908092052602, 0.3996202018837222, -0.22684195016271771, -0.32424020302374806, -0.016574621630164967, -0.23955267052327395, -0.01733990492035462, 0.25781234924318847, 0.0778353237526... |
709.0276 | Transport properties controlled by a thermostat: An extended dissipative
particle dynamics thermostat | We introduce a variation of the dissipative particle dynamics (DPD)
thermostat that allows for controlling transport properties of molecular
fluids. The standard DPD thermostat acts only on a relative velocity along the
interatomic axis. Our extension includes the damping of the perpendicular
components of the relati... | cond-mat.soft cond-mat.stat-mech | we introduce a variation of the dissipative particle dynamics dpd thermostat that allows for controlling transport properties of molecular fluids the standard dpd thermostat acts only on a relative velocity along the interatomic axis our extension includes the damping of the perpendicular components of the relative vel... | [['we', 'introduce', 'a', 'variation', 'of', 'the', 'dissipative', 'particle', 'dynamics', 'dpd', 'thermostat', 'that', 'allows', 'for', 'controlling', 'transport', 'properties', 'of', 'molecular', 'fluids', 'the', 'standard', 'dpd', 'thermostat', 'acts', 'only', 'on', 'a', 'relative', 'velocity', 'along', 'the', 'inte... | [-0.14539979013196866, 0.15123797958267146, -0.13774875300968514, 0.01586703833208644, -0.058401193872800676, -0.1410771234009158, -0.0032640106405998613, 0.3299046659970592, -0.30398868029487547, -0.27906326032404244, 0.03908979484112933, -0.2350804563869666, -0.10008457403886935, 0.1928184099407096, 0.005142450146377... |
709.0277 | Nuclear Structure Aspects of the Neutrinoless Double Beta Decay | In this article, we analyze some nuclear structure aspects of the
neutrinoless double beta decay nuclear matrix elements (NME), in the framework
of the Interacting Shell Model. We give results for the decays of 48Ca, 76Ge,
82Se, 124Sn, 128Te, 130Te, and 136Xe, using improved effective interactions and
valence spaces.... | nucl-th | in this article we analyze some nuclear structure aspects of the neutrinoless double beta decay nuclear matrix elements nme in the framework of the interacting shell model we give results for the decays of 48ca 76ge 82se 124sn 128te 130te and 136xe using improved effective interactions and valence spaces we examine the... | [['in', 'this', 'article', 'we', 'analyze', 'some', 'nuclear', 'structure', 'aspects', 'of', 'the', 'neutrinoless', 'double', 'beta', 'decay', 'nuclear', 'matrix', 'elements', 'nme', 'in', 'the', 'framework', 'of', 'the', 'interacting', 'shell', 'model', 'we', 'give', 'results', 'for', 'the', 'decays', 'of', '48ca', '7... | [-0.02781307366379398, 0.23315797276557126, -0.06037159744672418, 0.15171192373778236, 0.052866312625639615, -0.045075342584242846, 0.08353869038995633, 0.33387100438963857, -0.20384549842949243, -0.24463663148406417, -0.003191185238315387, -0.3237460141288156, -0.07925421759941952, 0.1322839469128744, 0.09998230032494... |
709.0278 | Galactic neutrino background from cosmic ray interaction with the ISM
content | We use a diffusive model for the propagation of Galactic cosmic rays to
estimate the charged pion production in interactions with protons of the
interstellar medium. Cosmic ray nuclei from proton to iron are considered and
the corresponding contribution to the neutrino secondary flux produced as a
result of spallatio... | astro-ph | we use a diffusive model for the propagation of galactic cosmic rays to estimate the charged pion production in interactions with protons of the interstellar medium cosmic ray nuclei from proton to iron are considered and the corresponding contribution to the neutrino secondary flux produced as a result of spallation i... | [['we', 'use', 'a', 'diffusive', 'model', 'for', 'the', 'propagation', 'of', 'galactic', 'cosmic', 'rays', 'to', 'estimate', 'the', 'charged', 'pion', 'production', 'in', 'interactions', 'with', 'protons', 'of', 'the', 'interstellar', 'medium', 'cosmic', 'ray', 'nuclei', 'from', 'proton', 'to', 'iron', 'are', 'consider... | [-0.024541035110025474, 0.27364903218156816, -0.030316560174435167, 0.20600794664505026, -0.030679198816629512, -7.108078263524287e-05, 0.004484032737618347, 0.3782995891458583, -0.255441778251585, -0.2942740284257902, -0.08948838022177301, -0.3825725385884069, 0.0713712380669642, 0.17888129871110167, 0.096137790712264... |
709.0279 | Accounting for the Unresolved X-ray Background with Sterile Neutrino
Dark Matter | We consider a scenario where keV sterile neutrinos constitute all of the
currently inferred dark matter abundance, whose radiative decays could
potentially account for the flux contributions to the X-ray background
attributed to unresolved sources. Here we apply integrated flux methods to
results from the observation... | astro-ph | we consider a scenario where kev sterile neutrinos constitute all of the currently inferred dark matter abundance whose radiative decays could potentially account for the flux contributions to the xray background attributed to unresolved sources here we apply integrated flux methods to results from the observations of ... | [['we', 'consider', 'a', 'scenario', 'where', 'kev', 'sterile', 'neutrinos', 'constitute', 'all', 'of', 'the', 'currently', 'inferred', 'dark', 'matter', 'abundance', 'whose', 'radiative', 'decays', 'could', 'potentially', 'account', 'for', 'the', 'flux', 'contributions', 'to', 'the', 'xray', 'background', 'attributed'... | [-0.041929335784740174, 0.19861740450589702, -0.037243650294840336, 0.19223188114567444, -0.12425062180174372, -0.07046116188598367, 0.05078897599059229, 0.34709498531256733, -0.1911270898122054, -0.3800566776798895, 0.046320103300520436, -0.33184955809265376, 0.02124461537370315, 0.19605893256286017, 0.028661654065721... |
709.028 | Asteroseismological constraints on the coolest GW Vir variable star (PG
1159-type)PG 0122+200 | We present an asteroseismological study on PG 0122+200, the coolest known
pulsating PG1159 (GW Vir) star. Our results are based on an augmented set of
the full PG1159 evolutionary models recently presented by Miller Bertolami &
Althaus (2006). We perform extensive computations of adiabatic g-mode pulsation
periods on... | astro-ph | we present an asteroseismological study on pg 0122200 the coolest known pulsating pg1159 gw vir star our results are based on an augmented set of the full pg1159 evolutionary models recently presented by miller bertolami althaus 2006 we perform extensive computations of adiabatic gmode pulsation periods on pg1159 evolu... | [['we', 'present', 'an', 'asteroseismological', 'study', 'on', 'pg', '0122200', 'the', 'coolest', 'known', 'pulsating', 'pg1159', 'gw', 'vir', 'star', 'our', 'results', 'are', 'based', 'on', 'an', 'augmented', 'set', 'of', 'the', 'full', 'pg1159', 'evolutionary', 'models', 'recently', 'presented', 'by', 'miller', 'bert... | [-0.06434443660609511, 0.11572322334963077, -0.10595814915960981, 0.0899440577855707, -0.07506430724609447, -0.06773616016456488, 0.12839499595194534, 0.382509296145725, -0.11192829487165835, -0.3974731516614846, 0.06825217072841085, -0.25144993519496106, -0.0423583689195628, 0.2256611610471963, -0.05995972521860399, 0... |
709.0281 | Detrended Cross-Correlation Analysis: A New Method for Analyzing Two
Non-stationary Time Series | Here we propose a method, based on detrended covariance which we call
detrended cross-correlation analysis (DXA), to investigate power-law
cross-correlations between different simultaneously-recorded time series in the
presence of non-stationarity. We illustrate the method by selected examples
from physics, physiolog... | q-fin.ST cond-mat.stat-mech | here we propose a method based on detrended covariance which we call detrended crosscorrelation analysis dxa to investigate powerlaw crosscorrelations between different simultaneouslyrecorded time series in the presence of nonstationarity we illustrate the method by selected examples from physics physiology and finance | [['here', 'we', 'propose', 'a', 'method', 'based', 'on', 'detrended', 'covariance', 'which', 'we', 'call', 'detrended', 'crosscorrelation', 'analysis', 'dxa', 'to', 'investigate', 'powerlaw', 'crosscorrelations', 'between', 'different', 'simultaneouslyrecorded', 'time', 'series', 'in', 'the', 'presence', 'of', 'nonstat... | [-0.02904214789500324, 0.043942662614693005, -0.17914192944129065, 0.14444939592262593, -0.03777351354322646, -0.12144743450122272, 0.04767899008513224, 0.39515785121063635, -0.27353622412263623, -0.29022959631118106, 0.06946959682433616, -0.31047740256095807, -0.2944752429952709, 0.2560359423798395, -0.035004224185263... |
709.0282 | Theoretical progress on the V_us determination from tau decays | A very precise determination of V_us can be obtained from the semi-inclusive
hadronic decay width of the tau lepton into final states with strangeness. The
ratio of the Cabibbo-suppressed and Cabibbo-allowed tau decay widths directly
measures (V_us/V_ud)^2, up to very small SU(3)-breaking corrections which can
be the... | hep-ph hep-ex | a very precise determination of v_us can be obtained from the semiinclusive hadronic decay width of the tau lepton into final states with strangeness the ratio of the cabibbosuppressed and cabibboallowed tau decay widths directly measures v_usv_ud2 up to very small su3breaking corrections which can be theoretically est... | [['a', 'very', 'precise', 'determination', 'of', 'v_us', 'can', 'be', 'obtained', 'from', 'the', 'semiinclusive', 'hadronic', 'decay', 'width', 'of', 'the', 'tau', 'lepton', 'into', 'final', 'states', 'with', 'strangeness', 'the', 'ratio', 'of', 'the', 'cabibbosuppressed', 'and', 'cabibboallowed', 'tau', 'decay', 'widt... | [-0.020578599155235747, 0.2412797946232156, -0.05988493122232075, 0.08632331632812006, -0.07117959083989263, -0.16784475278467514, 0.09696791455319796, 0.2828002679663209, -0.2336181585327722, -0.27768228651525884, 0.04577514378604694, -0.35643436170827886, 0.08488932804276164, 0.19384502969825498, 0.0613029242063371, ... |
709.0283 | Phylogenetic networks form partial trees | A contemporary and fundamental problem faced by many evolutionary biologists
is how to puzzle together a collection $\mathcal P$ of partial trees
(leaf-labelled trees whose leaves are bijectively labelled by species or, more
generally, taxa, each supported by e. g. a gene) into an overall parental
structure that disp... | math.CO | a contemporary and fundamental problem faced by many evolutionary biologists is how to puzzle together a collection mathcal p of partial trees leaflabelled trees whose leaves are bijectively labelled by species or more generally taxa each supported by e g a gene into an overall parental structure that displays all tree... | [['a', 'contemporary', 'and', 'fundamental', 'problem', 'faced', 'by', 'many', 'evolutionary', 'biologists', 'is', 'how', 'to', 'puzzle', 'together', 'a', 'collection', 'mathcal', 'p', 'of', 'partial', 'trees', 'leaflabelled', 'trees', 'whose', 'leaves', 'are', 'bijectively', 'labelled', 'by', 'species', 'or', 'more', ... | [-0.10722390184557543, 0.10535205567521953, -0.07154321220731304, 0.08712600398135661, -0.11854025845987205, -0.11199540995695323, 0.07961458242703777, 0.37483883050403427, -0.30343520912114813, -0.2897545518099229, 0.08814409845058627, -0.2650564548856884, -0.18760790317925868, 0.15457579251593997, -0.1039453324990957... |
709.0284 | Oort groups and lifting problems | Let k be an algebraically closed field of positive characteristic p. We
consider which finite groups G have the property that every faithful action of
G on a connected smooth projective curve over k lifts to characteristic zero.
Oort conjectured that cyclic groups have this property. We show that if a
cyclic-by-p gro... | math.AG math.GR | let k be an algebraically closed field of positive characteristic p we consider which finite groups g have the property that every faithful action of g on a connected smooth projective curve over k lifts to characteristic zero oort conjectured that cyclic groups have this property we show that if a cyclicbyp group g ha... | [['let', 'k', 'be', 'an', 'algebraically', 'closed', 'field', 'of', 'positive', 'characteristic', 'p', 'we', 'consider', 'which', 'finite', 'groups', 'g', 'have', 'the', 'property', 'that', 'every', 'faithful', 'action', 'of', 'g', 'on', 'a', 'connected', 'smooth', 'projective', 'curve', 'over', 'k', 'lifts', 'to', 'ch... | [-0.2632981562610006, 0.1667660718766066, -0.1672642635669382, -0.030969800947267295, -0.10463384306058288, -0.18606841234335056, -0.0296772346565766, 0.3844529584138876, -0.3513254901128156, -0.195593906427911, 0.050087585528325734, -0.18883160401102422, -0.12204891781134176, 0.17772347121665785, -0.0964341164411356, ... |
709.0285 | Gravitating Dyons with Large Electric Charge | We consider non-Abelian dyons in Einstein-Yang-Mills-Higgs theory. The dyons
are spherically symmetric with unit magnetic charge. For large values of the
electric charge the dyons approach limiting solutions, related to the Penney
solutions of Einstein-Maxwell-scalar theory.
| gr-qc | we consider nonabelian dyons in einsteinyangmillshiggs theory the dyons are spherically symmetric with unit magnetic charge for large values of the electric charge the dyons approach limiting solutions related to the penney solutions of einsteinmaxwellscalar theory | [['we', 'consider', 'nonabelian', 'dyons', 'in', 'einsteinyangmillshiggs', 'theory', 'the', 'dyons', 'are', 'spherically', 'symmetric', 'with', 'unit', 'magnetic', 'charge', 'for', 'large', 'values', 'of', 'the', 'electric', 'charge', 'the', 'dyons', 'approach', 'limiting', 'solutions', 'related', 'to', 'the', 'penney'... | [-0.19753578276787367, 0.18925449127952257, 0.016807750371905666, 0.11165967830715494, -0.02433725818991661, -0.1308345659635961, -0.05132234040259694, 0.2584908771225148, -0.08659138556362854, -0.2641337926809986, 0.01901176426650232, -0.32122163226207096, -0.11069217934790584, 0.09011850619895591, -0.0548728536297049... |
709.0286 | COSY-11 : How will we remember it ? | A personal selection is made of the highlights of the COSY-11 physics program
undertaken at the COoler SYnchrotron of the Forschungszentrum Juelich. This has
been particularly rich in the field of strange and non-strange meson production
in proton-proton and proton-deuteron collisions. The results are considered in
r... | nucl-ex | a personal selection is made of the highlights of the cosy11 physics program undertaken at the cooler synchrotron of the forschungszentrum juelich this has been particularly rich in the field of strange and nonstrange meson production in protonproton and protondeuteron collisions the results are considered in relation ... | [['a', 'personal', 'selection', 'is', 'made', 'of', 'the', 'highlights', 'of', 'the', 'cosy11', 'physics', 'program', 'undertaken', 'at', 'the', 'cooler', 'synchrotron', 'of', 'the', 'forschungszentrum', 'juelich', 'this', 'has', 'been', 'particularly', 'rich', 'in', 'the', 'field', 'of', 'strange', 'and', 'nonstrange'... | [-0.05355290332884197, 0.14653761400240323, -0.16926120482986012, 0.088849046988593, -0.05694543496675549, -0.09139464887970637, 0.025500854374014684, 0.3643449286840135, -0.18764081946198619, -0.26835069015731045, 0.016723518712340943, -0.3816677742081905, 0.03797525326691328, 0.204356292585632, 0.0533541840606279, 0.... |
709.0287 | The Dimension of the Torelli group | We prove that the cohomological dimension of the Torelli group for a closed
connected orientable surface of genus g at least 2 is equal to 3g-5. This
answers a question of Mess, who proved the lower bound and settled the case of
g=2. We also find the cohomological dimension of the Johnson kernel (the
subgroup of the ... | math.GT math.GR | we prove that the cohomological dimension of the torelli group for a closed connected orientable surface of genus g at least 2 is equal to 3g5 this answers a question of mess who proved the lower bound and settled the case of g2 we also find the cohomological dimension of the johnson kernel the subgroup of the torelli ... | [['we', 'prove', 'that', 'the', 'cohomological', 'dimension', 'of', 'the', 'torelli', 'group', 'for', 'a', 'closed', 'connected', 'orientable', 'surface', 'of', 'genus', 'g', 'at', 'least', '2', 'is', 'equal', 'to', '3g5', 'this', 'answers', 'a', 'question', 'of', 'mess', 'who', 'proved', 'the', 'lower', 'bound', 'and'... | [-0.20296667334298754, 0.11533217412571228, -0.15370915020823248, 0.08696643645196518, -0.10048420394431481, -0.14592887007436434, 0.0345693663134449, 0.2847803504487803, -0.2907909848402406, -0.26162776740831, 0.10976854171658065, -0.252087873475294, -0.14652492218224925, 0.2442171562448606, -0.17093690325390518, -0.0... |
709.0288 | Gluino Stransverse Mass | We introduce a new observable, 'gluino stransverse mass', which is an
application of the Cambridge $m_{T2}$ variable to the process where gluinos are
pair produced in proton-proton collision and each gluino subsequently decays
into two quarks and one LSP, $i.e. \tilde{g}\tilde{g} \to qq\tilde\chi_1^0\
qq\tilde\chi_1^... | hep-ph | we introduce a new observable gluino stransverse mass which is an application of the cambridge m_t2 variable to the process where gluinos are pair produced in protonproton collision and each gluino subsequently decays into two quarks and one lsp ie tildegtildeg to qqtildechi_10 qqtildechi_10 we show that the gluino str... | [['we', 'introduce', 'a', 'new', 'observable', 'gluino', 'stransverse', 'mass', 'which', 'is', 'an', 'application', 'of', 'the', 'cambridge', 'm_t2', 'variable', 'to', 'the', 'process', 'where', 'gluinos', 'are', 'pair', 'produced', 'in', 'protonproton', 'collision', 'and', 'each', 'gluino', 'subsequently', 'decays', '... | [-0.032040801189011994, 0.3389159386112523, -0.058412766699782674, 0.2372050392953396, -0.09475160069091039, -0.1656588786592086, 0.06289701601102328, 0.3443332618645703, -0.19934527312094966, -0.2973485389155232, 0.02309439211644025, -0.27152782012191085, 0.10107713910337124, 0.16098433955081015, 0.05103547333144686, ... |
709.0289 | Cryptography in the Bounded-Quantum-Storage Model | This thesis initiates the study of cryptographic protocols in the
bounded-quantum-storage model. On the practical side, simple protocols for
Rabin Oblivious Transfer, 1-2 Oblivious Transfer and Bit Commitment are
presented. No quantum memory is required for honest players, whereas the
protocols can only be broken by ... | quant-ph cs.CR | this thesis initiates the study of cryptographic protocols in the boundedquantumstorage model on the practical side simple protocols for rabin oblivious transfer 12 oblivious transfer and bit commitment are presented no quantum memory is required for honest players whereas the protocols can only be broken by an adversa... | [['this', 'thesis', 'initiates', 'the', 'study', 'of', 'cryptographic', 'protocols', 'in', 'the', 'boundedquantumstorage', 'model', 'on', 'the', 'practical', 'side', 'simple', 'protocols', 'for', 'rabin', 'oblivious', 'transfer', '12', 'oblivious', 'transfer', 'and', 'bit', 'commitment', 'are', 'presented', 'no', 'quan... | [-0.1929073793411909, 0.07011172606510675, -0.05754356139929581, 0.11876512499426613, -0.0005857633455222799, -0.33644615430455965, 0.12259101493902619, 0.35090281581595, -0.26576155841435867, -0.303825965401281, 0.08759510854191595, -0.2222786997890372, -0.04988796663477676, 0.25174424004872537, -0.19446132429306687, ... |
709.029 | $\mathbb{Z}_{2}^{2}$-cordiality of complete and complete bipartite
graphs | We prove that $K_{n}$ is $\mathbb{Z}_{2}^{2}$-cordial if and only if $1 \leq
n \leq 3$ and that $K_{m,n}$ is $\mathbb{Z}_{2}^{2}$ if and only if it is false
that $m=n=2$.
| math.CO | we prove that k_n is mathbbz_22cordial if and only if 1 leq n leq 3 and that k_mn is mathbbz_22 if and only if it is false that mn2 | [['we', 'prove', 'that', 'k_n', 'is', 'mathbbz_22cordial', 'if', 'and', 'only', 'if', '1', 'leq', 'n', 'leq', '3', 'and', 'that', 'k_mn', 'is', 'mathbbz_22', 'if', 'and', 'only', 'if', 'it', 'is', 'false', 'that', 'mn2']] | [-0.1301561841475112, 0.2592041424276041, 0.01472091388755611, 0.03333218009460585, -0.013209158745926939, -0.3105241077552949, 0.023420879883425578, 0.4428757881479604, -0.23017913473969592, -0.24891759448551706, 0.15919782538964813, -0.3923219812235662, -0.1694859516490916, 0.13504119639817094, -0.05817799290109958, ... |
709.0291 | Equivalences on Acyclic Orientations | The cyclic and dihedral groups can be made to act on the set Acyc(Y) of
acyclic orientations of an undirected graph Y, and this gives rise to the
equivalence relations ~kappa and ~delta, respectively. These two actions and
their corresponding equivalence classes are closely related to combinatorial
problems arising i... | math.CO math.DS | the cyclic and dihedral groups can be made to act on the set acycy of acyclic orientations of an undirected graph y and this gives rise to the equivalence relations kappa and delta respectively these two actions and their corresponding equivalence classes are closely related to combinatorial problems arising in the con... | [['the', 'cyclic', 'and', 'dihedral', 'groups', 'can', 'be', 'made', 'to', 'act', 'on', 'the', 'set', 'acycy', 'of', 'acyclic', 'orientations', 'of', 'an', 'undirected', 'graph', 'y', 'and', 'this', 'gives', 'rise', 'to', 'the', 'equivalence', 'relations', 'kappa', 'and', 'delta', 'respectively', 'these', 'two', 'actio... | [-0.13807090084188647, 0.11366067098792247, -0.05459956503315185, 0.052151500057774566, -0.08959538256999866, -0.12856898147435059, 0.0437166688811054, 0.3922268498728993, -0.3758256684447969, -0.2914075581963995, 0.07418144628610862, -0.28835424471163673, -0.13813772020480966, 0.15436555975447258, -0.13124388141647703... |
709.0292 | On the relation between the Schmidt and Kennicutt-Schmidt star formation
laws and its implications for numerical simulations | When averaged over large scales, star formation in galaxies is observed to
follow the empirical Kennicutt-Schmidt (KS) law for surface densities above a
constant threshold. While the observed law involves surface densities,
theoretical models and simulations generally work with volume density laws
(i.e. Schmidt laws)... | astro-ph | when averaged over large scales star formation in galaxies is observed to follow the empirical kennicuttschmidt ks law for surface densities above a constant threshold while the observed law involves surface densities theoretical models and simulations generally work with volume density laws ie schmidt laws we derive a... | [['when', 'averaged', 'over', 'large', 'scales', 'star', 'formation', 'in', 'galaxies', 'is', 'observed', 'to', 'follow', 'the', 'empirical', 'kennicuttschmidt', 'ks', 'law', 'for', 'surface', 'densities', 'above', 'a', 'constant', 'threshold', 'while', 'the', 'observed', 'law', 'involves', 'surface', 'densities', 'the... | [-0.06011662742756584, 0.10248181813871046, -0.12619259271279087, 0.11372237798513768, -0.10203272661845092, -0.0851279558167277, 0.05580644371666596, 0.3841139948251744, -0.19653899568915506, -0.37089307348635114, 0.039203510875034674, -0.24476406752343072, -0.0763050744820799, 0.1840000666213156, -0.01297840547659624... |
709.0293 | The Effective Field Theory of Inflation | We study the effective field theory of inflation, i.e. the most general
theory describing the fluctuations around a quasi de Sitter background, in the
case of single field models. The scalar mode can be eaten by the metric by
going to unitary gauge. In this gauge, the most general theory is built with
the lowest dime... | hep-th astro-ph hep-ph | we study the effective field theory of inflation ie the most general theory describing the fluctuations around a quasi de sitter background in the case of single field models the scalar mode can be eaten by the metric by going to unitary gauge in this gauge the most general theory is built with the lowest dimension ope... | [['we', 'study', 'the', 'effective', 'field', 'theory', 'of', 'inflation', 'ie', 'the', 'most', 'general', 'theory', 'describing', 'the', 'fluctuations', 'around', 'a', 'quasi', 'de', 'sitter', 'background', 'in', 'the', 'case', 'of', 'single', 'field', 'models', 'the', 'scalar', 'mode', 'can', 'be', 'eaten', 'by', 'th... | [-0.15998488855456897, 0.2052897893439627, -0.09080902615172509, 0.10339772225025846, -0.07758589339552119, -0.14700514865503495, -0.039280478381460496, 0.2966641480699668, -0.2238712794607006, -0.27009202467484605, 0.06473881241582408, -0.24448052242718213, -0.13702782951112763, 0.1600719198548034, -0.0347761384270829... |
709.0294 | Brane-world inflation: slow-roll corrections to the spectral index | We quantify the slow-roll corrections to primordial density perturbations
arising from inflation driven by a four-dimensional scalar field with a
monomial potential in a five-dimensional non-compact bulk spacetime. Although
the difference between the classical brane-world solutions and standard
four-dimensional solut... | astro-ph gr-qc hep-th | we quantify the slowroll corrections to primordial density perturbations arising from inflation driven by a fourdimensional scalar field with a monomial potential in a fivedimensional noncompact bulk spacetime although the difference between the classical braneworld solutions and standard fourdimensional solutions is l... | [['we', 'quantify', 'the', 'slowroll', 'corrections', 'to', 'primordial', 'density', 'perturbations', 'arising', 'from', 'inflation', 'driven', 'by', 'a', 'fourdimensional', 'scalar', 'field', 'with', 'a', 'monomial', 'potential', 'in', 'a', 'fivedimensional', 'noncompact', 'bulk', 'spacetime', 'although', 'the', 'diff... | [-0.13672379859384487, 0.16754825005773455, -0.10418894583232362, 0.09940674921778157, -0.051453447371551934, -0.09341710415901616, -0.06319687143232758, 0.2491701478985223, -0.19090884098973634, -0.2743804140270434, 0.06368271485023963, -0.28367957968095486, -0.12688891010475345, 0.1191402028171896, -0.077799194915728... |
709.0295 | On the consistency relation of the 3-point function in single field
inflation | The consistency relation for the 3-point function of the CMB is a very
powerful observational signature which is believed to be true for every
inflationary model in which there is only one dynamical degree of freedom. Its
importance relies on the fact that deviations from it might be detected in next
generation exper... | hep-th astro-ph hep-ph | the consistency relation for the 3point function of the cmb is a very powerful observational signature which is believed to be true for every inflationary model in which there is only one dynamical degree of freedom its importance relies on the fact that deviations from it might be detected in next generation experimen... | [['the', 'consistency', 'relation', 'for', 'the', '3point', 'function', 'of', 'the', 'cmb', 'is', 'a', 'very', 'powerful', 'observational', 'signature', 'which', 'is', 'believed', 'to', 'be', 'true', 'for', 'every', 'inflationary', 'model', 'in', 'which', 'there', 'is', 'only', 'one', 'dynamical', 'degree', 'of', 'free... | [-0.11665758513285815, 0.1093093403605263, -0.15251579237295887, 0.13415132326750048, -0.13702098223327014, -0.17726310469823567, 0.024575073752203025, 0.3120363918849482, -0.23326336722283697, -0.2849105157925246, 0.10735914344975474, -0.2140932515881454, -0.1403100537180972, 0.23133935859032834, -0.000189754476125996... |
709.0296 | The pattern of growth in viable f(R) cosmologies | We study the evolution of linear perturbations in metric f(R) models of
gravity and identify a potentially observable characteristic scale-dependent
pattern in the behavior of cosmological structures. While at the background
level viable f(R) models must closely mimic LCDM, the differences in their
prediction for the... | astro-ph gr-qc | we study the evolution of linear perturbations in metric fr models of gravity and identify a potentially observable characteristic scaledependent pattern in the behavior of cosmological structures while at the background level viable fr models must closely mimic lcdm the differences in their prediction for the growth o... | [['we', 'study', 'the', 'evolution', 'of', 'linear', 'perturbations', 'in', 'metric', 'fr', 'models', 'of', 'gravity', 'and', 'identify', 'a', 'potentially', 'observable', 'characteristic', 'scaledependent', 'pattern', 'in', 'the', 'behavior', 'of', 'cosmological', 'structures', 'while', 'at', 'the', 'background', 'lev... | [-0.17080893550847984, 0.09559099884238795, -0.10749308276682719, 0.11672615286605208, -0.07374678666041379, -0.10227241351953652, -0.0656265963615109, 0.33003170549847094, -0.26354175625391396, -0.3061384908568832, 0.08789481611148152, -0.23189760756774255, -0.1557528185630105, 0.16610991220966162, -0.0044281085930674... |
709.0297 | Goldilocks Supersymmetry: Simultaneous Solution to the Dark Matter and
Flavor Problems of Supersymmetry | Neutralino dark matter is well motivated, but also suffers from two
shortcomings: it requires gravity-mediated supersymmetry breaking, which
generically violates flavor constraints, and its thermal relic density \Omega
is typically too large. We propose a simple solution to both problems:
neutralinos freezeout with \... | hep-ph astro-ph hep-th | neutralino dark matter is well motivated but also suffers from two shortcomings it requires gravitymediated supersymmetry breaking which generically violates flavor constraints and its thermal relic density omega is typically too large we propose a simple solution to both problems neutralinos freezeout with omega 10100... | [['neutralino', 'dark', 'matter', 'is', 'well', 'motivated', 'but', 'also', 'suffers', 'from', 'two', 'shortcomings', 'it', 'requires', 'gravitymediated', 'supersymmetry', 'breaking', 'which', 'generically', 'violates', 'flavor', 'constraints', 'and', 'its', 'thermal', 'relic', 'density', 'omega', 'is', 'typically', 't... | [-0.11997135093649074, 0.28654818949871697, -0.10060427766681339, 0.20704928415216273, -0.1844625938538229, -0.22552476791558243, -0.003596088230551686, 0.3250477228163315, -0.271399915034029, -0.3609462816481634, 0.09886661395042513, -0.22125048809296763, 0.014116007776465267, 0.12353686956703314, -0.03976317818160169... |
709.0298 | Narrow-band surveys for very high redshift Lyman-alpha emitters | Context: Many current and future surveys aim to detect the highest redshift
(z >~ 7) sources through their Lyman-alpha (Ly-alpha) emission, using the
narrow-band imaging method. However, to date the surveys have only yielded
non-detections and upper limits as no survey has reached the necessary
combination of depth a... | astro-ph | context many current and future surveys aim to detect the highest redshift z 7 sources through their lymanalpha lyalpha emission using the narrowband imaging method however to date the surveys have only yielded nondetections and upper limits as no survey has reached the necessary combination of depth and area to detect... | [['context', 'many', 'current', 'and', 'future', 'surveys', 'aim', 'to', 'detect', 'the', 'highest', 'redshift', 'z', '7', 'sources', 'through', 'their', 'lymanalpha', 'lyalpha', 'emission', 'using', 'the', 'narrowband', 'imaging', 'method', 'however', 'to', 'date', 'the', 'surveys', 'have', 'only', 'yielded', 'nondete... | [-0.020220996612258155, 0.07643193437618769, -0.034335578845117155, 0.13612910969456557, -0.11864100388101949, -0.1375295262310995, 0.05641826870762352, 0.48383325472374566, -0.1389893895114651, -0.3603823678105899, 0.09228007039028568, -0.3313714361443888, -0.02277529579658374, 0.2500442682369079, 0.053755162521885294... |
709.0299 | Binary black hole merger: symmetry and the spin expansion | We regard binary black hole (BBH) merger as a map from a simple initial state
(two Kerr black holes, with dimensionless spins {\bf a} and {\bf b}) to a
simple final state (a Kerr black hole with mass m, dimensionless spin {\bf s},
and kick velocity {\bf k}). By expanding this map around {\bf a} = {\bf b} = 0
and appl... | gr-qc astro-ph hep-ph hep-th | we regard binary black hole bbh merger as a map from a simple initial state two kerr black holes with dimensionless spins bf a and bf b to a simple final state a kerr black hole with mass m dimensionless spin bf s and kick velocity bf k by expanding this map around bf a bf b 0 and applying symmetry constraints we obtai... | [['we', 'regard', 'binary', 'black', 'hole', 'bbh', 'merger', 'as', 'a', 'map', 'from', 'a', 'simple', 'initial', 'state', 'two', 'kerr', 'black', 'holes', 'with', 'dimensionless', 'spins', 'bf', 'a', 'and', 'bf', 'b', 'to', 'a', 'simple', 'final', 'state', 'a', 'kerr', 'black', 'hole', 'with', 'mass', 'm', 'dimensionl... | [-0.18192614108923957, 0.08868820679705455, -0.06029723597656902, 0.04373988746623467, -0.1510741715529212, -0.15713605747835055, 0.07207343156181008, 0.3425818390070318, -0.14673838530339905, -0.28022905016267624, 0.04913715194692617, -0.2628507282593296, -0.09439001262171177, 0.22156821175579083, 0.005887419908299102... |
709.03 | Decoding the spectra of SDSS early-type galaxies: New indicators of age
and recent star formation | (Abridged) We apply Principal Component Analysis (PCA) to a sample of
early-type galaxies from the Sloan Digital Sky Survey (SDSS) in order to infer
differences in their star formation histories. Out of the first few principal
components (PC), we study four which give information about stellar populations
and velocit... | astro-ph | abridged we apply principal component analysis pca to a sample of earlytype galaxies from the sloan digital sky survey sdss in order to infer differences in their star formation histories out of the first few principal components pc we study four which give information about stellar populations and velocity dispersion ... | [['abridged', 'we', 'apply', 'principal', 'component', 'analysis', 'pca', 'to', 'a', 'sample', 'of', 'earlytype', 'galaxies', 'from', 'the', 'sloan', 'digital', 'sky', 'survey', 'sdss', 'in', 'order', 'to', 'infer', 'differences', 'in', 'their', 'star', 'formation', 'histories', 'out', 'of', 'the', 'first', 'few', 'pri... | [-0.09383659883285872, 0.08971636135014706, -0.0940031291428022, 0.06877721860713791, -0.07969887610292062, -0.013699278717394918, 0.039396585747599605, 0.4177417769469321, -0.145875147197512, -0.35953641614876686, 0.05030205065617338, -0.28865281672682613, -0.059853327143937346, 0.18945843159861397, -0.047481947010064... |
709.0301 | Geometrically induced singular behavior of entanglement | We show that the geometry of the set of quantum states plays a crucial role
in the behavior of entanglement in different physical systems. More
specifically it is shown that singular points at the border of the set of
unentangled states appear as singularities in the dynamics of entanglement of
smoothly varying quant... | quant-ph | we show that the geometry of the set of quantum states plays a crucial role in the behavior of entanglement in different physical systems more specifically it is shown that singular points at the border of the set of unentangled states appear as singularities in the dynamics of entanglement of smoothly varying quantum ... | [['we', 'show', 'that', 'the', 'geometry', 'of', 'the', 'set', 'of', 'quantum', 'states', 'plays', 'a', 'crucial', 'role', 'in', 'the', 'behavior', 'of', 'entanglement', 'in', 'different', 'physical', 'systems', 'more', 'specifically', 'it', 'is', 'shown', 'that', 'singular', 'points', 'at', 'the', 'border', 'of', 'the... | [-0.15905987449237913, 0.17629370782995904, -0.12707350486771593, 0.055115679939147795, 0.018953249777985525, -0.1391382858899858, 0.03207247952423707, 0.3085384126516837, -0.2523408135092711, -0.25984873504766937, 0.05891604010675904, -0.28273700371007376, -0.191869861169282, 0.1872211795099834, -0.022541456455011155,... |
709.0302 | SN 2005ap: A Most Brilliant Explosion | We present unfiltered photometric observations with ROTSE-III and optical
spectroscopic follow-up with the HET and Keck of the most luminous supernova
yet identified, SN 2005ap. The spectra taken about 3 days before and 6 days
after maximum light show narrow emission lines (likely originating in the dwarf
host) and a... | astro-ph | we present unfiltered photometric observations with rotseiii and optical spectroscopic followup with the het and keck of the most luminous supernova yet identified sn 2005ap the spectra taken about 3 days before and 6 days after maximum light show narrow emission lines likely originating in the dwarf host and absorptio... | [['we', 'present', 'unfiltered', 'photometric', 'observations', 'with', 'rotseiii', 'and', 'optical', 'spectroscopic', 'followup', 'with', 'the', 'het', 'and', 'keck', 'of', 'the', 'most', 'luminous', 'supernova', 'yet', 'identified', 'sn', '2005ap', 'the', 'spectra', 'taken', 'about', '3', 'days', 'before', 'and', '6'... | [-0.022708810620935837, 0.09883332367571922, -0.031947221449001646, 0.08651597153750716, -0.12936972483125855, -0.17748087426954395, 0.06920203553698419, 0.496824155254774, -0.15976505182338427, -0.31168262725103796, 0.07995583357846613, -0.36550967673625734, 0.0002462328801932879, 0.20741966743296586, -0.0139876675962... |
709.0303 | Navigability of Complex Networks | Routing information through networks is a universal phenomenon in both
natural and manmade complex systems. When each node has full knowledge of the
global network connectivity, finding short communication paths is merely a
matter of distributed computation. However, in many real networks nodes
communicate efficientl... | physics.soc-ph cond-mat.dis-nn cs.NI | routing information through networks is a universal phenomenon in both natural and manmade complex systems when each node has full knowledge of the global network connectivity finding short communication paths is merely a matter of distributed computation however in many real networks nodes communicate efficiently even... | [['routing', 'information', 'through', 'networks', 'is', 'a', 'universal', 'phenomenon', 'in', 'both', 'natural', 'and', 'manmade', 'complex', 'systems', 'when', 'each', 'node', 'has', 'full', 'knowledge', 'of', 'the', 'global', 'network', 'connectivity', 'finding', 'short', 'communication', 'paths', 'is', 'merely', 'a... | [-0.21097560766886206, 0.06402589584767228, -0.03639136405384287, 0.10171524642352411, -0.1335283556081196, -0.16711443416932795, 0.08014471614601236, 0.4251025554010684, -0.3225354832590472, -0.3027546486638962, 0.07342573121133927, -0.23105787092172508, -0.31769261610403604, 0.16757801872453526, -0.07012431470471672,... |
709.0304 | Wind and boundary layers in Rayleigh-Benard convection. I: analysis and
modeling | The aim of this paper is to contribute to the understanding and to model the
processes controlling the amplitude of the wind of Rayleigh-Benard convection.
We analyze results from direct simulation of an L/H = 4 aspect-ratio domain
with periodic sidewalls at Ra = 1e5; 1e6; 1e7; 1e8 and at Pr = 1 by decomposing
indepe... | physics.flu-dyn | the aim of this paper is to contribute to the understanding and to model the processes controlling the amplitude of the wind of rayleighbenard convection we analyze results from direct simulation of an lh 4 aspectratio domain with periodic sidewalls at ra 1e5 1e6 1e7 1e8 and at pr 1 by decomposing independent realizati... | [['the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'contribute', 'to', 'the', 'understanding', 'and', 'to', 'model', 'the', 'processes', 'controlling', 'the', 'amplitude', 'of', 'the', 'wind', 'of', 'rayleighbenard', 'convection', 'we', 'analyze', 'results', 'from', 'direct', 'simulation', 'of', 'an', 'lh', '4', 'aspec... | [-0.15074887988649466, 0.19693427340805525, -0.017210232714811962, 0.03435298077491038, -0.02464911379269871, -0.059851164028853036, 0.013569206816467845, 0.31126681782147836, -0.27873280893643976, -0.3336029899582057, 0.07164611426065129, -0.24037445349916117, -0.07255667089615804, 0.21682319424701024, 0.0008452258678... |
709.0305 | A note on the uniqueness of global static decompositions | We discuss when static Killing vector fields are standard, that is, leading
to a global orthogonal splitting of the spacetime. We prove that such an
orthogonal splitting is unique whenever the natural space is compact. This is
carried out by proving that many notable spacelike submanifolds must be
contained in an ort... | gr-qc | we discuss when static killing vector fields are standard that is leading to a global orthogonal splitting of the spacetime we prove that such an orthogonal splitting is unique whenever the natural space is compact this is carried out by proving that many notable spacelike submanifolds must be contained in an orthogona... | [['we', 'discuss', 'when', 'static', 'killing', 'vector', 'fields', 'are', 'standard', 'that', 'is', 'leading', 'to', 'a', 'global', 'orthogonal', 'splitting', 'of', 'the', 'spacetime', 'we', 'prove', 'that', 'such', 'an', 'orthogonal', 'splitting', 'is', 'unique', 'whenever', 'the', 'natural', 'space', 'is', 'compact'... | [-0.21621475642126414, 0.12186530393204696, -0.06955385631731441, 0.10166925038473922, -0.12987526091596774, -0.10353609477169812, -0.06075664514285182, 0.41085736186153465, -0.2836592436783136, -0.15327757239461906, 0.12674804282752092, -0.2121257869406573, -0.15000809816222999, 0.1649103295283332, -0.0924431543061209... |
709.0306 | Hydrodynamic behavior of one dimensional subdiffusive exclusion
processes with random conductances | Consider a system of particles performing nearest neighbor random walks on
the lattice $\ZZ$ under hard--core interaction. The rate for a jump over a
given bond is direction--independent and the inverse of the jump rates are
i.i.d. random variables belonging to the domain of attraction of an
$\a$--stable law, $0<\a<1... | math.PR math-ph math.MP | consider a system of particles performing nearest neighbor random walks on the lattice zz under hardcore interaction the rate for a jump over a given bond is directionindependent and the inverse of the jump rates are iid random variables belonging to the domain of attraction of an astable law 0a1 this exclusion process... | [['consider', 'a', 'system', 'of', 'particles', 'performing', 'nearest', 'neighbor', 'random', 'walks', 'on', 'the', 'lattice', 'zz', 'under', 'hardcore', 'interaction', 'the', 'rate', 'for', 'a', 'jump', 'over', 'a', 'given', 'bond', 'is', 'directionindependent', 'and', 'the', 'inverse', 'of', 'the', 'jump', 'rates', ... | [-0.1481851818744184, 0.20030105147079888, -0.06895395872046853, 0.053088559601270034, -0.01883138702307805, -0.21220145608218977, 0.07027732449294091, 0.34844313509103547, -0.30456550780502034, -0.1640720773252613, 0.08610527881310412, -0.3045785185574304, -0.07991255713745997, 0.12370799697450044, 0.02174238016170154... |
709.0307 | Nonlinear growth in modified gravity theories of dark energy | Theoretical differences in the growth of structure offer the possibility that
we might distinguish between modified gravity theories of dark energy and
\LambdaCDM. A significant impediment to applying current and prospective large
scale galaxy and weak lensing surveys to this problem is that, while the mildly
nonline... | astro-ph gr-qc | theoretical differences in the growth of structure offer the possibility that we might distinguish between modified gravity theories of dark energy and lambdacdm a significant impediment to applying current and prospective large scale galaxy and weak lensing surveys to this problem is that while the mildly nonlinear re... | [['theoretical', 'differences', 'in', 'the', 'growth', 'of', 'structure', 'offer', 'the', 'possibility', 'that', 'we', 'might', 'distinguish', 'between', 'modified', 'gravity', 'theories', 'of', 'dark', 'energy', 'and', 'lambdacdm', 'a', 'significant', 'impediment', 'to', 'applying', 'current', 'and', 'prospective', 'l... | [-0.0808541494458263, 0.0634726842633534, -0.09841844861855217, 0.10637531410211364, -0.09440933797288865, -0.13383405968062906, -0.014391766994780815, 0.32697605687563663, -0.2389256170682414, -0.3376430099236262, 0.05439194381098755, -0.27296369045761343, -0.15358271332270584, 0.20270420878202405, -0.0167687497921206... |
709.0308 | More Rings to rule them all : Fragmentation, 4D/5D and Split-Spectral
Flows | In this note we set-up an explicit 5D construction of AdS-fragmentation,
whereby a single black ring splits-up into a multi-black ring configuration.
Furthermore it is seen that these fragmented rings are equivalent to a direct
5D lift of 4D multi-center black holes. Along the way we also determine the
4D/5D transfor... | hep-th | in this note we setup an explicit 5d construction of adsfragmentation whereby a single black ring splitsup into a multiblack ring configuration furthermore it is seen that these fragmented rings are equivalent to a direct 5d lift of 4d multicenter black holes along the way we also determine the 4d5d transformations rel... | [['in', 'this', 'note', 'we', 'setup', 'an', 'explicit', '5d', 'construction', 'of', 'adsfragmentation', 'whereby', 'a', 'single', 'black', 'ring', 'splitsup', 'into', 'a', 'multiblack', 'ring', 'configuration', 'furthermore', 'it', 'is', 'seen', 'that', 'these', 'fragmented', 'rings', 'are', 'equivalent', 'to', 'a', '... | [-0.163651198930754, 0.061828957698423455, -0.05407372839350737, 0.11060021611246927, -0.04456634924559097, -0.10580247095323929, -0.03255432261729912, 0.3413166632264398, -0.20943335885935613, -0.26643859166723055, 0.06576273569442645, -0.2549164274188455, -0.13234537018389478, 0.15899607326607895, -0.1000260592932379... |
709.0309 | Somewhat stochastic matrices | The standard theorem for regular stochastic matrices is generalized to
matrices with no sign restriction on the entries. The condition that column
sums be equal to 1 is kept, but the regularity condition is replaced by a
condition on the $\ell_1$-distances between columns.
| math.RA | the standard theorem for regular stochastic matrices is generalized to matrices with no sign restriction on the entries the condition that column sums be equal to 1 is kept but the regularity condition is replaced by a condition on the ell_1distances between columns | [['the', 'standard', 'theorem', 'for', 'regular', 'stochastic', 'matrices', 'is', 'generalized', 'to', 'matrices', 'with', 'no', 'sign', 'restriction', 'on', 'the', 'entries', 'the', 'condition', 'that', 'column', 'sums', 'be', 'equal', 'to', '1', 'is', 'kept', 'but', 'the', 'regularity', 'condition', 'is', 'replaced',... | [-0.13282527898194357, 0.1533716779778756, -0.01876869930752686, 0.06183730371551411, -0.06946308658059154, -0.17911129496947287, 0.038790237119731806, 0.33586196202252594, -0.28509504951181863, -0.2075608454068147, 0.19773776988898004, -0.2723580600826868, -0.0882614790240214, 0.12378798764465111, -0.10219799157320744... |
709.031 | On the uniformity of the Iitaka fibration | We study pluricanonical systems on smooth projective varieties of positive
Kodaira dimension, following the approach of Hacon-McKernan, Takayama and Tsuji
succesfully used in the case of varieties of general type. We prove a
uniformity result for the Iitaka fibration of smooth projective varieties of
positive Kodaira... | math.AG math.CV | we study pluricanonical systems on smooth projective varieties of positive kodaira dimension following the approach of haconmckernan takayama and tsuji succesfully used in the case of varieties of general type we prove a uniformity result for the iitaka fibration of smooth projective varieties of positive kodaira dimen... | [['we', 'study', 'pluricanonical', 'systems', 'on', 'smooth', 'projective', 'varieties', 'of', 'positive', 'kodaira', 'dimension', 'following', 'the', 'approach', 'of', 'haconmckernan', 'takayama', 'and', 'tsuji', 'succesfully', 'used', 'in', 'the', 'case', 'of', 'varieties', 'of', 'general', 'type', 'we', 'prove', 'a'... | [-0.2126660204140117, -0.05677633557619678, -0.08885270036203233, 0.10145954076339163, -0.06400571448879468, -0.23501765840007244, -0.035546412376837956, 0.2752621085697634, -0.27297459279400976, -0.14459244604851748, 0.08442429055277309, -0.24172436564254599, -0.16882319642683943, 0.23666492773761116, -0.2439581933053... |
709.0311 | Lower bounds for the volume of hyperbolic $n$-orbifolds | In this paper an explicit formula for a lower bound on the volume of a
hyperbolic orbifold, dependent on dimension and the maximal order of torsion in
the orbifolds' fundamental group, is constructed.
| math.GT math.DG | in this paper an explicit formula for a lower bound on the volume of a hyperbolic orbifold dependent on dimension and the maximal order of torsion in the orbifolds fundamental group is constructed | [['in', 'this', 'paper', 'an', 'explicit', 'formula', 'for', 'a', 'lower', 'bound', 'on', 'the', 'volume', 'of', 'a', 'hyperbolic', 'orbifold', 'dependent', 'on', 'dimension', 'and', 'the', 'maximal', 'order', 'of', 'torsion', 'in', 'the', 'orbifolds', 'fundamental', 'group', 'is', 'constructed']] | [-0.18401139997171634, 0.1175053657749562, -0.08766696164666703, 0.0887408610997778, -0.09480091420030504, -0.07337977367481499, 0.038088108134230206, 0.26851004068598605, -0.18268901019385367, -0.2542861953490611, 0.13825812699470783, -0.23463042505141912, -0.1516001567131642, 0.2485791352210623, -0.14716845598410477,... |
709.0312 | Vortices in a mesoscopic superconducting circular sector | In the present paper we develop an algorithm to solve the time dependent
Ginzburg-Landau (TDGL) equations, by using the link variables technique, for
circular geometries. In addition, we evaluate the Helmholtz and Gibbs free
energy, the magnetization, and the number of vortices. This algorithm is
applied to a circula... | cond-mat.supr-con | in the present paper we develop an algorithm to solve the time dependent ginzburglandau tdgl equations by using the link variables technique for circular geometries in addition we evaluate the helmholtz and gibbs free energy the magnetization and the number of vortices this algorithm is applied to a circular sector we ... | [['in', 'the', 'present', 'paper', 'we', 'develop', 'an', 'algorithm', 'to', 'solve', 'the', 'time', 'dependent', 'ginzburglandau', 'tdgl', 'equations', 'by', 'using', 'the', 'link', 'variables', 'technique', 'for', 'circular', 'geometries', 'in', 'addition', 'we', 'evaluate', 'the', 'helmholtz', 'and', 'gibbs', 'free'... | [-0.15622201224168142, 0.1409412911738036, -0.09319841479261716, 0.05955245281259219, -0.07668840741117795, -0.0675337867376705, 0.05886597124083588, 0.3669800830880801, -0.24123557347804309, -0.31229407761245964, 0.06607248759828507, -0.22230172254145145, -0.14439212920765082, 0.16730783476804695, 0.016668513181308905... |
709.0313 | Geodesic cusp excursions and metric diophantine approximation | We derive several results that describe the rate at which a generic geodesic
makes excursions into and out of a cusp on a finite area hyperbolic surface and
relate them to approximation with respect to the orbit of infinity for an
associated Fuchsian group. This provides proofs of some well known theorems
from metric... | math.GT math.DS math.NT | we derive several results that describe the rate at which a generic geodesic makes excursions into and out of a cusp on a finite area hyperbolic surface and relate them to approximation with respect to the orbit of infinity for an associated fuchsian group this provides proofs of some well known theorems from metric di... | [['we', 'derive', 'several', 'results', 'that', 'describe', 'the', 'rate', 'at', 'which', 'a', 'generic', 'geodesic', 'makes', 'excursions', 'into', 'and', 'out', 'of', 'a', 'cusp', 'on', 'a', 'finite', 'area', 'hyperbolic', 'surface', 'and', 'relate', 'them', 'to', 'approximation', 'with', 'respect', 'to', 'the', 'orb... | [-0.139375002158668, 0.045750269618969164, -0.15999659509594802, 0.09426239940082051, -0.11337085692605502, -0.11783334217362211, 0.06250162818797038, 0.30377601025442424, -0.28105900457299404, -0.22235610737206257, 0.11427186441142112, -0.2874007264388279, -0.16454270433529583, 0.3005290142306402, -0.12669889537066642... |
709.0314 | The Electric Dipole Moment of the Nucleons in Holographic QCD | We introduce the strong CP-violation in the framework of AdS/QCD model and
calculate the electric dipole moments of nucleons as well as the CP-violating
pion-nucleon coupling. Our holographic estimate of the electric dipole moments
gives for the neutron d_n=1.08 X 10^{-16} theta (e cm), which is comparable
with previ... | hep-ph hep-th nucl-th | we introduce the strong cpviolation in the framework of adsqcd model and calculate the electric dipole moments of nucleons as well as the cpviolating pionnucleon coupling our holographic estimate of the electric dipole moments gives for the neutron d_n108 x 1016 theta e cm which is comparable with previous estimates we... | [['we', 'introduce', 'the', 'strong', 'cpviolation', 'in', 'the', 'framework', 'of', 'adsqcd', 'model', 'and', 'calculate', 'the', 'electric', 'dipole', 'moments', 'of', 'nucleons', 'as', 'well', 'as', 'the', 'cpviolating', 'pionnucleon', 'coupling', 'our', 'holographic', 'estimate', 'of', 'the', 'electric', 'dipole', ... | [-0.10484442640753354, 0.21216064775910448, -0.03147892767344328, 0.11505830495152622, -0.08791530970484018, -0.034406890683834825, 0.052107649544418294, 0.3114773355205269, -0.18019868527703425, -0.3076406211975743, -0.06121962715405971, -0.30606850037241684, -0.011886677790350993, 0.10753555071868878, 0.0909161770935... |
709.0315 | Suppression of Meszaros' Effect in coupled DE | A phaenomenological DM-DE coupling could indicate their common origin.
Various constraint however exist to such coupling; here we outline that it can
suppress Meszaros' effect, yielding transfered spectra with a softer bending
above k_{hor,eq}. It could be therefore hard to reconcile these models with
both CMB and de... | astro-ph | a phaenomenological dmde coupling could indicate their common origin various constraint however exist to such coupling here we outline that it can suppress meszaros effect yielding transfered spectra with a softer bending above k_horeq it could be therefore hard to reconcile these models with both cmb and deep sample d... | [['a', 'phaenomenological', 'dmde', 'coupling', 'could', 'indicate', 'their', 'common', 'origin', 'various', 'constraint', 'however', 'exist', 'to', 'such', 'coupling', 'here', 'we', 'outline', 'that', 'it', 'can', 'suppress', 'meszaros', 'effect', 'yielding', 'transfered', 'spectra', 'with', 'a', 'softer', 'bending', ... | [-0.08097953700794364, 0.18036952642021034, -0.1185843716111948, 0.1267003538614174, -0.15943033821037356, -0.2003187640429527, 0.020798490611168573, 0.44744628597542924, -0.30007464378931614, -0.3806265528612542, 0.10273339041456017, -0.28367017550429086, -0.10361149042563618, 0.1788424032757867, -0.001183391214822823... |
709.0316 | Evolutionary Prisoner's Dilemma game on the Newman-Watts networks | Maintenance of cooperation was studied for a two-strategy evolutionary
Prisoner's Dilemma game where the players are located on a one-dimensional
chain and their payoff comes from games with the nearest and next-nearest
neighbor interactions. The applied host geometry makes possible to study the
impacts of two confli... | physics.soc-ph | maintenance of cooperation was studied for a twostrategy evolutionary prisoners dilemma game where the players are located on a onedimensional chain and their payoff comes from games with the nearest and nextnearest neighbor interactions the applied host geometry makes possible to study the impacts of two conflicting t... | [['maintenance', 'of', 'cooperation', 'was', 'studied', 'for', 'a', 'twostrategy', 'evolutionary', 'prisoners', 'dilemma', 'game', 'where', 'the', 'players', 'are', 'located', 'on', 'a', 'onedimensional', 'chain', 'and', 'their', 'payoff', 'comes', 'from', 'games', 'with', 'the', 'nearest', 'and', 'nextnearest', 'neigh... | [-0.15874758409948922, 0.11731364587403573, -0.1006108372315985, 0.14262001210488706, -0.054298913110407035, -0.19809706880519035, 0.14969489009736367, 0.38960988786104217, -0.26906983046220584, -0.31595652246553646, 0.0648780340500372, -0.27301948046997976, -0.19609138826643557, 0.03896508993286835, -0.015964324586093... |
709.0317 | Microstrain and defects in polycrystalline Zn_{1-x}Mg_{x}O (0 <= x <=
0.15) studied by X-ray diffraction, and optical and Raman spectroscopies | The properties of polycrystalline wurtzite Zn_{1-x}Mg_{x}O (0 <= x <= 0.15)
have been studied, by powder X-ray diffraction, including an analysis of the
X-ray line-broadening, and by luminescence, absorption, and Raman
spectroscopies. We have previously established from synchrotron X-ray
difffraction that with increa... | cond-mat.mtrl-sci | the properties of polycrystalline wurtzite zn_1xmg_xo 0 x 015 have been studied by powder xray diffraction including an analysis of the xray linebroadening and by luminescence absorption and raman spectroscopies we have previously established from synchrotron xray difffraction that with increasing mgconcentration the c... | [['the', 'properties', 'of', 'polycrystalline', 'wurtzite', 'zn_1xmg_xo', '0', 'x', '015', 'have', 'been', 'studied', 'by', 'powder', 'xray', 'diffraction', 'including', 'an', 'analysis', 'of', 'the', 'xray', 'linebroadening', 'and', 'by', 'luminescence', 'absorption', 'and', 'raman', 'spectroscopies', 'we', 'have', 'p... | [-0.047119829924080245, 0.19092441044027558, -0.06084672932443368, -0.021107503516301765, -0.021469459255176165, -0.0818130198112201, 0.11435503552376362, 0.5036339399208423, -0.2937074327543631, -0.27313562291262505, 0.037247615007107104, -0.3625749078053398, -0.06658509575451414, 0.15801422635638188, 0.04255551592364... |
709.0318 | Spin-Filtering Multiferroic-Semiconductor Heterojunctions | We report on the structural and electronic properties of the interface
between the multiferoic oxide YMnO$_3$ and wide band-gap semiconductor GaN
studied with the Hubbard-corrected local spin density approximation (LSDA+U) to
density-functional theory (DFT). We find that the band offsets at the interface
between anti... | cond-mat.mtrl-sci cond-mat.str-el | we report on the structural and electronic properties of the interface between the multiferoic oxide ymno_3 and wide bandgap semiconductor gan studied with the hubbardcorrected local spin density approximation lsdau to densityfunctional theory dft we find that the band offsets at the interface between antiferromagnetic... | [['we', 'report', 'on', 'the', 'structural', 'and', 'electronic', 'properties', 'of', 'the', 'interface', 'between', 'the', 'multiferoic', 'oxide', 'ymno_3', 'and', 'wide', 'bandgap', 'semiconductor', 'gan', 'studied', 'with', 'the', 'hubbardcorrected', 'local', 'spin', 'density', 'approximation', 'lsdau', 'to', 'densi... | [-0.15135634199583103, 0.15398109135387045, -0.02453280835235048, 0.015845098332058462, -0.01743333437258289, -0.09766960495062882, 0.07707920842027913, 0.4834886601815621, -0.3106692750627796, -0.3560712520903464, -0.06643166608243649, -0.3128494715406781, -0.11011103609842914, 0.12737522962547485, 0.06057348932538713... |
709.0319 | On the Bohr radius relationship to spin-orbit interaction, spin
magnitude, and Thomas precession | The dynamics of the spin-orbit interaction in atomic hydrogen are studied in
a classical electrodynamics-like setting. A Rutherfordian atomic model is used
assuming a circular electron orbit, without the quantum principle as imposed
arbitrarily in the Bohr model, but with an ad hoc incorporation in the electron
of in... | physics.gen-ph | the dynamics of the spinorbit interaction in atomic hydrogen are studied in a classical electrodynamicslike setting a rutherfordian atomic model is used assuming a circular electron orbit without the quantum principle as imposed arbitrarily in the bohr model but with an ad hoc incorporation in the electron of intrinsic... | [['the', 'dynamics', 'of', 'the', 'spinorbit', 'interaction', 'in', 'atomic', 'hydrogen', 'are', 'studied', 'in', 'a', 'classical', 'electrodynamicslike', 'setting', 'a', 'rutherfordian', 'atomic', 'model', 'is', 'used', 'assuming', 'a', 'circular', 'electron', 'orbit', 'without', 'the', 'quantum', 'principle', 'as', '... | [-0.20899305811988966, 0.18820113288739185, -0.05653317381015432, 0.0713669909010297, -0.06766725436363963, -0.07653262671391237, -0.009680676884615816, 0.35121536807153475, -0.254251499703799, -0.3213917521672896, -0.0025366427291253517, -0.24976815709097724, -0.006978586834315428, 0.1967327944709691, -0.0050306736986... |
709.032 | Thermal Giant Graviton with Non-commutative Dipole Field | Using the type II near-extremal 3D-branes solution we apply the T-duality and
smeared twist to construct the supergravity backgrounds which dual to the 4D
finite temperature non-commutative dipole field theories. We first consider the
zero-temperature system in which, depending on the property of dipole vectors
it ma... | hep-th | using the type ii nearextremal 3dbranes solution we apply the tduality and smeared twist to construct the supergravity backgrounds which dual to the 4d finite temperature noncommutative dipole field theories we first consider the zerotemperature system in which depending on the property of dipole vectors it may be n2 n... | [['using', 'the', 'type', 'ii', 'nearextremal', '3dbranes', 'solution', 'we', 'apply', 'the', 'tduality', 'and', 'smeared', 'twist', 'to', 'construct', 'the', 'supergravity', 'backgrounds', 'which', 'dual', 'to', 'the', '4d', 'finite', 'temperature', 'noncommutative', 'dipole', 'field', 'theories', 'we', 'first', 'cons... | [-0.13390138839035792, 0.19399604929325462, -0.08090721187181771, 0.11383246580290413, -0.10495567088080353, -0.1283574023958144, -0.017637896405256807, 0.3220978896956631, -0.15805103048508942, -0.25436147471543313, 0.07340573618231817, -0.26846546918413666, -0.12875260228377788, 0.13408319260816762, -0.01235817774479... |
709.0321 | A first--order irreversible thermodynamic approach to a simple energy
converter | Several authors have shown that dissipative thermal cycle models based on
Finite-Time Thermodynamics exhibit loop-shaped curves of power output versus
efficiency, such as it occurs with actual dissipative thermal engines. Within
the context of First-Order Irreversible Thermodynamics (FOIT), in this work we
show that ... | cond-mat.stat-mech | several authors have shown that dissipative thermal cycle models based on finitetime thermodynamics exhibit loopshaped curves of power output versus efficiency such as it occurs with actual dissipative thermal engines within the context of firstorder irreversible thermodynamics foit in this work we show that for an ene... | [['several', 'authors', 'have', 'shown', 'that', 'dissipative', 'thermal', 'cycle', 'models', 'based', 'on', 'finitetime', 'thermodynamics', 'exhibit', 'loopshaped', 'curves', 'of', 'power', 'output', 'versus', 'efficiency', 'such', 'as', 'it', 'occurs', 'with', 'actual', 'dissipative', 'thermal', 'engines', 'within', ... | [-0.12053399704621061, 0.11988060659877087, -0.04673954615441387, 0.03242843988443457, -0.007453749821693217, -0.11594461619678101, 0.09712012653646775, 0.34561940669301944, -0.21083099134226405, -0.30340311424446975, 0.05543698885332186, -0.2662894768208713, -0.1637252060368721, 0.2140033364879535, -0.0811077888871147... |
709.0322 | Promote cooperation by localised small-world communication | The emergence and maintenance of cooperation within sizable groups of
unrelated humans offer many challenges for our understanding. We propose that
the humans' capacity of communication, such as how many and how far away the
fellows can build up mutual communications, may affect the evolution of
cooperation. We study... | physics.soc-ph physics.gen-ph | the emergence and maintenance of cooperation within sizable groups of unrelated humans offer many challenges for our understanding we propose that the humans capacity of communication such as how many and how far away the fellows can build up mutual communications may affect the evolution of cooperation we study this i... | [['the', 'emergence', 'and', 'maintenance', 'of', 'cooperation', 'within', 'sizable', 'groups', 'of', 'unrelated', 'humans', 'offer', 'many', 'challenges', 'for', 'our', 'understanding', 'we', 'propose', 'that', 'the', 'humans', 'capacity', 'of', 'communication', 'such', 'as', 'how', 'many', 'and', 'how', 'far', 'away'... | [-0.15059091718809214, 0.1076651371549815, -0.08205695646853807, 0.061148353908987096, -0.09301376503581803, -0.1922536742935578, 0.1421060485749816, 0.395561233907938, -0.30704935027907293, -0.33433779848739503, 0.0712927936630634, -0.278246334111318, -0.1889441921080773, 0.09716110784560442, -0.0859701975233232, -0.0... |
709.0323 | Analysis of the Phase Structure of Thermal QED/QCD through the HTL
Improved Ladder Dyson-Schwinger Equation --On the Gauge Dependence of the
Solution-- | We solved with a numerical procedure the HTL improved ladder DS equation for
the retarded fermion self-energy function $\Sigma_R$ to study the spontaneous
generation of fermion mass in thermal QCD/QED, and studied the gauge-dependence
of the solution within a general covariant gauge where the gauge parameter
$\xi$ is... | hep-ph | we solved with a numerical procedure the htl improved ladder ds equation for the retarded fermion selfenergy function sigma_r to study the spontaneous generation of fermion mass in thermal qcdqed and studied the gaugedependence of the solution within a general covariant gauge where the gauge parameter xi is any constan... | [['we', 'solved', 'with', 'a', 'numerical', 'procedure', 'the', 'htl', 'improved', 'ladder', 'ds', 'equation', 'for', 'the', 'retarded', 'fermion', 'selfenergy', 'function', 'sigma_r', 'to', 'study', 'the', 'spontaneous', 'generation', 'of', 'fermion', 'mass', 'in', 'thermal', 'qcdqed', 'and', 'studied', 'the', 'gauged... | [-0.13745643879638567, 0.15476379985148941, -0.105159168889537, 0.0715100079126257, -0.1034912169526084, -0.14980918299691864, 0.06784419012042142, 0.32479981100186706, -0.2124690041133103, -0.2654005460469622, 0.06141668533471565, -0.2724105911804553, -0.11000763848471475, 0.12415610137870725, 0.02271901150780483, 0.0... |
709.0324 | Final Fate of Subcritical Evolutions of Boson Stars | We present results from a study of Type I critical phenomena in the dynamics
of general relativistic boson stars in spherical symmetry. The boson stars are
modelled with a minimally coupled, massive complex field (with no explicit
self-interaction), and are driven to the threshold of black hole formation via
their gr... | gr-qc | we present results from a study of type i critical phenomena in the dynamics of general relativistic boson stars in spherical symmetry the boson stars are modelled with a minimally coupled massive complex field with no explicit selfinteraction and are driven to the threshold of black hole formation via their gravitatio... | [['we', 'present', 'results', 'from', 'a', 'study', 'of', 'type', 'i', 'critical', 'phenomena', 'in', 'the', 'dynamics', 'of', 'general', 'relativistic', 'boson', 'stars', 'in', 'spherical', 'symmetry', 'the', 'boson', 'stars', 'are', 'modelled', 'with', 'a', 'minimally', 'coupled', 'massive', 'complex', 'field', 'with... | [-0.13038707328934715, 0.20514017698467915, -0.051668655509794395, 0.09364179493143009, -0.05393713009594889, -0.10896274205143718, 0.010500736824354505, 0.34422730705649646, -0.2042890380182723, -0.29841088550677014, 0.07219240007151921, -0.25257670494937595, -0.11114300738823898, 0.17770941645306135, -0.0011973317081... |
709.0325 | Ore extensions of principally quasi-Baer rings | Let $R$ be a ring and $(\sigma,\delta)$ a quasi-derivation of $R$. In this
paper, we show that if $R$ is an $(\sigma,\delta)$-skew Armendariz ring and
satisfies the condition $(\mathcal{C_{\sigma}})$, then $R$ is right p.q.-Baer
if and only if the Ore extension $R[x;\sigma,\delta]$ is right p.q.-Baer. As a
consequenc... | math.RA | let r be a ring and sigmadelta a quasiderivation of r in this paper we show that if r is an sigmadeltaskew armendariz ring and satisfies the condition mathcalc_sigma then r is right pqbaer if and only if the ore extension rxsigmadelta is right pqbaer as a consequence we obtain a generalization of citehong2000 | [['let', 'r', 'be', 'a', 'ring', 'and', 'sigmadelta', 'a', 'quasiderivation', 'of', 'r', 'in', 'this', 'paper', 'we', 'show', 'that', 'if', 'r', 'is', 'an', 'sigmadeltaskew', 'armendariz', 'ring', 'and', 'satisfies', 'the', 'condition', 'mathcalc_sigma', 'then', 'r', 'is', 'right', 'pqbaer', 'if', 'and', 'only', 'if', ... | [-0.1847759678889558, 0.03881714979591911, -0.11726177975816547, -0.005529234339570943, -0.07801942049332385, -0.22595514392234245, -0.07647102178329215, 0.3415508027548708, -0.37324280502661217, -0.10071249202526403, 0.16960860341391965, -0.26198241100558695, -0.12015232739021194, 0.15005386980219726, -0.1491219874532... |
709.0326 | Monomial bases for the centres of the group algebra and Iwahori--Hecke
algebra of S_4 | G. E. Murphy showed in 1983 that the centre of every symmetric group algebra
has an integral basis consisting of a specific set of monomial symmetric
polynomials in the Jucys--Murphy elements. While we have shown in earlier work
that the centre of the group algebra of S_3 has exactly three additional such
bases, we s... | math.GR math.CO math.RT | g e murphy showed in 1983 that the centre of every symmetric group algebra has an integral basis consisting of a specific set of monomial symmetric polynomials in the jucysmurphy elements while we have shown in earlier work that the centre of the group algebra of s_3 has exactly three additional such bases we show in t... | [['g', 'e', 'murphy', 'showed', 'in', '1983', 'that', 'the', 'centre', 'of', 'every', 'symmetric', 'group', 'algebra', 'has', 'an', 'integral', 'basis', 'consisting', 'of', 'a', 'specific', 'set', 'of', 'monomial', 'symmetric', 'polynomials', 'in', 'the', 'jucysmurphy', 'elements', 'while', 'we', 'have', 'shown', 'in',... | [-0.17961573703141767, 0.05661997661018177, -0.07086401949636638, -0.022740813227574107, -0.07982244025333785, -0.06709809902822599, -0.04131124256746262, 0.33149070969666355, -0.33380117813067045, -0.1967563049052842, 0.10754526798045845, -0.2430537084932439, -0.15795536379155237, 0.17755962269147857, -0.0837632902810... |
709.0327 | The Faint Stellar Object SDSS J1257+3419 is a Dark Matter Dominated
System | A recent study has revealed SDSS J1257+3419 is either a faint and small dwarf
galaxy or a faint and widely extended globular cluster. In this Letter, the
author suggests this stellar system is a dwarf spheroidal (dSph). Adopting an
observational relation between binding energy and mass of old stellar systems,
we deri... | astro-ph gr-qc hep-th nucl-th | a recent study has revealed sdss j12573419 is either a faint and small dwarf galaxy or a faint and widely extended globular cluster in this letter the author suggests this stellar system is a dwarf spheroidal dsph adopting an observational relation between binding energy and mass of old stellar systems we derive a rela... | [['a', 'recent', 'study', 'has', 'revealed', 'sdss', 'j12573419', 'is', 'either', 'a', 'faint', 'and', 'small', 'dwarf', 'galaxy', 'or', 'a', 'faint', 'and', 'widely', 'extended', 'globular', 'cluster', 'in', 'this', 'letter', 'the', 'author', 'suggests', 'this', 'stellar', 'system', 'is', 'a', 'dwarf', 'spheroidal', '... | [-0.08767923548622357, 0.09184997093841722, -0.10539426995185955, 0.1446441263392297, -0.1397482989461071, -0.04012865201014305, 0.05430021102074534, 0.3749862650950109, -0.11329603187491998, -0.4088463527150452, -0.01986850780667737, -0.3089826629701776, -0.045281217252317395, 0.19734581567407136, -0.09746045870856652... |
709.0328 | Candidate Members and Age Estimate of the Family of Kuiper Belt Object
2003 EL61 | The collisional family of Kuiper belt object (KBO) 2003 EL61 opens the
possibility for many interesting new studies of processes important in the
formation and evolution of the outer solar system. As the first family in the
Kuiper belt, it can be studied using techniques developed for studying asteroid
families, alth... | astro-ph | the collisional family of kuiper belt object kbo 2003 el61 opens the possibility for many interesting new studies of processes important in the formation and evolution of the outer solar system as the first family in the kuiper belt it can be studied using techniques developed for studying asteroid families although so... | [['the', 'collisional', 'family', 'of', 'kuiper', 'belt', 'object', 'kbo', '2003', 'el61', 'opens', 'the', 'possibility', 'for', 'many', 'interesting', 'new', 'studies', 'of', 'processes', 'important', 'in', 'the', 'formation', 'and', 'evolution', 'of', 'the', 'outer', 'solar', 'system', 'as', 'the', 'first', 'family',... | [-0.09881941778618263, 0.11156307405106863, -0.10627000668209116, 0.10686008507256256, -0.11008421774022281, -0.08914410818713049, 0.019085847694681572, 0.3396553605133755, -0.22948592440840207, -0.3704193613825823, 0.08335159342562481, -0.2612597524389028, -0.13131869341497188, 0.23456009288915908, -0.1102056544068717... |
709.0329 | Schizophrenia - a parameters' game? | Schizophrenia is a severe, currently incurable, relatively common mental
condition. Its symptoms are complex and widespread. It structurally and
functionally affects cortical and subcortical regions involved in cognitive,
emotional and motivational aspects of behavior. Its cause is unknown, its
diagnosis is based on ... | q-bio.QM q-bio.TO | schizophrenia is a severe currently incurable relatively common mental condition its symptoms are complex and widespread it structurally and functionally affects cortical and subcortical regions involved in cognitive emotional and motivational aspects of behavior its cause is unknown its diagnosis is based on statistic... | [['schizophrenia', 'is', 'a', 'severe', 'currently', 'incurable', 'relatively', 'common', 'mental', 'condition', 'its', 'symptoms', 'are', 'complex', 'and', 'widespread', 'it', 'structurally', 'and', 'functionally', 'affects', 'cortical', 'and', 'subcortical', 'regions', 'involved', 'in', 'cognitive', 'emotional', 'and... | [-0.11888527586631993, 0.09339647028263252, -0.08180760922334572, 0.09537676277819394, -0.12662927041033117, -0.1601567336422677, 0.06269407714025514, 0.35336730528696636, -0.22807787878365063, -0.25904150192837905, 0.12404777881767748, -0.25279437240655767, -0.30673292572471766, 0.18743380505619295, -0.152297862621005... |
709.033 | Penrose Model potential, compared with Coleman-Weinberg Potential for
early universe scalar evolution | We present an overview of Dr. Penrose's model of a cyclic universe, minus the
big crunch which relies upon black hole collection of matter after an a long
term expansion phase from an initial big bang . We affirm that the suggested
evolution equation presented at his lecture for his model meets requirements as
to an ... | physics.gen-ph | we present an overview of dr penroses model of a cyclic universe minus the big crunch which relies upon black hole collection of matter after an a long term expansion phase from an initial big bang we affirm that the suggested evolution equation presented at his lecture for his model meets requirements as to an emergen... | [['we', 'present', 'an', 'overview', 'of', 'dr', 'penroses', 'model', 'of', 'a', 'cyclic', 'universe', 'minus', 'the', 'big', 'crunch', 'which', 'relies', 'upon', 'black', 'hole', 'collection', 'of', 'matter', 'after', 'an', 'a', 'long', 'term', 'expansion', 'phase', 'from', 'an', 'initial', 'big', 'bang', 'we', 'affir... | [-0.11005756255873866, 0.09896505369023889, -0.15254890456779208, 0.09585869741271687, -0.1188984420645026, -0.1377134911254444, 0.039394273188797575, 0.26995428208780964, -0.24559495146427535, -0.295207972201494, 0.11162344920881653, -0.30630446180899057, -0.11802340302599874, 0.1475757669772854, -0.11366133939936361,... |
709.0331 | The use of cosmic muons in detecting heterogeneities in large volumes | The muon intensity attenuation method to detect heterogeneities in large
matter volumes is analyzed. Approximate analytical expressions to estimate the
collection time and the signal to noise ratio, are proposed and validated by
Monte Carlo simulations. Important parameters, including point spread function
and coordi... | physics.ins-det | the muon intensity attenuation method to detect heterogeneities in large matter volumes is analyzed approximate analytical expressions to estimate the collection time and the signal to noise ratio are proposed and validated by monte carlo simulations important parameters including point spread function and coordinate r... | [['the', 'muon', 'intensity', 'attenuation', 'method', 'to', 'detect', 'heterogeneities', 'in', 'large', 'matter', 'volumes', 'is', 'analyzed', 'approximate', 'analytical', 'expressions', 'to', 'estimate', 'the', 'collection', 'time', 'and', 'the', 'signal', 'to', 'noise', 'ratio', 'are', 'proposed', 'and', 'validated'... | [-0.0554742554761689, 0.0910739124453855, -0.08178514406801078, 0.16948367775865952, -0.006489126890335443, -0.08501271228745298, 0.016172411781296414, 0.4404291588602201, -0.25380166732477694, -0.3883174038580004, 0.12166382559302773, -0.31566670508000927, -0.0941376679297976, 0.20438573115839148, 0.03622100621743022,... |
709.0332 | Effective base point free theorem for log canonical pairs--Koll\'ar type
theorem | We prove Koll\'ar's effective base point free theorem for log canonical
pairs.
| math.AG | we prove kollars effective base point free theorem for log canonical pairs | [['we', 'prove', 'kollars', 'effective', 'base', 'point', 'free', 'theorem', 'for', 'log', 'canonical', 'pairs']] | [-0.22093990988408527, 0.04903287603519857, -0.13735806309462836, 0.26132864768927294, -0.05018788374339541, -0.20814162461707988, 0.17463350373630723, 0.276073948169748, -0.2831759487744421, -0.22305255383253098, -0.0742042656832685, -0.27346508391201496, -0.12172438794126113, 0.2275646597457429, -0.16966921587785086,... |
709.0333 | Dynamic nuclear polarisation in biased quantum wires with spin-orbit
interaction | We propose a new method for dynamic nuclear polarisation in a quasi
one-dimensional quantum wire utilising the spin-orbit interaction, the
hyperfine interaction, and a finite source-drain potential difference. In
contrast with current methods, our scheme does not rely on external magnetic or
optical sources which mak... | cond-mat.mes-hall | we propose a new method for dynamic nuclear polarisation in a quasi onedimensional quantum wire utilising the spinorbit interaction the hyperfine interaction and a finite sourcedrain potential difference in contrast with current methods our scheme does not rely on external magnetic or optical sources which makes indepe... | [['we', 'propose', 'a', 'new', 'method', 'for', 'dynamic', 'nuclear', 'polarisation', 'in', 'a', 'quasi', 'onedimensional', 'quantum', 'wire', 'utilising', 'the', 'spinorbit', 'interaction', 'the', 'hyperfine', 'interaction', 'and', 'a', 'finite', 'sourcedrain', 'potential', 'difference', 'in', 'contrast', 'with', 'cur... | [-0.16550186568462588, 0.14756150669330415, -0.0167636164157368, 0.0194367289066508, -0.06907132436205053, -0.2126424337587899, 0.06261747400056711, 0.4467261405837423, -0.22894274515872998, -0.318073559394282, 0.06126900464801539, -0.24787105802218165, -0.09569336730055511, 0.27781754390134494, -0.01739165490001159, 0... |
709.0334 | Maximum likelihood estimation of a log-concave density and its
distribution function: Basic properties and uniform consistency | We study nonparametric maximum likelihood estimation of a log-concave
probability density and its distribution and hazard function. Some general
properties of these estimators are derived from two characterizations. It is
shown that the rate of convergence with respect to supremum norm on a compact
interval for the d... | math.ST stat.ME stat.TH | we study nonparametric maximum likelihood estimation of a logconcave probability density and its distribution and hazard function some general properties of these estimators are derived from two characterizations it is shown that the rate of convergence with respect to supremum norm on a compact interval for the densit... | [['we', 'study', 'nonparametric', 'maximum', 'likelihood', 'estimation', 'of', 'a', 'logconcave', 'probability', 'density', 'and', 'its', 'distribution', 'and', 'hazard', 'function', 'some', 'general', 'properties', 'of', 'these', 'estimators', 'are', 'derived', 'from', 'two', 'characterizations', 'it', 'is', 'shown', ... | [-0.07269631427354054, 0.03669998499036238, -0.12451144748853482, 0.12149832536925788, 0.006551570252741914, -0.10076810345934653, 0.05048984769933127, 0.4307688665450425, -0.2589155983783909, -0.24850311404411882, 0.17990887441319992, -0.2850575512023391, -0.10552236602666813, 0.186520394705538, -0.08959506122345054, ... |
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