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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708.0249 | Classifying the Unclassifiables | In 1955 George Mackey suggested that there is a fundamental dichotomy in the
unitary representation theory of locally compact second countable groups. He
felt that there cannnot be a reasonable classification theory for the unitary
representations of a group G for which the dual is a non-smooth Borel space.
Mackey's ... | math.LO math.RT | in 1955 george mackey suggested that there is a fundamental dichotomy in the unitary representation theory of locally compact second countable groups he felt that there cannnot be a reasonable classification theory for the unitary representations of a group g for which the dual is a nonsmooth borel space mackeys precis... | [['in', '1955', 'george', 'mackey', 'suggested', 'that', 'there', 'is', 'a', 'fundamental', 'dichotomy', 'in', 'the', 'unitary', 'representation', 'theory', 'of', 'locally', 'compact', 'second', 'countable', 'groups', 'he', 'felt', 'that', 'there', 'cannnot', 'be', 'a', 'reasonable', 'classification', 'theory', 'for', ... | [-0.10276333443963757, 0.12651042601792142, -0.15658511028875813, 0.09548579448780331, -0.12225513845109022, -0.13587305329453486, 0.014256421510631648, 0.36565962789866785, -0.2759381252520073, -0.2226222942941464, 0.12379014263860881, -0.22209518373979686, -0.17064375071428142, 0.22028376110157785, -0.156752177768458... |
708.025 | Holography from loop quantum gravity | We show that holography arises naturally in the context of spherically
symmetric loop quantum gravity. The result is not dependent on detailed
assumptions about the dynamics of the theory being considered. It ties strongly
the amount of information contained in a region of space to the tight
mathematical underpinning... | gr-qc hep-th | we show that holography arises naturally in the context of spherically symmetric loop quantum gravity the result is not dependent on detailed assumptions about the dynamics of the theory being considered it ties strongly the amount of information contained in a region of space to the tight mathematical underpinnings of... | [['we', 'show', 'that', 'holography', 'arises', 'naturally', 'in', 'the', 'context', 'of', 'spherically', 'symmetric', 'loop', 'quantum', 'gravity', 'the', 'result', 'is', 'not', 'dependent', 'on', 'detailed', 'assumptions', 'about', 'the', 'dynamics', 'of', 'the', 'theory', 'being', 'considered', 'it', 'ties', 'strong... | [-0.1348164707848455, 0.11767204103880893, -0.08476706434798947, 0.10789936881954387, -0.0767326210546544, -0.09641489912992564, 0.009751113098098944, 0.3214557562694269, -0.2683237768330817, -0.2606437606579166, 0.10182918419753659, -0.22952239692874127, -0.18999932933661898, 0.16861315781124314, -0.10283520884498148,... |
708.0251 | An Event-Driven Hybrid Molecular Dynamics and Direct Simulation Monte
Carlo Algorithm | A novel Stochastic Event-Driven Molecular Dynamics (SEDMD) algorithm is
developed for the simulation of polymer chains suspended in a solvent. The
polymers are represented as chains of hard spheres tethered by square wells and
interact with the solvent particles with hard core potentials. The algorithm
uses Event-Dri... | cond-mat.mtrl-sci cond-mat.stat-mech | a novel stochastic eventdriven molecular dynamics sedmd algorithm is developed for the simulation of polymer chains suspended in a solvent the polymers are represented as chains of hard spheres tethered by square wells and interact with the solvent particles with hard core potentials the algorithm uses eventdriven mole... | [['a', 'novel', 'stochastic', 'eventdriven', 'molecular', 'dynamics', 'sedmd', 'algorithm', 'is', 'developed', 'for', 'the', 'simulation', 'of', 'polymer', 'chains', 'suspended', 'in', 'a', 'solvent', 'the', 'polymers', 'are', 'represented', 'as', 'chains', 'of', 'hard', 'spheres', 'tethered', 'by', 'square', 'wells', ... | [-0.13711762200519828, 0.1623227741916717, -0.08520398731818458, 0.026498097700182677, 0.03238905312908437, -0.1456488303579583, -0.010598427687235987, 0.43098634378164236, -0.2784669214058571, -0.3017183367194309, 0.027818067863081712, -0.2617412689962265, -0.09348582203253872, 0.1176149149442217, 0.06580199436356984,... |
708.0252 | The Edge of the Wedge Theorem for Tempered Ultrahyperfunctions II. A
Generalized Version | Withdrawn by author - Superseded by arXiv:0910.5106 [math.FA].
| math.CV math-ph math.MP | withdrawn by author superseded by arxiv09105106 mathfa | [['withdrawn', 'by', 'author', 'superseded', 'by', 'arxiv09105106', 'mathfa']] | [-0.0847174731704096, 0.09590316098183393, -0.031101011981566746, -0.044491579135258995, -0.16919190188248953, -0.137128840200603, 0.006634952345242103, 0.21343454470237097, -0.3137222683678071, -0.44022813873986405, 0.05057659652084112, -0.3168029623727004, -0.09515842671195666, -0.0008506799737612406, -0.384343380729... |
708.0253 | Many-body quantum coherence and interaction blockade in Josephson-linked
Bose-Einstein condensates | We study many-body quantum coherence and interaction blockade in two
Josephson-linked Bose-Einstein condensates. We introduce universal operators
for characterizing many-body coherence without limitations on the system
symmetry and total particle number $N$. We reproduce the results for both
coherence fluctuations an... | quant-ph | we study manybody quantum coherence and interaction blockade in two josephsonlinked boseeinstein condensates we introduce universal operators for characterizing manybody coherence without limitations on the system symmetry and total particle number n we reproduce the results for both coherence fluctuations and number s... | [['we', 'study', 'manybody', 'quantum', 'coherence', 'and', 'interaction', 'blockade', 'in', 'two', 'josephsonlinked', 'boseeinstein', 'condensates', 'we', 'introduce', 'universal', 'operators', 'for', 'characterizing', 'manybody', 'coherence', 'without', 'limitations', 'on', 'the', 'system', 'symmetry', 'and', 'total'... | [-0.21980994870109077, 0.23668590659566305, -0.038174699362065176, 0.1110900381625482, 0.025828760143505127, -0.18967416205301585, 0.019699719359802192, 0.36496797469228703, -0.2530075565862488, -0.3083311566922641, -0.0066800846445331016, -0.32055676068928685, -0.14292404423946775, 0.19820280503312016, 0.0347347811037... |
708.0254 | The Far-Infrared Properties of Spatially Resolved AKARI Observations | We present the spatially resolved observations of IRAS sources from the Japanese infrared astronomy satellite AKARI All-Sky Survey during the performance verification (PV) phase of the mission. We extracted reliable point sources matched with IRAS point source catalogue. By comparing IRAS and AKARI fluxes, we found t... | astro-ph astro-ph.GA | we present the spatially resolved observations of iras sources from the japanese infrared astronomy satellite akari allsky survey during the performance verification pv phase of the mission we extracted reliable point sources matched with iras point source catalogue by comparing iras and akari fluxes we found that the ... | [['we', 'present', 'the', 'spatially', 'resolved', 'observations', 'of', 'iras', 'sources', 'from', 'the', 'japanese', 'infrared', 'astronomy', 'satellite', 'akari', 'allsky', 'survey', 'during', 'the', 'performance', 'verification', 'pv', 'phase', 'of', 'the', 'mission', 'we', 'extracted', 'reliable', 'point', 'source... | [-0.049816981776038535, 0.026575221663324145, -0.08868339025994411, 0.08826260753647164, -0.10327453495145918, -0.019773802025189104, 0.07515684848751973, 0.48265830256246234, -0.12763665757469228, -0.3571409561864293, 0.08889842653638674, -0.40503478021704936, -0.007967037251554765, 0.2248080667487958, -0.037598617290... |
708.0255 | On algebraically integrable outer billiards | We prove that if the outer billiard map around a plane oval is algebraically
integrable in a certain non-degenerate sense then the oval is an ellipse.
| math.DS math.AG | we prove that if the outer billiard map around a plane oval is algebraically integrable in a certain nondegenerate sense then the oval is an ellipse | [['we', 'prove', 'that', 'if', 'the', 'outer', 'billiard', 'map', 'around', 'a', 'plane', 'oval', 'is', 'algebraically', 'integrable', 'in', 'a', 'certain', 'nondegenerate', 'sense', 'then', 'the', 'oval', 'is', 'an', 'ellipse']] | [-0.240456597163127, 0.07411889504930094, -0.1313652306293639, 0.06895586598413782, -0.06339220473399529, -0.1542380153774642, -0.10328971680540305, 0.38177106701410735, -0.3799565921609218, -0.07255906672575153, 0.12601699059954485, -0.3320514058443503, -0.22201026381494907, 0.21212330002051133, -0.14879650687082455, ... |
708.0256 | Narrow-line Seyfert 1 Galaxies and the M_BH - sigma Relation | We have studied the location of narrow-line Seyfert 1 (NLS1) galaxies and
broad-line Seyfert 1 (BLS1) galaxies on the M_BH - sigma relation of non-active
galaxies. We find that NLS1 galaxies as a class - as well as the BLS1 galaxies
of our comparison sample - do follow the M_BH-sigma relation of non-active
galaxies i... | astro-ph | we have studied the location of narrowline seyfert 1 nls1 galaxies and broadline seyfert 1 bls1 galaxies on the m_bh sigma relation of nonactive galaxies we find that nls1 galaxies as a class as well as the bls1 galaxies of our comparison sample do follow the m_bhsigma relation of nonactive galaxies if we use the width... | [['we', 'have', 'studied', 'the', 'location', 'of', 'narrowline', 'seyfert', '1', 'nls1', 'galaxies', 'and', 'broadline', 'seyfert', '1', 'bls1', 'galaxies', 'on', 'the', 'm_bh', 'sigma', 'relation', 'of', 'nonactive', 'galaxies', 'we', 'find', 'that', 'nls1', 'galaxies', 'as', 'a', 'class', 'as', 'well', 'as', 'the', ... | [-0.02369431186692131, 0.03172643019803869, -0.003599502500702641, 0.1965202470947131, -0.11259427154205036, -0.12055097998754673, 0.04723389532917471, 0.5547533908775494, -0.05324840022538284, -0.29150590471997484, -0.007141809018597526, -0.32795892601638144, -0.018243787895925158, 0.1939350500597447, -0.0156614320597... |
708.0257 | Universal localisations of hereditary rings | We describe all possible universal localisations of a hereditary ring in
terms of suitable full subcategories of the category of finitely presented
modules. For these universal localisations we then identify the category of
finitely presented bound modules over the universal localisation as being
equivalent to a cert... | math.RA | we describe all possible universal localisations of a hereditary ring in terms of suitable full subcategories of the category of finitely presented modules for these universal localisations we then identify the category of finitely presented bound modules over the universal localisation as being equivalent to a certain... | [['we', 'describe', 'all', 'possible', 'universal', 'localisations', 'of', 'a', 'hereditary', 'ring', 'in', 'terms', 'of', 'suitable', 'full', 'subcategories', 'of', 'the', 'category', 'of', 'finitely', 'presented', 'modules', 'for', 'these', 'universal', 'localisations', 'we', 'then', 'identify', 'the', 'category', 'o... | [-0.15836818732541838, 0.0316200820655611, -0.04165116155912217, 0.07957169219949528, -0.0379640183129691, -0.14463922158373813, -0.07908083583644934, 0.36116182176690353, -0.4481345500895067, -0.13083698169793934, 0.0805954776664485, -0.14552635921312398, -0.08596946447352438, 0.2704522712891431, -0.16965965644799566,... |
708.0258 | On the penetration of meridional circulation below the solar convection
zone | Meridional flows with velocities of a few meters per second are observed in
the uppermost regions of the solar convection zone. The amplitude and pattern
of the flows deeper in the solar interior, in particular near the top of the
radiative region, are of crucial importance to a wide range of solar
magnetohydrodynami... | astro-ph | meridional flows with velocities of a few meters per second are observed in the uppermost regions of the solar convection zone the amplitude and pattern of the flows deeper in the solar interior in particular near the top of the radiative region are of crucial importance to a wide range of solar magnetohydrodynamical p... | [['meridional', 'flows', 'with', 'velocities', 'of', 'a', 'few', 'meters', 'per', 'second', 'are', 'observed', 'in', 'the', 'uppermost', 'regions', 'of', 'the', 'solar', 'convection', 'zone', 'the', 'amplitude', 'and', 'pattern', 'of', 'the', 'flows', 'deeper', 'in', 'the', 'solar', 'interior', 'in', 'particular', 'nea... | [-0.11821129154365433, 0.14550619989394262, -0.029067356918757368, 0.06833546479336089, -0.05883223489541302, -0.017831994000718825, 0.04785423731098288, 0.3183854393104816, -0.2781716075777594, -0.29642553491673124, 0.09673289234342519, -0.24618503583405982, -0.10367518356360961, 0.235605936174074, -0.0421816242251225... |
708.0259 | Dynamic Boundaries in Asymmetric Exclusion Processes | We investigate the dynamics of a one-dimensional asymmetric exclusion process
with Langmuir kinetics and a fluctuating wall. At the left boundary, particles
are injected onto the lattice; from there, the particles hop to the right.
Along the lattice, particles can adsorb or desorb, and the right boundary is
defined b... | cond-mat.stat-mech cond-mat.soft | we investigate the dynamics of a onedimensional asymmetric exclusion process with langmuir kinetics and a fluctuating wall at the left boundary particles are injected onto the lattice from there the particles hop to the right along the lattice particles can adsorb or desorb and the right boundary is defined by a wall p... | [['we', 'investigate', 'the', 'dynamics', 'of', 'a', 'onedimensional', 'asymmetric', 'exclusion', 'process', 'with', 'langmuir', 'kinetics', 'and', 'a', 'fluctuating', 'wall', 'at', 'the', 'left', 'boundary', 'particles', 'are', 'injected', 'onto', 'the', 'lattice', 'from', 'there', 'the', 'particles', 'hop', 'to', 'th... | [-0.11513028886157331, 0.25205724168817994, -0.09019246584347265, 0.003246328102076329, -0.02330418477119629, -0.1632205146086064, 0.04850838599343944, 0.39495825798363443, -0.31422955400435026, -0.22309349890157676, 0.0965535869187183, -0.31073050412118053, -0.0017820792183707095, 0.09529144954526572, 0.00770563495814... |
708.026 | Recoilless Resonance Absorption of Tritium Antineutrinos and Time-Energy
Uncertainty Relation | We discuss neutrino oscillations in an experiment with M\"ossbauer recoilless
resonance absorbtion of tritium antineutrinos, proposed recently by Raghavan.
We demonstrate that small energy uncertainty of antineutrinos which ensures a
large resonance absorption cross section is in a conflict with the energy
uncertaint... | hep-ph | we discuss neutrino oscillations in an experiment with mossbauer recoilless resonance absorbtion of tritium antineutrinos proposed recently by raghavan we demonstrate that small energy uncertainty of antineutrinos which ensures a large resonance absorption cross section is in a conflict with the energy uncertainty whic... | [['we', 'discuss', 'neutrino', 'oscillations', 'in', 'an', 'experiment', 'with', 'mossbauer', 'recoilless', 'resonance', 'absorbtion', 'of', 'tritium', 'antineutrinos', 'proposed', 'recently', 'by', 'raghavan', 'we', 'demonstrate', 'that', 'small', 'energy', 'uncertainty', 'of', 'antineutrinos', 'which', 'ensures', 'a'... | [-0.0985283233593543, 0.2407189051564485, -0.04700813117588675, 0.20568074085912125, -0.07824075572885746, -0.09612783716536712, 0.09791688185434269, 0.32251243414573894, -0.23311399577488734, -0.3421652904430101, 0.0019106494390059175, -0.3243256011046469, -0.05015272848567991, 0.21816484690481408, -0.0123821899922954... |
708.0261 | An Introduction to Quantum Computing | Quantum Computing is a new and exciting field at the intersection of
mathematics, computer science and physics. It concerns a utilization of quantum
mechanics to improve the efficiency of computation. Here we present a gentle
introduction to some of the ideas in quantum computing. The paper begins by
motivating the c... | quant-ph | quantum computing is a new and exciting field at the intersection of mathematics computer science and physics it concerns a utilization of quantum mechanics to improve the efficiency of computation here we present a gentle introduction to some of the ideas in quantum computing the paper begins by motivating the central... | [['quantum', 'computing', 'is', 'a', 'new', 'and', 'exciting', 'field', 'at', 'the', 'intersection', 'of', 'mathematics', 'computer', 'science', 'and', 'physics', 'it', 'concerns', 'a', 'utilization', 'of', 'quantum', 'mechanics', 'to', 'improve', 'the', 'efficiency', 'of', 'computation', 'here', 'we', 'present', 'a', ... | [-0.09525925055055356, 0.15017867856848288, -0.11050453575752009, 0.03310003584133446, -0.08241755439619708, -0.2069735951471801, 0.05014000254365184, 0.2936329020421982, -0.2706426989620294, -0.30383302139618046, 0.07135768884289403, -0.2429433569493817, -0.1792774282829321, 0.2394337192162629, -0.12622290654264096, 0... |
708.0262 | Magnifying perfect lens and superlens design by coordinate
transformation | The coordinate transformation technique is applied to the design of perfect
lenses and superlenses. In particular, anisotropic metamaterials that magnify
two-dimensional planar images beyond the diffraction limit are designed by the
use of oblate spheroidal coordinates. The oblate spheroidal perfect lens or
superlens... | physics.optics | the coordinate transformation technique is applied to the design of perfect lenses and superlenses in particular anisotropic metamaterials that magnify twodimensional planar images beyond the diffraction limit are designed by the use of oblate spheroidal coordinates the oblate spheroidal perfect lens or superlens can n... | [['the', 'coordinate', 'transformation', 'technique', 'is', 'applied', 'to', 'the', 'design', 'of', 'perfect', 'lenses', 'and', 'superlenses', 'in', 'particular', 'anisotropic', 'metamaterials', 'that', 'magnify', 'twodimensional', 'planar', 'images', 'beyond', 'the', 'diffraction', 'limit', 'are', 'designed', 'by', 't... | [-0.08295276065526361, 0.10697756128554994, -0.09485810416411947, 0.031092940010553734, -0.1612057633359324, -0.13543766747144134, -0.09981142600828952, 0.4720961302391846, -0.23620013763958758, -0.3098554443229328, 0.03762689173983579, -0.2533825947479768, -0.2067806779618629, 0.20677669257856907, -0.04674751830541274... |
708.0263 | Type Ia and II supernovae contributions to the metal enrichment in
intra-cluster medium observed with Suzaku | We studied the properties of the intra-cluster medium (ICM) in two clusters
of galaxies (AWM 7 and Abell 1060) and two groups (HCG 62 and NGC 507) with the
X-ray Observatory Suzaku. Based on spatially resolved energy spectra, we
measured for the first time precise cumulative ICM metal masses within 0.1 and
~0.3 r_{18... | astro-ph | we studied the properties of the intracluster medium icm in two clusters of galaxies awm 7 and abell 1060 and two groups hcg 62 and ngc 507 with the xray observatory suzaku based on spatially resolved energy spectra we measured for the first time precise cumulative icm metal masses within 01 and 03 r_180 comparing our ... | [['we', 'studied', 'the', 'properties', 'of', 'the', 'intracluster', 'medium', 'icm', 'in', 'two', 'clusters', 'of', 'galaxies', 'awm', '7', 'and', 'abell', '1060', 'and', 'two', 'groups', 'hcg', '62', 'and', 'ngc', '507', 'with', 'the', 'xray', 'observatory', 'suzaku', 'based', 'on', 'spatially', 'resolved', 'energy',... | [-0.014063006978560711, 0.0919850837131044, -0.007516831851524996, 0.12139250679699128, -0.08803759254744722, -0.06559002868713103, 0.07861775286089052, 0.4477016583714687, -0.15236485727511767, -0.3361896314513935, 0.022853508081720014, -0.33843757563703497, 0.040262578174957195, 0.21930020870878625, 0.006419656376852... |
708.0264 | Field-induced incommensurate order for the quasi-one-dimensional XXZ
model in a magnetic field | We investigate phase transitions of the quasi-one-dimensional XXZ model in a
magnetic field, using the bosonization combined with the mean field treatment
of the inter-chain interaction. We then find that the field induced
incommensurate order is certainly realized in the low field region, while the
transverse stagge... | cond-mat.str-el cond-mat.stat-mech | we investigate phase transitions of the quasionedimensional xxz model in a magnetic field using the bosonization combined with the mean field treatment of the interchain interaction we then find that the field induced incommensurate order is certainly realized in the low field region while the transverse staggered orde... | [['we', 'investigate', 'phase', 'transitions', 'of', 'the', 'quasionedimensional', 'xxz', 'model', 'in', 'a', 'magnetic', 'field', 'using', 'the', 'bosonization', 'combined', 'with', 'the', 'mean', 'field', 'treatment', 'of', 'the', 'interchain', 'interaction', 'we', 'then', 'find', 'that', 'the', 'field', 'induced', '... | [-0.22138525396585465, 0.22036761825105974, -0.02276321763971022, 0.045494164142291994, -0.019584656204096974, -0.057501131249591705, 0.034881834629257875, 0.4021774458033698, -0.2154125787783414, -0.27034858490473457, 0.049884903918219994, -0.23861896354439002, -0.1310620341583022, 0.10681816721002438, 0.0766294580011... |
708.0265 | Hydrogen Balmer line formation in solar flares affected by return
currents | Aims. We investigate the effect of the electric return currents in solar
flares on the profiles of hydrogen Balmer lines. We consider the monoenergetic
approximation for the primary beam and runaway model of the neutralizing return
current. Methods. Propagation of the 10 keV electron beam from a coronal
reconnection ... | astro-ph | aims we investigate the effect of the electric return currents in solar flares on the profiles of hydrogen balmer lines we consider the monoenergetic approximation for the primary beam and runaway model of the neutralizing return current methods propagation of the 10 kev electron beam from a coronal reconnection site i... | [['aims', 'we', 'investigate', 'the', 'effect', 'of', 'the', 'electric', 'return', 'currents', 'in', 'solar', 'flares', 'on', 'the', 'profiles', 'of', 'hydrogen', 'balmer', 'lines', 'we', 'consider', 'the', 'monoenergetic', 'approximation', 'for', 'the', 'primary', 'beam', 'and', 'runaway', 'model', 'of', 'the', 'neutr... | [-0.0444700200008577, 0.14751682308059558, 0.04902789928019047, 0.14233710966633265, 0.03317686183786488, -0.07963491691635015, 0.055727987420710334, 0.45109126474807926, -0.16375670461033914, -0.3524658844313201, -0.007338679350793043, -0.3279524766416712, 0.04322252866225616, 0.18519184869753924, 0.022453488605246347... |
708.0266 | A Comprehensive View of Circumstellar Disks in Chamaeleon I: Infrared
Excess, Accretion Signatures and Binarity | We present a comprehensive study of disks around 81 young low-mass stars and
brown dwarfs in the nearby ~2-Myr-old Chamaeleon I star-forming region. We use
mid-infrared photometry from the Spitzer Space Telescope, supplemented by
findings from ground-based high-resolution optical spectroscopy and adaptive
optics imag... | astro-ph | we present a comprehensive study of disks around 81 young lowmass stars and brown dwarfs in the nearby 2myrold chamaeleon i starforming region we use midinfrared photometry from the spitzer space telescope supplemented by findings from groundbased highresolution optical spectroscopy and adaptive optics imaging we deriv... | [['we', 'present', 'a', 'comprehensive', 'study', 'of', 'disks', 'around', '81', 'young', 'lowmass', 'stars', 'and', 'brown', 'dwarfs', 'in', 'the', 'nearby', '2myrold', 'chamaeleon', 'i', 'starforming', 'region', 'we', 'use', 'midinfrared', 'photometry', 'from', 'the', 'spitzer', 'space', 'telescope', 'supplemented', ... | [-0.057048992104119206, 0.1108222948211515, -0.05395854578491195, 0.08084843039018202, -0.05446426374231085, -0.0722835946374763, 0.06647522858070197, 0.44641190641362904, -0.14715896827303215, -0.38364517544297844, 0.08005819633409617, -0.3018508073283543, -0.014223680157594802, 0.18672065077346264, -0.075217960226004... |
708.0267 | Probing e-e interactions in a periodic array of GaAs quantum wires | We present the results of non-linear tunnelling spectroscopy between an array
of independent quantum wires and an adjacent two-dimensional electron gas
(2DEG) in a double-quantum-well structure. The two layers are separately
contacted using a surface-gate scheme, and the wires are all very regular, with
dimensions ch... | cond-mat.mes-hall cond-mat.str-el | we present the results of nonlinear tunnelling spectroscopy between an array of independent quantum wires and an adjacent twodimensional electron gas 2deg in a doublequantumwell structure the two layers are separately contacted using a surfacegate scheme and the wires are all very regular with dimensions chosen careful... | [['we', 'present', 'the', 'results', 'of', 'nonlinear', 'tunnelling', 'spectroscopy', 'between', 'an', 'array', 'of', 'independent', 'quantum', 'wires', 'and', 'an', 'adjacent', 'twodimensional', 'electron', 'gas', '2deg', 'in', 'a', 'doublequantumwell', 'structure', 'the', 'two', 'layers', 'are', 'separately', 'contac... | [-0.18908254747164743, 0.17510651699025098, -0.01721662126686887, 0.013890372190815369, 0.02081105382303181, -0.23383079811942226, 0.06199454216240263, 0.40000782519150874, -0.26113942267643636, -0.31030975585305914, 0.0019431313454977566, -0.3131050159287008, -0.09579134739715583, 0.1903802747071738, 0.043257222169582... |
708.0268 | Generalized Parton Distributions from Hadronic Observables: Non-Zero
Skewness | We propose a physically motivated parametrization for the unpolarized
generalized parton distributions, H and E, valid at both zero and non-zero
values of the skewness variable, \zeta. Our approach follows a previous
detailed study of the \zeta=0 case where H and E were determined using
constraints from simultaneous ... | hep-ph | we propose a physically motivated parametrization for the unpolarized generalized parton distributions h and e valid at both zero and nonzero values of the skewness variable zeta our approach follows a previous detailed study of the zeta0 case where h and e were determined using constraints from simultaneous fits of th... | [['we', 'propose', 'a', 'physically', 'motivated', 'parametrization', 'for', 'the', 'unpolarized', 'generalized', 'parton', 'distributions', 'h', 'and', 'e', 'valid', 'at', 'both', 'zero', 'and', 'nonzero', 'values', 'of', 'the', 'skewness', 'variable', 'zeta', 'our', 'approach', 'follows', 'a', 'previous', 'detailed',... | [-0.06576726552803949, 0.10621177962562392, -0.14809053753399187, 0.09786504516184019, -0.08424573423366787, -0.10976538343820721, 0.06641725675306387, 0.3567449385274409, -0.23809292866693188, -0.2568066442049005, 0.02724200969419649, -0.2870800205997916, -0.07804389159686656, 0.18403367054027817, 0.03874049725049594,... |
708.0269 | Sharp k-order Sobolev inequalities in the hyperbolic space ${\Bbb H}^n$ | In this paper, we obtain the sharp $k$-th order Sobolev inequalities in the
hyperbolic space ${\H}^n$ for all $k=1,2,3,\cdots$. This gives an answer to an
open question raised by Aubin in [5, p.$\;$176-177] for $W^{k,2}({\H}^n)$ with
$k>1$. In addition, we prove that the associated Sobolev constants are optimal.
| math.AP math.DG | in this paper we obtain the sharp kth order sobolev inequalities in the hyperbolic space hn for all k123cdots this gives an answer to an open question raised by aubin in 5 p176177 for wk2hn with k1 in addition we prove that the associated sobolev constants are optimal | [['in', 'this', 'paper', 'we', 'obtain', 'the', 'sharp', 'kth', 'order', 'sobolev', 'inequalities', 'in', 'the', 'hyperbolic', 'space', 'hn', 'for', 'all', 'k123cdots', 'this', 'gives', 'an', 'answer', 'to', 'an', 'open', 'question', 'raised', 'by', 'aubin', 'in', '5', 'p176177', 'for', 'wk2hn', 'with', 'k1', 'in', 'ad... | [-0.1399583559948951, 0.06447010266452304, 0.02285332259618574, 0.09281888239396115, -0.05536993322893977, -0.10528344843122694, 0.010221275006834831, 0.34259317252371047, -0.31269779726862906, -0.25419160057273177, 0.12261662695349919, -0.30894279742820396, -0.13320661111631327, 0.21897256317444974, -0.162906337074107... |
708.027 | Solar cycle variation of real CME latitudes | With the assumption of radial motion and uniform longitudinal distribution of
coronal mass ejections (CMEs), we propose a method to eliminate projection
effects from the apparent observed CME latitude distribution. This method has
been applied to SOHO LASCO data from 1996 January to 2006 December. As a
result, we fin... | astro-ph | with the assumption of radial motion and uniform longitudinal distribution of coronal mass ejections cmes we propose a method to eliminate projection effects from the apparent observed cme latitude distribution this method has been applied to soho lasco data from 1996 january to 2006 december as a result we find that t... | [['with', 'the', 'assumption', 'of', 'radial', 'motion', 'and', 'uniform', 'longitudinal', 'distribution', 'of', 'coronal', 'mass', 'ejections', 'cmes', 'we', 'propose', 'a', 'method', 'to', 'eliminate', 'projection', 'effects', 'from', 'the', 'apparent', 'observed', 'cme', 'latitude', 'distribution', 'this', 'method',... | [-0.12316374685615301, 0.24590378745575436, -0.0017021338688209652, 0.11844577098963782, -0.07083270808449015, -0.0012745631963480264, 0.0362105493718991, 0.4117356368748005, -0.1729487242916366, -0.3994901329337154, 0.07756405002844985, -0.24228531716158613, -0.13999381014145912, 0.18382082986470777, -0.08691144127864... |
708.0271 | Capacity Region of the Finite-State Multiple Access Channel with and
without Feedback | The capacity region of the Finite-State Multiple Access Channel (FS-MAC) with
feedback that may be an arbitrary time-invariant function of the channel output
samples is considered. We characterize both an inner and an outer bound for
this region, using Masseys's directed information. These bounds are shown to
coincid... | cs.IT math.IT | the capacity region of the finitestate multiple access channel fsmac with feedback that may be an arbitrary timeinvariant function of the channel output samples is considered we characterize both an inner and an outer bound for this region using masseyss directed information these bounds are shown to coincide and hence... | [['the', 'capacity', 'region', 'of', 'the', 'finitestate', 'multiple', 'access', 'channel', 'fsmac', 'with', 'feedback', 'that', 'may', 'be', 'an', 'arbitrary', 'timeinvariant', 'function', 'of', 'the', 'channel', 'output', 'samples', 'is', 'considered', 'we', 'characterize', 'both', 'an', 'inner', 'and', 'an', 'outer'... | [-0.14926375849768087, 0.1193711342135049, -0.043597924986550976, 0.011663190651521544, -0.05871233465583172, -0.21441209352856805, 0.11466997991380996, 0.3589692064081752, -0.290739956888002, -0.2443066934892518, 0.13799494515703775, -0.2296807505926767, -0.10752356412907153, 0.197312652250362, -0.10510580093643174, 0... |
708.0272 | Wavelength-scale stationary-wave integrated Fourier-transform
spectrometry | Spectrometry is a general physical-analysis approach for investigating
light-matter interactions. However, the complex designs of existing
spectrometers render them resistant to simplification and miniaturization, both
of which are vital for applications in micro- and nanotechnology and which are
now undergoing inten... | physics.optics | spectrometry is a general physicalanalysis approach for investigating lightmatter interactions however the complex designs of existing spectrometers render them resistant to simplification and miniaturization both of which are vital for applications in micro and nanotechnology and which are now undergoing intensive res... | [['spectrometry', 'is', 'a', 'general', 'physicalanalysis', 'approach', 'for', 'investigating', 'lightmatter', 'interactions', 'however', 'the', 'complex', 'designs', 'of', 'existing', 'spectrometers', 'render', 'them', 'resistant', 'to', 'simplification', 'and', 'miniaturization', 'both', 'of', 'which', 'are', 'vital'... | [-0.07285704990848899, 0.10345787164066375, -0.07612018795257124, 0.017820294729123512, -0.10754108188052972, -0.14326679808398088, 0.008819601540453732, 0.45069794381658235, -0.23334842454021176, -0.32736979006479183, 0.12243514841732879, -0.2681848746041457, -0.1439900105431055, 0.2777941827584679, -0.029370394203191... |
708.0273 | A simply connected surface of general type with p_g=0 and K^2=3 | Motivated by a recent result of Y. Lee and the second author[7], we construct
a simply connected minimal complex surface of general type with p_g=0 and K^2=3
using a rational blow-down surgery and Q-Gorenstein smoothing theory. In a
similar fashion, we also construct a new simply connected symplectic 4-manifold
with ... | math.AG math.SG | motivated by a recent result of y lee and the second author7 we construct a simply connected minimal complex surface of general type with p_g0 and k23 using a rational blowdown surgery and qgorenstein smoothing theory in a similar fashion we also construct a new simply connected symplectic 4manifold with b_21 and k24 | [['motivated', 'by', 'a', 'recent', 'result', 'of', 'y', 'lee', 'and', 'the', 'second', 'author7', 'we', 'construct', 'a', 'simply', 'connected', 'minimal', 'complex', 'surface', 'of', 'general', 'type', 'with', 'p_g0', 'and', 'k23', 'using', 'a', 'rational', 'blowdown', 'surgery', 'and', 'qgorenstein', 'smoothing', 't... | [-0.16451107774180576, 0.06286410928274003, -0.11301551395669006, 0.07293591007160452, -0.1328250993258105, -0.2475944739820149, 0.05771167111323358, 0.34024534900135434, -0.24236738524184778, -0.24628730727216372, 0.09986149932284696, -0.2377654667585515, -0.2633708682663452, 0.21912165122249952, -0.22430520674858528,... |
708.0274 | Efficiency of feedback process in cavity quantum electrodynamics | Utilizing the continuous frequency mode quantization scheme, we study from
first principle the efficiency of a feedback scheme that can generate maximally
entangled states of two atoms in an optical cavity through their interactions
with a single input photon. The spectral function of the photon emitted from
the cavi... | quant-ph | utilizing the continuous frequency mode quantization scheme we study from first principle the efficiency of a feedback scheme that can generate maximally entangled states of two atoms in an optical cavity through their interactions with a single input photon the spectral function of the photon emitted from the cavity w... | [['utilizing', 'the', 'continuous', 'frequency', 'mode', 'quantization', 'scheme', 'we', 'study', 'from', 'first', 'principle', 'the', 'efficiency', 'of', 'a', 'feedback', 'scheme', 'that', 'can', 'generate', 'maximally', 'entangled', 'states', 'of', 'two', 'atoms', 'in', 'an', 'optical', 'cavity', 'through', 'their', ... | [-0.10353171316408875, 0.1527694870896769, -0.09835479517137669, -0.005892574345305566, -0.0010019352043540008, -0.15103263209693799, 0.10770772705730604, 0.3914391924949861, -0.2916366050001418, -0.2873324358024367, 0.06555057278405506, -0.26541585748955276, -0.09584952185004211, 0.21322806318760804, -0.02778037156135... |
708.0275 | A new formulation of asset trading games in continuous time with
essential forcing of variation exponent | We introduce a new formulation of asset trading games in continuous time in
the framework of the game-theoretic probability established by Shafer and Vovk
(Probability and Finance: It's Only a Game! (2001) Wiley). In our formulation,
the market moves continuously, but an investor trades in discrete times, which
can d... | q-fin.TR math.PR | we introduce a new formulation of asset trading games in continuous time in the framework of the gametheoretic probability established by shafer and vovk probability and finance its only a game 2001 wiley in our formulation the market moves continuously but an investor trades in discrete times which can depend on the p... | [['we', 'introduce', 'a', 'new', 'formulation', 'of', 'asset', 'trading', 'games', 'in', 'continuous', 'time', 'in', 'the', 'framework', 'of', 'the', 'gametheoretic', 'probability', 'established', 'by', 'shafer', 'and', 'vovk', 'probability', 'and', 'finance', 'its', 'only', 'a', 'game', '2001', 'wiley', 'in', 'our', '... | [-0.05044080480001867, 0.04796416180277862, -0.1684406743784929, 0.10114058739877417, -0.057923317039557325, -0.14321622302780715, 0.11633080985997148, 0.39136415674669933, -0.2944200267802749, -0.25004717408743493, 0.1439673004221896, -0.28566669889619484, -0.17961165522250203, 0.14445113018155098, -0.1934366229704374... |
708.0276 | Area Invariance of Apparent Horizons under Arbitrary Boosts | It is a well known analytic result in general relativity that the
2-dimensional area of the apparent horizon of a black hole remains invariant
regardless of the motion of the observer, and in fact is independent of the $
t=constant $ slice, which can be quite arbitrary in general relativity.
Nonetheless the explicit ... | gr-qc | it is a well known analytic result in general relativity that the 2dimensional area of the apparent horizon of a black hole remains invariant regardless of the motion of the observer and in fact is independent of the tconstant slice which can be quite arbitrary in general relativity nonetheless the explicit computation... | [['it', 'is', 'a', 'well', 'known', 'analytic', 'result', 'in', 'general', 'relativity', 'that', 'the', '2dimensional', 'area', 'of', 'the', 'apparent', 'horizon', 'of', 'a', 'black', 'hole', 'remains', 'invariant', 'regardless', 'of', 'the', 'motion', 'of', 'the', 'observer', 'and', 'in', 'fact', 'is', 'independent', ... | [-0.1300977339459401, 0.08092382895409937, -0.08847838230228619, 0.13050079216718322, -0.09074996247806627, -0.14398874698604958, -0.012713854977451063, 0.34872280498561653, -0.20404565430826682, -0.2972127226572754, 0.1262156487791799, -0.27475352727882296, -0.12087493623012974, 0.21401605543771596, -0.092544629076471... |
708.0277 | Discreteness-induced Transition in Catalytic Reaction Networks | Drastic change in dynamics and statistics in a chemical reaction system,
induced by smallness in the molecule number, is reported. Through stochastic
simulations for random catalytic reaction networks, transition to a novel state
is observed with the decrease in the total molecule number N, characterized by:
i) large... | nlin.AO nlin.PS | drastic change in dynamics and statistics in a chemical reaction system induced by smallness in the molecule number is reported through stochastic simulations for random catalytic reaction networks transition to a novel state is observed with the decrease in the total molecule number n characterized by i large fluctuat... | [['drastic', 'change', 'in', 'dynamics', 'and', 'statistics', 'in', 'a', 'chemical', 'reaction', 'system', 'induced', 'by', 'smallness', 'in', 'the', 'molecule', 'number', 'is', 'reported', 'through', 'stochastic', 'simulations', 'for', 'random', 'catalytic', 'reaction', 'networks', 'transition', 'to', 'a', 'novel', 's... | [-0.14275429833602782, 0.18293339431285857, -0.029743386383634062, 0.014798775894256929, 0.05926571115230521, -0.10503879758839806, 0.11047137200366705, 0.3250123330702384, -0.26665080978224676, -0.3268639133125544, 0.0005913752208774289, -0.2921352008357644, -0.09686379595659673, 0.12178944683168083, 0.015391702724155... |
708.0278 | Quenching Dynamics of a quantum XY spin-1/2 chain in presence of a
transverse field | We study the quantum dynamics of a one-dimensional spin-1/2 anisotropic XY
model in a transverse field when the transverse field or the anisotropic
interaction is quenched at a slow but uniform rate. The two quenching schemes
are called transverse and anisotropic quenching respectively. Our emphasis in
this paper is ... | cond-mat.stat-mech quant-ph | we study the quantum dynamics of a onedimensional spin12 anisotropic xy model in a transverse field when the transverse field or the anisotropic interaction is quenched at a slow but uniform rate the two quenching schemes are called transverse and anisotropic quenching respectively our emphasis in this paper is on the ... | [['we', 'study', 'the', 'quantum', 'dynamics', 'of', 'a', 'onedimensional', 'spin12', 'anisotropic', 'xy', 'model', 'in', 'a', 'transverse', 'field', 'when', 'the', 'transverse', 'field', 'or', 'the', 'anisotropic', 'interaction', 'is', 'quenched', 'at', 'a', 'slow', 'but', 'uniform', 'rate', 'the', 'two', 'quenching',... | [-0.16038377576592114, 0.20771903527294186, -0.0787553341021832, 0.05057831362157945, -0.005666800000496555, -0.12047209168139861, 0.015224895789287984, 0.36866142180205996, -0.2621564002479682, -0.23781196098923998, 0.05749054918387897, -0.27852632236698416, -0.08041476959830252, 0.16760600784809215, 0.035422312687170... |
708.0279 | Expert Elicitation for Reliable System Design | This paper reviews the role of expert judgement to support reliability
assessments within the systems engineering design process. Generic design
processes are described to give the context and a discussion is given about the
nature of the reliability assessments required in the different systems
engineering phases. I... | stat.ME | this paper reviews the role of expert judgement to support reliability assessments within the systems engineering design process generic design processes are described to give the context and a discussion is given about the nature of the reliability assessments required in the different systems engineering phases it is... | [['this', 'paper', 'reviews', 'the', 'role', 'of', 'expert', 'judgement', 'to', 'support', 'reliability', 'assessments', 'within', 'the', 'systems', 'engineering', 'design', 'process', 'generic', 'design', 'processes', 'are', 'described', 'to', 'give', 'the', 'context', 'and', 'a', 'discussion', 'is', 'given', 'about',... | [-0.10105243320304162, 0.04659813888874933, -0.07947572919871523, 0.07634946191018087, -0.09851279812403493, -0.11841390674896035, 0.05058893682537412, 0.36883085295306267, -0.22938401738248831, -0.3269424803307498, 0.12716995230414443, -0.246001198937118, -0.1608286656613403, 0.2103002460606329, -0.12163843496215974, ... |
708.028 | Searching for Stable Na-ordered Phases in Single Crystal Samples of
gamma-NaxCoO2 | We report on the preparation and characterization of single crystal gamma
phase NaxCoO2 with 0.25 < x < 0.84 using a non-aqueous electrochemical
chronoamperemetry technique. By carefully mapping the overpotential versus x
(for x < 0.84), we find six distinct stable phases with Na levels corresponding
to x ~ 0.75, 0.7... | cond-mat.str-el cond-mat.supr-con | we report on the preparation and characterization of single crystal gamma phase naxcoo2 with 025 x 084 using a nonaqueous electrochemical chronoamperemetry technique by carefully mapping the overpotential versus x for x 084 we find six distinct stable phases with na levels corresponding to x 075 071 050 043 033 and 025... | [['we', 'report', 'on', 'the', 'preparation', 'and', 'characterization', 'of', 'single', 'crystal', 'gamma', 'phase', 'naxcoo2', 'with', '025', 'x', '084', 'using', 'a', 'nonaqueous', 'electrochemical', 'chronoamperemetry', 'technique', 'by', 'carefully', 'mapping', 'the', 'overpotential', 'versus', 'x', 'for', 'x', '0... | [-0.08921186475486342, 0.23474463162052073, -0.025065704984115485, -0.05139047831010914, 0.04409084309805277, -0.17510531668722704, 0.15455874148292922, 0.40046508580594514, -0.2527185539826195, -0.33522375724486897, 0.01896485870047264, -0.3672491078501317, -0.026134943047455, 0.14353248425087525, 0.04756169586873321,... |
708.0281 | Stochastic Programming with Probability | In this work we study optimization problems subject to a failure constraint.
This constraint is expressed in terms of a condition that causes failure,
representing a physical or technical breakdown. We formulate the problem in
terms of a probability constraint, where the level of "confidence" is a
modelling parameter... | math.OC | in this work we study optimization problems subject to a failure constraint this constraint is expressed in terms of a condition that causes failure representing a physical or technical breakdown we formulate the problem in terms of a probability constraint where the level of confidence is a modelling parameter and has... | [['in', 'this', 'work', 'we', 'study', 'optimization', 'problems', 'subject', 'to', 'a', 'failure', 'constraint', 'this', 'constraint', 'is', 'expressed', 'in', 'terms', 'of', 'a', 'condition', 'that', 'causes', 'failure', 'representing', 'a', 'physical', 'or', 'technical', 'breakdown', 'we', 'formulate', 'the', 'probl... | [-0.11771200659374396, 0.011532195601498842, -0.09699699390129005, 0.0709899746301824, -0.06913324746847996, -0.09246198788472691, 0.09132947130773053, 0.3462570491217592, -0.2679583769754372, -0.3164936215968205, 0.14874112548280227, -0.23904487786451414, -0.16638219876232435, 0.19046989932462996, -0.09557142833821804... |
708.0282 | Precise dipole moments and quadrupole coupling constants of the cis and
trans conformers of 3-aminophenol: Determination of the absolute conformation | The rotational constants and the nitrogen nuclear quadrupole coupling
constants of cis-3-aminophenol and trans-3-aminophenol are determined using
Fourier-transform microwave spectroscopy. We examine several $J=2\leftarrow{}1$
and $1\leftarrow{}0$ hyperfine-resolved rotational transitions for both
conformers. The tran... | physics.chem-ph physics.atom-ph | the rotational constants and the nitrogen nuclear quadrupole coupling constants of cis3aminophenol and trans3aminophenol are determined using fouriertransform microwave spectroscopy we examine several j2leftarrow1 and 1leftarrow0 hyperfineresolved rotational transitions for both conformers the transitions are fit to a ... | [['the', 'rotational', 'constants', 'and', 'the', 'nitrogen', 'nuclear', 'quadrupole', 'coupling', 'constants', 'of', 'cis3aminophenol', 'and', 'trans3aminophenol', 'are', 'determined', 'using', 'fouriertransform', 'microwave', 'spectroscopy', 'we', 'examine', 'several', 'j2leftarrow1', 'and', '1leftarrow0', 'hyperfine... | [-0.11268525373447558, 0.17099015167593185, 0.03549722180990823, 0.030528279014959418, -0.03214619393492567, -0.13890176081773023, 0.08097460390197049, 0.46208851972016796, -0.18828010657673766, -0.31150002175107083, 0.013982706455963438, -0.24720627738098647, -0.002655176169656474, 0.16612565220124892, 0.0991728405500... |
708.0283 | Localizing the Elliott conjecture at strongly self-absorbing C*-algebras | We formally introduce the concept of localizing the Elliott conjecture at a
given strongly self-absorbing C*-algebra $D$; we also explain how the known
classification theorems for nuclear C*-algebras fit into this concept. As a new
result in this direction, we employ recent results of Lin to show that (under a
mild K... | math.OA math.FA math.KT | we formally introduce the concept of localizing the elliott conjecture at a given strongly selfabsorbing calgebra d we also explain how the known classification theorems for nuclear calgebras fit into this concept as a new result in this direction we employ recent results of lin to show that under a mild ktheoretic con... | [['we', 'formally', 'introduce', 'the', 'concept', 'of', 'localizing', 'the', 'elliott', 'conjecture', 'at', 'a', 'given', 'strongly', 'selfabsorbing', 'calgebra', 'd', 'we', 'also', 'explain', 'how', 'the', 'known', 'classification', 'theorems', 'for', 'nuclear', 'calgebras', 'fit', 'into', 'this', 'concept', 'as', 'a... | [-0.08378764442467142, 0.08673809412446694, -0.09378940464950489, 0.0579075316299688, -0.08673645079644136, -0.1456238477190065, -0.005994126843904591, 0.3596308285520858, -0.3257055620441815, -0.2139258346545731, 0.12123112567810972, -0.2168628863439599, -0.14576603826099158, 0.21035808596691183, -0.13986028831249198,... |
708.0284 | Uniqueness of ground states of some coupled nonlinear Schrodinger
systems and their application | We establish the uniqueness of ground states of some coupled nonlinear
Schrodinger systems in the whole space. We firstly use Schwartz symmetrization
to obtain the existence of ground states for a more general case. To prove the
uniqueness of ground states, we use the radial symmetry of the ground states to
transform... | math.AP | we establish the uniqueness of ground states of some coupled nonlinear schrodinger systems in the whole space we firstly use schwartz symmetrization to obtain the existence of ground states for a more general case to prove the uniqueness of ground states we use the radial symmetry of the ground states to transform the ... | [['we', 'establish', 'the', 'uniqueness', 'of', 'ground', 'states', 'of', 'some', 'coupled', 'nonlinear', 'schrodinger', 'systems', 'in', 'the', 'whole', 'space', 'we', 'firstly', 'use', 'schwartz', 'symmetrization', 'to', 'obtain', 'the', 'existence', 'of', 'ground', 'states', 'for', 'a', 'more', 'general', 'case', 't... | [-0.14221858350450503, 0.028303580317879096, -0.10403645057505106, 0.11362455255242393, -0.05426106054116698, -0.08875729484374033, 0.02473066598176956, 0.29396311556372573, -0.2907787942464518, -0.21490696444011786, 0.12979145931381295, -0.2864707175532685, -0.14627287883092374, 0.18618650476119536, -0.033773660407785... |
708.0285 | Comment: Expert Elicitation for Reliable System Design | Comment: Expert Elicitation for Reliable System Design [arXiv:0708.0279]
| stat.ME | comment expert elicitation for reliable system design arxiv07080279 | [['comment', 'expert', 'elicitation', 'for', 'reliable', 'system', 'design', 'arxiv07080279']] | [-0.13158880593255162, -0.08253678819164634, 0.01359944191062823, 0.08462143456563354, -0.34635184425860643, -0.3816389739513397, 0.23191173910163343, 0.4227041760459542, 0.01668366463854909, -0.3733164742588997, 0.10472536156885326, -0.2193321269005537, -0.17297693388536572, 0.1792470645159483, -0.18648051284253597, 0... |
708.0286 | Uniqueness of positive bound states to Schrodinger systems with critical
exponents | We prove the uniqueness for the positive solutions of the following elliptic
systems: \begin{eqnarray*} \left\{\begin{array}{ll} - \lap (u(x)) =
u(x)^{\alpha}v(x)^{\beta}
- \lap (v(x)) = u(x)^{\beta} v(x)^{\alpha} \end{array} \right.
\end{eqnarray*} Here $x\in R^n$, $n\geq 3$, and $1\leq \alpha, \beta\leq
\frac{n+2... | math.AP | we prove the uniqueness for the positive solutions of the following elliptic systems begineqnarray leftbeginarrayll lap ux uxalphavxbeta lap vx uxbeta vxalpha endarray right endeqnarray here xin rn ngeq 3 and 1leq alpha betaleq fracn2n2 with alphabetafracn2n2 in the special case when n3 and alpha 2 beta3 the systems co... | [['we', 'prove', 'the', 'uniqueness', 'for', 'the', 'positive', 'solutions', 'of', 'the', 'following', 'elliptic', 'systems', 'begineqnarray', 'leftbeginarrayll', 'lap', 'ux', 'uxalphavxbeta', 'lap', 'vx', 'uxbeta', 'vxalpha', 'endarray', 'right', 'endeqnarray', 'here', 'xin', 'rn', 'ngeq', '3', 'and', '1leq', 'alpha',... | [-0.2077321389194908, 0.07739081869161205, 0.01612540532516528, 0.010060722161603124, 0.013728610207871946, -0.28192494912780347, -0.05238575592071195, 0.285682647657003, -0.27066342424176915, -0.13417260813279241, 0.14120351274857368, -0.44596133006536226, -0.07393403203651026, 0.17250651439439646, -0.0191516662782789... |
708.0287 | Comment: Expert Elicitation for Reliable System Design | Comment: Expert Elicitation for Reliable System Design [arXiv:0708.0279]
| stat.ME | comment expert elicitation for reliable system design arxiv07080279 | [['comment', 'expert', 'elicitation', 'for', 'reliable', 'system', 'design', 'arxiv07080279']] | [-0.13158880593255162, -0.08253678819164634, 0.01359944191062823, 0.08462143456563354, -0.34635184425860643, -0.3816389739513397, 0.23191173910163343, 0.4227041760459542, 0.01668366463854909, -0.3733164742588997, 0.10472536156885326, -0.2193321269005537, -0.17297693388536572, 0.1792470645159483, -0.18648051284253597, 0... |
708.0288 | Comment: Expert Elicitation for Reliable System Design | Comment: Expert Elicitation for Reliable System Design [arXiv:0708.0279]
| stat.ME | comment expert elicitation for reliable system design arxiv07080279 | [['comment', 'expert', 'elicitation', 'for', 'reliable', 'system', 'design', 'arxiv07080279']] | [-0.13158880593255162, -0.08253678819164634, 0.01359944191062823, 0.08462143456563354, -0.34635184425860643, -0.3816389739513397, 0.23191173910163343, 0.4227041760459542, 0.01668366463854909, -0.3733164742588997, 0.10472536156885326, -0.2193321269005537, -0.17297693388536572, 0.1792470645159483, -0.18648051284253597, 0... |
708.0289 | Pulsation tomography of rapidly oscillating Ap stars. Resolving the
third dimension in peculiar pulsating stellar atmospheres | We present detailed analysis of the vertical pulsation mode cross-section in
ten rapidly oscillating Ap (roAp) stars based on spectroscopic time-series
observations. The aim of this analysis is to derive from observations a
complete picture of how the amplitude and phase of magnetoacoustic waves depend
on depth. We f... | astro-ph | we present detailed analysis of the vertical pulsation mode crosssection in ten rapidly oscillating ap roap stars based on spectroscopic timeseries observations the aim of this analysis is to derive from observations a complete picture of how the amplitude and phase of magnetoacoustic waves depend on depth we find comm... | [['we', 'present', 'detailed', 'analysis', 'of', 'the', 'vertical', 'pulsation', 'mode', 'crosssection', 'in', 'ten', 'rapidly', 'oscillating', 'ap', 'roap', 'stars', 'based', 'on', 'spectroscopic', 'timeseries', 'observations', 'the', 'aim', 'of', 'this', 'analysis', 'is', 'to', 'derive', 'from', 'observations', 'a', ... | [-0.11772731447044733, 0.19537571480851884, -0.02669837873127364, 0.05116569833226607, -0.1167535670241013, -0.10314124837537414, 0.1350563815786687, 0.38060981315613107, -0.1987652957187736, -0.27366083127144775, 0.037453202376204454, -0.3214497019563028, -0.06512213328731915, 0.1924666086907423, -0.002535509454696373... |
708.029 | HST multi-epoch imaging of the PSR B0540-69 system unveils a highly
dynamic synchrotron nebula | PSR B0540-69 is the Crab twin in the Large Magellanic Cloud. Age, energetic
and overall behaviour of the two pulsars are very similar. The same is true for
the general appearance of their pulsar wind nebulae (PWNe). Analysis of Hubble
Space Telescope images spanning 10 years unveiled significant variability in
the PW... | astro-ph | psr b054069 is the crab twin in the large magellanic cloud age energetic and overall behaviour of the two pulsars are very similar the same is true for the general appearance of their pulsar wind nebulae pwne analysis of hubble space telescope images spanning 10 years unveiled significant variability in the pwn surroun... | [['psr', 'b054069', 'is', 'the', 'crab', 'twin', 'in', 'the', 'large', 'magellanic', 'cloud', 'age', 'energetic', 'and', 'overall', 'behaviour', 'of', 'the', 'two', 'pulsars', 'are', 'very', 'similar', 'the', 'same', 'is', 'true', 'for', 'the', 'general', 'appearance', 'of', 'their', 'pulsar', 'wind', 'nebulae', 'pwne'... | [-0.1314956473440609, 0.116314062530349, -0.0640435712535007, 0.13122212038036773, -0.18024783792389817, -0.06766632743456885, 0.04702663694172597, 0.40589511253647814, -0.22180456027661813, -0.36435945836196015, 0.05015888339974571, -0.2802693526960971, 0.02896500100220038, 0.2575305704314123, -0.07324624949804515, -0... |
708.0291 | Quantum Entanglement of Neutrino Pairs | It is practically shown that a pair of neutrinos from tau decay can form a
flavor entangled state. With this kind of state we show that the locality
constrains imposed by Bell inequality are violated by the quantum mechanics,
and an experimental test of this effect is feasible within the earth's length
scale. Theoret... | quant-ph hep-ph | it is practically shown that a pair of neutrinos from tau decay can form a flavor entangled state with this kind of state we show that the locality constrains imposed by bell inequality are violated by the quantum mechanics and an experimental test of this effect is feasible within the earths length scale theoretically... | [['it', 'is', 'practically', 'shown', 'that', 'a', 'pair', 'of', 'neutrinos', 'from', 'tau', 'decay', 'can', 'form', 'a', 'flavor', 'entangled', 'state', 'with', 'this', 'kind', 'of', 'state', 'we', 'show', 'that', 'the', 'locality', 'constrains', 'imposed', 'by', 'bell', 'inequality', 'are', 'violated', 'by', 'the', '... | [-0.13651959652242324, 0.2340735100668285, -0.12378667783326446, 0.11990862893752563, -0.014053688121911807, -0.1838032656128351, 0.032027562226479254, 0.3293247888915432, -0.29475789395627755, -0.25804987743210334, 0.028687657300347034, -0.2424679245465459, -0.06838888114986894, 0.20067525435334596, -0.031267978265905... |
708.0292 | Comment on ``Geometric phase of entangled spin pairs in a magnetic
field'' | The degree of entanglement between two spins may change due to interaction.
About this we find that a wrong result in a recent work by Ge and Wadati [Phys.
Rev. A {\bf72}, 052101(2005)] which breach the basic principle.
| quant-ph | the degree of entanglement between two spins may change due to interaction about this we find that a wrong result in a recent work by ge and wadati phys rev a bf72 0521012005 which breach the basic principle | [['the', 'degree', 'of', 'entanglement', 'between', 'two', 'spins', 'may', 'change', 'due', 'to', 'interaction', 'about', 'this', 'we', 'find', 'that', 'a', 'wrong', 'result', 'in', 'a', 'recent', 'work', 'by', 'ge', 'and', 'wadati', 'phys', 'rev', 'a', 'bf72', '0521012005', 'which', 'breach', 'the', 'basic', 'principl... | [-0.10790771253717442, 0.13440394420952848, -0.053569068770027824, -0.046889940370520994, -0.05361664900556207, -0.12258457373051594, 0.11682984626127614, 0.28015563261902166, -0.20730201665881193, -0.354292137030926, -0.02860760740845257, -0.26087258766508764, -0.19556006045442903, 0.15812209683159986, -0.120854269894... |
708.0293 | Rejoinder: Expert Elicitation for Reliable System Design | Rejoinder: Expert Elicitation for Reliable System Design [arXiv:0708.0279]
| stat.ME | rejoinder expert elicitation for reliable system design arxiv07080279 | [['rejoinder', 'expert', 'elicitation', 'for', 'reliable', 'system', 'design', 'arxiv07080279']] | [-0.0324556571431458, -0.1502893059514463, -0.01868487987667322, 0.09884654870256782, -0.31732478458434343, -0.3486605007201433, 0.21135418652556837, 0.4424263034015894, -0.014701442327350378, -0.39473528042435646, 0.08371124207042158, -0.26857726089656353, -0.16580774309113622, 0.15166439302265644, -0.2243771739304065... |
708.0294 | The influence of device geometry on many-body effects in quantum point
contacts: Signatures of the 0.7 anomaly, exchange and Kondo | The conductance of a quantum point contact (QPC) shows several features that
result from many-body electron interactions. The spin degeneracy in zero
magnetic field appears to be spontaneously lifted due to the so-called 0.7
anomaly. Further, the g-factor for electrons in the QPC is enhanced, and a
zero-bias peak in ... | cond-mat.mes-hall | the conductance of a quantum point contact qpc shows several features that result from manybody electron interactions the spin degeneracy in zero magnetic field appears to be spontaneously lifted due to the socalled 07 anomaly further the gfactor for electrons in the qpc is enhanced and a zerobias peak in the conductan... | [['the', 'conductance', 'of', 'a', 'quantum', 'point', 'contact', 'qpc', 'shows', 'several', 'features', 'that', 'result', 'from', 'manybody', 'electron', 'interactions', 'the', 'spin', 'degeneracy', 'in', 'zero', 'magnetic', 'field', 'appears', 'to', 'be', 'spontaneously', 'lifted', 'due', 'to', 'the', 'socalled', '07... | [-0.20666820532642305, 0.15805935516087874, -0.10191688369112936, 0.09498272934019494, -0.04419087097895416, -0.17594727086634085, 0.08387656512215698, 0.3515849086215372, -0.27790413391592567, -0.3242487057098789, -0.017857776778754577, -0.3289792468708953, -0.16638062083336155, 0.1823497953887084, 0.0178709420928081,... |
708.0295 | Reliability | This special volume of Statistical Sciences presents some innovative, if not
provocative, ideas in the area of reliability, or perhaps more appropriately
named, integrated system assessment. In this age of exponential growth in
science, engineering and technology, the capability to evaluate the
performance, reliabili... | stat.ME | this special volume of statistical sciences presents some innovative if not provocative ideas in the area of reliability or perhaps more appropriately named integrated system assessment in this age of exponential growth in science engineering and technology the capability to evaluate the performance reliability and saf... | [['this', 'special', 'volume', 'of', 'statistical', 'sciences', 'presents', 'some', 'innovative', 'if', 'not', 'provocative', 'ideas', 'in', 'the', 'area', 'of', 'reliability', 'or', 'perhaps', 'more', 'appropriately', 'named', 'integrated', 'system', 'assessment', 'in', 'this', 'age', 'of', 'exponential', 'growth', 'i... | [-0.059970176405499155, 0.027758276702441048, -0.07411250668775403, 0.07683820707977496, -0.1591943615624173, -0.1266575358187159, 0.07677587534329205, 0.38774971241752304, -0.24840910626067356, -0.389833982624678, 0.14971503992988305, -0.28239958186520997, -0.16331541366931615, 0.24310505265849783, -0.1656481372390055... |
708.0296 | Quantum Ergodicity for products of hyperbolic planes | For manifolds with geodesic flow that is ergodic on the unit tangent bundle,
the quantum ergodicity theorem implies that almost all Laplacian eigenfunctions
become equidistributed as the eigenvalue goes to infinity. For a locally
symmetric space with a universal cover that is a product of several upper half
planes, t... | math-ph math.MP | for manifolds with geodesic flow that is ergodic on the unit tangent bundle the quantum ergodicity theorem implies that almost all laplacian eigenfunctions become equidistributed as the eigenvalue goes to infinity for a locally symmetric space with a universal cover that is a product of several upper half planes the ge... | [['for', 'manifolds', 'with', 'geodesic', 'flow', 'that', 'is', 'ergodic', 'on', 'the', 'unit', 'tangent', 'bundle', 'the', 'quantum', 'ergodicity', 'theorem', 'implies', 'that', 'almost', 'all', 'laplacian', 'eigenfunctions', 'become', 'equidistributed', 'as', 'the', 'eigenvalue', 'goes', 'to', 'infinity', 'for', 'a',... | [-0.19626532602970573, 0.1740178453566676, -0.08398454950127582, 0.08826899847454941, -0.06986232797498815, -0.14647687550909308, -0.016729398728454147, 0.37925647778055543, -0.286572661139706, -0.128411294024607, 0.17337548319880047, -0.32049423082604667, -0.1336615853360854, 0.22895849007181823, -0.11439878262833438,... |
708.0297 | Partition test and sexual motivation in male mice | Theoretical analysis of own and literature investigations of sexual
motivation with the use of the partition test [Kudryavtseva, 1987, 1994] in
male mice was carried out. It has been shown that appearance of a receptive
female in the neighboring compartment of common cage separated by perforated
transparent partition... | q-bio.OT | theoretical analysis of own and literature investigations of sexual motivation with the use of the partition test kudryavtseva 1987 1994 in male mice was carried out it has been shown that appearance of a receptive female in the neighboring compartment of common cage separated by perforated transparent partition produc... | [['theoretical', 'analysis', 'of', 'own', 'and', 'literature', 'investigations', 'of', 'sexual', 'motivation', 'with', 'the', 'use', 'of', 'the', 'partition', 'test', 'kudryavtseva', '1987', '1994', 'in', 'male', 'mice', 'was', 'carried', 'out', 'it', 'has', 'been', 'shown', 'that', 'appearance', 'of', 'a', 'receptive'... | [-0.03058825889407505, 0.12761163406734508, -0.0637582308144251, 0.08778438743934837, -0.09241548040881753, -0.166906305829961, 0.07432900039725882, 0.4076449340394887, -0.18954898356144648, -0.3147433316594813, 0.011093812852270485, -0.2899178263491977, -0.2378051201209975, 0.12301674154791165, -0.15509353542099316, -... |
708.0298 | First polarimetric observations and modeling of the FeH F^4 Delta-X^4
Delta system | Lines of diatomic molecules are more temperature and pressure sensitive than
atomic lines, which makes them ideal tools for studying cool stellar
atmospheres an internal structure of sunspots and starspots. The FeH F^4
Delta-X^4 Delta system represents such an example that exhibits in addition a
large magnetic field ... | astro-ph | lines of diatomic molecules are more temperature and pressure sensitive than atomic lines which makes them ideal tools for studying cool stellar atmospheres an internal structure of sunspots and starspots the feh f4 deltax4 delta system represents such an example that exhibits in addition a large magnetic field sensiti... | [['lines', 'of', 'diatomic', 'molecules', 'are', 'more', 'temperature', 'and', 'pressure', 'sensitive', 'than', 'atomic', 'lines', 'which', 'makes', 'them', 'ideal', 'tools', 'for', 'studying', 'cool', 'stellar', 'atmospheres', 'an', 'internal', 'structure', 'of', 'sunspots', 'and', 'starspots', 'the', 'feh', 'f4', 'de... | [-0.09039338191784918, 0.11807978329912294, -0.010550957281142474, 0.07836918353289365, -0.09850786303170025, -0.12008587478660047, 0.04208658251538873, 0.4020100054591894, -0.18997411711327733, -0.38668019290268424, 0.04077974479086697, -0.25514744772302217, -0.06925762442304403, 0.22451709290593863, 0.005896692568436... |
708.0299 | Spectral properties of quarks above T_c in quenched lattice QCD | We analyze the quark spectral function above the critical temperature for
deconfinement in quenched lattice QCD using clover improved Wilson fermions in
Landau gauge. We show that the temporal quark correlator is well reproduced by
a two-pole approximation for the spectral function and analyze the bare quark
mass dep... | hep-lat hep-ph | we analyze the quark spectral function above the critical temperature for deconfinement in quenched lattice qcd using clover improved wilson fermions in landau gauge we show that the temporal quark correlator is well reproduced by a twopole approximation for the spectral function and analyze the bare quark mass depende... | [['we', 'analyze', 'the', 'quark', 'spectral', 'function', 'above', 'the', 'critical', 'temperature', 'for', 'deconfinement', 'in', 'quenched', 'lattice', 'qcd', 'using', 'clover', 'improved', 'wilson', 'fermions', 'in', 'landau', 'gauge', 'we', 'show', 'that', 'the', 'temporal', 'quark', 'correlator', 'is', 'well', 'r... | [-0.08469034380941969, 0.26504519708051355, -0.1200861967668014, 0.1469430660123255, -0.014079185193116517, -0.06273703061082621, 0.09644945776186038, 0.3787004703982282, -0.14458828158292575, -0.25050397689655884, 0.011107897173151849, -0.27105593005406486, -0.0710624316947285, 0.06526829851503224, 0.06640405762345367... |
708.03 | Asymptotic behavior of flat surfaces in hyperbolic 3-space | In this paper, we investigate the asymptotic behavior of regular ends of flat
surfaces in the hyperbolic 3-space H^3. Galvez, Martinez and Milan showed that
when the singular set does not accumulate at an end, the end is asymptotic to a
rotationally symmetric flat surface. As a refinement of their result, we show
tha... | math.DG | in this paper we investigate the asymptotic behavior of regular ends of flat surfaces in the hyperbolic 3space h3 galvez martinez and milan showed that when the singular set does not accumulate at an end the end is asymptotic to a rotationally symmetric flat surface as a refinement of their result we show that the asym... | [['in', 'this', 'paper', 'we', 'investigate', 'the', 'asymptotic', 'behavior', 'of', 'regular', 'ends', 'of', 'flat', 'surfaces', 'in', 'the', 'hyperbolic', '3space', 'h3', 'galvez', 'martinez', 'and', 'milan', 'showed', 'that', 'when', 'the', 'singular', 'set', 'does', 'not', 'accumulate', 'at', 'an', 'end', 'the', 'e... | [-0.18341168934544225, 0.14361982549953656, -0.10056585777291463, 0.046869242417890186, -0.07485726305899855, -0.14422466261405034, 0.009061245506036267, 0.35383668169379234, -0.24344062606169292, -0.22628220771867968, 0.10001738339637067, -0.29052158127033817, -0.14409576261077836, 0.145625014563522, -0.08982071472304... |
708.0301 | Fast recognition of single molecules based on single event photon
statistics | Mandel Q-parameter, which is determined from single event photon statistics,
provides an alternative to differentiate single-molecule with fluorescence
detection. In this work, by using the Q-parameter of the sample fluorescence
compared to that of an ideal double-molecule system with the same average
photon number, ... | quant-ph | mandel qparameter which is determined from single event photon statistics provides an alternative to differentiate singlemolecule with fluorescence detection in this work by using the qparameter of the sample fluorescence compared to that of an ideal doublemolecule system with the same average photon number we present ... | [['mandel', 'qparameter', 'which', 'is', 'determined', 'from', 'single', 'event', 'photon', 'statistics', 'provides', 'an', 'alternative', 'to', 'differentiate', 'singlemolecule', 'with', 'fluorescence', 'detection', 'in', 'this', 'work', 'by', 'using', 'the', 'qparameter', 'of', 'the', 'sample', 'fluorescence', 'compa... | [-0.03430142654779266, 0.08525184683637772, -0.09940743982702134, 0.06360331282625536, 0.007659780299178807, -0.1542654332244791, 0.047283430199464224, 0.35757523512535067, -0.1811100529052362, -0.35904967771416685, -0.002057271550903209, -0.3292290486215827, -0.05482809912099178, 0.2954423719994634, -0.014277671037398... |
708.0302 | Monitoring Networked Applications With Incremental Quantile Estimation | Networked applications have software components that reside on different
computers. Email, for example, has database, processing, and user interface
components that can be distributed across a network and shared by users in
different locations or work groups. End-to-end performance and reliability
metrics describe th... | stat.ME | networked applications have software components that reside on different computers email for example has database processing and user interface components that can be distributed across a network and shared by users in different locations or work groups endtoend performance and reliability metrics describe the software... | [['networked', 'applications', 'have', 'software', 'components', 'that', 'reside', 'on', 'different', 'computers', 'email', 'for', 'example', 'has', 'database', 'processing', 'and', 'user', 'interface', 'components', 'that', 'can', 'be', 'distributed', 'across', 'a', 'network', 'and', 'shared', 'by', 'users', 'in', 'di... | [-0.13514716610940092, 0.023432615479538545, -0.06619042884077593, 0.04922772720759815, -0.08956572072676626, -0.1708038964475829, 0.049478938191896304, 0.44494881979999656, -0.2432150006289189, -0.3512330472813514, 0.13564074839561488, -0.2895739421061159, -0.11279812991573557, 0.2279621542737637, -0.13007925159510467... |
708.0303 | Adiabatically switched-on electrical bias in continuous systems, and the
Landauer-Buttiker formula | Consider a three dimensional system which looks like a cross-connected pipe
system, i.e. a small sample coupled to a finite number of leads. We investigate
the current running through this system, in the linear response regime, when we
adiabatically turn on an electrical bias between leads. The main technical tool
is... | cond-mat.mes-hall cond-mat.stat-mech math-ph math.MP | consider a three dimensional system which looks like a crossconnected pipe system ie a small sample coupled to a finite number of leads we investigate the current running through this system in the linear response regime when we adiabatically turn on an electrical bias between leads the main technical tool is the use o... | [['consider', 'a', 'three', 'dimensional', 'system', 'which', 'looks', 'like', 'a', 'crossconnected', 'pipe', 'system', 'ie', 'a', 'small', 'sample', 'coupled', 'to', 'a', 'finite', 'number', 'of', 'leads', 'we', 'investigate', 'the', 'current', 'running', 'through', 'this', 'system', 'in', 'the', 'linear', 'response',... | [-0.16059095438416163, 0.10775979347758058, -0.10118970743826945, 0.010106452665118905, -0.06944551774973924, -0.13821741154167763, 0.055597353978658615, 0.3054889264353311, -0.27721132333246395, -0.2557929223307322, 0.09996789506847788, -0.24783524515640745, -0.14124201090295904, 0.2156877217948744, -0.061091080885236... |
708.0304 | Improved measurement of time-dependent CP violation in B0 -> J/Psi pi0
decays | We report improved measurements of time-dependent CP violation parameters for
$B^0(\bar{B}^0) \to J/\psi \pi^0$ decay. This analysis is based on 535 million
$B\bar{B}$ pairs accumulated at the $\Upsilon(4S)$ resonance with the Belle
detector at the KEKB asymmetric-energy e^+e^- collider. From the distribution
of prop... | hep-ex | we report improved measurements of timedependent cp violation parameters for b0barb0 to jpsi pi0 decay this analysis is based on 535 million bbarb pairs accumulated at the upsilon4s resonance with the belle detector at the kekb asymmetricenergy ee collider from the distribution of proper time intervals between the two ... | [['we', 'report', 'improved', 'measurements', 'of', 'timedependent', 'cp', 'violation', 'parameters', 'for', 'b0barb0', 'to', 'jpsi', 'pi0', 'decay', 'this', 'analysis', 'is', 'based', 'on', '535', 'million', 'bbarb', 'pairs', 'accumulated', 'at', 'the', 'upsilon4s', 'resonance', 'with', 'the', 'belle', 'detector', 'at... | [-0.09242939096210258, 0.1918308861221054, -0.10122472707714353, 0.06647405917756259, -0.08556913741465126, -0.15429611172127936, 0.11758849770662241, 0.27000556997954844, -0.12889091458304652, -0.25549013407102655, -0.08329369888441371, -0.4882314646483532, 0.10570765483592237, 0.1658157793272819, 0.12788413861500367,... |
708.0305 | Quantization of Atomic and Nuclear Rest Masses | We were able to quantize phenomenologically the first time the atomic and
nuclear rest masses. Note that this quantization rule is justified for atoms
and nuclei with different A, N and Z and the nuclei and atoms represent a
coherent synchronized systems -- a complex of coupled oscillators (resonators).
The cooperati... | physics.gen-ph nucl-th | we were able to quantize phenomenologically the first time the atomic and nuclear rest masses note that this quantization rule is justified for atoms and nuclei with different a n and z and the nuclei and atoms represent a coherent synchronized systems a complex of coupled oscillators resonators the cooperative resonan... | [['we', 'were', 'able', 'to', 'quantize', 'phenomenologically', 'the', 'first', 'time', 'the', 'atomic', 'and', 'nuclear', 'rest', 'masses', 'note', 'that', 'this', 'quantization', 'rule', 'is', 'justified', 'for', 'atoms', 'and', 'nuclei', 'with', 'different', 'a', 'n', 'and', 'z', 'and', 'the', 'nuclei', 'and', 'atom... | [-0.10836527127158378, 0.2615369262452098, -0.029936748816385524, 0.10110586658976543, -0.0019598075499137244, -0.17415699112796407, 0.08034844161011279, 0.38612850876418, -0.23115425700343203, -0.27899230907446354, -0.008610850724595031, -0.271627022445887, -0.10562463185814178, 0.17756382708341398, 0.0455481293397131... |
708.0306 | Rapid formation of exponential disks and bulges at high redshift from
the dynamical evolution of clump cluster and chain galaxies | Many galaxies at high redshift have peculiar morphologies dominated by
10^8-10^9 Mo kpc-sized clumps. Using numerical simulations, we show that these
"clump clusters" can result from fragmentation in gravitationally unstable
primordial disks. They appear as "chain galaxies" when observed edge-on. In
less than 1 Gyr, ... | astro-ph | many galaxies at high redshift have peculiar morphologies dominated by 108109 mo kpcsized clumps using numerical simulations we show that these clump clusters can result from fragmentation in gravitationally unstable primordial disks they appear as chain galaxies when observed edgeon in less than 1 gyr clump formation ... | [['many', 'galaxies', 'at', 'high', 'redshift', 'have', 'peculiar', 'morphologies', 'dominated', 'by', '108109', 'mo', 'kpcsized', 'clumps', 'using', 'numerical', 'simulations', 'we', 'show', 'that', 'these', 'clump', 'clusters', 'can', 'result', 'from', 'fragmentation', 'in', 'gravitationally', 'unstable', 'primordial... | [-0.09681271894568175, 0.13542028182425597, -0.09098338830897856, 0.1110151880643045, -0.06803585293974222, -0.016033416255915433, -0.03083228621042179, 0.4363813249478538, -0.16397628192813252, -0.3012903038863954, 0.05138179168266586, -0.257009710994872, -0.012823918399087449, 0.16911493171937764, 0.00340684031103573... |
708.0307 | Color-flavor locked superconductor in a magnetic field | We study the effects of moderately strong magnetic fields on the properties
of color-flavor locked color superconducting quark matter in the framework of
the Nambu-Jona-Lasinio model. We find that the energy gaps, which describe the
color superconducting pairing as well as the magnetization, are oscillating
functions... | hep-ph astro-ph hep-th | we study the effects of moderately strong magnetic fields on the properties of colorflavor locked color superconducting quark matter in the framework of the nambujonalasinio model we find that the energy gaps which describe the color superconducting pairing as well as the magnetization are oscillating functions of the ... | [['we', 'study', 'the', 'effects', 'of', 'moderately', 'strong', 'magnetic', 'fields', 'on', 'the', 'properties', 'of', 'colorflavor', 'locked', 'color', 'superconducting', 'quark', 'matter', 'in', 'the', 'framework', 'of', 'the', 'nambujonalasinio', 'model', 'we', 'find', 'that', 'the', 'energy', 'gaps', 'which', 'des... | [-0.1653318892319485, 0.27052877438206646, -0.07867025923387137, 0.0942360976190047, -0.07034242091719638, -0.03449178233109031, 0.05988473771860074, 0.38459905693979607, -0.23408845681505105, -0.30695905025625964, 0.003669783811459375, -0.23153430629598418, -0.06522194861876059, 0.15406424650615178, 0.0411584511682506... |
708.0308 | Galaxies:kinematics as a proof of the existence of a universal field of
minimum acceleration | Taking into account only luminous objects, the kinematics of clusters of
galaxies, galaxies and their interior, require a much higher mass than the
luminous one to explain the observations. This situation has provoked more than
30 years of intense research and has stimulated hypothesis like the dark
matter. Also new ... | physics.gen-ph | taking into account only luminous objects the kinematics of clusters of galaxies galaxies and their interior require a much higher mass than the luminous one to explain the observations this situation has provoked more than 30 years of intense research and has stimulated hypothesis like the dark matter also new mechani... | [['taking', 'into', 'account', 'only', 'luminous', 'objects', 'the', 'kinematics', 'of', 'clusters', 'of', 'galaxies', 'galaxies', 'and', 'their', 'interior', 'require', 'a', 'much', 'higher', 'mass', 'than', 'the', 'luminous', 'one', 'to', 'explain', 'the', 'observations', 'this', 'situation', 'has', 'provoked', 'more... | [-0.07387187447108581, 0.12549703977623003, -0.13281978473906625, 0.08513649285449014, -0.09539183722176578, -0.08283924434426022, 0.008871708681841416, 0.349332205837673, -0.20154019922339989, -0.3502813550517147, 0.05941593964270857, -0.25125947663054604, -0.05183474023188292, 0.17845636764897432, -0.0375428191705227... |
708.0309 | Curvature of almost quaternion-Hermitian manifolds | We study the decomposition of the Riemannian curvature R tensor of an almost
quaternion-Hermitian manifold under the action of its structure group
Sp(n)Sp(1). Using the minimal connection, we show that most components are
determined by the intrinsic torsion \xi and its covariant derivative
\widetilde\nabla\xi and det... | math.DG | we study the decomposition of the riemannian curvature r tensor of an almost quaternionhermitian manifold under the action of its structure group spnsp1 using the minimal connection we show that most components are determined by the intrinsic torsion xi and its covariant derivative widetildenablaxi and determine relati... | [['we', 'study', 'the', 'decomposition', 'of', 'the', 'riemannian', 'curvature', 'r', 'tensor', 'of', 'an', 'almost', 'quaternionhermitian', 'manifold', 'under', 'the', 'action', 'of', 'its', 'structure', 'group', 'spnsp1', 'using', 'the', 'minimal', 'connection', 'we', 'show', 'that', 'most', 'components', 'are', 'det... | [-0.21916551357417396, 0.07689712475478176, -0.11194761411223392, 0.04992639437092073, -0.12665506116481443, -0.0954375597789432, -0.06109094997924386, 0.3951457023521829, -0.2843589467423347, -0.22113290570224775, 0.12645842385421874, -0.27829166230830277, -0.18889309690249237, 0.10252468160240713, -0.0456048150010632... |
708.031 | Large inductive dimension of the Smirnov remainder | The purpose of this paper is to investigate the large inductive dimension of
the remainder of the Smirnov compactification of the n-dimensional Euclidean
space with the usual metric, and give an application of it.
| math.GN math.MG | the purpose of this paper is to investigate the large inductive dimension of the remainder of the smirnov compactification of the ndimensional euclidean space with the usual metric and give an application of it | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'investigate', 'the', 'large', 'inductive', 'dimension', 'of', 'the', 'remainder', 'of', 'the', 'smirnov', 'compactification', 'of', 'the', 'ndimensional', 'euclidean', 'space', 'with', 'the', 'usual', 'metric', 'and', 'give', 'an', 'application', 'of', 'it']] | [-0.1165980847333284, 0.08366029628472033, -0.06504184352781843, 0.09149459338582613, -0.09103403628036819, -0.016521245432908043, -0.014639414021717933, 0.24844168137539835, -0.25193608995280503, -0.23518918801838642, 0.15454796803019502, -0.23243093515253244, -0.1586211495758856, 0.1571993473917246, -0.12339714314679... |
708.0311 | Lagrangian Structure Functions in Turbulence: A Quantitative Comparison
between Experiment and Direct Numerical Simulation | A detailed comparison between data from experimental measurements and
numerical simulations of Lagrangian velocity structure functions in turbulence
is presented. By integrating information from experiments and numerics, a
quantitative understanding of the velocity scaling properties over a wide range
of time scales ... | nlin.CD cond-mat.stat-mech physics.flu-dyn | a detailed comparison between data from experimental measurements and numerical simulations of lagrangian velocity structure functions in turbulence is presented by integrating information from experiments and numerics a quantitative understanding of the velocity scaling properties over a wide range of time scales and ... | [['a', 'detailed', 'comparison', 'between', 'data', 'from', 'experimental', 'measurements', 'and', 'numerical', 'simulations', 'of', 'lagrangian', 'velocity', 'structure', 'functions', 'in', 'turbulence', 'is', 'presented', 'by', 'integrating', 'information', 'from', 'experiments', 'and', 'numerics', 'a', 'quantitative... | [-0.14433378312375625, 0.1248948362665441, -0.11457149748101222, 0.08670943013359127, -0.035756048247484226, -0.07077720776029235, 0.02250020709886615, 0.3648267633528734, -0.2694770324005916, -0.35209175134647863, 0.050162951459594984, -0.30723517572944414, -0.06444830188233101, 0.2687274684953712, 0.03426663271550621... |
708.0312 | Anomalous Scaling and Refined Similarity of an Active Scalar in a Model
of Homogeneous Turbulent Convection | Anomalous scaling in the statistics of an active scalar in homogeneous
turbulent convection is studied using a dynamical shell model. We extend
refined similarity ideas for homogeneous and isotropic turbulence to
homogeneous turbulent convection and attribute the origin of the anomalous
scaling to variations of the e... | nlin.CD | anomalous scaling in the statistics of an active scalar in homogeneous turbulent convection is studied using a dynamical shell model we extend refined similarity ideas for homogeneous and isotropic turbulence to homogeneous turbulent convection and attribute the origin of the anomalous scaling to variations of the entr... | [['anomalous', 'scaling', 'in', 'the', 'statistics', 'of', 'an', 'active', 'scalar', 'in', 'homogeneous', 'turbulent', 'convection', 'is', 'studied', 'using', 'a', 'dynamical', 'shell', 'model', 'we', 'extend', 'refined', 'similarity', 'ideas', 'for', 'homogeneous', 'and', 'isotropic', 'turbulence', 'to', 'homogeneous'... | [-0.12453132086271321, 0.18837671289254235, -0.09564245690541741, 0.1015576927883168, -0.020100832020814, -0.09568674414289749, 0.054347794935373325, 0.28904669825195534, -0.2596896999166347, -0.27100990030781497, 0.07660947456731394, -0.2651552693818563, -0.11899362185171672, 0.2020566491867482, 0.010223126213531941, ... |
708.0313 | Heating by Acoustic Waves of Multiphase Media | We study the emission and dissipation of acoustic waves from cool dense
clouds in pressure equilibrium with a hot, volume-filling dilute gas component.
In our model, the clouds are exposed to a source of ionizing radiation whose
flux level varies with time, forcing the clouds to pulsate. We estimate the
rate at which... | astro-ph | we study the emission and dissipation of acoustic waves from cool dense clouds in pressure equilibrium with a hot volumefilling dilute gas component in our model the clouds are exposed to a source of ionizing radiation whose flux level varies with time forcing the clouds to pulsate we estimate the rate at which acousti... | [['we', 'study', 'the', 'emission', 'and', 'dissipation', 'of', 'acoustic', 'waves', 'from', 'cool', 'dense', 'clouds', 'in', 'pressure', 'equilibrium', 'with', 'a', 'hot', 'volumefilling', 'dilute', 'gas', 'component', 'in', 'our', 'model', 'the', 'clouds', 'are', 'exposed', 'to', 'a', 'source', 'of', 'ionizing', 'rad... | [-0.11429765300476753, 0.19681296873850265, -0.04816086071214693, 0.027525384370937604, -0.028617725579761992, 0.003972976757639569, 0.054767698722928033, 0.3728581030725264, -0.2530914749037109, -0.3048578980211412, 0.06652864260413362, -0.33348927881227797, -0.0046502708512954904, 0.211228152601584, -0.00152194541970... |
708.0314 | Imaging correlated wave functions of few-electron quantum dots: Theory
and scanning tunneling spectroscopy experiments | We show both theoretically and experimentally that scanning tunneling
spectroscopy (STS) images of semiconductor quantum dots may display clear
signatures of electron-electron correlation. We apply many-body tunneling
theory to a realistic model which fully takes into account correlation effects
and dot anisotropy. C... | cond-mat.mes-hall cond-mat.str-el | we show both theoretically and experimentally that scanning tunneling spectroscopy sts images of semiconductor quantum dots may display clear signatures of electronelectron correlation we apply manybody tunneling theory to a realistic model which fully takes into account correlation effects and dot anisotropy comparing... | [['we', 'show', 'both', 'theoretically', 'and', 'experimentally', 'that', 'scanning', 'tunneling', 'spectroscopy', 'sts', 'images', 'of', 'semiconductor', 'quantum', 'dots', 'may', 'display', 'clear', 'signatures', 'of', 'electronelectron', 'correlation', 'we', 'apply', 'manybody', 'tunneling', 'theory', 'to', 'a', 're... | [-0.11159343546395131, 0.11701672721748299, -0.08481568956321621, 0.10738149430587927, 0.05028942030696, -0.20859370424729237, 0.012153332636869968, 0.4400832841886168, -0.260396014361833, -0.3149822138360097, -0.08820685847944758, -0.3678223896236654, -0.1625534332099747, 0.19034735455940616, 0.05729593665873448, 0.06... |
708.0315 | Anisotropic thermo-elasticity in 2D -- Part II: Applications | In this note we present concrete applications of the general treatment of
anisotropic thermo-elasticity developed in Part I.
| math.AP math-ph math.MP | in this note we present concrete applications of the general treatment of anisotropic thermoelasticity developed in part i | [['in', 'this', 'note', 'we', 'present', 'concrete', 'applications', 'of', 'the', 'general', 'treatment', 'of', 'anisotropic', 'thermoelasticity', 'developed', 'in', 'part', 'i']] | [-0.08865298330783844, 0.022784335176563926, -0.03205791778034634, 0.011650273621651448, -0.07111953623178932, -0.07218254419664542, -0.06198565678722742, 0.3537618675165706, -0.2153659506390492, -0.2105364037884606, 0.09340775179831932, -0.19725881351364982, -0.22966955705649322, 0.13876466535859638, -0.13868151211904... |
708.0316 | Searching For Helical Magnetic Fields in Active Galactic Nuclei | Previously, a multi-wavelength (2cm, 4cm and 6cm) polarization study by
Gabuzda, Murray and Cronin (2004) showed systematic Faraday Rotation gradients
across the parsec-scale jets of several BL Lac objects, interpreted as evidence
for helical magnetic (B) fields - the gradients were taken to be due to the
systematic ... | astro-ph | previously a multiwavelength 2cm 4cm and 6cm polarization study by gabuzda murray and cronin 2004 showed systematic faraday rotation gradients across the parsecscale jets of several bl lac objects interpreted as evidence for helical magnetic b fields the gradients were taken to be due to the systematic variation of the... | [['previously', 'a', 'multiwavelength', '2cm', '4cm', 'and', '6cm', 'polarization', 'study', 'by', 'gabuzda', 'murray', 'and', 'cronin', '2004', 'showed', 'systematic', 'faraday', 'rotation', 'gradients', 'across', 'the', 'parsecscale', 'jets', 'of', 'several', 'bl', 'lac', 'objects', 'interpreted', 'as', 'evidence', '... | [-0.10429711733545576, 0.12481402919561203, -0.048758268899151254, 0.10042002566092248, -0.06660417240379111, -0.059134404794978244, -0.005514857115756188, 0.4906362216919661, -0.21155183716277992, -0.3470970070960798, 0.09233247445763222, -0.2525939577605043, -0.013266063053160906, 0.21471669812287603, -0.002212728896... |
708.0317 | Comment: Monitoring Networked Applications With Incremental Quantile
Estimation | Comment: Monitoring Networked Applications With Incremental Quantile
Estimation [arXiv:0708.0302]
| stat.ME | comment monitoring networked applications with incremental quantile estimation arxiv07080302 | [['comment', 'monitoring', 'networked', 'applications', 'with', 'incremental', 'quantile', 'estimation', 'arxiv07080302']] | [-0.14180646360748345, -0.061008553124136396, -0.022818914873318538, -0.04242407299009048, -0.18278559876812828, -0.3424644395709038, 0.05223862397381001, 0.4318316388461325, -0.15059460865126717, -0.2871013937724961, 0.3038245534731282, -0.24358591685692468, -0.23661380861368445, 0.16721839809583294, -0.32034927979111... |
708.0318 | Blind background prediction using a bifurcated analysis scheme | A technique for background prediction using data, but maintaining a closed
signal box is described. The result is extended to two background sources.
Conditions on the applicability under correlated cuts are described. This
technique is applied to both a toy model and an analysis of data from a rare
neutral kaon deca... | physics.data-an | a technique for background prediction using data but maintaining a closed signal box is described the result is extended to two background sources conditions on the applicability under correlated cuts are described this technique is applied to both a toy model and an analysis of data from a rare neutral kaon decay expe... | [['a', 'technique', 'for', 'background', 'prediction', 'using', 'data', 'but', 'maintaining', 'a', 'closed', 'signal', 'box', 'is', 'described', 'the', 'result', 'is', 'extended', 'to', 'two', 'background', 'sources', 'conditions', 'on', 'the', 'applicability', 'under', 'correlated', 'cuts', 'are', 'described', 'this',... | [-0.06136608085559927, 0.1034894551807808, -0.10067982107559044, 0.14057199687275262, -0.04004524282250061, -0.16058060966150942, 0.05168839473330047, 0.35584258267058516, -0.20067071557958732, -0.2946171402439194, 0.1130885415455713, -0.31317294427668146, -0.05701943686372548, 0.24359974243572718, -0.00440596156525162... |
708.0319 | Global asymptotic stability for a class of nonlinear chemical equations | We consider a class of nonlinear differential equations that arises in the
study of chemical reaction systems that are known to be locally asymptotically
stable and prove that they are in fact globally asymptotically stable. More
specifically, we will consider chemical reaction systems that are weakly
reversible, hav... | math.DS math.CA | we consider a class of nonlinear differential equations that arises in the study of chemical reaction systems that are known to be locally asymptotically stable and prove that they are in fact globally asymptotically stable more specifically we will consider chemical reaction systems that are weakly reversible have a d... | [['we', 'consider', 'a', 'class', 'of', 'nonlinear', 'differential', 'equations', 'that', 'arises', 'in', 'the', 'study', 'of', 'chemical', 'reaction', 'systems', 'that', 'are', 'known', 'to', 'be', 'locally', 'asymptotically', 'stable', 'and', 'prove', 'that', 'they', 'are', 'in', 'fact', 'globally', 'asymptotically',... | [-0.15624652102627834, 0.13246115062956146, -0.042539508937277704, 0.019947693843060908, -0.013648988686001567, -0.16638611245955995, -0.003634069898554972, 0.37247508897015186, -0.2929873338165526, -0.20039813451246538, 0.12169113123108313, -0.28475113171361277, -0.13703289794832912, 0.1745572450988641, -0.08854557826... |
708.032 | Analytic results on long distance entanglement mediated by gapped spin
chains | We give an analytical description of long distance entanglement (LDE)
mediated by one-dimensional quantum spin chains recently found in numerical
studies. We develop a formalism that allows the computation of LDE for weakly
interacting probes with gapped many-body systems. At zero temperature, a DC
response function ... | quant-ph | we give an analytical description of long distance entanglement lde mediated by onedimensional quantum spin chains recently found in numerical studies we develop a formalism that allows the computation of lde for weakly interacting probes with gapped manybody systems at zero temperature a dc response function determine... | [['we', 'give', 'an', 'analytical', 'description', 'of', 'long', 'distance', 'entanglement', 'lde', 'mediated', 'by', 'onedimensional', 'quantum', 'spin', 'chains', 'recently', 'found', 'in', 'numerical', 'studies', 'we', 'develop', 'a', 'formalism', 'that', 'allows', 'the', 'computation', 'of', 'lde', 'for', 'weakly',... | [-0.1872459179989631, 0.253033765335284, -0.07062788112748382, 0.07195238337699587, -0.02160858666211103, -0.21807620045522938, 0.027102360035837793, 0.35311636546280534, -0.24643586558265101, -0.23384914590268338, 0.015124345658783825, -0.32475095123798997, -0.09453210064655054, 0.20745228033768326, 0.0904844515934788... |
708.0321 | Brown-York Energy and Radial Geodesics | We compare the Brown-York (BY) and the standard Misner-Sharp (MS) quasilocal
energies for round spheres in spherically symmetric space-times from the point
of view of radial geodesics. In particular, we show that the relation between
the BY and MS energies is precisely analogous to that between the
(relativistic) ene... | gr-qc hep-th | we compare the brownyork by and the standard misnersharp ms quasilocal energies for round spheres in spherically symmetric spacetimes from the point of view of radial geodesics in particular we show that the relation between the by and ms energies is precisely analogous to that between the relativistic energy e of a ge... | [['we', 'compare', 'the', 'brownyork', 'by', 'and', 'the', 'standard', 'misnersharp', 'ms', 'quasilocal', 'energies', 'for', 'round', 'spheres', 'in', 'spherically', 'symmetric', 'spacetimes', 'from', 'the', 'point', 'of', 'view', 'of', 'radial', 'geodesics', 'in', 'particular', 'we', 'show', 'that', 'the', 'relation',... | [-0.14009975189067148, 0.12683232091022312, -0.12192632477661526, 0.1399638666495405, -0.05994566581729385, -0.08852906699326855, 0.03762176525261667, 0.3364447790025561, -0.21749104308309378, -0.3084815161233699, 0.010517573246249447, -0.3150261423378079, -0.13846680910533501, 0.17881617864800825, -0.03448959244587631... |
708.0322 | Harmonic Analysis over adelic spaces | Extending ideas of A.N. Parshin and D.V. Osipov, Harmonic Analysis is
developed for filtered infinite dimensional modules over a ring. We establish
Pontryagin duality, the Fourier inversion formula, Plancherel formula and
Poisson summation formula for all dimensions.
| math.NT math.AC | extending ideas of an parshin and dv osipov harmonic analysis is developed for filtered infinite dimensional modules over a ring we establish pontryagin duality the fourier inversion formula plancherel formula and poisson summation formula for all dimensions | [['extending', 'ideas', 'of', 'an', 'parshin', 'and', 'dv', 'osipov', 'harmonic', 'analysis', 'is', 'developed', 'for', 'filtered', 'infinite', 'dimensional', 'modules', 'over', 'a', 'ring', 'we', 'establish', 'pontryagin', 'duality', 'the', 'fourier', 'inversion', 'formula', 'plancherel', 'formula', 'and', 'poisson', ... | [-0.15753140876925475, 0.020041257058462204, -0.16650759051176342, 0.10238181107765618, -0.11937449944230753, -0.2058413273252144, -0.0035692944216567115, 0.28465440909604767, -0.29272742146575775, -0.14392750740454002, 0.11918083117091777, -0.19276277640381376, -0.180239552883683, 0.25577001857596476, -0.1040312403410... |
708.0323 | Multi-dimensional Numerical Scheme for Resistive Relativistic MHD | The paper describes a new upwind conservative numerical scheme for special
relativistic resistive magnetohydrodynamics with scalar resistivity. The
magnetic field is kept approximately divergence free and the divergence of the
electric field consistent with the electric charge distribution via the method
of Generaliz... | astro-ph | the paper describes a new upwind conservative numerical scheme for special relativistic resistive magnetohydrodynamics with scalar resistivity the magnetic field is kept approximately divergence free and the divergence of the electric field consistent with the electric charge distribution via the method of generalized ... | [['the', 'paper', 'describes', 'a', 'new', 'upwind', 'conservative', 'numerical', 'scheme', 'for', 'special', 'relativistic', 'resistive', 'magnetohydrodynamics', 'with', 'scalar', 'resistivity', 'the', 'magnetic', 'field', 'is', 'kept', 'approximately', 'divergence', 'free', 'and', 'the', 'divergence', 'of', 'the', 'e... | [-0.1497546203927585, 0.1539906369531, -0.058554487228217836, 0.10373695091814471, -0.06525576423923925, -0.14254892591984486, -0.04744799847534489, 0.32742037079384867, -0.25751822287181636, -0.3147677856163596, 0.06055491481565009, -0.2083024387753059, -0.0664475297693708, 0.28576911662547094, 0.024193611448490113, 0... |
708.0324 | Transverse Quark Spin Effects and the Flavor Dependence of the
Boer-Mulders Function | The naive time reversal odd (``T-odd'') parton distribution $h_{1}^{\perp}$,
the so-called Boer-Mulders function, for both up ($u$) and down ($d$) quarks is
considered in the diquark spectator model. While the results of different
articles in the literature suggest that the signs of the Boer-Mulders function
in semi-... | hep-ph | the naive time reversal odd todd parton distribution h_1perp the socalled boermulders function for both up u and down d quarks is considered in the diquark spectator model while the results of different articles in the literature suggest that the signs of the boermulders function in semiinclusive dis for both flavors u... | [['the', 'naive', 'time', 'reversal', 'odd', 'todd', 'parton', 'distribution', 'h_1perp', 'the', 'socalled', 'boermulders', 'function', 'for', 'both', 'up', 'u', 'and', 'down', 'd', 'quarks', 'is', 'considered', 'in', 'the', 'diquark', 'spectator', 'model', 'while', 'the', 'results', 'of', 'different', 'articles', 'in'... | [-0.07023508103364813, 0.19327259178140332, -0.13436975826487121, 0.1411344439151608, -0.03180216867033215, -0.06684074287990197, 0.03302139108002718, 0.3944596334050099, -0.20517217960829537, -0.22128941029576318, -0.06581399993294673, -0.32010346694878533, -0.04754605111222537, 0.12202234300784767, 0.0850698592274316... |
708.0325 | On the multi-spin magnon and spike solutions from membranes | Recently important classes of solitonic string solutions were obtained -
giant magnons and single spikes. In previous study we showed the existence of
giant magnon-like membrane solutions and studied their properties. In this
paper we investigate classical rotating membranes representing analog of a
specific class of... | hep-th | recently important classes of solitonic string solutions were obtained giant magnons and single spikes in previous study we showed the existence of giant magnonlike membrane solutions and studied their properties in this paper we investigate classical rotating membranes representing analog of a specific class of string... | [['recently', 'important', 'classes', 'of', 'solitonic', 'string', 'solutions', 'were', 'obtained', 'giant', 'magnons', 'and', 'single', 'spikes', 'in', 'previous', 'study', 'we', 'showed', 'the', 'existence', 'of', 'giant', 'magnonlike', 'membrane', 'solutions', 'and', 'studied', 'their', 'properties', 'in', 'this', '... | [-0.1819734172260558, 0.10286785776472905, -0.026001108561600136, 0.08229382419085596, -0.04951456877064298, -0.10893521657404066, 0.016535648799617775, 0.3062093659589829, -0.2087017544227737, -0.29245918782808905, 0.09598513476719911, -0.30049215377816424, -0.16685600635934283, 0.15897172461898829, -0.060755213055844... |
708.0326 | Holographic Nuclear Physics | We analyze the phases of the Sakai-Sugimoto model at finite temperature and
baryon chemical potential. Baryonic matter is represented either by 4-branes in
the 8-branes or by strings stretched from the 8-branes to the horizon. We find
the explicit configurations and use them to determine the phase diagram and
equatio... | hep-th hep-ph | we analyze the phases of the sakaisugimoto model at finite temperature and baryon chemical potential baryonic matter is represented either by 4branes in the 8branes or by strings stretched from the 8branes to the horizon we find the explicit configurations and use them to determine the phase diagram and equation of sta... | [['we', 'analyze', 'the', 'phases', 'of', 'the', 'sakaisugimoto', 'model', 'at', 'finite', 'temperature', 'and', 'baryon', 'chemical', 'potential', 'baryonic', 'matter', 'is', 'represented', 'either', 'by', '4branes', 'in', 'the', '8branes', 'or', 'by', 'strings', 'stretched', 'from', 'the', '8branes', 'to', 'the', 'ho... | [-0.12940090058670778, 0.25948381827994516, -0.1306573384391543, 0.06948835857994189, -0.022375805800714132, -0.07838601789636804, 0.0637137152154797, 0.32307947924626723, -0.2009606106872005, -0.27627902030944823, 0.06351720572731989, -0.30013878018528756, -0.037774717436903825, 0.045868891539118654, 0.055520636844448... |
708.0327 | Transition probabilities in the U(6) limit of the Symplectic Interacting
Vector Boson Model | The tensor properties of the algebra generators and the basis are determined
in respect to the reduction chain $Sp(12,R) \supset U(6)% \supset U(3)\otimes
U(2)\supset O(3)\otimes (U(1)\otimes U(1))$, which defines one of the dynamical
symmetries of the Interacting Vector Boson Model. The action of the Sp(12,R)
genera... | nucl-th | the tensor properties of the algebra generators and the basis are determined in respect to the reduction chain sp12r supset u6 supset u3otimes u2supset o3otimes u1otimes u1 which defines one of the dynamical symmetries of the interacting vector boson model the action of the sp12r generators as transition operators betw... | [['the', 'tensor', 'properties', 'of', 'the', 'algebra', 'generators', 'and', 'the', 'basis', 'are', 'determined', 'in', 'respect', 'to', 'the', 'reduction', 'chain', 'sp12r', 'supset', 'u6', 'supset', 'u3otimes', 'u2supset', 'o3otimes', 'u1otimes', 'u1', 'which', 'defines', 'one', 'of', 'the', 'dynamical', 'symmetries... | [-0.13379899381473662, 0.17263316221546848, -0.015980438992381097, 0.06320016643125564, -0.0019929459895938633, -0.07068936716485769, 0.029232118345797063, 0.34562696221470834, -0.23409950098395346, -0.22590483719902113, 0.07143821417633445, -0.3165305666029453, -0.1265486622788012, 0.12731331061199308, 0.0515658702624... |
708.0328 | Adaptive thresholds for neural networks with synaptic noise | The inclusion of a macroscopic adaptive threshold is studied for the
retrieval dynamics of both layered feedforward and fully connected neural
network models with synaptic noise. These two types of architectures require a
different method to be solved numerically. In both cases it is shown that, if
the threshold is c... | cond-mat.dis-nn cond-mat.stat-mech | the inclusion of a macroscopic adaptive threshold is studied for the retrieval dynamics of both layered feedforward and fully connected neural network models with synaptic noise these two types of architectures require a different method to be solved numerically in both cases it is shown that if the threshold is chosen... | [['the', 'inclusion', 'of', 'a', 'macroscopic', 'adaptive', 'threshold', 'is', 'studied', 'for', 'the', 'retrieval', 'dynamics', 'of', 'both', 'layered', 'feedforward', 'and', 'fully', 'connected', 'neural', 'network', 'models', 'with', 'synaptic', 'noise', 'these', 'two', 'types', 'of', 'architectures', 'require', 'a'... | [-0.14013334310126352, 0.0972395928511105, -0.05263308386094178, 0.058892538268267985, -0.016012489366672794, -0.14747742986461768, 0.05554268298739636, 0.3818309186802556, -0.3142207676794863, -0.29491447643549357, 0.09316548191256718, -0.2360694803883908, -0.20930481057277778, 0.1597916950876997, -0.08710755212706756... |
708.0329 | The Central Limit Theorem for the Smoluchovski Coagulation Model | The general model of coagulation is considered.
For basic classes of unbounded coagulation kernels the central limit theorem
(CLT) is obtained for the fluctuations around the dynamic law of large numbers
(LLN). A rather precise rate of convergence is given both for LLN and CLT.
| math.PR math-ph math.MP | the general model of coagulation is considered for basic classes of unbounded coagulation kernels the central limit theorem clt is obtained for the fluctuations around the dynamic law of large numbers lln a rather precise rate of convergence is given both for lln and clt | [['the', 'general', 'model', 'of', 'coagulation', 'is', 'considered', 'for', 'basic', 'classes', 'of', 'unbounded', 'coagulation', 'kernels', 'the', 'central', 'limit', 'theorem', 'clt', 'is', 'obtained', 'for', 'the', 'fluctuations', 'around', 'the', 'dynamic', 'law', 'of', 'large', 'numbers', 'lln', 'a', 'rather', 'p... | [-0.1418977822487553, 0.09015390741535359, -0.09194791888197264, 0.15866368060879824, 0.02544644537071387, -0.1264004867006507, 0.044532597147756155, 0.236048364556498, -0.26221331294832956, -0.22950807561477024, 0.14437148357845014, -0.23228463244934877, -0.013445082927743594, 0.23472403072131176, -0.09199082829679052... |
708.033 | Sub-Shot-Noise Magnetometry with a Correlated Spin-Relaxation Dominated
Alkali-Metal Vapor | Spin noise sets fundamental limits to the precision of measurements using
spin-polarized atomic vapors, such as performed with sensitive atomic
magnetometers. Spin squeezing offers the possibility to extend the measurement
precision beyond the standard quantum limit of uncorrelated atoms. Contrary to
the current unde... | physics.atom-ph | spin noise sets fundamental limits to the precision of measurements using spinpolarized atomic vapors such as performed with sensitive atomic magnetometers spin squeezing offers the possibility to extend the measurement precision beyond the standard quantum limit of uncorrelated atoms contrary to the current understand... | [['spin', 'noise', 'sets', 'fundamental', 'limits', 'to', 'the', 'precision', 'of', 'measurements', 'using', 'spinpolarized', 'atomic', 'vapors', 'such', 'as', 'performed', 'with', 'sensitive', 'atomic', 'magnetometers', 'spin', 'squeezing', 'offers', 'the', 'possibility', 'to', 'extend', 'the', 'measurement', 'precisi... | [-0.11245695276087836, 0.2474003018972182, -0.010865320914768075, 0.026790833473205565, 0.01789316393827137, -0.12319228928536177, 0.0669211925914217, 0.33968502698760283, -0.2779566260054708, -0.2712121642684858, 0.05123272348734501, -0.2800898820897074, -0.030910928312100863, 0.22812248984057654, -0.00358025615936831... |
708.0331 | Notes on the geometry of space of polynomials | We show that the symmetric injective tensor product space
$\hat{\otimes}_{n,s,\epsilon}E$ is not complex strictly convex if E is a
complex Banach space of $\dim E \ge 2$ and if $n\ge 2$ holds. It is also
reproved that $\ell_\infty$ is finitely represented in
$\hat{\otimes}_{n,s,\epsilon}E$ if E is infinite dimensiona... | math.FA | we show that the symmetric injective tensor product space hatotimes_nsepsilone is not complex strictly convex if e is a complex banach space of dim e ge 2 and if nge 2 holds it is also reproved that ell_infty is finitely represented in hatotimes_nsepsilone if e is infinite dimensional and if nge 2 holds which was prove... | [['we', 'show', 'that', 'the', 'symmetric', 'injective', 'tensor', 'product', 'space', 'hatotimes_nsepsilone', 'is', 'not', 'complex', 'strictly', 'convex', 'if', 'e', 'is', 'a', 'complex', 'banach', 'space', 'of', 'dim', 'e', 'ge', '2', 'and', 'if', 'nge', '2', 'holds', 'it', 'is', 'also', 'reproved', 'that', 'ell_inf... | [-0.12184964226148391, 0.2001441489684127, -0.03312265847699117, 0.06635833426055072, -0.048379143857854905, -0.22466600974390316, -0.12145709625240099, 0.4273389943449174, -0.312306051663423, -0.14259605267542905, 0.1081310252982618, -0.28615951098371456, -0.18783537089682611, 0.18956496782790302, -0.1080976626046507,... |
708.0332 | Coherent Dark Resonances in Atomic Barium | The observation of dark-resonances in the two-electron atom barium and their
influence on optical cooling is reported. In heavy alkali earth atoms, i.e.
barium or radium, optical cooling can be achieved using n^1S_0-n^1P_1
transitions and optical repumping from the low lying n^1D_2 and n^3D_{1,2}
states to which the ... | physics.atom-ph | the observation of darkresonances in the twoelectron atom barium and their influence on optical cooling is reported in heavy alkali earth atoms ie barium or radium optical cooling can be achieved using n1s_0n1p_1 transitions and optical repumping from the low lying n1d_2 and n3d_12 states to which the atoms decay with ... | [['the', 'observation', 'of', 'darkresonances', 'in', 'the', 'twoelectron', 'atom', 'barium', 'and', 'their', 'influence', 'on', 'optical', 'cooling', 'is', 'reported', 'in', 'heavy', 'alkali', 'earth', 'atoms', 'ie', 'barium', 'or', 'radium', 'optical', 'cooling', 'can', 'be', 'achieved', 'using', 'n1s_0n1p_1', 'trans... | [-0.03305993894601295, 0.25942692308750587, -0.029963132735871364, 0.0033347498004635177, -0.03622363234057511, -0.17901730618677011, 0.1382703537215004, 0.4236754451732279, -0.20365222252211443, -0.31249469759709697, 0.04507613092131328, -0.2881692931189843, 0.015887816212888733, 0.19219302030636326, 0.036404842041734... |
708.0333 | Polaris B, an optical companion of Polaris (alpha UMi) system:
atmospheric parameters, chemical composition, distance and mass | We present an analysis of high-resolution spectroscopic observations of
Polaris B, the optical companion of the Polaris Ab system. The star has a
radial velocity V_r of -16.6km/s to -18.9km/s, and a projected rotational
velocity vsini=110 km/s. The derived atmospheric parameters are: Teff=6900K;
logg=4.3; V_t=2.5km/s... | astro-ph | we present an analysis of highresolution spectroscopic observations of polaris b the optical companion of the polaris ab system the star has a radial velocity v_r of 166kms to 189kms and a projected rotational velocity vsini110 kms the derived atmospheric parameters are teff6900k logg43 v_t25kms polaris b has elemental... | [['we', 'present', 'an', 'analysis', 'of', 'highresolution', 'spectroscopic', 'observations', 'of', 'polaris', 'b', 'the', 'optical', 'companion', 'of', 'the', 'polaris', 'ab', 'system', 'the', 'star', 'has', 'a', 'radial', 'velocity', 'v_r', 'of', '166kms', 'to', '189kms', 'and', 'a', 'projected', 'rotational', 'veloc... | [-0.09108606340330944, 0.10470490783617399, -0.08324306393287291, -0.012598233325039282, -0.0939856975568099, -0.06641559376740795, 0.0817773741845597, 0.3919205783229125, -0.18300773221345848, -0.35986509262339067, 0.029638175513562664, -0.25100041332929357, -0.0318521497640432, 0.2033515328606754, -0.0967677402261056... |
708.0334 | The Structure of Integrable One-Dimensional Systems | We explain the relationship between the classical description of an
integrable system in terms of invariant tori and action-angle variables, and
the quantum description in terms of the asymptotic Bethe ansatz.
| cond-mat.other cond-mat.stat-mech | we explain the relationship between the classical description of an integrable system in terms of invariant tori and actionangle variables and the quantum description in terms of the asymptotic bethe ansatz | [['we', 'explain', 'the', 'relationship', 'between', 'the', 'classical', 'description', 'of', 'an', 'integrable', 'system', 'in', 'terms', 'of', 'invariant', 'tori', 'and', 'actionangle', 'variables', 'and', 'the', 'quantum', 'description', 'in', 'terms', 'of', 'the', 'asymptotic', 'bethe', 'ansatz']] | [-0.19782075985905626, 0.05346106748038437, -0.13630002746058087, 0.1413141094869183, 0.004677802144039062, -0.06504682766934557, 0.0033459792199033883, 0.24201639633505576, -0.2576138721778989, -0.2720437749258934, 0.02734395614900296, -0.2537501266887111, -0.2118775428783509, 0.1586210356364327, -0.06263451428423004,... |
708.0335 | Eccentricity evolution of giant planet orbits due to circumstellar disk
torques | The extrasolar planets discovered to date possess unexpected orbital
elements. Most orbit their host stars with larger eccentricities and smaller
semi-major axes than similarly sized planets in our own solar system do. It is
generally agreed that the interaction between giant planets and circumstellar
disks (Type II ... | astro-ph | the extrasolar planets discovered to date possess unexpected orbital elements most orbit their host stars with larger eccentricities and smaller semimajor axes than similarly sized planets in our own solar system do it is generally agreed that the interaction between giant planets and circumstellar disks type ii migrat... | [['the', 'extrasolar', 'planets', 'discovered', 'to', 'date', 'possess', 'unexpected', 'orbital', 'elements', 'most', 'orbit', 'their', 'host', 'stars', 'with', 'larger', 'eccentricities', 'and', 'smaller', 'semimajor', 'axes', 'than', 'similarly', 'sized', 'planets', 'in', 'our', 'own', 'solar', 'system', 'do', 'it', ... | [-0.18901928625223263, 0.1735955367967108, -0.06507571967927106, 0.06441284708171224, -0.13412658112883946, -0.062266075972729595, 0.03356959563870987, 0.4011813982797321, -0.19868546027373668, -0.31717889664105314, 0.05375860529511556, -0.2431049192455248, -0.07781781870562554, 0.2373962952410693, -0.05450930638755835... |
708.0336 | Comment: Monitoring Networked Applications With Incremental Quantile
Estimation | Our comments are in two parts. First, we make some observations regarding the
methodology in Chambers et al. [arXiv:0708.0302]. Second, we briefly describe
another interesting network monitoring problem that arises in the context of
assessing quality of service, such as loss rates and delay distributions, in
packet-s... | stat.ME | our comments are in two parts first we make some observations regarding the methodology in chambers et al arxiv07080302 second we briefly describe another interesting network monitoring problem that arises in the context of assessing quality of service such as loss rates and delay distributions in packetswitched networ... | [['our', 'comments', 'are', 'in', 'two', 'parts', 'first', 'we', 'make', 'some', 'observations', 'regarding', 'the', 'methodology', 'in', 'chambers', 'et', 'al', 'arxiv07080302', 'second', 'we', 'briefly', 'describe', 'another', 'interesting', 'network', 'monitoring', 'problem', 'that', 'arises', 'in', 'the', 'context'... | [-0.14519100892357528, 0.01431051839608699, -0.004411909457606574, 0.06679790994773309, -0.06915099730637546, -0.10800361982546747, 0.04977688184590079, 0.4393902542651631, -0.23699887110463655, -0.32747264408196014, 0.12458827414957341, -0.28255715463698533, -0.21250008752879998, 0.20260676566977054, -0.17506613897664... |
708.0337 | Revisiting the valence-band and core-level photoemission spectra of NiO | We have re-examined the valence-band (VB) and core-level electronic structure
of NiO by means of hard and soft x-ray photoemission spectroscopy (PES). The
spectral weight of the lowest energy state found to be enhanced in the bulk
sensitive Ni 2p core-level PES. A configuration-interaction model including the
bound s... | cond-mat.str-el | we have reexamined the valenceband vb and corelevel electronic structure of nio by means of hard and soft xray photoemission spectroscopy pes the spectral weight of the lowest energy state found to be enhanced in the bulk sensitive ni 2p corelevel pes a configurationinteraction model including the bound state screening... | [['we', 'have', 'reexamined', 'the', 'valenceband', 'vb', 'and', 'corelevel', 'electronic', 'structure', 'of', 'nio', 'by', 'means', 'of', 'hard', 'and', 'soft', 'xray', 'photoemission', 'spectroscopy', 'pes', 'the', 'spectral', 'weight', 'of', 'the', 'lowest', 'energy', 'state', 'found', 'to', 'be', 'enhanced', 'in', ... | [-0.02357935934233698, 0.10888059643258778, -0.07143612703954687, 0.11563723020692718, 0.041695936649505584, -0.15599543854656003, 0.12992307976273135, 0.4339826227526884, -0.24392081975784838, -0.35488773132579365, -0.08042602898429471, -0.3953525508963028, -0.10375205969571002, 0.08177116971786078, 0.1211237537446526... |
708.0338 | Comment: Monitoring Networked Applications With Incremental Quantile
Estimation | Comment: Monitoring Networked Applications With Incremental Quantile
Estimation [arXiv:0708.0302]
| stat.ME | comment monitoring networked applications with incremental quantile estimation arxiv07080302 | [['comment', 'monitoring', 'networked', 'applications', 'with', 'incremental', 'quantile', 'estimation', 'arxiv07080302']] | [-0.14180646360748345, -0.061008553124136396, -0.022818914873318538, -0.04242407299009048, -0.18278559876812828, -0.3424644395709038, 0.05223862397381001, 0.4318316388461325, -0.15059460865126717, -0.2871013937724961, 0.3038245534731282, -0.24358591685692468, -0.23661380861368445, 0.16721839809583294, -0.32034927979111... |
708.0339 | Rejoinder: Monitoring Networked Applications With Incremental Quantile
Estimation | Rejoinder: Monitoring Networked Applications With Incremental Quantile
Estimation [arXiv:0708.0302]
| stat.ME | rejoinder monitoring networked applications with incremental quantile estimation arxiv07080302 | [['rejoinder', 'monitoring', 'networked', 'applications', 'with', 'incremental', 'quantile', 'estimation', 'arxiv07080302']] | [-0.0536881091280116, -0.1212330133550697, -0.051516089795364275, -0.029779527090593345, -0.1569837679465612, -0.31315024114317364, 0.033965243906196624, 0.4493624187178082, -0.17849248150984445, -0.30614033258623546, 0.2851453361411889, -0.2873593692978223, -0.2302411945743693, 0.1427004678795735, -0.3540352007581128,... |
708.034 | Coarse Grained Density Functional Theories for Metallic Alloys:
Generalized Coherent Potential Approximations and Charge Excess Functional
Theory | The class of the Generalized Coherent Potential Approximations (GCPA) to the
Density Functional Theory (DFT) is introduced within the Multiple Scattering
Theory formalism for dealing with, ordered or disordered, metallic alloys. All
GCPA theories are based on a common ansatz for the kinetic part of the
Hohenberg-Kohn... | cond-mat.mtrl-sci cond-mat.dis-nn | the class of the generalized coherent potential approximations gcpa to the density functional theory dft is introduced within the multiple scattering theory formalism for dealing with ordered or disordered metallic alloys all gcpa theories are based on a common ansatz for the kinetic part of the hohenbergkohn functiona... | [['the', 'class', 'of', 'the', 'generalized', 'coherent', 'potential', 'approximations', 'gcpa', 'to', 'the', 'density', 'functional', 'theory', 'dft', 'is', 'introduced', 'within', 'the', 'multiple', 'scattering', 'theory', 'formalism', 'for', 'dealing', 'with', 'ordered', 'or', 'disordered', 'metallic', 'alloys', 'al... | [-0.10629837335185302, 0.09556035327213272, -0.06277324962691744, 0.05692616683891476, -0.02165106079039401, -0.07479576509324765, 0.05345288661568051, 0.3400322299594974, -0.20701594401676743, -0.3140553012009146, -0.0007317965825318575, -0.291203334074473, -0.1353604920874352, 0.13478246388606369, 0.00086849638367436... |
708.0341 | Time-dependent density functional theory calculation of van der Waals
coefficient of sodium clusters | In this paper we employ all-electron \textit{ab-initio} time-dependent
density functional theory based method to calculate the long range
dipole-dipole dispersion coefficient (van der Waals coefficient) $C_{6}$ of
sodium atom clusters containing even number of atoms ranging from 2 to 20
atoms. The dispersion coeffici... | physics.atm-clus physics.chem-ph | in this paper we employ allelectron textitabinitio timedependent density functional theory based method to calculate the long range dipoledipole dispersion coefficient van der waals coefficient c_6 of sodium atom clusters containing even number of atoms ranging from 2 to 20 atoms the dispersion coefficients are obtaine... | [['in', 'this', 'paper', 'we', 'employ', 'allelectron', 'textitabinitio', 'timedependent', 'density', 'functional', 'theory', 'based', 'method', 'to', 'calculate', 'the', 'long', 'range', 'dipoledipole', 'dispersion', 'coefficient', 'van', 'der', 'waals', 'coefficient', 'c_6', 'of', 'sodium', 'atom', 'clusters', 'conta... | [-0.09940644684299994, 0.07831888208021881, -0.06785307762250985, 0.03460276105605966, 0.006600306969753393, -0.1375087525857759, 0.051315927140289146, 0.39608440195273065, -0.20213662541544672, -0.32073477584491955, -0.050636113480680485, -0.37507361474478346, -0.1542855747975409, 0.18244434860561126, 0.09049143861806... |
708.0342 | Transcription and noise in negative feedback loops | Recently, several studies have investigated the transcription process
associated to specific genetic regulatory networks. In this work, we present a
stochastic approach for analyzing the dynamics and effect of negative feedback
loops (FBL) on the transcriptional noise. First, our analysis allows us to
identify a bimo... | q-bio.MN | recently several studies have investigated the transcription process associated to specific genetic regulatory networks in this work we present a stochastic approach for analyzing the dynamics and effect of negative feedback loops fbl on the transcriptional noise first our analysis allows us to identify a bimodal activ... | [['recently', 'several', 'studies', 'have', 'investigated', 'the', 'transcription', 'process', 'associated', 'to', 'specific', 'genetic', 'regulatory', 'networks', 'in', 'this', 'work', 'we', 'present', 'a', 'stochastic', 'approach', 'for', 'analyzing', 'the', 'dynamics', 'and', 'effect', 'of', 'negative', 'feedback', ... | [-0.15206108794423967, 0.11915642095435053, -0.02334004882091688, 0.08737972859491729, -0.04154811450740649, -0.12445296321095804, 0.06918694565169997, 0.3634395190951346, -0.2423496094879584, -0.2979098374002987, 0.03501399133504384, -0.2390145491612161, -0.20023376267340223, 0.18465401683171084, -0.029203827569680815... |
708.0343 | Dynamic Modeling and Statistical Analysis of Event Times | This review article provides an overview of recent work in the modeling and
analysis of recurrent events arising in engineering, reliability, public
health, biomedicine and other areas. Recurrent event modeling possesses unique
facets making it different and more difficult to handle than single event
settings. For in... | stat.ME | this review article provides an overview of recent work in the modeling and analysis of recurrent events arising in engineering reliability public health biomedicine and other areas recurrent event modeling possesses unique facets making it different and more difficult to handle than single event settings for instance ... | [['this', 'review', 'article', 'provides', 'an', 'overview', 'of', 'recent', 'work', 'in', 'the', 'modeling', 'and', 'analysis', 'of', 'recurrent', 'events', 'arising', 'in', 'engineering', 'reliability', 'public', 'health', 'biomedicine', 'and', 'other', 'areas', 'recurrent', 'event', 'modeling', 'possesses', 'unique'... | [-0.08526844632275321, 0.06458052106904359, -0.041431705097910825, 0.11859774996739124, -0.09630762958440228, -0.14950638955485993, 0.021960742343082162, 0.39615267639358837, -0.2593272792182161, -0.3243211258870914, 0.13093771695107073, -0.28945842333326954, -0.14325242223676996, 0.24060313256484442, -0.09912080609448... |
708.0344 | Anomalous temperature evolution of the internal magnetic field
distribution in the charge-ordered triangular antiferromagnet AgNiO2 | Zero-field muon-spin relaxation measurements of the frustrated triangular
quantum magnet AgNiO2 are consistent with a model of charge disproportionation
that has been advanced to explain the structural and magnetic properties of
this compound. Below an ordering temperature of T_N=19.9(2) K we observe six
distinct muo... | cond-mat.str-el | zerofield muonspin relaxation measurements of the frustrated triangular quantum magnet agnio2 are consistent with a model of charge disproportionation that has been advanced to explain the structural and magnetic properties of this compound below an ordering temperature of t_n1992 k we observe six distinct muon precess... | [['zerofield', 'muonspin', 'relaxation', 'measurements', 'of', 'the', 'frustrated', 'triangular', 'quantum', 'magnet', 'agnio2', 'are', 'consistent', 'with', 'a', 'model', 'of', 'charge', 'disproportionation', 'that', 'has', 'been', 'advanced', 'to', 'explain', 'the', 'structural', 'and', 'magnetic', 'properties', 'of'... | [-0.19549890443505274, 0.2614340734632736, -0.01746443079762338, 0.0400761370879731, -0.07507250897054162, -0.13039562681556813, 0.016064225529719676, 0.38314506431509343, -0.25904701426181764, -0.30448175920173526, 0.022971016803889403, -0.3032432066808854, -0.04852754161471412, 0.18189252719527021, 0.0865036750522752... |
708.0345 | Quasi-classical rate coefficient calculations for the rotational
(de)excitation of H2O by H2 | The interpretation of water line emission from existing observations and
future HIFI/Herschel data requires a detailed knowledge of collisional rate
coefficients. Among all relevant collisional mechanisms, the rotational
(de)excitation of H2O by H2 molecules is the process of most interest in
interstellar space. To d... | astro-ph | the interpretation of water line emission from existing observations and future hifiherschel data requires a detailed knowledge of collisional rate coefficients among all relevant collisional mechanisms the rotational deexcitation of h2o by h2 molecules is the process of most interest in interstellar space to determine... | [['the', 'interpretation', 'of', 'water', 'line', 'emission', 'from', 'existing', 'observations', 'and', 'future', 'hifiherschel', 'data', 'requires', 'a', 'detailed', 'knowledge', 'of', 'collisional', 'rate', 'coefficients', 'among', 'all', 'relevant', 'collisional', 'mechanisms', 'the', 'rotational', 'deexcitation', ... | [-0.08364475091479512, 0.14842740526526338, -0.007881151111279096, 0.054557808377740005, 0.00042359283219815954, -0.09931394022165073, 0.04383287078364649, 0.4200979201744, -0.18450179908379344, -0.31556938692358216, 0.046875158889452, -0.26282569204664064, -0.0023037468710552073, 0.20023734969759566, 0.039347767298911... |
708.0346 | Threshold Regression for Survival Analysis: Modeling Event Times by a
Stochastic Process Reaching a Boundary | Many researchers have investigated first hitting times as models for survival
data. First hitting times arise naturally in many types of stochastic
processes, ranging from Wiener processes to Markov chains. In a survival
context, the state of the underlying process represents the strength of an item
or the health of ... | stat.ME | many researchers have investigated first hitting times as models for survival data first hitting times arise naturally in many types of stochastic processes ranging from wiener processes to markov chains in a survival context the state of the underlying process represents the strength of an item or the health of an ind... | [['many', 'researchers', 'have', 'investigated', 'first', 'hitting', 'times', 'as', 'models', 'for', 'survival', 'data', 'first', 'hitting', 'times', 'arise', 'naturally', 'in', 'many', 'types', 'of', 'stochastic', 'processes', 'ranging', 'from', 'wiener', 'processes', 'to', 'markov', 'chains', 'in', 'a', 'survival', '... | [-0.07147437395901149, 0.14265373475296036, -0.06126851468934869, 0.08646987281280036, -0.08130235956810045, -0.12497530523885755, 0.07538150595451527, 0.3840606045357698, -0.31256939927182087, -0.2687512094036062, 0.16475867349531623, -0.282795592587679, -0.10793698242872107, 0.1758822918611955, -0.07347077806893049, ... |
708.0347 | Predictability of band-limited, high-frequency, and mixed processes in
the presence of ideal low-pass filters | Pathwise predictability of continuous time processes is studied in
deterministic setting. We discuss uniform prediction in some weak sense with
respect to certain classes of inputs. More precisely, we study possibility of
approximation of convolution integrals over future time by integrals over past
time. We found th... | math.OC | pathwise predictability of continuous time processes is studied in deterministic setting we discuss uniform prediction in some weak sense with respect to certain classes of inputs more precisely we study possibility of approximation of convolution integrals over future time by integrals over past time we found that all... | [['pathwise', 'predictability', 'of', 'continuous', 'time', 'processes', 'is', 'studied', 'in', 'deterministic', 'setting', 'we', 'discuss', 'uniform', 'prediction', 'in', 'some', 'weak', 'sense', 'with', 'respect', 'to', 'certain', 'classes', 'of', 'inputs', 'more', 'precisely', 'we', 'study', 'possibility', 'of', 'ap... | [-0.11402916217131819, 0.14417784191797162, -0.0678160375856591, 0.10230264351349465, -0.047879538560371804, -0.11021833656484196, 0.057606374823499, 0.45420719905831347, -0.34521489931891364, -0.20813090940362014, 0.12672548923753843, -0.20885416314048671, -0.16018198602886377, 0.23641094459413453, -0.0890250167255450... |
708.0348 | An application of Kapteyn series to a problem from queueing theory | We obtain exact solutions of a problem arising from queueing theory using
properties of Kapteyn series.
| math.CA | we obtain exact solutions of a problem arising from queueing theory using properties of kapteyn series | [['we', 'obtain', 'exact', 'solutions', 'of', 'a', 'problem', 'arising', 'from', 'queueing', 'theory', 'using', 'properties', 'of', 'kapteyn', 'series']] | [-0.12595567127573304, -0.06924769777106121, -0.15997655477258377, 0.0659208347206004, -0.05086172791197896, -0.07230093461112119, 0.1087673228685162, 0.2554282940691337, -0.32687707187142223, -0.27968535176478326, 0.1564537875528913, -0.33088614232838154, -0.2040920564904809, 0.23135501402430236, -0.06612266012234613,... |
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