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710.3153 | Electronic correlation in nanoscale junctions: Comparison of the GW
approximation to a numerically exact solution of the single-impurity Anderson
model | The impact of electronic correlation in nanoscale junctions, e.g. formed by
single molecules, is analyzed using the single-impurity Anderson model.
Numerically exact Quantum Monte Carlo calculations are performed to map out the
orbital filling, linear response conductance and spectral function as a
function of the Co... | cond-mat.mtrl-sci cond-mat.str-el | the impact of electronic correlation in nanoscale junctions eg formed by single molecules is analyzed using the singleimpurity anderson model numerically exact quantum monte carlo calculations are performed to map out the orbital filling linear response conductance and spectral function as a function of the coulomb int... | [['the', 'impact', 'of', 'electronic', 'correlation', 'in', 'nanoscale', 'junctions', 'eg', 'formed', 'by', 'single', 'molecules', 'is', 'analyzed', 'using', 'the', 'singleimpurity', 'anderson', 'model', 'numerically', 'exact', 'quantum', 'monte', 'carlo', 'calculations', 'are', 'performed', 'to', 'map', 'out', 'the', ... | [-0.10431087081988585, 0.09997170644341427, -0.0705335527988306, 0.13163382430987744, -0.00669888983524981, -0.17165392098970533, 0.05423877548864333, 0.39433675527661327, -0.24550862276616195, -0.2996982691221915, 0.03296550994578172, -0.30309669490504476, -0.1257961928855539, 0.17719218297445746, 0.07274829497328028,... |
710.3154 | Intersubband decay of 1-D exciton resonances in carbon nanotubes | We have studied intersubband decay of E22 excitons in semiconducting carbon
nanotubes experimentally and theoretically. Photoluminescence excitation line
widths of semiconducting nanotubes with chiral indicess (n, m) can be mapped
onto a connectivity grid with curves of constant (n-m) and (2n+m). Moreover,
the global... | cond-mat.mtrl-sci | we have studied intersubband decay of e22 excitons in semiconducting carbon nanotubes experimentally and theoretically photoluminescence excitation line widths of semiconducting nanotubes with chiral indicess n m can be mapped onto a connectivity grid with curves of constant nm and 2nm moreover the global behavior of e... | [['we', 'have', 'studied', 'intersubband', 'decay', 'of', 'e22', 'excitons', 'in', 'semiconducting', 'carbon', 'nanotubes', 'experimentally', 'and', 'theoretically', 'photoluminescence', 'excitation', 'line', 'widths', 'of', 'semiconducting', 'nanotubes', 'with', 'chiral', 'indicess', 'n', 'm', 'can', 'be', 'mapped', '... | [-0.13610119797728246, 0.21428226400063727, 0.0032359454121473614, -0.006299861292643225, 0.018565752946841735, -0.1874661431853882, 0.10152786156879656, 0.4857255941734905, -0.20844274957095626, -0.2797302250478384, -0.026612326928282536, -0.3102908895342751, -0.043996979233157714, 0.1430393408193764, 0.06564847752863... |
710.3155 | Dynamics of Localized Waves | We have measured pulsed microwave transmission through quasi-1D samples with
lengths up to three localization lengths. For times approaching four times the
diffusion time \tau_D, transmission is diffusive in accord with the
self-consistent theory of localization for the renormalized diffusion
coefficient in space and... | cond-mat.dis-nn cond-mat.mes-hall | we have measured pulsed microwave transmission through quasi1d samples with lengths up to three localization lengths for times approaching four times the diffusion time tau_d transmission is diffusive in accord with the selfconsistent theory of localization for the renormalized diffusion coefficient in space and freque... | [['we', 'have', 'measured', 'pulsed', 'microwave', 'transmission', 'through', 'quasi1d', 'samples', 'with', 'lengths', 'up', 'to', 'three', 'localization', 'lengths', 'for', 'times', 'approaching', 'four', 'times', 'the', 'diffusion', 'time', 'tau_d', 'transmission', 'is', 'diffusive', 'in', 'accord', 'with', 'the', 's... | [-0.14066385850310326, 0.2122282701845203, -0.0315631201180319, 0.020167988803829456, 0.04787862592881235, -0.16464338559793154, 0.04256223446524624, 0.3659172006106625, -0.25489110344400007, -0.23144912046457952, 0.06873209978463517, -0.3136459217542627, -0.03529736411049574, 0.23330073700587187, 0.0857281210871103, 0... |
710.3156 | CP-violation in $b \to s$ Penguin Decays at BaBar | We present the new and updated $BABAR$ measurements of CP-violation studies
for many $b\to s $ penguin decay modes. We report the first observation of
mixing-induced CP-violation in $B^0 \to \eta ^{'} K^0$ with a significance
(including systematic uncertainties) of 5.5$\sigma$. We also present the first
observation o... | hep-ex | we present the new and updated babar measurements of cpviolation studies for many bto s penguin decay modes we report the first observation of mixinginduced cpviolation in b0 to eta k0 with a significance including systematic uncertainties of 55sigma we also present the first observation of the decay b0 to rho 0 k0 usi... | [['we', 'present', 'the', 'new', 'and', 'updated', 'babar', 'measurements', 'of', 'cpviolation', 'studies', 'for', 'many', 'bto', 's', 'penguin', 'decay', 'modes', 'we', 'report', 'the', 'first', 'observation', 'of', 'mixinginduced', 'cpviolation', 'in', 'b0', 'to', 'eta', 'k0', 'with', 'a', 'significance', 'including'... | [-0.12490412976210381, 0.21716879562728048, -0.09499826435530126, 0.059682217920014005, -0.07113811500148465, -0.18063973966332164, 0.1293198472437825, 0.25305336929968747, -0.19508393354935955, -0.20366114865223697, -0.04898196852547024, -0.4722428544368965, 0.06183116093419788, 0.13585861482802433, 0.1385067298650643... |
710.3157 | Exponent Inequalities in Dynamical Systems | In this letter we derive exponent inequalities relating the dynamic exponent
$z$ to the steady state exponent $\Gamma$ for a general class of stochastically
driven dynamical systems. We begin by deriving a general exact inequality,
relating the response function and the correlation function, from which the
various ex... | cond-mat.stat-mech cond-mat.dis-nn cond-mat.mtrl-sci cond-mat.soft nlin.CD | in this letter we derive exponent inequalities relating the dynamic exponent z to the steady state exponent gamma for a general class of stochastically driven dynamical systems we begin by deriving a general exact inequality relating the response function and the correlation function from which the various exponent ine... | [['in', 'this', 'letter', 'we', 'derive', 'exponent', 'inequalities', 'relating', 'the', 'dynamic', 'exponent', 'z', 'to', 'the', 'steady', 'state', 'exponent', 'gamma', 'for', 'a', 'general', 'class', 'of', 'stochastically', 'driven', 'dynamical', 'systems', 'we', 'begin', 'by', 'deriving', 'a', 'general', 'exact', 'i... | [-0.11924334466245702, 0.14218377557964149, -0.09424821241885763, 0.1202168704092566, -0.02476790952972475, -0.19988722693233285, 0.06578669712193501, 0.2635012695735151, -0.33093914184031414, -0.27472131653815846, 0.10188899774617642, -0.28477394622115587, -0.19189726912670516, 0.2742210194780703, 0.02275180792309005,... |
710.3158 | Superfluid-insulator transition and BCS-BEC crossover in dirty ultracold
Fermi gas | Superfluid-insulator transition in an ultracold Fermi gas in the external
disorder potential of the amplitude $V_0$ is studied as a function of the
concentration of the gas $n$ and magnetic field $B$ in the presence of the
Feshbach resonance. We find the zero temperature phase diagrams in the plane
($B,n$) at a given... | cond-mat.dis-nn | superfluidinsulator transition in an ultracold fermi gas in the external disorder potential of the amplitude v_0 is studied as a function of the concentration of the gas n and magnetic field b in the presence of the feshbach resonance we find the zero temperature phase diagrams in the plane bn at a given v_0 and in the... | [['superfluidinsulator', 'transition', 'in', 'an', 'ultracold', 'fermi', 'gas', 'in', 'the', 'external', 'disorder', 'potential', 'of', 'the', 'amplitude', 'v_0', 'is', 'studied', 'as', 'a', 'function', 'of', 'the', 'concentration', 'of', 'the', 'gas', 'n', 'and', 'magnetic', 'field', 'b', 'in', 'the', 'presence', 'of'... | [-0.20246730336052624, 0.20043012361951784, -0.0441450101312205, 0.0009324056761204658, 0.054212274456239606, -0.12467824117875242, 0.09407950307141585, 0.3528249410979719, -0.2139156246221209, -0.22016157732760333, 0.005240055510819137, -0.30448640833597584, -0.08244059291522367, 0.1559160585257124, 0.0716125384332185... |
710.3159 | Unveiling dark halos in lensing galaxies | We present a spatially resolved comparison of the stellar-mass and total-mass
surface distributions of nine early-type galaxies. The galaxies are a subset of
the Sloan Lens ACS survey (or SLACS; Bolton et al. 2006). The total-mass
distributions are obtained by exploring pixelated mass models that reproduce
the lensed... | astro-ph | we present a spatially resolved comparison of the stellarmass and totalmass surface distributions of nine earlytype galaxies the galaxies are a subset of the sloan lens acs survey or slacs bolton et al 2006 the totalmass distributions are obtained by exploring pixelated mass models that reproduce the lensed images the ... | [['we', 'present', 'a', 'spatially', 'resolved', 'comparison', 'of', 'the', 'stellarmass', 'and', 'totalmass', 'surface', 'distributions', 'of', 'nine', 'earlytype', 'galaxies', 'the', 'galaxies', 'are', 'a', 'subset', 'of', 'the', 'sloan', 'lens', 'acs', 'survey', 'or', 'slacs', 'bolton', 'et', 'al', '2006', 'the', 't... | [-0.04907680596474983, 0.10107227863318868, -0.08775864063436713, 0.17242954998048984, -0.10330693594073789, -0.06056316022529898, -0.017027325639126185, 0.4097411723044895, -0.12249943596895334, -0.4034513690377642, 0.03835015413945153, -0.3122354691579388, -0.025362776523471995, 0.20360818202333875, -0.05106961538533... |
710.316 | Resolving the Formation of Protogalaxies. III. Feedback from the First
Stars | The first stars form in dark matter halos of masses ~10^6 M_sun as suggested
by an increasing number of numerical simulations. Radiation feedback from these
stars expels most of the gas from their shallow potential well of their
surrounding dark matter halos. We use cosmological adaptive mesh refinement
simulations t... | astro-ph | the first stars form in dark matter halos of masses 106 m_sun as suggested by an increasing number of numerical simulations radiation feedback from these stars expels most of the gas from their shallow potential well of their surrounding dark matter halos we use cosmological adaptive mesh refinement simulations that in... | [['the', 'first', 'stars', 'form', 'in', 'dark', 'matter', 'halos', 'of', 'masses', '106', 'm_sun', 'as', 'suggested', 'by', 'an', 'increasing', 'number', 'of', 'numerical', 'simulations', 'radiation', 'feedback', 'from', 'these', 'stars', 'expels', 'most', 'of', 'the', 'gas', 'from', 'their', 'shallow', 'potential', '... | [-0.05081315854516574, 0.18209601786611337, -0.002141245741155544, 0.10738408263766881, -0.09198724170055661, -0.011075431128835236, 0.06858089086784744, 0.3896770579389698, -0.14694341065052305, -0.38431201617780947, -0.0038324200307607464, -0.3006957378899669, 0.027710553730163862, 0.1704079207743101, 0.0450718742497... |
710.3161 | Formation of central massive objects via tidal compression | For a density that is not too sharply peaked towards the center, the local
tidal field becomes compressive in all three directions. Available gas can then
collapse and form a cluster of stars in the center, including or even being
dominated by a central black hole. We show that for a wide range of
(deprojected) Sersi... | astro-ph | for a density that is not too sharply peaked towards the center the local tidal field becomes compressive in all three directions available gas can then collapse and form a cluster of stars in the center including or even being dominated by a central black hole we show that for a wide range of deprojected sersic profil... | [['for', 'a', 'density', 'that', 'is', 'not', 'too', 'sharply', 'peaked', 'towards', 'the', 'center', 'the', 'local', 'tidal', 'field', 'becomes', 'compressive', 'in', 'all', 'three', 'directions', 'available', 'gas', 'can', 'then', 'collapse', 'and', 'form', 'a', 'cluster', 'of', 'stars', 'in', 'the', 'center', 'inclu... | [-0.1065053604378643, 0.14971949380434835, -0.06323039745643774, 0.08785545990158711, -0.04674536942172776, -0.06360158905708743, -0.0009182755645188986, 0.38058052387537133, -0.17890512024440086, -0.31435944030490454, 0.0518617660912846, -0.2835156050856903, -0.04655525516304163, 0.20605374185986455, -0.02121741621382... |
710.3162 | String junctions in curved backgrounds, their stability and dyon
interactions in SYM | We provide a systematic construction of string junctions in curved
backgrounds which are relevant in computing, within the gauge/gravity
correspondence, the interaction energy of heavy dyons, notably of
quark-monopole pairs, in strongly coupled SYM theories. To isolate the
configurations of physical interest we exami... | hep-th | we provide a systematic construction of string junctions in curved backgrounds which are relevant in computing within the gaugegravity correspondence the interaction energy of heavy dyons notably of quarkmonopole pairs in strongly coupled sym theories to isolate the configurations of physical interest we examine their ... | [['we', 'provide', 'a', 'systematic', 'construction', 'of', 'string', 'junctions', 'in', 'curved', 'backgrounds', 'which', 'are', 'relevant', 'in', 'computing', 'within', 'the', 'gaugegravity', 'correspondence', 'the', 'interaction', 'energy', 'of', 'heavy', 'dyons', 'notably', 'of', 'quarkmonopole', 'pairs', 'in', 'st... | [-0.18305350878440282, 0.15848455250299737, -0.059942631062357594, 0.15834989530541113, -0.037033698699601436, -0.14202931864522672, -0.007902752500776128, 0.3462858122896732, -0.1733345113404771, -0.2591811672546992, 0.07236664777726629, -0.26910327892640934, -0.16337472278916954, 0.17872410225134125, -0.0582790712337... |
710.3163 | The Turbulent Story of X-ray Bursts: Effects of Shear Mixing on
Accreting Neutron Stars | During accretion, a neutron star (NS) is spun up as angular momentum is
transported through its liquid surface layers. We study the resulting
differentially rotating profile, focusing on the impact this has for type I
X-ray bursts. The viscous heating is found to be negligible, but turbulent
mixing can be activated. ... | astro-ph | during accretion a neutron star ns is spun up as angular momentum is transported through its liquid surface layers we study the resulting differentially rotating profile focusing on the impact this has for type i xray bursts the viscous heating is found to be negligible but turbulent mixing can be activated mixing has ... | [['during', 'accretion', 'a', 'neutron', 'star', 'ns', 'is', 'spun', 'up', 'as', 'angular', 'momentum', 'is', 'transported', 'through', 'its', 'liquid', 'surface', 'layers', 'we', 'study', 'the', 'resulting', 'differentially', 'rotating', 'profile', 'focusing', 'on', 'the', 'impact', 'this', 'has', 'for', 'type', 'i', ... | [-0.09038188305812472, 0.299336153177926, -0.05313845088772745, 0.09030201249960698, -0.08155810283721392, -0.1164257010523544, 0.048259681517101194, 0.37737981349521554, -0.2717505864047232, -0.2873522767836385, 0.08204930667493335, -0.28295527164633555, -0.00648212867946061, 0.20530682143401804, -0.027226631120071714... |
710.3164 | The Importance of Satellite Quenching for the Build-Up of the Red
Sequence of Present Day Galaxies | In the current paradigm, red sequence galaxies are believed to have formed as
blue disk galaxies that subsequently had their star formation quenched. Since
red-sequence galaxies typically have an early-type morphology, the transition
from the blue to the red sequence also involves a morphological transformation.
In t... | astro-ph | in the current paradigm red sequence galaxies are believed to have formed as blue disk galaxies that subsequently had their star formation quenched since redsequence galaxies typically have an earlytype morphology the transition from the blue to the red sequence also involves a morphological transformation in this pape... | [['in', 'the', 'current', 'paradigm', 'red', 'sequence', 'galaxies', 'are', 'believed', 'to', 'have', 'formed', 'as', 'blue', 'disk', 'galaxies', 'that', 'subsequently', 'had', 'their', 'star', 'formation', 'quenched', 'since', 'redsequence', 'galaxies', 'typically', 'have', 'an', 'earlytype', 'morphology', 'the', 'tra... | [-0.05819589172041918, 0.15526602876767961, -0.10013750190917177, 0.13709115143203895, -0.08224041971455638, 0.00915979655771728, 0.032730595842374234, 0.4627298621573683, -0.0974776060320437, -0.3584431733540965, 0.022050935510461302, -0.29264537072176056, -0.06335851875844652, 0.18191417190599057, -0.0690335865903321... |
710.3165 | A 15.65 solar mass black hole in an eclipsing binary in the nearby
spiral galaxy Messier 33 | Stellar-mass black holes are discovered in X-ray emitting binary systems,
where their mass can be determined from the dynamics of their companion stars.
Models of stellar evolution have difficulty producing black holes in close
binaries with masses >10 solar masses, which is consistent with the fact that
the most mas... | astro-ph | stellarmass black holes are discovered in xray emitting binary systems where their mass can be determined from the dynamics of their companion stars models of stellar evolution have difficulty producing black holes in close binaries with masses 10 solar masses which is consistent with the fact that the most massive ste... | [['stellarmass', 'black', 'holes', 'are', 'discovered', 'in', 'xray', 'emitting', 'binary', 'systems', 'where', 'their', 'mass', 'can', 'be', 'determined', 'from', 'the', 'dynamics', 'of', 'their', 'companion', 'stars', 'models', 'of', 'stellar', 'evolution', 'have', 'difficulty', 'producing', 'black', 'holes', 'in', '... | [-0.0989237061398112, 0.14950143781889103, -0.03623089637804268, 0.10925012492802454, -0.07167678549147256, -0.061298247693426546, 0.04278181932993758, 0.36701465953584544, -0.1334801486222533, -0.38828162674993144, 0.11392317273928927, -0.30817527820803386, -0.0387469031878784, 0.2013158540722595, -0.07980859569183629... |
710.3166 | Constraining the Type Ia Supernova Progenitor: The Search for Hydrogen
in Nebular Spectra | Despite intense scrutiny, the progenitor system(s) that gives rise to Type Ia
supernovae remains unknown. The favored theory invokes a carbon-oxygen white
dwarf accreting hydrogen-rich material from a close companion until a
thermonuclear runaway ensues that incinerates the white dwarf. However,
simulations resulting... | astro-ph | despite intense scrutiny the progenitor systems that gives rise to type ia supernovae remains unknown the favored theory invokes a carbonoxygen white dwarf accreting hydrogenrich material from a close companion until a thermonuclear runaway ensues that incinerates the white dwarf however simulations resulting from this... | [['despite', 'intense', 'scrutiny', 'the', 'progenitor', 'systems', 'that', 'gives', 'rise', 'to', 'type', 'ia', 'supernovae', 'remains', 'unknown', 'the', 'favored', 'theory', 'invokes', 'a', 'carbonoxygen', 'white', 'dwarf', 'accreting', 'hydrogenrich', 'material', 'from', 'a', 'close', 'companion', 'until', 'a', 'th... | [-0.04691340097774481, 0.09844466146305128, -0.04208754613343197, 0.08940968115026483, -0.14942112871314817, -0.1413419596563321, 0.10877695635405331, 0.40776694921373224, -0.15020935200068944, -0.30138948577142877, 0.06384620586011026, -0.3161346150502082, -0.05227470065119423, 0.21443284127200324, -0.0908801370968734... |
710.3167 | Binary Stars and Globular Cluster Dynamics | In this brief proceedings article I summarize the review talk I gave at the
IAU 246 meeting in Capri, Italy, glossing over the well-known results from the
literature, but paying particular attention to new, previously unpublished
material. This new material includes a careful comparison of the apparently
contradictor... | astro-ph | in this brief proceedings article i summarize the review talk i gave at the iau 246 meeting in capri italy glossing over the wellknown results from the literature but paying particular attention to new previously unpublished material this new material includes a careful comparison of the apparently contradictory result... | [['in', 'this', 'brief', 'proceedings', 'article', 'i', 'summarize', 'the', 'review', 'talk', 'i', 'gave', 'at', 'the', 'iau', '246', 'meeting', 'in', 'capri', 'italy', 'glossing', 'over', 'the', 'wellknown', 'results', 'from', 'the', 'literature', 'but', 'paying', 'particular', 'attention', 'to', 'new', 'previously', ... | [-0.025212052938632806, 0.03825326453433067, -0.11851221838504702, 0.03598466020068763, -0.11475323168473824, -0.08739071180521746, 0.053862787008494416, 0.35622942844562444, -0.17621689007365118, -0.37288807964857634, 0.06023901628839531, -0.27729469078166463, -0.16220516725182185, 0.24669730762306985, -0.134225296021... |
710.3168 | Supplementary Information for "A 15.65 solar mass black hole in an
eclipsing binary in the nearby spiral galaxy Messier 33" | This Supplementary Information provides details about the spectral extraction
(crowding issues and the removal of nebular lines), a discussion about the
distance to M33, a model for the O-star wind and the measurement of the true
photospheric X-ray eclipse width Theta, and details about ellipsoidal
modelling. It also... | astro-ph | this supplementary information provides details about the spectral extraction crowding issues and the removal of nebular lines a discussion about the distance to m33 a model for the ostar wind and the measurement of the true photospheric xray eclipse width theta and details about ellipsoidal modelling it also contains ... | [['this', 'supplementary', 'information', 'provides', 'details', 'about', 'the', 'spectral', 'extraction', 'crowding', 'issues', 'and', 'the', 'removal', 'of', 'nebular', 'lines', 'a', 'discussion', 'about', 'the', 'distance', 'to', 'm33', 'a', 'model', 'for', 'the', 'ostar', 'wind', 'and', 'the', 'measurement', 'of', ... | [-0.09257005697822776, 0.024287595930469127, -0.05862010076063974, 0.1327006141715362, -0.15101044812914113, -0.13986206487230635, 0.07955595980004954, 0.40131314137372476, -0.2278997894248058, -0.3564025140849167, 0.13525445326552565, -0.33487745454727574, -0.07537987128157041, 0.1879240017312033, -0.08232482044218943... |
710.3169 | New Gamma-Ray Contributions to Supersymmetric Dark Matter Annihilation | We compute the electromagnetic radiative corrections to all leading
annihilation processes which may occur in the Galactic dark matter halo, for
dark matter in the framework of supersymmetric extensions of the Standard Model
(MSSM and mSUGRA), and present the results of scans over the parameter space
that is consiste... | hep-ph astro-ph | we compute the electromagnetic radiative corrections to all leading annihilation processes which may occur in the galactic dark matter halo for dark matter in the framework of supersymmetric extensions of the standard model mssm and msugra and present the results of scans over the parameter space that is consistent wit... | [['we', 'compute', 'the', 'electromagnetic', 'radiative', 'corrections', 'to', 'all', 'leading', 'annihilation', 'processes', 'which', 'may', 'occur', 'in', 'the', 'galactic', 'dark', 'matter', 'halo', 'for', 'dark', 'matter', 'in', 'the', 'framework', 'of', 'supersymmetric', 'extensions', 'of', 'the', 'standard', 'mod... | [-0.07918911946577177, 0.17511514371885956, -0.08974230946367415, 0.17224390963389474, -0.09888795918857855, -0.0958691074564639, 0.023527825084503417, 0.339794029847004, -0.19377303934261325, -0.35522183678553676, 0.05956060176144197, -0.26750308843310383, -0.033165235446053154, 0.23626942001115492, 0.038852929160523,... |
710.317 | Fast Intrinsic Mode Decomposition of Time Series Data with Sawtooth
Transform | An efficient method is introduced in this paper to find the intrinsic mode
function (IMF) components of time series data. This method is faster and more
predictable than the Empirical Mode Decomposition (EMD) method devised by the
author of Hilbert Huang Transform (HHT). The approach is to transforms the
original dat... | cs.NA | an efficient method is introduced in this paper to find the intrinsic mode function imf components of time series data this method is faster and more predictable than the empirical mode decomposition emd method devised by the author of hilbert huang transform hht the approach is to transforms the original data function... | [['an', 'efficient', 'method', 'is', 'introduced', 'in', 'this', 'paper', 'to', 'find', 'the', 'intrinsic', 'mode', 'function', 'imf', 'components', 'of', 'time', 'series', 'data', 'this', 'method', 'is', 'faster', 'and', 'more', 'predictable', 'than', 'the', 'empirical', 'mode', 'decomposition', 'emd', 'method', 'devi... | [-0.06782132135069167, 0.07191626782066922, -0.14146503173379285, 0.09613706037469621, -0.07952668913781191, -0.08377477725629102, 0.04593028712410931, 0.4019070892735864, -0.2902611336699038, -0.2892065098847855, 0.09731532617253393, -0.22429141350316278, -0.15052740623694705, 0.1983327369671315, -0.019385246757530804... |
710.3171 | Dependency and false discovery rate: Asymptotics | Some effort has been undertaken over the last decade to provide conditions
for the control of the false discovery rate by the linear step-up procedure
(LSU) for testing $n$ hypotheses when test statistics are dependent. In this
paper we investigate the expected error rate (EER) and the false discovery rate
(FDR) in s... | math.ST stat.TH | some effort has been undertaken over the last decade to provide conditions for the control of the false discovery rate by the linear stepup procedure lsu for testing n hypotheses when test statistics are dependent in this paper we investigate the expected error rate eer and the false discovery rate fdr in some extreme ... | [['some', 'effort', 'has', 'been', 'undertaken', 'over', 'the', 'last', 'decade', 'to', 'provide', 'conditions', 'for', 'the', 'control', 'of', 'the', 'false', 'discovery', 'rate', 'by', 'the', 'linear', 'stepup', 'procedure', 'lsu', 'for', 'testing', 'n', 'hypotheses', 'when', 'test', 'statistics', 'are', 'dependent',... | [-0.1121333437411522, 0.04982300023257267, -0.08046501604112563, 0.1339562991015555, -0.03092153149918886, -0.15186487330356613, 0.12488329419684305, 0.34903829680988563, -0.18352913843118585, -0.296037473436445, 0.14186971659655684, -0.23357922202558257, -0.1360453815519577, 0.24053456233814358, -0.09530103810784567, ... |
710.3172 | Model study of the sign problem in a mean-field approximation | We study the sign problem of the fermion determinant at nonzero baryon
chemical potential. For this purpose we apply a simple model derived from
Quantum Chromodynamics, in the limit of large chemical potential and mass. For
SU(2) color, there is no sign problem and the mean-field approximation is
similar to data from... | hep-lat | we study the sign problem of the fermion determinant at nonzero baryon chemical potential for this purpose we apply a simple model derived from quantum chromodynamics in the limit of large chemical potential and mass for su2 color there is no sign problem and the meanfield approximation is similar to data from the latt... | [['we', 'study', 'the', 'sign', 'problem', 'of', 'the', 'fermion', 'determinant', 'at', 'nonzero', 'baryon', 'chemical', 'potential', 'for', 'this', 'purpose', 'we', 'apply', 'a', 'simple', 'model', 'derived', 'from', 'quantum', 'chromodynamics', 'in', 'the', 'limit', 'of', 'large', 'chemical', 'potential', 'and', 'mas... | [-0.08909915268178219, 0.10691541115469906, -0.11863190031347229, 0.1549580571489692, -0.02622243897665454, -0.10229571330685007, 0.11998560853332849, 0.3527875551144066, -0.24279164012683474, -0.2660770077035641, 0.042453892334141645, -0.28303622332927975, -0.13024958142183174, 0.08945010248925941, 0.00697736007303161... |
710.3173 | Noise auto-correlation spectroscopy with coherent Raman scattering | Ultrafast lasers have become one of the most powerful tools in coherent
nonlinear optical spectroscopy. Short pulses enable direct observation of fast
molecular dynamics, whereas broad spectral bandwidth offers ways of controlling
nonlinear optical processes by means of quantum interferences. Special care is
usually ... | physics.chem-ph | ultrafast lasers have become one of the most powerful tools in coherent nonlinear optical spectroscopy short pulses enable direct observation of fast molecular dynamics whereas broad spectral bandwidth offers ways of controlling nonlinear optical processes by means of quantum interferences special care is usually taken... | [['ultrafast', 'lasers', 'have', 'become', 'one', 'of', 'the', 'most', 'powerful', 'tools', 'in', 'coherent', 'nonlinear', 'optical', 'spectroscopy', 'short', 'pulses', 'enable', 'direct', 'observation', 'of', 'fast', 'molecular', 'dynamics', 'whereas', 'broad', 'spectral', 'bandwidth', 'offers', 'ways', 'of', 'control... | [-0.097735037254073, 0.15398049184353005, -0.09600924132086038, 0.04140556968501409, -0.04274824665306242, -0.14417862746352125, 0.061514968458943345, 0.49251360604010813, -0.2755300957271341, -0.2984525948787295, 0.06529712176517742, -0.2351928566761445, -0.10796065527160843, 0.246621123640127, -0.03663021478574219, 0... |
710.3174 | Rigidity of gradient Ricci Solitons | We define a gradient Ricci soliton to be rigid if it is a flat bundle $%
N\times_{\Gamma}\mathbb{R}^{k}$ where $N$ is Einstein. It is known that not all
gradient solitons are rigid. Here we offer several natural conditions on the
curvature that characterize rigid gradient solitons. Other related results on
rigidity o... | math.DG | we define a gradient ricci soliton to be rigid if it is a flat bundle ntimes_gammamathbbrk where n is einstein it is known that not all gradient solitons are rigid here we offer several natural conditions on the curvature that characterize rigid gradient solitons other related results on rigidity of ricci solitons are ... | [['we', 'define', 'a', 'gradient', 'ricci', 'soliton', 'to', 'be', 'rigid', 'if', 'it', 'is', 'a', 'flat', 'bundle', 'ntimes_gammamathbbrk', 'where', 'n', 'is', 'einstein', 'it', 'is', 'known', 'that', 'not', 'all', 'gradient', 'solitons', 'are', 'rigid', 'here', 'we', 'offer', 'several', 'natural', 'conditions', 'on',... | [-0.1899733293223484, 0.14233135879200337, -0.11827351371275968, 0.08677978514781992, -0.15229023576730155, -0.19725749277156487, -0.142026475823388, 0.48498383941578455, -0.26562339549177677, -0.15730200692457308, 0.15296720701133318, -0.24473592879828707, -0.19074958078322354, 0.18225312563349846, -0.1199133906690082... |
710.3175 | Filling real hypersurfaces by pseudoholomorphic discs | We study pseudoholomorphic discs with boundaries attached to a real
hypersurface in an almost complex manifold. We give sufficient conditions for
filling a one sided neighborhood of the hypersurface by the discs.
| math.CV math.AP | we study pseudoholomorphic discs with boundaries attached to a real hypersurface in an almost complex manifold we give sufficient conditions for filling a one sided neighborhood of the hypersurface by the discs | [['we', 'study', 'pseudoholomorphic', 'discs', 'with', 'boundaries', 'attached', 'to', 'a', 'real', 'hypersurface', 'in', 'an', 'almost', 'complex', 'manifold', 'we', 'give', 'sufficient', 'conditions', 'for', 'filling', 'a', 'one', 'sided', 'neighborhood', 'of', 'the', 'hypersurface', 'by', 'the', 'discs']] | [-0.2387653975165449, 0.0014320386585495726, -0.08036412240471691, 0.07031861558789387, -0.058700704474176746, -0.12566923882695846, -0.0402749451022828, 0.36609551357105374, -0.21107234538067132, -0.2069842328201048, 0.13331031212510425, -0.2240972324507311, -0.16381418710807338, 0.17315616086125374, -0.15563085141184... |
710.3176 | Local Normal Mode Coupling and Energy Band Splitting in Elliptically
Birefringent 1D Magnetophotonic Crystals | An analysis is presented of wave-vector dispersion in elliptically
birefringent stratified magneto-optic media having one-dimensional periodicity.
It is found that local normal-mode polarization-state differences between
adjacent layers lead to mode coupling and impact the wave-vector dispersion and
the character of ... | physics.optics | an analysis is presented of wavevector dispersion in elliptically birefringent stratified magnetooptic media having onedimensional periodicity it is found that local normalmode polarizationstate differences between adjacent layers lead to mode coupling and impact the wavevector dispersion and the character of the bloch... | [['an', 'analysis', 'is', 'presented', 'of', 'wavevector', 'dispersion', 'in', 'elliptically', 'birefringent', 'stratified', 'magnetooptic', 'media', 'having', 'onedimensional', 'periodicity', 'it', 'is', 'found', 'that', 'local', 'normalmode', 'polarizationstate', 'differences', 'between', 'adjacent', 'layers', 'lead'... | [-0.2448257461241255, 0.18217149685539244, -0.05648313316337968, 0.02188154318679303, -0.07230029752229225, -0.1117198505623853, 0.06686731757698199, 0.42935638726778225, -0.30413632745510094, -0.2535973292574516, 0.006890779356344616, -0.2513961028180098, -0.15007386355954286, 0.1649800383115876, 0.03785521957755395, ... |
710.3177 | On Monotonic Strengthening of Newman-like Phenomenon on (2m+1)-multiples
in Base 2m | We obtain exact and asymptotic expressions for the excess of nonnegative
(2m+1)-multiples less than (2m)^k with even digit sums in the base 2m.
| math.NT | we obtain exact and asymptotic expressions for the excess of nonnegative 2m1multiples less than 2mk with even digit sums in the base 2m | [['we', 'obtain', 'exact', 'and', 'asymptotic', 'expressions', 'for', 'the', 'excess', 'of', 'nonnegative', '2m1multiples', 'less', 'than', '2mk', 'with', 'even', 'digit', 'sums', 'in', 'the', 'base', '2m']] | [-0.1608990736475045, 0.04322643751617183, -0.0453564351932569, 0.1104151653972539, -0.02876086202873425, -0.17394930551844565, 0.07891022244637663, 0.32559776915745303, -0.11704683617096055, -0.27209322146055376, 0.16263922091721641, -0.3689954446798021, -0.09851206737485799, 0.19778088632632385, -0.008047408508983526... |
710.3178 | Modeling Context, Collaboration, and Civilization in End-User
Informatics | End-user informatics applications are Internet data web management automation
solutions. These are mass modeling and mass management collaborative communal
consensus solutions. They are made and maintained by managerial, professional,
technical and specialist end-users. In end-user informatics the end-users are
alway... | cs.OH | enduser informatics applications are internet data web management automation solutions these are mass modeling and mass management collaborative communal consensus solutions they are made and maintained by managerial professional technical and specialist endusers in enduser informatics the endusers are always right so ... | [['enduser', 'informatics', 'applications', 'are', 'internet', 'data', 'web', 'management', 'automation', 'solutions', 'these', 'are', 'mass', 'modeling', 'and', 'mass', 'management', 'collaborative', 'communal', 'consensus', 'solutions', 'they', 'are', 'made', 'and', 'maintained', 'by', 'managerial', 'professional', '... | [-0.09416815266155987, 0.07842511462156256, -0.0763850978009997, 0.10158204078242937, -0.20244337704341195, -0.1999841233279929, 0.04009156147349466, 0.4178185372276266, -0.27221513987501705, -0.3284065171939098, 0.15220233165170494, -0.32051209151242044, -0.18092555731022159, 0.1758909376546672, -0.1603046418710446, 0... |
710.3179 | Spectral weight transfer in a disorder-broadened Landau level | In the absence of disorder, the degeneracy of a Landau level (LL) is
$N=BA/\phi_0$, where $B$ is the magnetic field, $A$ is the area of the sample
and $\phi_0=h/e$ is the magnetic flux quantum. With disorder, localized states
appear at the top and bottom of the broadened LL, while states in the center of
the LL (the ... | cond-mat.dis-nn | in the absence of disorder the degeneracy of a landau level ll is nbaphi_0 where b is the magnetic field a is the area of the sample and phi_0he is the magnetic flux quantum with disorder localized states appear at the top and bottom of the broadened ll while states in the center of the ll the critical region remain de... | [['in', 'the', 'absence', 'of', 'disorder', 'the', 'degeneracy', 'of', 'a', 'landau', 'level', 'll', 'is', 'nbaphi_0', 'where', 'b', 'is', 'the', 'magnetic', 'field', 'a', 'is', 'the', 'area', 'of', 'the', 'sample', 'and', 'phi_0he', 'is', 'the', 'magnetic', 'flux', 'quantum', 'with', 'disorder', 'localized', 'states',... | [-0.1893577352863084, 0.23312877879484373, -0.03338087068080307, 0.07006219783433568, -0.0021772048512131584, -0.13705343348892773, 0.06267207192627675, 0.28840729506721174, -0.2543369560291813, -0.31500745263128055, 0.04658329326558073, -0.29080974061650283, -0.11210878915945385, 0.13467023305145098, -0.00556459343163... |
710.318 | The remarkable properties of the symbiotic star AE Circinus | We present new optical spectroscopy and photometry, 2MASS infrared
observations and 24 years of combined AAVSO and AFOEV photometry of the
symbiotic star candidate \ae. The long-term light curve is characterized by
outbursts lasting several years and having a slow decline of $\sim 2 \times
10^{-4}$ mag/day. The whole... | astro-ph | we present new optical spectroscopy and photometry 2mass infrared observations and 24 years of combined aavso and afoev photometry of the symbiotic star candidate ae the longterm light curve is characterized by outbursts lasting several years and having a slow decline of sim 2 times 104 magday the whole range of variab... | [['we', 'present', 'new', 'optical', 'spectroscopy', 'and', 'photometry', '2mass', 'infrared', 'observations', 'and', '24', 'years', 'of', 'combined', 'aavso', 'and', 'afoev', 'photometry', 'of', 'the', 'symbiotic', 'star', 'candidate', 'ae', 'the', 'longterm', 'light', 'curve', 'is', 'characterized', 'by', 'outbursts'... | [-0.07484629189852497, 0.08252291761113908, -0.05608135162238513, 0.06538990637034595, -0.07137687537008254, -0.13433640204361993, 0.09413574255023409, 0.41952025616874694, -0.204393870552504, -0.3269359044176687, 0.08347059205196525, -0.3553310838961524, -0.021572123131371537, 0.17166758257422018, -0.06408519382966915... |
710.3181 | An improved calculation of the isospin-symmetry-breaking corrections to
superallowed Fermi beta decay | We report new shell-model calculations of the isospin-symmetry-breaking
correction to superallowed nuclear beta decay. The most important improvement
is the inclusion of core orbitals, which are demonstrated to have a significant
impact on the mismatch in the radial wave functions of the parent and daughter
states. W... | nucl-th hep-ph nucl-ex | we report new shellmodel calculations of the isospinsymmetrybreaking correction to superallowed nuclear beta decay the most important improvement is the inclusion of core orbitals which are demonstrated to have a significant impact on the mismatch in the radial wave functions of the parent and daughter states we determ... | [['we', 'report', 'new', 'shellmodel', 'calculations', 'of', 'the', 'isospinsymmetrybreaking', 'correction', 'to', 'superallowed', 'nuclear', 'beta', 'decay', 'the', 'most', 'important', 'improvement', 'is', 'the', 'inclusion', 'of', 'core', 'orbitals', 'which', 'are', 'demonstrated', 'to', 'have', 'a', 'significant', ... | [-0.0642159960243081, 0.12328524656625342, -0.04343308362551814, 0.08018980101765492, -0.020451852115256162, -0.09449722188883904, 0.05848397425630822, 0.3114711346037103, -0.2140819722111467, -0.2925365967780102, 0.049518360896816466, -0.3281594251891255, -0.08391935931383399, 0.18589830455011247, 0.02764657943629186,... |
710.3182 | Schubert polynomials and classes of Hessenberg varieties | Regular semisimple Hessenberg varieties are a family of subvarieties of the
flag variety that arise in number theory, numerical analysis, representation
theory, algebraic geometry, and combinatorics. We give a "Giambelli formula"
expressing the classes of regular semisimple Hessenberg varieties in terms of
Chern clas... | math.AG math.CO | regular semisimple hessenberg varieties are a family of subvarieties of the flag variety that arise in number theory numerical analysis representation theory algebraic geometry and combinatorics we give a giambelli formula expressing the classes of regular semisimple hessenberg varieties in terms of chern classes in fa... | [['regular', 'semisimple', 'hessenberg', 'varieties', 'are', 'a', 'family', 'of', 'subvarieties', 'of', 'the', 'flag', 'variety', 'that', 'arise', 'in', 'number', 'theory', 'numerical', 'analysis', 'representation', 'theory', 'algebraic', 'geometry', 'and', 'combinatorics', 'we', 'give', 'a', 'giambelli', 'formula', 'e... | [-0.19902344381057277, -0.001108496253275209, -0.05726556401706249, 0.06936254649405817, -0.14649558696481918, -0.14873387711122632, -0.04614666870415762, 0.29828830769768466, -0.36887275194749236, -0.1852295836330288, 0.0882882388446618, -0.18320102578511946, -0.24423336076239746, 0.25976738074311506, -0.1880740513605... |
710.3183 | Probabilistic coherence and proper scoring rules | We provide self-contained proof of a theorem relating probabilistic coherence
of forecasts to their non-domination by rival forecasts with respect to any
proper scoring rule. The theorem appears to be new but is closely related to
results achieved by other investigators.
| stat.ML | we provide selfcontained proof of a theorem relating probabilistic coherence of forecasts to their nondomination by rival forecasts with respect to any proper scoring rule the theorem appears to be new but is closely related to results achieved by other investigators | [['we', 'provide', 'selfcontained', 'proof', 'of', 'a', 'theorem', 'relating', 'probabilistic', 'coherence', 'of', 'forecasts', 'to', 'their', 'nondomination', 'by', 'rival', 'forecasts', 'with', 'respect', 'to', 'any', 'proper', 'scoring', 'rule', 'the', 'theorem', 'appears', 'to', 'be', 'new', 'but', 'is', 'closely',... | [-0.041049441578230116, 0.08465232705788278, -0.1761942333907383, 0.10519262500073216, -0.1556920195679839, -0.19596515085957036, 0.11287407557587935, 0.3613930768901255, -0.23792930315362243, -0.2934334890579055, 0.1261627930443643, -0.23581949476061798, -0.07731758416971056, 0.2808472194322726, -0.19456822936218687, ... |
710.3184 | 19F (p, alpha gamma) 16O reaction: HPGe detector response function and
gamma-ray relative yields | The 6.1, 6.9 and 7.1 MeV photon yields in the reaction with protons in the
1.32 to 1.42 MeV energy range were determined from the comparison between
experimental and simulated spectrum. The gamma-ray spectra were measured with a
HPGe detector which was 72.5 mm in diameter and 60.5 mm in length. The reaction
kinematic... | physics.ins-det nucl-ex | the 61 69 and 71 mev photon yields in the reaction with protons in the 132 to 142 mev energy range were determined from the comparison between experimental and simulated spectrum the gammaray spectra were measured with a hpge detector which was 725 mm in diameter and 605 mm in length the reaction kinematics and the det... | [['the', '61', '69', 'and', '71', 'mev', 'photon', 'yields', 'in', 'the', 'reaction', 'with', 'protons', 'in', 'the', '132', 'to', '142', 'mev', 'energy', 'range', 'were', 'determined', 'from', 'the', 'comparison', 'between', 'experimental', 'and', 'simulated', 'spectrum', 'the', 'gammaray', 'spectra', 'were', 'measure... | [0.02619071877287591, 0.14691203192570337, -0.08715888103966683, 0.05622404935831368, 0.03138102864214292, -0.07809308956961568, 0.01640285050733855, 0.4173410134253037, -0.19620417295863815, -0.46817162006582114, -0.016320666677190687, -0.3919622007958299, 0.029673964460836907, 0.21792856489728188, 0.05996758796676409... |
710.3185 | Fuzzy Modeling of Electrical Impedance Tomography Image of the Lungs | Electrical Impedance Tomography (EIT) is a functional imaging method that is
being developed for bedside use in critical care medicine. Aiming at improving
the chest anatomical resolution of EIT images we developed a fuzzy model based
on EIT high temporal resolution and the functional information contained in the
pul... | cs.AI cs.CV | electrical impedance tomography eit is a functional imaging method that is being developed for bedside use in critical care medicine aiming at improving the chest anatomical resolution of eit images we developed a fuzzy model based on eit high temporal resolution and the functional information contained in the pulmonar... | [['electrical', 'impedance', 'tomography', 'eit', 'is', 'a', 'functional', 'imaging', 'method', 'that', 'is', 'being', 'developed', 'for', 'bedside', 'use', 'in', 'critical', 'care', 'medicine', 'aiming', 'at', 'improving', 'the', 'chest', 'anatomical', 'resolution', 'of', 'eit', 'images', 'we', 'developed', 'a', 'fuzz... | [-0.018426673716469985, 0.03940335665345745, -0.06342001405297927, 0.08926511249828183, -0.024628484162361654, -0.1404212814804643, 0.006626349480473968, 0.41051976366359827, -0.20359823711165417, -0.2962532520813008, 0.1533661906009558, -0.315636972331157, -0.16650644031812578, 0.2720130744877114, -0.14332965359551042... |
710.3186 | D-branes as coherent states in the open string channel | We show that bosonic D-brane states may be represented as coherent states in
an open string representation. By using the Thermo-Field Dynamics (TFD)
formalism, we may construct a condensed state of open string modes which
encodes the information on the D-brane configuration.
We also introduce a construction alterna... | hep-th | we show that bosonic dbrane states may be represented as coherent states in an open string representation by using the thermofield dynamics tfd formalism we may construct a condensed state of open string modes which encodes the information on the dbrane configuration we also introduce a construction alternative to tfd ... | [['we', 'show', 'that', 'bosonic', 'dbrane', 'states', 'may', 'be', 'represented', 'as', 'coherent', 'states', 'in', 'an', 'open', 'string', 'representation', 'by', 'using', 'the', 'thermofield', 'dynamics', 'tfd', 'formalism', 'we', 'may', 'construct', 'a', 'condensed', 'state', 'of', 'open', 'string', 'modes', 'which... | [-0.12683542639951684, 0.1673166280292004, -0.1615034684789582, 0.1136114345570388, -0.06394835060032514, -0.11930475723962267, 0.04192869403721908, 0.3307865952447682, -0.26430154708051284, -0.2392013940497764, 0.09897631927966498, -0.20867358520789842, -0.17350075809102689, 0.16590159192316598, -0.09846025123749372, ... |
710.3187 | On the Quantum Origin of Structure in the Inflationary Universe | In this lecture I give a pedagogical introduction to inflationary cosmology
with a special focus on the quantum generation of cosmological perturbations.
| hep-th | in this lecture i give a pedagogical introduction to inflationary cosmology with a special focus on the quantum generation of cosmological perturbations | [['in', 'this', 'lecture', 'i', 'give', 'a', 'pedagogical', 'introduction', 'to', 'inflationary', 'cosmology', 'with', 'a', 'special', 'focus', 'on', 'the', 'quantum', 'generation', 'of', 'cosmological', 'perturbations']] | [-0.12397339889271693, 0.15506600376895882, -0.1105164172635837, 0.09707359425109727, -0.15034060874445873, -0.22161454847082496, -0.11808556577571752, 0.22980495440689, -0.15360499105670236, -0.24874230842529374, 0.12340444344921377, -0.20467583937782116, -0.12908945768140256, 0.14606718908445063, -0.11308609971522608... |
710.3188 | Powers of Coxeter elements in infinite groups are reduced | Let W be an infinite irreducible Coxeter group with (s_1, ..., s_n) the
simple generators. We give a simple proof that the word s_1 s_2 ... s_n s_1 s_2
>... s_n ... s_1 s_2 ... s_n is reduced for any number of repetitions of s_1
s_2 >... s_n. This result was proved for simply-laced, crystallographic groups
by Kleiner... | math.CO | let w be an infinite irreducible coxeter group with s_1 s_n the simple generators we give a simple proof that the word s_1 s_2 s_n s_1 s_2 s_n s_1 s_2 s_n is reduced for any number of repetitions of s_1 s_2 s_n this result was proved for simplylaced crystallographic groups by kleiner and pelley using methods from the t... | [['let', 'w', 'be', 'an', 'infinite', 'irreducible', 'coxeter', 'group', 'with', 's_1', 's_n', 'the', 'simple', 'generators', 'we', 'give', 'a', 'simple', 'proof', 'that', 'the', 'word', 's_1', 's_2', 's_n', 's_1', 's_2', 's_n', 's_1', 's_2', 's_n', 'is', 'reduced', 'for', 'any', 'number', 'of', 'repetitions', 'of', 's... | [-0.16804440926735928, 0.21847092196836265, -0.07699955173915154, 0.014286261395012078, -0.06386504449734562, -0.18074367115102513, -0.017481080705214192, 0.36761478562594246, -0.34937574692364587, -0.20066879858802023, 0.07413642074434872, -0.2940276072507626, -0.06464318722167886, 0.19689501351431796, -0.147540521379... |
710.3189 | Multimass spherical structure models for N-body simulations | We present a simple and efficient method to set up spherical structure models
for N-body simulations with a multimass technique. This technique reduces by a
substantial factor the computer run time needed in order to resolve a given
scale as compared to single-mass models. It therefore allows to resolve smaller
scale... | astro-ph | we present a simple and efficient method to set up spherical structure models for nbody simulations with a multimass technique this technique reduces by a substantial factor the computer run time needed in order to resolve a given scale as compared to singlemass models it therefore allows to resolve smaller scales in n... | [['we', 'present', 'a', 'simple', 'and', 'efficient', 'method', 'to', 'set', 'up', 'spherical', 'structure', 'models', 'for', 'nbody', 'simulations', 'with', 'a', 'multimass', 'technique', 'this', 'technique', 'reduces', 'by', 'a', 'substantial', 'factor', 'the', 'computer', 'run', 'time', 'needed', 'in', 'order', 'to'... | [-0.08589675589354043, 0.11969916396291455, -0.08933480535555818, 0.08438357050170188, -0.04027267551705158, -0.07543967640958726, 0.016923628656412136, 0.37778856053781906, -0.20651777795198575, -0.38335344018661754, 0.06756025270426219, -0.2353613797573447, -0.07495486285724787, 0.20575695114038553, 0.001084523818711... |
710.319 | Chandra Observations of Type Ia Supernovae: Upper Limits to the X-ray
Flux of SN 2002bo, SN 2002ic, SN 2005gj, and SN 2005ke | We set sensitive upper limits to the X-ray emission of four Type Ia
supernovae (SNe Ia) using the Chandra X-ray Observatory. SN 2002bo, a normal,
although reddened, nearby SN Ia, was observed 9.3 days after explosion. For an
absorbed, high temperature bremsstrahlung model the flux limits are 3.2E-16
ergs/cm^2/s (0.5-... | astro-ph | we set sensitive upper limits to the xray emission of four type ia supernovae sne ia using the chandra xray observatory sn 2002bo a normal although reddened nearby sn ia was observed 93 days after explosion for an absorbed high temperature bremsstrahlung model the flux limits are 32e16 ergscm2s 052 kev band and 41e15 e... | [['we', 'set', 'sensitive', 'upper', 'limits', 'to', 'the', 'xray', 'emission', 'of', 'four', 'type', 'ia', 'supernovae', 'sne', 'ia', 'using', 'the', 'chandra', 'xray', 'observatory', 'sn', '2002bo', 'a', 'normal', 'although', 'reddened', 'nearby', 'sn', 'ia', 'was', 'observed', '93', 'days', 'after', 'explosion', 'fo... | [-0.010623797129287764, 0.10213176152907114, 0.006561561282379208, 0.16570737652644446, -0.14338562743203645, -0.12958767173328886, 0.13061968462662427, 0.4884633556146313, -0.1300071066133333, -0.3335930468928483, 0.055652570327381704, -0.36329101390400426, 0.05992817454626439, 0.22187133276731605, -0.0198433004424495... |
710.3191 | Galaxy Structural Parameters in Source Extractor | Over the last decade, the Concentration, Asymmetry and Smoothness (CAS), as
well as the M20 and GINI parameters have become popular to automatically
classify distant galaxies in images. Ellipticals, spirals and irregular
galaxies all appear to occupy different regions of this parameter space. At the
same time, the So... | astro-ph | over the last decade the concentration asymmetry and smoothness cas as well as the m20 and gini parameters have become popular to automatically classify distant galaxies in images ellipticals spirals and irregular galaxies all appear to occupy different regions of this parameter space at the same time the source extrac... | [['over', 'the', 'last', 'decade', 'the', 'concentration', 'asymmetry', 'and', 'smoothness', 'cas', 'as', 'well', 'as', 'the', 'm20', 'and', 'gini', 'parameters', 'have', 'become', 'popular', 'to', 'automatically', 'classify', 'distant', 'galaxies', 'in', 'images', 'ellipticals', 'spirals', 'and', 'irregular', 'galaxie... | [-0.05741876872305415, 0.021837146590776773, -0.07323610995281563, 0.12293667371973004, -0.10059878931980323, -0.13395887256980787, 0.026815744030180007, 0.40385849363649423, -0.2588528500791396, -0.3487157642517073, 0.09971054671860115, -0.2774183030564504, -0.03622618637534107, 0.20595398886875826, -0.090936270080552... |
710.3192 | The Environment of M85 optical transient 2006-1: constraints on the
progenitor age and mass | M85 optical transient 2006-1 (M85 OT 2006-1) is the most luminous member of
the small family of V838 Mon-like objects, whose nature is still a mystery.
This event took place in the Virgo cluster of galaxies and peaked at an
absolute magnitude of I~-13. Here we present Hubble Space Telescope images of
M85 OT 2006-1 an... | astro-ph | m85 optical transient 20061 m85 ot 20061 is the most luminous member of the small family of v838 monlike objects whose nature is still a mystery this event took place in the virgo cluster of galaxies and peaked at an absolute magnitude of i13 here we present hubble space telescope images of m85 ot 20061 and its environ... | [['m85', 'optical', 'transient', '20061', 'm85', 'ot', '20061', 'is', 'the', 'most', 'luminous', 'member', 'of', 'the', 'small', 'family', 'of', 'v838', 'monlike', 'objects', 'whose', 'nature', 'is', 'still', 'a', 'mystery', 'this', 'event', 'took', 'place', 'in', 'the', 'virgo', 'cluster', 'of', 'galaxies', 'and', 'pe... | [-0.048524642558933226, 0.11070051959122632, -0.07909316637355472, 0.11033047012679806, -0.12663696288436124, -0.0824120173204239, 0.06816933181011159, 0.4222067016284023, -0.1419001079346795, -0.3798270555670513, 0.09209272327041665, -0.2841908806250884, -0.05626000906546823, 0.21766222792017142, -0.11059540914141354,... |
710.3193 | On the effects of conformal degrees of freedom inside a neutron star | In this paper a neutron star with an inner core which undergoes a phase
transition, which is characterized by conformal degrees of freedom on the phase
boundary, is considered. Typical cases of such a phase transition are e.g.
quantum Hall effect, superconductivity and superfluidity. Assuming the
mechanical stability... | gr-qc astro-ph cond-mat.stat-mech hep-ph hep-th | in this paper a neutron star with an inner core which undergoes a phase transition which is characterized by conformal degrees of freedom on the phase boundary is considered typical cases of such a phase transition are eg quantum hall effect superconductivity and superfluidity assuming the mechanical stability of this ... | [['in', 'this', 'paper', 'a', 'neutron', 'star', 'with', 'an', 'inner', 'core', 'which', 'undergoes', 'a', 'phase', 'transition', 'which', 'is', 'characterized', 'by', 'conformal', 'degrees', 'of', 'freedom', 'on', 'the', 'phase', 'boundary', 'is', 'considered', 'typical', 'cases', 'of', 'such', 'a', 'phase', 'transiti... | [-0.1695284044657378, 0.2089240631331972, -0.10816662607991949, 0.01047760390706281, -0.06583886631922994, -0.08523141639703449, 0.057750582319258295, 0.3005053847433722, -0.2565135537844865, -0.28375398251921574, 0.12742080046210755, -0.2369276907948896, -0.10722480773866336, 0.13342084915456462, -0.03256182412597093,... |
710.3194 | On a classification of the gradient shrinking solitons | The main purpose of this article is to provide an alternate proof to a result
of Perelman on gradient shrinking solitons. In dimension three we also
generalize the result by removing the $\kappa$-non-collapsing assumption. In
high dimension this new method allows us to prove a classification result on
gradient shrink... | math.DG math.AP | the main purpose of this article is to provide an alternate proof to a result of perelman on gradient shrinking solitons in dimension three we also generalize the result by removing the kappanoncollapsing assumption in high dimension this new method allows us to prove a classification result on gradient shrinking solit... | [['the', 'main', 'purpose', 'of', 'this', 'article', 'is', 'to', 'provide', 'an', 'alternate', 'proof', 'to', 'a', 'result', 'of', 'perelman', 'on', 'gradient', 'shrinking', 'solitons', 'in', 'dimension', 'three', 'we', 'also', 'generalize', 'the', 'result', 'by', 'removing', 'the', 'kappanoncollapsing', 'assumption', ... | [-0.13947884630291693, 0.06998939320446, -0.1257047840251377, 0.037047335117559636, -0.11730769473398404, -0.12896166569102677, -0.025301593641239788, 0.33610638729747266, -0.22911746433425334, -0.2183939664654674, 0.10741419030068021, -0.22998209274021886, -0.15105719993551892, 0.16077147184630797, -0.1484770783854107... |
710.3195 | On 4-dimensional gradient shrinking solitons | In this paper we classify the four dimensional gradient shrinking solitons
under certain curvature conditions satisfied by all solitons arising from
finite time singularities of Ricci flow on compact four manifolds with positive
isotropic curvature. As a corollary we generalize a result of Perelman on three
dimension... | math.DG math.AP | in this paper we classify the four dimensional gradient shrinking solitons under certain curvature conditions satisfied by all solitons arising from finite time singularities of ricci flow on compact four manifolds with positive isotropic curvature as a corollary we generalize a result of perelman on three dimensional ... | [['in', 'this', 'paper', 'we', 'classify', 'the', 'four', 'dimensional', 'gradient', 'shrinking', 'solitons', 'under', 'certain', 'curvature', 'conditions', 'satisfied', 'by', 'all', 'solitons', 'arising', 'from', 'finite', 'time', 'singularities', 'of', 'ricci', 'flow', 'on', 'compact', 'four', 'manifolds', 'with', 'p... | [-0.2172470167630686, 0.12268114560898745, -0.08103259687997261, 0.05912930150033098, -0.08886619999495177, -0.16558343778311643, -0.10645305004875825, 0.3793913459159293, -0.21497984905287904, -0.15295784020761274, 0.1912209016319259, -0.27102267917878226, -0.14180531510907524, 0.18092176482907302, -0.0938933561643901... |
710.3196 | Simulation of Grover's quantum search algorithm in a Ising nuclear spin
chain quantum computer with first and second nearest neighbour couplings | We implement Grover's quantum search algorithm on a nuclear spin chain
quantum computer, taking into Ising type interactions between nearest and
second nearest neighbours into account. The performance of the realisation of
the algorithm is studied by numerical simulations with four spins. We determine
the temporal be... | quant-ph | we implement grovers quantum search algorithm on a nuclear spin chain quantum computer taking into ising type interactions between nearest and second nearest neighbours into account the performance of the realisation of the algorithm is studied by numerical simulations with four spins we determine the temporal behaviou... | [['we', 'implement', 'grovers', 'quantum', 'search', 'algorithm', 'on', 'a', 'nuclear', 'spin', 'chain', 'quantum', 'computer', 'taking', 'into', 'ising', 'type', 'interactions', 'between', 'nearest', 'and', 'second', 'nearest', 'neighbours', 'into', 'account', 'the', 'performance', 'of', 'the', 'realisation', 'of', 't... | [-0.1447664139034984, 0.10790323547937059, -0.02924523453591494, 0.0793484678801538, -0.023805619309564215, -0.15159397295440782, 0.07686465507332277, 0.3984040707800087, -0.23644786701629777, -0.29396568604931744, 0.06198724181196847, -0.25932503092501846, -0.11484148887569433, 0.17494783780517076, 0.08768254348619299... |
710.3197 | Orientational relaxation in a dispersive dynamic medium : Generalization
of the Kubo-Ivanov-Anderson jump diffusion model to include fractional
environmental dynamics | Ivanov-Anderson (IA) model (and an earlier treatment by Kubo) envisages a
decay of the orientational correlation by random but large amplitude molecular
jumps, as opposed to infinitesimal small jumps assumed in Brownian diffusion.
Recent computer simulation studies on water and supercooled liquids have shown
that lar... | cond-mat.soft | ivanovanderson ia model and an earlier treatment by kubo envisages a decay of the orientational correlation by random but large amplitude molecular jumps as opposed to infinitesimal small jumps assumed in brownian diffusion recent computer simulation studies on water and supercooled liquids have shown that large amplit... | [['ivanovanderson', 'ia', 'model', 'and', 'an', 'earlier', 'treatment', 'by', 'kubo', 'envisages', 'a', 'decay', 'of', 'the', 'orientational', 'correlation', 'by', 'random', 'but', 'large', 'amplitude', 'molecular', 'jumps', 'as', 'opposed', 'to', 'infinitesimal', 'small', 'jumps', 'assumed', 'in', 'brownian', 'diffusi... | [-0.12910569220604465, 0.2012432085285372, -0.12139290747179005, 0.11631669324672728, -0.056368562067571196, -0.1659681529361898, 0.03778715175520539, 0.3602079893395197, -0.28450098807493657, -0.2678990691156986, 0.07135844229364571, -0.2716238796016954, -0.11181527747808453, 0.17943020472459745, 0.002178526557355116,... |
710.3198 | Equation of State and Transport Coefficients of Relativistic Nuclear
Matter | In order to evaluate qualitatively the space-time evolution of hot and dense
nuclear matter the underlying equation of state and transport coefficients must
be known. In this study a specific equation of state is studied: the pion gas.
The classical or standard transport coefficients, namely the bulk viscosity,
shear... | nucl-th | in order to evaluate qualitatively the spacetime evolution of hot and dense nuclear matter the underlying equation of state and transport coefficients must be known in this study a specific equation of state is studied the pion gas the classical or standard transport coefficients namely the bulk viscosity shear viscsoi... | [['in', 'order', 'to', 'evaluate', 'qualitatively', 'the', 'spacetime', 'evolution', 'of', 'hot', 'and', 'dense', 'nuclear', 'matter', 'the', 'underlying', 'equation', 'of', 'state', 'and', 'transport', 'coefficients', 'must', 'be', 'known', 'in', 'this', 'study', 'a', 'specific', 'equation', 'of', 'state', 'is', 'stud... | [-0.1038945549851832, 0.18610690569039434, -0.08166941357393788, 0.047548498058921265, -0.020494724030619207, -0.06885513163822359, -0.022901596080460777, 0.3032540916784169, -0.2958272575107339, -0.25656946303246364, 0.10415493931512872, -0.2749622831605885, -0.04008261721632252, 0.141442418197323, 0.03710859381172755... |
710.3199 | Pion dominance in RPV SUSY induced neutrinoless double beta decay | At the quark level there are basically two types of contributions of R-parity
violating SUSY (RPV SUSY) to neutrinoless double beta decay: the short-range
contribution involving only heavy virtual superpartners and the long-range one
with the virtual squark and neutrino. Hadronization of the effective operators,
corr... | hep-ph | at the quark level there are basically two types of contributions of rparity violating susy rpv susy to neutrinoless double beta decay the shortrange contribution involving only heavy virtual superpartners and the longrange one with the virtual squark and neutrino hadronization of the effective operators corresponding ... | [['at', 'the', 'quark', 'level', 'there', 'are', 'basically', 'two', 'types', 'of', 'contributions', 'of', 'rparity', 'violating', 'susy', 'rpv', 'susy', 'to', 'neutrinoless', 'double', 'beta', 'decay', 'the', 'shortrange', 'contribution', 'involving', 'only', 'heavy', 'virtual', 'superpartners', 'and', 'the', 'longran... | [-0.08798933345302619, 0.36866258870276364, -0.007925686085243421, 0.24310701407275387, -0.053563131740043776, -0.16753602541726212, 0.03774766585141559, 0.28233393653424393, -0.23543220358611694, -0.23830286035884235, -0.06919993626672358, -0.3502113700940691, -0.05107853017391884, 0.09967628927853216, 0.1069197384841... |
710.32 | Ultrafast response of surface electromagnetic waves in an aluminum film
perforated with subwavelength hole arrays | The ultrafast dynamics of surface electromagnetic waves photogenerated on
aluminum film perforated with subwavelength holes array was studied in the
visible spectral range by the technique of transient photomodulation with 100
fs time resolution. We observed a pronounced blueshift of the resonant
transmission band th... | cond-mat.mtrl-sci cond-mat.mes-hall | the ultrafast dynamics of surface electromagnetic waves photogenerated on aluminum film perforated with subwavelength holes array was studied in the visible spectral range by the technique of transient photomodulation with 100 fs time resolution we observed a pronounced blueshift of the resonant transmission band that ... | [['the', 'ultrafast', 'dynamics', 'of', 'surface', 'electromagnetic', 'waves', 'photogenerated', 'on', 'aluminum', 'film', 'perforated', 'with', 'subwavelength', 'holes', 'array', 'was', 'studied', 'in', 'the', 'visible', 'spectral', 'range', 'by', 'the', 'technique', 'of', 'transient', 'photomodulation', 'with', '100'... | [-0.16859628830461929, 0.1623687355694248, -0.0425203472166975, 0.02929088115261293, -0.015636403670656347, -0.1271074593772189, 0.021603836509329486, 0.4527828388403509, -0.24961358717877732, -0.3022147963720017, 0.009557219066604903, -0.3085927859766879, -0.13082119845132403, 0.19589153328196746, 0.04933599098672586,... |
710.3201 | Energy-dependent Lorentz covariant parameterization of the NN
interaction between 50 and 200 MeV | For laboratory kinetic energies between 50 and 200 MeV, we focus on
generating an energy-dependent Lorentz covariant parameterization of the
on-shell nucleon-nucleon (NN) scattering amplitudes in terms of a number of
Yukawa-type meson exchanges in first-order Born approximation. This
parameterization provides a good ... | nucl-th | for laboratory kinetic energies between 50 and 200 mev we focus on generating an energydependent lorentz covariant parameterization of the onshell nucleonnucleon nn scattering amplitudes in terms of a number of yukawatype meson exchanges in firstorder born approximation this parameterization provides a good description... | [['for', 'laboratory', 'kinetic', 'energies', 'between', '50', 'and', '200', 'mev', 'we', 'focus', 'on', 'generating', 'an', 'energydependent', 'lorentz', 'covariant', 'parameterization', 'of', 'the', 'onshell', 'nucleonnucleon', 'nn', 'scattering', 'amplitudes', 'in', 'terms', 'of', 'a', 'number', 'of', 'yukawatype', ... | [-0.11514452533006217, 0.24192793402934595, -0.09654940621729827, 0.16453855396354233, -0.021697461757646648, -0.05848636545389044, 0.059399042701856655, 0.3680721241980791, -0.18690951107154516, -0.3605012665784946, -0.13313677903285928, -0.3164684101233654, -0.005249371244148774, 0.18615231352547804, 0.12959867324256... |
710.3202 | The Eccentric Accretion Disc of the Black Hole A0620-00 | We present spectroscopic observations of the quiescent black hole binary
A0620-00 with the the 6.5-m Magellan Clay telescope at Las Campanas
Observatory. We measure absorption-line radial velocities of the secondary and
make the most precise determination to date (K2 = 435.4 +/- 0.5 km/s). By
fitting the rotational b... | astro-ph | we present spectroscopic observations of the quiescent black hole binary a062000 with the the 65m magellan clay telescope at las campanas observatory we measure absorptionline radial velocities of the secondary and make the most precise determination to date k2 4354 05 kms by fitting the rotational broadening of the se... | [['we', 'present', 'spectroscopic', 'observations', 'of', 'the', 'quiescent', 'black', 'hole', 'binary', 'a062000', 'with', 'the', 'the', '65m', 'magellan', 'clay', 'telescope', 'at', 'las', 'campanas', 'observatory', 'we', 'measure', 'absorptionline', 'radial', 'velocities', 'of', 'the', 'secondary', 'and', 'make', 't... | [-0.11095109518273465, 0.10710013204505064, -0.059552937411575524, 0.0753346942908835, -0.09659667997171885, -0.10786301856104115, 0.04751361965740733, 0.4258835026226125, -0.16791195335010833, -0.356708515217991, 0.07384103324458116, -0.2995141320554587, -0.045165203965557406, 0.20112278698919916, -0.07033001906640336... |
710.3203 | Non-Relativistic Superstring Theories | We construct a supersymmetric version of the ``critical'' non-relativistic
bosonic string theory\cite{Kim:2007hb} with its manifest global symmetry. We
introduce the anticommuting $bc$ CFT which is the super partner of the
$\beta\gamma$ CFT. The conformal weights of the $b$ and $c$ fields are both
1/2. The action of ... | hep-th | we construct a supersymmetric version of the critical nonrelativistic bosonic string theorycitekim2007hb with its manifest global symmetry we introduce the anticommuting bc cft which is the super partner of the betagamma cft the conformal weights of the b and c fields are both 12 the action of the fermionic sector can ... | [['we', 'construct', 'a', 'supersymmetric', 'version', 'of', 'the', 'critical', 'nonrelativistic', 'bosonic', 'string', 'theorycitekim2007hb', 'with', 'its', 'manifest', 'global', 'symmetry', 'we', 'introduce', 'the', 'anticommuting', 'bc', 'cft', 'which', 'is', 'the', 'super', 'partner', 'of', 'the', 'betagamma', 'cft... | [-0.14289032787029796, 0.2100546007115875, -0.07206350874142065, 0.11116222939659458, -0.08146126597078845, -0.19492797050214208, -0.02337672101052971, 0.29823091390597467, -0.19512265871419324, -0.20339906907311694, 0.05294683238710551, -0.3045730575617841, -0.1943243774414227, 0.07139419000732768, -0.0346973610897240... |
710.3204 | Computational Model for Electron-Nucleon Scattering and Weak Charge of
the Nucleon | We show how computational symbolic packages such as FeynArts and FormCalc can
be adopted for the evaluation of one-loop hadronic electroweak radiative
corrections for electron-nucleon scattering and applied to calculations of the
nucleon weak charge. Several numerical results are listed, and found to be in
good agree... | physics.comp-ph nucl-ex nucl-th | we show how computational symbolic packages such as feynarts and formcalc can be adopted for the evaluation of oneloop hadronic electroweak radiative corrections for electronnucleon scattering and applied to calculations of the nucleon weak charge several numerical results are listed and found to be in good agreement w... | [['we', 'show', 'how', 'computational', 'symbolic', 'packages', 'such', 'as', 'feynarts', 'and', 'formcalc', 'can', 'be', 'adopted', 'for', 'the', 'evaluation', 'of', 'oneloop', 'hadronic', 'electroweak', 'radiative', 'corrections', 'for', 'electronnucleon', 'scattering', 'and', 'applied', 'to', 'calculations', 'of', '... | [-0.0210217561510105, 0.09980243099674296, -0.04941522137960419, 0.17742637371142897, -0.05843104500896656, -0.0987857853134091, 0.0025996272634074558, 0.39557132440117687, -0.20360624856458834, -0.31587400790662146, 0.04794748974381946, -0.3193590513502176, -0.05962547688530041, 0.2572133940993808, 0.06113632042140055... |
710.3205 | SU(1,1) symmetry of multimode squeezed states | We show that a class of multimode optical transformations that employ linear
optics plus two-mode squeezing can be expressed as SU(1,1) operators. These
operations are relevant to state-of-the-art continuous variable quantum
information experiments including quantum state sharing, quantum teleportation,
and multipart... | quant-ph | we show that a class of multimode optical transformations that employ linear optics plus twomode squeezing can be expressed as su11 operators these operations are relevant to stateoftheart continuous variable quantum information experiments including quantum state sharing quantum teleportation and multipartite entangle... | [['we', 'show', 'that', 'a', 'class', 'of', 'multimode', 'optical', 'transformations', 'that', 'employ', 'linear', 'optics', 'plus', 'twomode', 'squeezing', 'can', 'be', 'expressed', 'as', 'su11', 'operators', 'these', 'operations', 'are', 'relevant', 'to', 'stateoftheart', 'continuous', 'variable', 'quantum', 'informa... | [-0.11420031715236718, 0.1445759986907396, -0.10106989807907815, 0.062010209695008416, -0.05538112363464446, -0.1761191472582215, 0.04879013860446154, 0.3976187483996761, -0.29338772280844955, -0.20284892071266564, 0.09727841409811826, -0.22852824349906675, -0.18759929417271395, 0.2218666248384635, -0.07154738384403517... |
710.3206 | Generalized Jacquet modules of parabolic induction | In this paper we study a generalization of the Jacquet module of a parabolic
induction and construct a filtration on it. The successive quotient of the
filtration is written by using the twisting functor.
| math.RT | in this paper we study a generalization of the jacquet module of a parabolic induction and construct a filtration on it the successive quotient of the filtration is written by using the twisting functor | [['in', 'this', 'paper', 'we', 'study', 'a', 'generalization', 'of', 'the', 'jacquet', 'module', 'of', 'a', 'parabolic', 'induction', 'and', 'construct', 'a', 'filtration', 'on', 'it', 'the', 'successive', 'quotient', 'of', 'the', 'filtration', 'is', 'written', 'by', 'using', 'the', 'twisting', 'functor']] | [-0.160080158699523, 0.014697225737001966, -0.13767894023262403, 0.005679453449214206, -0.09515506702968303, -0.052926084478659666, -0.012473935340120293, 0.3139080307720339, -0.45219004570561294, -0.174691310919383, 0.11993618409820449, -0.156661945848849, -0.2027337603709277, 0.20305350883042111, -0.19360761582741842... |
710.3207 | Extracting the Gluon Piece of the Spin Puzzle: New Inclusive Jet Results
from STAR | This contribution presents the most recent mid-rapidity inclusive jet results
from 3 pb^-1 of data collected from longitudinally polarized proton collisions
at sqrt(s)=200 GeV during the 2005 RHIC run. The inclusive jet asymmetry, a_LL,
with it's increased transverse momentum range and precision, provides strong
cons... | hep-ex | this contribution presents the most recent midrapidity inclusive jet results from 3 pb1 of data collected from longitudinally polarized proton collisions at sqrts200 gev during the 2005 rhic run the inclusive jet asymmetry a_ll with its increased transverse momentum range and precision provides strong constraints on th... | [['this', 'contribution', 'presents', 'the', 'most', 'recent', 'midrapidity', 'inclusive', 'jet', 'results', 'from', '3', 'pb1', 'of', 'data', 'collected', 'from', 'longitudinally', 'polarized', 'proton', 'collisions', 'at', 'sqrts200', 'gev', 'during', 'the', '2005', 'rhic', 'run', 'the', 'inclusive', 'jet', 'asymmetr... | [-0.03007997274083101, 0.22466797373746916, -0.18454161723602122, 0.10106232852114648, -0.06156255408995232, -0.051421922105719664, -0.07001704691072642, 0.3808831941273253, -0.15492694694114753, -0.3063911497592926, -0.09574833878521193, -0.4032960587291647, 0.2299414779675209, 0.15452939158273957, 0.10532913285986346... |
710.3208 | The Large Vector Multiplet Action | We discuss possible actions for the d=2, N=(2,2) large vector multiplet that
gauges isometries of generalized Kahler geometries. We explore two scenarios
that allow us to write kinetic and superpotential terms for the scalar
field-strengths, and write kinetic terms for the spinor invariants that can
introduce topolog... | hep-th | we discuss possible actions for the d2 n22 large vector multiplet that gauges isometries of generalized kahler geometries we explore two scenarios that allow us to write kinetic and superpotential terms for the scalar fieldstrengths and write kinetic terms for the spinor invariants that can introduce topological terms ... | [['we', 'discuss', 'possible', 'actions', 'for', 'the', 'd2', 'n22', 'large', 'vector', 'multiplet', 'that', 'gauges', 'isometries', 'of', 'generalized', 'kahler', 'geometries', 'we', 'explore', 'two', 'scenarios', 'that', 'allow', 'us', 'to', 'write', 'kinetic', 'and', 'superpotential', 'terms', 'for', 'the', 'scalar'... | [-0.16719569857506192, 0.16153576345566442, 0.003993047310002879, 0.14294329499962793, -0.15185949823581704, -0.176360875989, -0.03715715067935925, 0.31844686152066526, -0.18714418431045488, -0.2596564854623056, 0.04654820108165344, -0.2260202422153716, -0.1992705944633367, 0.09858798257568303, -0.028540266677737236, -... |
710.3209 | Chaotic scattering in solitary wave interactions: A singular
iterated-map description | We derive a family of singular iterated maps--closely related to Poincare
maps--that describe chaotic interactions between colliding solitary waves. The
chaotic behavior of such solitary wave collisions depends on the transfer of
energy to a secondary mode of oscillation, often an internal mode of the pulse.
Unlike p... | nlin.PS nlin.CD | we derive a family of singular iterated mapsclosely related to poincare mapsthat describe chaotic interactions between colliding solitary waves the chaotic behavior of such solitary wave collisions depends on the transfer of energy to a secondary mode of oscillation often an internal mode of the pulse unlike previous a... | [['we', 'derive', 'a', 'family', 'of', 'singular', 'iterated', 'mapsclosely', 'related', 'to', 'poincare', 'mapsthat', 'describe', 'chaotic', 'interactions', 'between', 'colliding', 'solitary', 'waves', 'the', 'chaotic', 'behavior', 'of', 'such', 'solitary', 'wave', 'collisions', 'depends', 'on', 'the', 'transfer', 'of... | [-0.18983532905046901, 0.1076013614987692, -0.15257108763127805, 0.09147419397395554, -0.09818031744542696, -0.12477678102763132, -0.009150594378762106, 0.29066974236398724, -0.28279375707968435, -0.23276900212075693, 0.07738373349569341, -0.29603427870992527, -0.1667598750151641, 0.21087303722164996, -0.03986167119393... |
710.321 | Entanglement, Invariants, and Phylogenetics | This thesis develops and expands upon known techniques of mathematical
physics relevant to the analysis of the popular Markov model of phylogenetic
trees required in biology to reconstruct the evolutionary relationships of
taxonomic units from biomolecular sequence data. The techniques of mathematical
physics are ple... | q-bio.QM q-bio.PE | this thesis develops and expands upon known techniques of mathematical physics relevant to the analysis of the popular markov model of phylogenetic trees required in biology to reconstruct the evolutionary relationships of taxonomic units from biomolecular sequence data the techniques of mathematical physics are pletho... | [['this', 'thesis', 'develops', 'and', 'expands', 'upon', 'known', 'techniques', 'of', 'mathematical', 'physics', 'relevant', 'to', 'the', 'analysis', 'of', 'the', 'popular', 'markov', 'model', 'of', 'phylogenetic', 'trees', 'required', 'in', 'biology', 'to', 'reconstruct', 'the', 'evolutionary', 'relationships', 'of',... | [-0.0527917031225786, 0.07474014849110679, -0.13594629805572708, 0.07236174797329875, -0.10028651547194882, -0.0977082175197964, 0.034692377745140945, 0.33022665408806817, -0.298374958473935, -0.31425656239746724, 0.11287798016094555, -0.21670037639477865, -0.16838948158876538, 0.19994864249166872, -0.06331405879910847... |
710.3211 | Universal Scaling in Non-equilibrium Transport Through a Single-Channel
Kondo Dot | Scaling laws and universality play an important role in our understanding of
critical phenomena and the Kondo effect. Here we present measurements of
non-equilibrium transport through a single-channel Kondo quantum dot at low
temperature and bias. We find that the low-energy Kondo conductance is
consistent with unive... | cond-mat.mes-hall | scaling laws and universality play an important role in our understanding of critical phenomena and the kondo effect here we present measurements of nonequilibrium transport through a singlechannel kondo quantum dot at low temperature and bias we find that the lowenergy kondo conductance is consistent with universality... | [['scaling', 'laws', 'and', 'universality', 'play', 'an', 'important', 'role', 'in', 'our', 'understanding', 'of', 'critical', 'phenomena', 'and', 'the', 'kondo', 'effect', 'here', 'we', 'present', 'measurements', 'of', 'nonequilibrium', 'transport', 'through', 'a', 'singlechannel', 'kondo', 'quantum', 'dot', 'at', 'lo... | [-0.15203435345334404, 0.23010578238348517, -0.11447850328203245, 0.0869085383615859, 0.016019711793360106, -0.24295233733331165, 0.08972428854336434, 0.28039620936572274, -0.26427487451813103, -0.31097511538695316, -0.021495707708203957, -0.3188523772448577, -0.16071257015322277, 0.22841223551213374, 0.060711346917360... |
710.3212 | Analytic derivation of the leading-order gluon distribution function
G(x,Q^2) = xg(x,Q^2) from the proton structure function F_2^p(x,Q^2) | We derive a second-order linear differential equation for the leading order
gluon distribution function G(x,Q^2) = xg(x,Q^2) which determines G(x,Q^2)
directly from the proton structure function F_2^p(x,Q^2). This equation is
derived from the leading order DGLAP evolution equation for F_2^p(x,Q^2), and
does not requi... | hep-ph | we derive a secondorder linear differential equation for the leading order gluon distribution function gxq2 xgxq2 which determines gxq2 directly from the proton structure function f_2pxq2 this equation is derived from the leading order dglap evolution equation for f_2pxq2 and does not require knowledge of either the in... | [['we', 'derive', 'a', 'secondorder', 'linear', 'differential', 'equation', 'for', 'the', 'leading', 'order', 'gluon', 'distribution', 'function', 'gxq2', 'xgxq2', 'which', 'determines', 'gxq2', 'directly', 'from', 'the', 'proton', 'structure', 'function', 'f_2pxq2', 'this', 'equation', 'is', 'derived', 'from', 'the', ... | [-0.048368053481871495, 0.1024842980460247, -0.1487278504680623, 0.11502421740214248, -0.09549870602543058, -0.08673680662078588, 0.016263288007501292, 0.3335528375422643, -0.19536194083086075, -0.2813225812324341, 0.0050988742675376585, -0.26796594904005233, -0.047813930658294874, 0.13803656327422537, 0.01698102095937... |
710.3213 | Latest Results on Bottom Spectroscopy and Production with CDF | Using data collected with the CDF Run II detector, new measurements on bottom
production cross-sections are presented. The latest achievements in bottom
hadron spectroscopy are discussed. The results are based on a large sample of
semileptonic and hadronic decays of bottom states made available by triggers
based on t... | hep-ex | using data collected with the cdf run ii detector new measurements on bottom production crosssections are presented the latest achievements in bottom hadron spectroscopy are discussed the results are based on a large sample of semileptonic and hadronic decays of bottom states made available by triggers based on the pre... | [['using', 'data', 'collected', 'with', 'the', 'cdf', 'run', 'ii', 'detector', 'new', 'measurements', 'on', 'bottom', 'production', 'crosssections', 'are', 'presented', 'the', 'latest', 'achievements', 'in', 'bottom', 'hadron', 'spectroscopy', 'are', 'discussed', 'the', 'results', 'are', 'based', 'on', 'a', 'large', 's... | [-0.020182138796509156, 0.1747877853922546, -0.05774044055702551, 0.04187398874815905, -0.07007813727799451, -0.1597750302940115, 0.04867352683422208, 0.308221823307422, -0.13813684004763105, -0.2916378954530887, 0.07944585615549377, -0.4373668211705561, 0.07305167970370571, 0.22626115995424115, 0.0677646977908224, 0.1... |
710.3214 | Chemical Functionalization of Graphene Nanoribbons by Carboxyl Groups on
Stone-Wales Defects | Using the density functional theory, we have demonstrated the chemical
functionalization of semiconducting graphene nanoribbons (GNRs) with
Stone-Wales (SW) defects by carboxyl (COOH) groups. It is found that the
geometrical structures and electronic properties of the GNRs changed
significantly, and the electrical co... | cond-mat.mtrl-sci | using the density functional theory we have demonstrated the chemical functionalization of semiconducting graphene nanoribbons gnrs with stonewales sw defects by carboxyl cooh groups it is found that the geometrical structures and electronic properties of the gnrs changed significantly and the electrical conductivity o... | [['using', 'the', 'density', 'functional', 'theory', 'we', 'have', 'demonstrated', 'the', 'chemical', 'functionalization', 'of', 'semiconducting', 'graphene', 'nanoribbons', 'gnrs', 'with', 'stonewales', 'sw', 'defects', 'by', 'carboxyl', 'cooh', 'groups', 'it', 'is', 'found', 'that', 'the', 'geometrical', 'structures'... | [-0.15336349131265545, 0.1437409390129295, -0.054131850823942645, -0.08068536254851257, -0.0021292942909377755, -0.18059082951524533, 0.1008602720719543, 0.4561000684933627, -0.26818093742408294, -0.29739659579069005, -0.01890071849886547, -0.3156132187109952, -0.20804438779276668, 0.1547143801352849, 0.009378921909385... |
710.3215 | A model for a plasma ball | A detailed simple model is applied to study a high temperature plasma ball.
It is assumed that the ions and delocalized electrons are distributed randomly
throughout the charged plasma ball (extra/missing charge is assumed to be found
in a thin layer on the surface of a ball). The energy of the microscopic
electrosta... | physics.plasm-ph physics.space-ph | a detailed simple model is applied to study a high temperature plasma ball it is assumed that the ions and delocalized electrons are distributed randomly throughout the charged plasma ball extramissing charge is assumed to be found in a thin layer on the surface of a ball the energy of the microscopic electrostatic fie... | [['a', 'detailed', 'simple', 'model', 'is', 'applied', 'to', 'study', 'a', 'high', 'temperature', 'plasma', 'ball', 'it', 'is', 'assumed', 'that', 'the', 'ions', 'and', 'delocalized', 'electrons', 'are', 'distributed', 'randomly', 'throughout', 'the', 'charged', 'plasma', 'ball', 'extramissing', 'charge', 'is', 'assume... | [-0.08704256871358815, 0.2257008435246499, -0.07904750381938505, 0.059273789737763226, 0.03468149074600363, -0.1473108316505594, 0.0018342878403408186, 0.384649645765217, -0.25339816546789845, -0.24341419120604285, 0.042224770038844825, -0.2755553205212464, -0.008513948975168929, 0.13497998053089202, -0.036580462008714... |
710.3216 | Knot homology via derived categories of coherent sheaves II, sl(m) case | Using derived categories of equivariant coherent sheaves we construct a knot
homology theory which categorifies the quantum sl(m) knot polynomial. Our knot
homology naturally satisfies the categorified MOY relations and is
conjecturally isomorphic to Khovanov-Rozansky homology. Our construction is
motivated by the ge... | math.AG math.QA | using derived categories of equivariant coherent sheaves we construct a knot homology theory which categorifies the quantum slm knot polynomial our knot homology naturally satisfies the categorified moy relations and is conjecturally isomorphic to khovanovrozansky homology our construction is motivated by the geometric... | [['using', 'derived', 'categories', 'of', 'equivariant', 'coherent', 'sheaves', 'we', 'construct', 'a', 'knot', 'homology', 'theory', 'which', 'categorifies', 'the', 'quantum', 'slm', 'knot', 'polynomial', 'our', 'knot', 'homology', 'naturally', 'satisfies', 'the', 'categorified', 'moy', 'relations', 'and', 'is', 'conj... | [-0.2483622260408959, 0.052115051748438015, -0.21891017197803767, 0.1518625154588975, -0.1604851079000919, -0.24932745201685638, -0.0692563121254487, 0.307505880534235, -0.45125316083431244, -0.23206720193330613, 0.05896762406660451, -0.1341629542444867, -0.2699530627492263, 0.14768568443617336, -0.3266738303333383, -0... |
710.3217 | A natural prime-generating recurrence | For the sequence defined by a(n) = a(n-1) + gcd(n, a(n-1)) with a(1) = 7 we
prove that a(n) - a(n-1) takes on only 1s and primes, making this recurrence a
rare "naturally occurring" generator of primes. Toward a generalization of this
result to an arbitrary initial condition, we also study the limiting behavior
of a(... | math.NT | for the sequence defined by an an1 gcdn an1 with a1 7 we prove that an an1 takes on only 1s and primes making this recurrence a rare naturally occurring generator of primes toward a generalization of this result to an arbitrary initial condition we also study the limiting behavior of ann and a transience property of th... | [['for', 'the', 'sequence', 'defined', 'by', 'an', 'an1', 'gcdn', 'an1', 'with', 'a1', '7', 'we', 'prove', 'that', 'an', 'an1', 'takes', 'on', 'only', '1s', 'and', 'primes', 'making', 'this', 'recurrence', 'a', 'rare', 'naturally', 'occurring', 'generator', 'of', 'primes', 'toward', 'a', 'generalization', 'of', 'this',... | [-0.17762682781854677, 0.11109895238497934, -0.0904207003886922, 0.08593793765452327, -0.005615909299734286, -0.11057601090110207, 0.03256311872382096, 0.32395498870114275, -0.28806511381388467, -0.21534788657879553, 0.08408284681391413, -0.23869540422397145, -0.153297781525969, 0.15620993139316974, -0.0842063361936706... |
710.3218 | Representations of Temperley--Lieb Algebras | We define a commuting family of operators $T_0,T_1,...,T_n$ in the
Temperley--Lieb algebra $\mathcal{A}_n(x)$ of type $A_{n-1}$. Using an
appropriate analogue to Murphy basis of the Iwahori--Hecke algebra of the
symmetric group, we describe the eigenvalues arising from the triangular action
of the said operators on t... | math.RT | we define a commuting family of operators t_0t_1t_n in the temperleylieb algebra mathcala_nx of type a_n1 using an appropriate analogue to murphy basis of the iwahorihecke algebra of the symmetric group we describe the eigenvalues arising from the triangular action of the said operators on the cell modules of mathcala_... | [['we', 'define', 'a', 'commuting', 'family', 'of', 'operators', 't_0t_1t_n', 'in', 'the', 'temperleylieb', 'algebra', 'mathcala_nx', 'of', 'type', 'a_n1', 'using', 'an', 'appropriate', 'analogue', 'to', 'murphy', 'basis', 'of', 'the', 'iwahorihecke', 'algebra', 'of', 'the', 'symmetric', 'group', 'we', 'describe', 'the... | [-0.13123443003511057, 0.06723840122799932, -0.026155143169065316, 0.03957468912005425, -0.10633026339734594, -0.12007587884242336, -0.027203740316132704, 0.3256613976260026, -0.31112386994063856, -0.1570023809125026, 0.1552866667183116, -0.26472249982878565, -0.1726441008100907, 0.1803131130213539, -0.1121384023999174... |
710.3219 | On some explicit evaluations of multiple zeta-star values | In this paper, we give some explicit evaluations of multiple zeta-star values
which are rational multiple of powers of $\pi^2$.
| math.NT | in this paper we give some explicit evaluations of multiple zetastar values which are rational multiple of powers of pi2 | [['in', 'this', 'paper', 'we', 'give', 'some', 'explicit', 'evaluations', 'of', 'multiple', 'zetastar', 'values', 'which', 'are', 'rational', 'multiple', 'of', 'powers', 'of', 'pi2']] | [-0.30368525004014374, 0.08500369158573448, -0.03736378841567785, 0.000576544419163838, -0.10293638436123728, -0.12899691369384528, 0.0658386149967555, 0.3734807984903455, -0.23951989486813546, -0.25755937343928964, 0.07852196758030913, -0.22573352616745979, -0.2035336741246283, 0.259936149418354, -0.05267648990266025,... |
710.322 | Violation of an inequality in an experimental test of Leggett's
non-local hidden variable theory | I impose previously neglected symmetry conditions in Leggett's non-local
hidden variable theory that are required by the conditions in a recent
experimental test of this theory. These conditions lead to an inequality for
the polarization correlation function that has a maximal violation from the
quantum predictions t... | quant-ph | i impose previously neglected symmetry conditions in leggetts nonlocal hidden variable theory that are required by the conditions in a recent experimental test of this theory these conditions lead to an inequality for the polarization correlation function that has a maximal violation from the quantum predictions that i... | [['i', 'impose', 'previously', 'neglected', 'symmetry', 'conditions', 'in', 'leggetts', 'nonlocal', 'hidden', 'variable', 'theory', 'that', 'are', 'required', 'by', 'the', 'conditions', 'in', 'a', 'recent', 'experimental', 'test', 'of', 'this', 'theory', 'these', 'conditions', 'lead', 'to', 'an', 'inequality', 'for', '... | [-0.09831154794287082, 0.18068374490970898, -0.10838158952689113, 0.09870584752235272, -0.050309209020010064, -0.1773940020349699, 0.004885182070376521, 0.33516838994215836, -0.21640581915808188, -0.3001363407578561, 0.07296386189220545, -0.2668679439789289, -0.16277276588507095, 0.17668269775118436, -0.041376750867862... |
710.3221 | Toward gauge independent study of confinement in SU(3) Yang-Mills theory | Dual superconductivity is believed to be a promising mechanism for quark
confinement and has been investigated on a lattice effectively by a particular
gauge called the maximal Abelian (MA) gauge. We propose a new formulation of
SU(3) Yang-Mills theory on a lattice based on a non-linear change of variables
where the ... | hep-lat | dual superconductivity is believed to be a promising mechanism for quark confinement and has been investigated on a lattice effectively by a particular gauge called the maximal abelian ma gauge we propose a new formulation of su3 yangmills theory on a lattice based on a nonlinear change of variables where the new field... | [['dual', 'superconductivity', 'is', 'believed', 'to', 'be', 'a', 'promising', 'mechanism', 'for', 'quark', 'confinement', 'and', 'has', 'been', 'investigated', 'on', 'a', 'lattice', 'effectively', 'by', 'a', 'particular', 'gauge', 'called', 'the', 'maximal', 'abelian', 'ma', 'gauge', 'we', 'propose', 'a', 'new', 'form... | [-0.09600070662976357, 0.16413084949658094, -0.12437890992356987, 0.04055257452616133, -0.12755302358270873, -0.09974882284317303, 0.05712560486361365, 0.3581096686905733, -0.21681344026216753, -0.2619030934630058, 0.07533867543602668, -0.2112111144073347, -0.1405712781060073, 0.09467189179526435, -0.08987100388997643,... |
710.3222 | Infrared catastrophe in two-quasiparticle collision integral | Relaxation of a non-equilibrium state in a disordered metal with a
spin-dependent electron energy distribution is considered. The collision
integral due to the electron-electron interaction is computed within the
approximation of a two-quasiparticle scattering. We show that the spin-flip
scattering processes with a s... | cond-mat.mes-hall | relaxation of a nonequilibrium state in a disordered metal with a spindependent electron energy distribution is considered the collision integral due to the electronelectron interaction is computed within the approximation of a twoquasiparticle scattering we show that the spinflip scattering processes with a small ener... | [['relaxation', 'of', 'a', 'nonequilibrium', 'state', 'in', 'a', 'disordered', 'metal', 'with', 'a', 'spindependent', 'electron', 'energy', 'distribution', 'is', 'considered', 'the', 'collision', 'integral', 'due', 'to', 'the', 'electronelectron', 'interaction', 'is', 'computed', 'within', 'the', 'approximation', 'of',... | [-0.1676549093958826, 0.18382169572741477, -0.10244049292893331, 0.1294847722274086, -0.014247346917498056, -0.11861898156457415, 0.0199071264708258, 0.3601330147934294, -0.24931511027024728, -0.25164961424073046, -0.024202064505482318, -0.2999310758417455, -0.043904081896539326, 0.12960681095327659, 0.0681557660796200... |
710.3223 | Observational Test of Coronal Magnetic Field Models I. Comparison with
Potential Field Model | Recent advances have made it possible to obtain two-dimensional line-of-sight
magnetic field maps of the solar corona from spectropolarimetric observations
of the Fe XIII 1075 nm forbidden coronal emission line. Together with the
linear polarization measurements that map the azimuthal direction of the
coronal magneti... | astro-ph | recent advances have made it possible to obtain twodimensional lineofsight magnetic field maps of the solar corona from spectropolarimetric observations of the fe xiii 1075 nm forbidden coronal emission line together with the linear polarization measurements that map the azimuthal direction of the coronal magnetic fiel... | [['recent', 'advances', 'have', 'made', 'it', 'possible', 'to', 'obtain', 'twodimensional', 'lineofsight', 'magnetic', 'field', 'maps', 'of', 'the', 'solar', 'corona', 'from', 'spectropolarimetric', 'observations', 'of', 'the', 'fe', 'xiii', '1075', 'nm', 'forbidden', 'coronal', 'emission', 'line', 'together', 'with', ... | [-0.11601800351410968, 0.15129757295630833, 0.03758544187794113, 0.08189588086801479, -0.07176796282539193, -0.064172152698001, 0.030975597122493956, 0.4427368722768276, -0.19448880584305883, -0.35766846753890913, 0.058938224089858535, -0.22305179780339382, -0.08439897227525243, 0.22481655995288366, 0.01324845789730578... |
710.3224 | Outflowing atomic and molecular gas at $z \sim 0.67$ towards 1504+377 | We report the detection of OH 1667 MHz and wide HI 21cm absorption at $z \sim
0.67$ towards the red quasar 1504+377, with the Green Bank Telescope and the
Giant Metrewave Radio Telescope. The HI 21cm absorption extends over a velocity
range of $\sim 600$ km/s blueward of the quasar redshift ($z=0.674$), with the
new ... | astro-ph | we report the detection of oh 1667 mhz and wide hi 21cm absorption at z sim 067 towards the red quasar 1504377 with the green bank telescope and the giant metrewave radio telescope the hi 21cm absorption extends over a velocity range of sim 600 kms blueward of the quasar redshift z0674 with the new oh 1667 mhz absorpti... | [['we', 'report', 'the', 'detection', 'of', 'oh', '1667', 'mhz', 'and', 'wide', 'hi', '21cm', 'absorption', 'at', 'z', 'sim', '067', 'towards', 'the', 'red', 'quasar', '1504377', 'with', 'the', 'green', 'bank', 'telescope', 'and', 'the', 'giant', 'metrewave', 'radio', 'telescope', 'the', 'hi', '21cm', 'absorption', 'ex... | [-0.09806778362908915, 0.10946918061623971, 0.0960328098109165, 0.006780144361565347, -0.05945647341870993, -0.07381761309186943, 0.04845585996193475, 0.4716301098303065, -0.13841093850927683, -0.3168985753070787, 0.016865660079571677, -0.29692737317944323, 0.03612854381096982, 0.16718351447959864, 0.08355163582355538,... |
710.3225 | Phenomenological and ontological models in natural science | The observation of the nature and world represents the main source of human
knowledge on the basis of our reason. At the present it is also the use of
precise measurement approaches, which may contribute significantly to the
knowledge of the world but cannot substitute fully the knowledge of the whole
reality obtaine... | physics.hist-ph physics.gen-ph | the observation of the nature and world represents the main source of human knowledge on the basis of our reason at the present it is also the use of precise measurement approaches which may contribute significantly to the knowledge of the world but cannot substitute fully the knowledge of the whole reality obtained al... | [['the', 'observation', 'of', 'the', 'nature', 'and', 'world', 'represents', 'the', 'main', 'source', 'of', 'human', 'knowledge', 'on', 'the', 'basis', 'of', 'our', 'reason', 'at', 'the', 'present', 'it', 'is', 'also', 'the', 'use', 'of', 'precise', 'measurement', 'approaches', 'which', 'may', 'contribute', 'significan... | [-0.038917900946484334, 0.06381243627725376, -0.10528843450433045, 0.09221320361769424, -0.1542057047531106, -0.12977910668169165, 0.053526133367353505, 0.37758131758035984, -0.21144364645181138, -0.34422909750244, 0.10805954691098724, -0.23517024226991148, -0.1399683862105864, 0.2036648041803049, -0.0899324069711535, ... |
710.3226 | Lens sequences | A family of sequences produced by a non-homogeneous linear recurrence formula
derived from the geometry of circles inscribed in lenses is introduced and
studied. Mysterious ``underground'' sequences underlying them are discovered in
this paper.
| math.NT math.MG | a family of sequences produced by a nonhomogeneous linear recurrence formula derived from the geometry of circles inscribed in lenses is introduced and studied mysterious underground sequences underlying them are discovered in this paper | [['a', 'family', 'of', 'sequences', 'produced', 'by', 'a', 'nonhomogeneous', 'linear', 'recurrence', 'formula', 'derived', 'from', 'the', 'geometry', 'of', 'circles', 'inscribed', 'in', 'lenses', 'is', 'introduced', 'and', 'studied', 'mysterious', 'underground', 'sequences', 'underlying', 'them', 'are', 'discovered', '... | [-0.17336892706396825, 0.10846436188063201, -0.0692646524266285, 0.1349335140274728, -0.06548166077803164, -0.12877997193102012, -0.02242171164150076, 0.3236954892602037, -0.2997172612916021, -0.2694256277207066, 0.12096690667984898, -0.3020532933228156, -0.22910459076657014, 0.2087422201738638, -0.09312919916256386, 0... |
710.3227 | Multi-peak solutions for magnetic NLS equations without non--degeneracy
conditions | In the work we consider the magnetic NLS equation
(\frac{\hbar}{i} \nabla -A(x))^2 u + V(x)u - f(|u|^2)u = 0 \quad {in} \R^N
where $N \geq 3$, $A \colon \R^N \to \R^N$ is a magnetic potential, possibly
unbounded, $V \colon \R^N \to \R$ is a multi-well electric potential, which can
vanish somewhere, $f$ is a subcrit... | math.AP | in the work we consider the magnetic nls equation frachbari nabla ax2 u vxu fu2u 0 quad in rn where n geq 3 a colon rn to rn is a magnetic potential possibly unbounded v colon rn to r is a multiwell electric potential which can vanish somewhere f is a subcritical nonlinear term we prove the existence of a semiclassical... | [['in', 'the', 'work', 'we', 'consider', 'the', 'magnetic', 'nls', 'equation', 'frachbari', 'nabla', 'ax2', 'u', 'vxu', 'fu2u', '0', 'quad', 'in', 'rn', 'where', 'n', 'geq', '3', 'a', 'colon', 'rn', 'to', 'rn', 'is', 'a', 'magnetic', 'potential', 'possibly', 'unbounded', 'v', 'colon', 'rn', 'to', 'r', 'is', 'a', 'multi... | [-0.2520607321120396, 0.060800340423058416, 0.04902532621211297, -0.011404638038633542, -0.08006495611138038, -0.23006085771438037, -0.08208734886343214, 0.32929206412990353, -0.3126646466238575, -0.11035113498518193, 0.09618519304785877, -0.3905123223273738, -0.13343518745544292, 0.14064980000005783, -0.05607593912832... |
710.3228 | Have loose globular clusters collapsed yet? | We report on the discovery of a surprising observed correlation between the
slope of the low-mass stellar global mass function (GMF) of globular clusters
(GCs) and their central concentration parameter c = log(r_t/r_c), i.e. the
logarithmic ratio of tidal and core radii. This result is based on the analysis
of a samp... | astro-ph | we report on the discovery of a surprising observed correlation between the slope of the lowmass stellar global mass function gmf of globular clusters gcs and their central concentration parameter c logr_tr_c ie the logarithmic ratio of tidal and core radii this result is based on the analysis of a sample of twenty gal... | [['we', 'report', 'on', 'the', 'discovery', 'of', 'a', 'surprising', 'observed', 'correlation', 'between', 'the', 'slope', 'of', 'the', 'lowmass', 'stellar', 'global', 'mass', 'function', 'gmf', 'of', 'globular', 'clusters', 'gcs', 'and', 'their', 'central', 'concentration', 'parameter', 'c', 'logr_tr_c', 'ie', 'the', ... | [-0.053765296776885095, 0.14422858319783638, -0.12475946197926778, 0.1407172518378548, -0.12463163922099742, -0.06606439950400453, 0.05360924569805907, 0.4026710939385343, -0.1680389456274106, -0.36573396860435214, 0.035906951601876395, -0.2648824741945991, -0.04913153465177062, 0.17850669018947815, -0.0357491715633377... |
710.3229 | Using the QBO to predict the number of hurricanes hitting the U.S | A simple study of the relationship between the QBO and the number of
hurricanes in the Atlantic, both in the Basin and hitting the U.S. coastline,
demonstrates that the QBO is not a particularly useful index to help predict
hurricane numbers on five-year time scales. It is shown that there is very
little difference b... | physics.ao-ph | a simple study of the relationship between the qbo and the number of hurricanes in the atlantic both in the basin and hitting the us coastline demonstrates that the qbo is not a particularly useful index to help predict hurricane numbers on fiveyear time scales it is shown that there is very little difference between t... | [['a', 'simple', 'study', 'of', 'the', 'relationship', 'between', 'the', 'qbo', 'and', 'the', 'number', 'of', 'hurricanes', 'in', 'the', 'atlantic', 'both', 'in', 'the', 'basin', 'and', 'hitting', 'the', 'us', 'coastline', 'demonstrates', 'that', 'the', 'qbo', 'is', 'not', 'a', 'particularly', 'useful', 'index', 'to', ... | [-0.11567636926599678, 0.15206595496003272, -0.1014114127684276, 0.1350060457361464, -0.06485072976358018, -0.03809844128769434, 0.05181809191284611, 0.3414106589642543, -0.23281145036148215, -0.3227632841438923, 0.11884016245241882, -0.2644098365127823, -0.17827559612890326, 0.2564251121965427, -0.1101849044094459, -0... |
710.323 | Superstring in the Presence of the Worldsheet Gauge Field | We study the superstring theory with an Abelian worldsheet gauge field. The
components of the gauge field appear as a space and a time coordinates. We call
them as "fictitious coordinates". The worldsheet supersymmetry and the
Poincar\'e symmetry of this model will be analyzed. The $T$-duality and
quantization of the... | hep-th | we study the superstring theory with an abelian worldsheet gauge field the components of the gauge field appear as a space and a time coordinates we call them as fictitious coordinates the worldsheet supersymmetry and the poincare symmetry of this model will be analyzed the tduality and quantization of the two fictitio... | [['we', 'study', 'the', 'superstring', 'theory', 'with', 'an', 'abelian', 'worldsheet', 'gauge', 'field', 'the', 'components', 'of', 'the', 'gauge', 'field', 'appear', 'as', 'a', 'space', 'and', 'a', 'time', 'coordinates', 'we', 'call', 'them', 'as', 'fictitious', 'coordinates', 'the', 'worldsheet', 'supersymmetry', 'a... | [-0.20636309617149987, 0.199855048089184, -0.13600101236972892, 0.1242509378965846, -0.1123686710601313, -0.10684134905929105, -0.02832992335070709, 0.35418215514928625, -0.25280082918572844, -0.2362412783202895, 0.10474950312064928, -0.2229315435285108, -0.18381441438472584, 0.06597304954847093, -0.06936751031561901, ... |
710.3231 | Optical Excitation of Nuclear Spin Coherence in Tm3+:YAG | A thulium-doped crystal is experimentally shown to be an excellent candidate
for broadband quantum storage in a solid-state medium. For the first time,
nuclear spin coherence is optically excited, detected and characterized in such
a crystal. The lifetime of the spin coherence -- the potential storage entity
-- is me... | quant-ph | a thuliumdoped crystal is experimentally shown to be an excellent candidate for broadband quantum storage in a solidstate medium for the first time nuclear spin coherence is optically excited detected and characterized in such a crystal the lifetime of the spin coherence the potential storage entity is measured by mean... | [['a', 'thuliumdoped', 'crystal', 'is', 'experimentally', 'shown', 'to', 'be', 'an', 'excellent', 'candidate', 'for', 'broadband', 'quantum', 'storage', 'in', 'a', 'solidstate', 'medium', 'for', 'the', 'first', 'time', 'nuclear', 'spin', 'coherence', 'is', 'optically', 'excited', 'detected', 'and', 'characterized', 'in... | [-0.08862064323045121, 0.2015771874362342, -0.01651096654266281, 0.012669711386400235, -0.008059070000182028, -0.15781675785294044, 0.06803240070534546, 0.4721205296075862, -0.2877621803301103, -0.30339831659448857, 0.03955597891826588, -0.2899068172555417, -1.6416180069031924e-05, 0.23167625778233228, 0.03865057596957... |
710.3232 | Reflection Groups and Differential Forms | We study differential forms invariant under a finite reflection group over a
field of arbitrary characteristic. In particular, we prove an analogue of
Saito's freeness criterion for invariant differential 1-forms. We also discuss
how twisted wedging endows the invariant forms with the structure of a free
exterior alg... | math.RT math.AC | we study differential forms invariant under a finite reflection group over a field of arbitrary characteristic in particular we prove an analogue of saitos freeness criterion for invariant differential 1forms we also discuss how twisted wedging endows the invariant forms with the structure of a free exterior algebra in... | [['we', 'study', 'differential', 'forms', 'invariant', 'under', 'a', 'finite', 'reflection', 'group', 'over', 'a', 'field', 'of', 'arbitrary', 'characteristic', 'in', 'particular', 'we', 'prove', 'an', 'analogue', 'of', 'saitos', 'freeness', 'criterion', 'for', 'invariant', 'differential', '1forms', 'we', 'also', 'disc... | [-0.2274130790669849, 0.0754039812366144, -0.13717204130565128, 0.07227846148315871, -0.10347898523120777, -0.09152735652321059, -0.0620812511584465, 0.33687267414685607, -0.32063085732279695, -0.22602204759554614, 0.09803500827199416, -0.20634374436854885, -0.19350747999640694, 0.20533957321574722, -0.1240342870030714... |
710.3233 | Summary of the COSY-11 Measurements of Hyperon Production | The studies of hyperon production performed at COSY-11 are summarized. The
results of the experiments in the reaction channels pp-->pK+Lambda,
pp-->pK+Sigma0, and pp-->nK+Sigma+ are shown. Excitation functions
fromthreshold up to about 90MeV excess energies have been evaluated with high
precision for the Lambda and S... | nucl-ex | the studies of hyperon production performed at cosy11 are summarized the results of the experiments in the reaction channels pppklambda pppksigma0 and ppnksigma are shown excitation functions fromthreshold up to about 90mev excess energies have been evaluated with high precision for the lambda and sigma0 production the... | [['the', 'studies', 'of', 'hyperon', 'production', 'performed', 'at', 'cosy11', 'are', 'summarized', 'the', 'results', 'of', 'the', 'experiments', 'in', 'the', 'reaction', 'channels', 'pppklambda', 'pppksigma0', 'and', 'ppnksigma', 'are', 'shown', 'excitation', 'functions', 'fromthreshold', 'up', 'to', 'about', '90mev'... | [-0.03524922136224747, 0.21173212340929443, -0.04269779877254872, 0.10132292315127357, 0.06350417894316793, -0.10543362302557817, 0.02792952883811224, 0.37195930032739566, -0.17865661822909873, -0.34576652151724646, 0.014671594457006052, -0.43142856078015435, 0.09302353875208942, 0.16299460325685758, 0.1452124161970993... |
710.3234 | The Landau gauge gluon propagator: Gribov problem and finite-size
effects | The SU(2) gluon propagator in Landau gauge is studied on the lattice. Our
gauge fixing procedure employs simulated annealing and Z(2)-flips. It finds
higher maxima of the gauge functional compared with those obtained with the
standard overrelaxation and leads to systematic deviations of the gluon
propagator in the in... | hep-lat | the su2 gluon propagator in landau gauge is studied on the lattice our gauge fixing procedure employs simulated annealing and z2flips it finds higher maxima of the gauge functional compared with those obtained with the standard overrelaxation and leads to systematic deviations of the gluon propagator in the infrared re... | [['the', 'su2', 'gluon', 'propagator', 'in', 'landau', 'gauge', 'is', 'studied', 'on', 'the', 'lattice', 'our', 'gauge', 'fixing', 'procedure', 'employs', 'simulated', 'annealing', 'and', 'z2flips', 'it', 'finds', 'higher', 'maxima', 'of', 'the', 'gauge', 'functional', 'compared', 'with', 'those', 'obtained', 'with', '... | [-0.06715759148200352, 0.21769998842229446, -0.1360846364311874, 0.10199399850176026, -0.015210070788937931, -0.09112474888563156, 0.09699298042027901, 0.39056462603310743, -0.13683903602262337, -0.30544594101607797, 0.009679966210387646, -0.31562503742674985, -0.04309412701676289, 0.12200615635452171, 0.04496132621813... |
710.3235 | Studies of CP-conserving and CP-violating Bs mixing parameters with the
D0 experiment | This paper summarises the recent results of the Run IIa D0 experiment at the
Tevatron Collider at Fermilab on the observable parameters of the $B_{s}$
meson. A measurement of the branching fraction $B_s->D_s^{(*)}D_s^{(*)}$ is
reported, which provides an estimate of the width difference
$\Delta\Gamma_{s}^{CP}/\Delta\... | hep-ex | this paper summarises the recent results of the run iia d0 experiment at the tevatron collider at fermilab on the observable parameters of the b_s meson a measurement of the branching fraction b_sd_sd_s is reported which provides an estimate of the width difference deltagamma_scpdeltagamma_s through the decay b_s to jp... | [['this', 'paper', 'summarises', 'the', 'recent', 'results', 'of', 'the', 'run', 'iia', 'd0', 'experiment', 'at', 'the', 'tevatron', 'collider', 'at', 'fermilab', 'on', 'the', 'observable', 'parameters', 'of', 'the', 'b_s', 'meson', 'a', 'measurement', 'of', 'the', 'branching', 'fraction', 'b_sd_sd_s', 'is', 'reported'... | [-0.1210542119826704, 0.21229069511524545, -0.11239945797528002, 0.03267656277661779, -0.07781265898682606, -0.09461772360239477, 0.07695714002287808, 0.281721836662498, -0.2285628541340602, -0.2510016733652045, 0.019102201066461617, -0.3664183546842515, 0.02932129283475786, 0.17422276514785728, 0.03722473863383819, 0.... |
710.3236 | Phase transitions in a 3 dimensional lattice loop gas | We investigate, via Monte Carlo simulations, the phase structure of a system
of closed, nonintersecting but otherwise non-interacting, loops in 3 Euclidean
dimensions. The loops correspond to closed trajectories of massive particles
and we find a phase transition as a function of their mass. We identify the
order par... | hep-lat hep-th | we investigate via monte carlo simulations the phase structure of a system of closed nonintersecting but otherwise noninteracting loops in 3 euclidean dimensions the loops correspond to closed trajectories of massive particles and we find a phase transition as a function of their mass we identify the order parameter as... | [['we', 'investigate', 'via', 'monte', 'carlo', 'simulations', 'the', 'phase', 'structure', 'of', 'a', 'system', 'of', 'closed', 'nonintersecting', 'but', 'otherwise', 'noninteracting', 'loops', 'in', '3', 'euclidean', 'dimensions', 'the', 'loops', 'correspond', 'to', 'closed', 'trajectories', 'of', 'massive', 'particl... | [-0.17910382820141574, 0.2369045723942636, -0.07505760110481535, 0.07959139423901808, -0.02494287099828769, -0.1183974095341167, 0.06935026673059422, 0.36195970904988967, -0.21489792231998794, -0.2728710234102406, 0.06788608534976645, -0.2766100610449408, -0.13860687286859424, 0.09419584418176098, 0.009981997169847235,... |
710.3237 | Hyperfine Structure of S-States in Muonic Helium Ion | Corrections of orders alpha^5 and alpha^6 are calculated in the hyperfine
splittings of 1S and 2S - energy levels in the ion of muonic helium. The
electron vacuum polarization effects, the nuclear structure corrections and
recoil corrections are taken into account. The obtained numerical values of the
hyperfine split... | hep-ph | corrections of orders alpha5 and alpha6 are calculated in the hyperfine splittings of 1s and 2s energy levels in the ion of muonic helium the electron vacuum polarization effects the nuclear structure corrections and recoil corrections are taken into account the obtained numerical values of the hyperfine splittings 133... | [['corrections', 'of', 'orders', 'alpha5', 'and', 'alpha6', 'are', 'calculated', 'in', 'the', 'hyperfine', 'splittings', 'of', '1s', 'and', '2s', 'energy', 'levels', 'in', 'the', 'ion', 'of', 'muonic', 'helium', 'the', 'electron', 'vacuum', 'polarization', 'effects', 'the', 'nuclear', 'structure', 'corrections', 'and',... | [-0.07824387308751601, 0.23819538028260998, 0.02495522938971949, 0.16441861291004475, 0.053566510905850094, -0.125626536210739, 0.05147960991327932, 0.38024705193590286, -0.16322667029859542, -0.34650421255744646, -0.03534009486036158, -0.33826867963165735, 0.14634422053850993, 0.15030191154327505, 0.12554917596063989,... |
710.3238 | The inverse integrating factor and the Poincar\'e map | This work is concerned with planar real analytic differential systems with an
analytic inverse integrating factor defined in a neighborhood of a regular
orbit. We show that the inverse integrating factor defines an ordinary
differential equation for the transition map along the orbit. When the regular
orbit is a limi... | math.DS | this work is concerned with planar real analytic differential systems with an analytic inverse integrating factor defined in a neighborhood of a regular orbit we show that the inverse integrating factor defines an ordinary differential equation for the transition map along the orbit when the regular orbit is a limit cy... | [['this', 'work', 'is', 'concerned', 'with', 'planar', 'real', 'analytic', 'differential', 'systems', 'with', 'an', 'analytic', 'inverse', 'integrating', 'factor', 'defined', 'in', 'a', 'neighborhood', 'of', 'a', 'regular', 'orbit', 'we', 'show', 'that', 'the', 'inverse', 'integrating', 'factor', 'defines', 'an', 'ordi... | [-0.18620513402265945, 0.05638599554220094, -0.09604859007002436, 0.057215449401428024, -0.054177402627422724, -0.06550950254668213, 0.024740541763934615, 0.3049622190227439, -0.31708152470921125, -0.2206429820247751, 0.11921979921401908, -0.2576396162468771, -0.190012936693082, 0.22595179680413402, -0.0692199531016010... |
710.3239 | Phase Diagram of the One Dimensional $S=1/2$ $XXZ$ model with
Ferromagnetic nearest-neighbor and Antiferromagnetic next-nearest neighbor
interactions | We have studied the phase diagram of the one dimensional $S=1/2$ $XXZ$ model
with ferromagnetic nearest-neighbor and antiferromagnetic next-nearest neighbor
interactions. We have applied the quantum renormalization group (QRG) approach
to get the stable fixed points and the running of coupling constants. The
second o... | cond-mat.str-el | we have studied the phase diagram of the one dimensional s12 xxz model with ferromagnetic nearestneighbor and antiferromagnetic nextnearest neighbor interactions we have applied the quantum renormalization group qrg approach to get the stable fixed points and the running of coupling constants the second order qrg has b... | [['we', 'have', 'studied', 'the', 'phase', 'diagram', 'of', 'the', 'one', 'dimensional', 's12', 'xxz', 'model', 'with', 'ferromagnetic', 'nearestneighbor', 'and', 'antiferromagnetic', 'nextnearest', 'neighbor', 'interactions', 'we', 'have', 'applied', 'the', 'quantum', 'renormalization', 'group', 'qrg', 'approach', 'to... | [-0.18928203036335017, 0.18360342749946038, -0.08254363282314656, 0.022642160186010583, -0.035897852900410886, -0.18206404421695518, 0.047910106770730425, 0.39550871798967563, -0.23809693249177585, -0.2545096363727618, 0.058768383357266994, -0.3042515308406312, -0.11424158159100893, 0.10175318822481678, 0.1020774401100... |
710.324 | Hawking radiation in a Rotating Kaluza-Klein Black Hole with Squashed
Horizons | We explore the signature of the extra dimension in the Hawking radiation in a
rotating Kaluza-Klein black hole with squashed horizons. Comparing with the
spherical case, we find that the rotating parameter brings richer physics. We
obtain the appropriate size of the extra dimension which can enhance the
Hawking radia... | hep-th | we explore the signature of the extra dimension in the hawking radiation in a rotating kaluzaklein black hole with squashed horizons comparing with the spherical case we find that the rotating parameter brings richer physics we obtain the appropriate size of the extra dimension which can enhance the hawking radiation a... | [['we', 'explore', 'the', 'signature', 'of', 'the', 'extra', 'dimension', 'in', 'the', 'hawking', 'radiation', 'in', 'a', 'rotating', 'kaluzaklein', 'black', 'hole', 'with', 'squashed', 'horizons', 'comparing', 'with', 'the', 'spherical', 'case', 'we', 'find', 'that', 'the', 'rotating', 'parameter', 'brings', 'richer',... | [-0.137766882913517, 0.17081957935976486, -0.08829381577670574, 0.143558640157183, -0.11162115246988832, -0.18023718246258796, 0.009825942102664461, 0.26336432825773953, -0.1528241947448502, -0.3053146238128344, 0.07878869694735234, -0.3028894177948435, -0.061446562952672444, 0.14929396660688024, -0.06114327964314725, ... |
710.3241 | Compactness in vector-valued Banach function spaces | We give a new proof of a recent characterization by Diaz and Mayoral of
compactness in the Lebesgue-Bochner spaces $L_X^p$, where $X$ is a Banach space
and $1\le p<\infty$, and extend the result to vector-valued Banach function
spaces $E_X$, where $E$ is a Banach function space with order continuous norm.
| math.FA | we give a new proof of a recent characterization by diaz and mayoral of compactness in the lebesguebochner spaces l_xp where x is a banach space and 1le pinfty and extend the result to vectorvalued banach function spaces e_x where e is a banach function space with order continuous norm | [['we', 'give', 'a', 'new', 'proof', 'of', 'a', 'recent', 'characterization', 'by', 'diaz', 'and', 'mayoral', 'of', 'compactness', 'in', 'the', 'lebesguebochner', 'spaces', 'l_xp', 'where', 'x', 'is', 'a', 'banach', 'space', 'and', '1le', 'pinfty', 'and', 'extend', 'the', 'result', 'to', 'vectorvalued', 'banach', 'func... | [-0.09295827486761371, 0.11410148871340314, -0.07981946429164073, 0.11144677263076361, -0.09681533594444698, -0.057126082365914266, 0.018526374077310368, 0.3803317708780571, -0.31160376897575903, -0.12835339532822979, 0.13704233916656933, -0.24694317841560257, -0.10218293383261379, 0.18482218793004143, -0.1854573101641... |
710.3242 | The interplay between boundary conditions and flow geometries in shear
banding: hysteresis, band configurations, and surface transitions | We study shear banding flows in models of wormlike micelles or polymer
solutions, and explore the effects of different boundary conditions for the
viscoelastic stress. These are needed because the equations of motion are
inherently non-local and include ``diffusive'' or square-gradient terms. Using
the diffusive John... | cond-mat.soft cond-mat.other | we study shear banding flows in models of wormlike micelles or polymer solutions and explore the effects of different boundary conditions for the viscoelastic stress these are needed because the equations of motion are inherently nonlocal and include diffusive or squaregradient terms using the diffusive johnsonsegalman... | [['we', 'study', 'shear', 'banding', 'flows', 'in', 'models', 'of', 'wormlike', 'micelles', 'or', 'polymer', 'solutions', 'and', 'explore', 'the', 'effects', 'of', 'different', 'boundary', 'conditions', 'for', 'the', 'viscoelastic', 'stress', 'these', 'are', 'needed', 'because', 'the', 'equations', 'of', 'motion', 'are... | [-0.17713421025940812, 0.2094238333732974, -0.06531945629840304, 0.007970005925549934, -0.05903889498162906, -0.12528635338572278, -0.009294294607026745, 0.3447602432382889, -0.3322045077632131, -0.2294940354466189, 0.14333097287405003, -0.21732099344525252, -0.12964665810636022, 0.13295327761565104, -0.028852974838152... |
710.3243 | Macroion adsorption: The crucial role of excluded volume and coions | The adsorption of charged colloids (macroions) onto an oppositely charged
planar substrate is investigated theoretically. Taking properly into account
the finite size of the macroions, unusual behaviors are reported. It is found
that the role of the coions (the little salt-ions carrying the same sign of
charge as tha... | cond-mat.soft cond-mat.stat-mech | the adsorption of charged colloids macroions onto an oppositely charged planar substrate is investigated theoretically taking properly into account the finite size of the macroions unusual behaviors are reported it is found that the role of the coions the little saltions carrying the same sign of charge as that of the ... | [['the', 'adsorption', 'of', 'charged', 'colloids', 'macroions', 'onto', 'an', 'oppositely', 'charged', 'planar', 'substrate', 'is', 'investigated', 'theoretically', 'taking', 'properly', 'into', 'account', 'the', 'finite', 'size', 'of', 'the', 'macroions', 'unusual', 'behaviors', 'are', 'reported', 'it', 'is', 'found'... | [-0.12085783453265497, 0.22872984335433091, -0.06645917239408176, 0.052645876736585114, 0.01755081160914108, -0.1558458082411573, 0.029400897694818944, 0.39740527932902414, -0.22972944075892487, -0.2778820297400276, -0.02241294191594808, -0.3130324841533081, -0.13677560437066727, 0.1159172724169421, -0.0028862417843866... |
710.3244 | Cellular resolutions of Cohen-Macaulay monomial quotient rings | We investigate monomial labellings on cell complexes, giving a minimal
cellular resolution of the ideal generated by these monomials, and such that
the associated quotient ring is Cohen-Macaulay. We introduce a notion of such a
labelling being maximal. There is only a finite number of maximal labellings
for each cell... | math.AC math.CO | we investigate monomial labellings on cell complexes giving a minimal cellular resolution of the ideal generated by these monomials and such that the associated quotient ring is cohenmacaulay we introduce a notion of such a labelling being maximal there is only a finite number of maximal labellings for each cell comple... | [['we', 'investigate', 'monomial', 'labellings', 'on', 'cell', 'complexes', 'giving', 'a', 'minimal', 'cellular', 'resolution', 'of', 'the', 'ideal', 'generated', 'by', 'these', 'monomials', 'and', 'such', 'that', 'the', 'associated', 'quotient', 'ring', 'is', 'cohenmacaulay', 'we', 'introduce', 'a', 'notion', 'of', 's... | [-0.1839194696639543, 0.10565820976794846, 0.0239637131276338, 0.07079154212851131, -0.05405527495009744, -0.1280431070000581, 0.02315967108892358, 0.3928754677037722, -0.36502735640691675, -0.1831131164200496, 0.13749462659673198, -0.2588219934993464, -0.15323386203659617, 0.16344915942180957, -0.1670957603154407, -0.... |
710.3245 | The decomposition of the spinor bundle of Grassmann manifolds | The decomposition of the spinor bundle of the spin Grassmann manifolds
$G_{m,n}=SO(m+n)/SO(m)\times SO(n)$ into irreducible representations of
$\mathfrak{so}(m)\oplus\mathfrak{so}(n)$ is presented. A universal construction
is developed and the general statement is proven for $G_{2k+1,3}$, $G_{2k,4}$,
and $G_{2k+1,5}$... | math.DG math-ph math.MP | the decomposition of the spinor bundle of the spin grassmann manifolds g_mnsomnsomtimes son into irreducible representations of mathfraksomoplusmathfrakson is presented a universal construction is developed and the general statement is proven for g_2k13 g_2k4 and g_2k15 for all k the decomposition is used to discuss pr... | [['the', 'decomposition', 'of', 'the', 'spinor', 'bundle', 'of', 'the', 'spin', 'grassmann', 'manifolds', 'g_mnsomnsomtimes', 'son', 'into', 'irreducible', 'representations', 'of', 'mathfraksomoplusmathfrakson', 'is', 'presented', 'a', 'universal', 'construction', 'is', 'developed', 'and', 'the', 'general', 'statement'... | [-0.17388499754608847, 0.10334615814773475, -0.11223577342781366, 0.0497929352591289, -0.10495549775477425, -0.0903202031885146, -0.06246541159264013, 0.3061608062947498, -0.25202783540475604, -0.1950044089964792, 0.10919841775195856, -0.24227560937915946, -0.1590527735796629, 0.17422781826234332, -0.030782127205063316... |
710.3246 | Bloom maps | We consider the problem of succinctly encoding a static map to support
approximate queries. We derive upper and lower bounds on the space requirements
in terms of the error rate and the entropy of the distribution of values over
keys: our bounds differ by a factor log e. For the upper bound we introduce a
novel data ... | cs.DS cs.IT math.IT | we consider the problem of succinctly encoding a static map to support approximate queries we derive upper and lower bounds on the space requirements in terms of the error rate and the entropy of the distribution of values over keys our bounds differ by a factor log e for the upper bound we introduce a novel data struc... | [['we', 'consider', 'the', 'problem', 'of', 'succinctly', 'encoding', 'a', 'static', 'map', 'to', 'support', 'approximate', 'queries', 'we', 'derive', 'upper', 'and', 'lower', 'bounds', 'on', 'the', 'space', 'requirements', 'in', 'terms', 'of', 'the', 'error', 'rate', 'and', 'the', 'entropy', 'of', 'the', 'distribution... | [-0.12752249867159438, 0.04183885961481485, -0.10034952409468688, 0.11161732535004955, -0.0677545898436726, -0.10571093979448855, 0.1813646158711477, 0.27346292462248306, -0.29392086592043276, -0.35281957722232715, 0.12444765537874411, -0.2708470893346451, -0.12553130043670535, 0.20857481395087943, -0.09889684817390879... |
710.3247 | Generating random networks with given degree-degree correlations and
degree-dependent clustering | Random networks are widely used to model complex networks and research their
properties. In order to get a good approximation of complex networks
encountered in various disciplines of science, the ability to tune various
statistical properties of random networks is very important. In this manuscript
we present an alg... | cond-mat.dis-nn cond-mat.stat-mech | random networks are widely used to model complex networks and research their properties in order to get a good approximation of complex networks encountered in various disciplines of science the ability to tune various statistical properties of random networks is very important in this manuscript we present an algorith... | [['random', 'networks', 'are', 'widely', 'used', 'to', 'model', 'complex', 'networks', 'and', 'research', 'their', 'properties', 'in', 'order', 'to', 'get', 'a', 'good', 'approximation', 'of', 'complex', 'networks', 'encountered', 'in', 'various', 'disciplines', 'of', 'science', 'the', 'ability', 'to', 'tune', 'various... | [-0.0880835785509579, 0.04593619009041034, -0.09769862528178799, 0.12675773818699873, -0.07256485570452353, -0.1754184228661104, 0.004387782232605674, 0.48518816277049903, -0.29213543255091384, -0.33949231624268417, 0.026163676650305227, -0.2429435096335796, -0.28179497810687576, 0.15068989016084272, -0.033968001536716... |
710.3248 | Using COSY-11 apparatus for the precise studies of the natural width of
the eta prime meson | We present preliminary results and motivation of measurement of the total
width of the eta prime meson.
| nucl-ex | we present preliminary results and motivation of measurement of the total width of the eta prime meson | [['we', 'present', 'preliminary', 'results', 'and', 'motivation', 'of', 'measurement', 'of', 'the', 'total', 'width', 'of', 'the', 'eta', 'prime', 'meson']] | [-0.16879234112360897, 0.15876468432628932, -0.09149262210463777, 0.03216389983015902, -0.036624900777550304, -0.06338654085993767, 0.1083007918752949, 0.30613059386172714, -0.18259809779770234, -0.3051979042151395, -0.023919694153044152, -0.2920463593567119, -0.05863606118980576, 0.1834324151277542, 0.0167498707990436... |
710.3249 | A theorem about three quadratic forms | We prove a self-improvement property regarding quadratic forms on arbitrary
vector spaces. We discuss several consequences of this result, in particular
those concerning dimension-free L^p estimates of certain singular integral
operators (Riesz transforms).
| math.FA | we prove a selfimprovement property regarding quadratic forms on arbitrary vector spaces we discuss several consequences of this result in particular those concerning dimensionfree lp estimates of certain singular integral operators riesz transforms | [['we', 'prove', 'a', 'selfimprovement', 'property', 'regarding', 'quadratic', 'forms', 'on', 'arbitrary', 'vector', 'spaces', 'we', 'discuss', 'several', 'consequences', 'of', 'this', 'result', 'in', 'particular', 'those', 'concerning', 'dimensionfree', 'lp', 'estimates', 'of', 'certain', 'singular', 'integral', 'oper... | [-0.19756531204576744, 0.05747819285501133, -0.10226661370446284, 0.20250726131030894, -0.1397345773946268, -0.0875293969063822, 0.005959365573344809, 0.34176799045367673, -0.3443752145112464, -0.11579242946975159, 0.18807751347776502, -0.2622490478679538, -0.21398322581962653, 0.25486724962000595, -0.13159127293549705... |
710.325 | Algebraic dependence of commuting elements in algebras | The aim of this paper to draw attention to several aspects of the algebraic
dependence in algebras. The article starts with discussions of the algebraic
dependence problem in commutative algebras. Then the Burchnall-Chaundy
construction for proving algebraic dependence and obtaining the corresponding
algebraic curves... | math.RA math.QA | the aim of this paper to draw attention to several aspects of the algebraic dependence in algebras the article starts with discussions of the algebraic dependence problem in commutative algebras then the burchnallchaundy construction for proving algebraic dependence and obtaining the corresponding algebraic curves for ... | [['the', 'aim', 'of', 'this', 'paper', 'to', 'draw', 'attention', 'to', 'several', 'aspects', 'of', 'the', 'algebraic', 'dependence', 'in', 'algebras', 'the', 'article', 'starts', 'with', 'discussions', 'of', 'the', 'algebraic', 'dependence', 'problem', 'in', 'commutative', 'algebras', 'then', 'the', 'burchnallchaundy'... | [-0.13793528413185008, 0.08911526839155057, -0.09169827627394828, 0.09506477408528251, -0.16373494619458345, -0.13400553252560915, -0.0468925714691674, 0.2703627162296066, -0.32764799273960915, -0.19918096985849035, 0.12805906091509517, -0.3137060782246408, -0.12515918461981024, 0.23563055379781872, -0.1204872427689325... |
710.3251 | Glueballs and mesons in the superfluid phase of two-color QCD | QCD with two colors undergoes a transition to a superfluid phase with diquark
condensate when the quark chemical potential equals half the pion mass. We
investigate the gluonic aspects of the transition by inspecting the behavior of
the glueball correlators evaluated via a multi-step smearing procedure for
several va... | hep-lat | qcd with two colors undergoes a transition to a superfluid phase with diquark condensate when the quark chemical potential equals half the pion mass we investigate the gluonic aspects of the transition by inspecting the behavior of the glueball correlators evaluated via a multistep smearing procedure for several values... | [['qcd', 'with', 'two', 'colors', 'undergoes', 'a', 'transition', 'to', 'a', 'superfluid', 'phase', 'with', 'diquark', 'condensate', 'when', 'the', 'quark', 'chemical', 'potential', 'equals', 'half', 'the', 'pion', 'mass', 'we', 'investigate', 'the', 'gluonic', 'aspects', 'of', 'the', 'transition', 'by', 'inspecting', ... | [-0.12513287397089348, 0.25583615122118347, -0.12623373504417637, 0.05984352085909812, 0.00403235135052134, -0.06453269197806424, 0.10285975760323744, 0.3142230720259249, -0.17059647703080688, -0.25701951667715134, 0.02900504655801247, -0.3220106401279861, -0.0740750312099075, 0.1111374991349389, 0.09517391447550039, 0... |
710.3252 | Iron abundances from optical Fe III absorption lines in B-type stellar
spectra | The role of optical Fe III absorption lines in B-type stars as iron abundance
diagnostics is considered. To date, ultraviolet Fe lines have been widely used
in B-type stars, although line blending can severely hinder their diagnostic
power. Using optical spectra, covering a wavelength range ~ 3560 - 9200 A, a
sample ... | astro-ph | the role of optical fe iii absorption lines in btype stars as iron abundance diagnostics is considered to date ultraviolet fe lines have been widely used in btype stars although line blending can severely hinder their diagnostic power using optical spectra covering a wavelength range 3560 9200 a a sample of galactic bt... | [['the', 'role', 'of', 'optical', 'fe', 'iii', 'absorption', 'lines', 'in', 'btype', 'stars', 'as', 'iron', 'abundance', 'diagnostics', 'is', 'considered', 'to', 'date', 'ultraviolet', 'fe', 'lines', 'have', 'been', 'widely', 'used', 'in', 'btype', 'stars', 'although', 'line', 'blending', 'can', 'severely', 'hinder', '... | [0.017073639863310685, 0.05971310217103927, 0.01888793359321901, 0.08523132471562503, -0.06756518453320037, -0.12647253643794387, 0.09600984256903282, 0.492361689339471, -0.09694993047932395, -0.3713788255026527, 0.021079161396901445, -0.3112999321771116, 0.026334898564599307, 0.1694082066103256, -0.03170544644125305, ... |
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