id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
710.2453 | Quasi-Hermitian supersymmetric extensions of a non-Hermitian oscillator
Hamiltonian and of its generalizations | A harmonic oscillator Hamiltonian augmented by a non-Hermitian \pt-symmetric
part and its su(1,1) generalizations, for which a family of positive-definite
metric operators was recently constructed, are re-examined in a supersymmetric
context. Quasi-Hermitian supersymmetric extensions of such Hamiltonians are
proposed... | math-ph hep-th math.MP quant-ph | a harmonic oscillator hamiltonian augmented by a nonhermitian ptsymmetric part and its su11 generalizations for which a family of positivedefinite metric operators was recently constructed are reexamined in a supersymmetric context quasihermitian supersymmetric extensions of such hamiltonians are proposed by enlarging ... | [['a', 'harmonic', 'oscillator', 'hamiltonian', 'augmented', 'by', 'a', 'nonhermitian', 'ptsymmetric', 'part', 'and', 'its', 'su11', 'generalizations', 'for', 'which', 'a', 'family', 'of', 'positivedefinite', 'metric', 'operators', 'was', 'recently', 'constructed', 'are', 'reexamined', 'in', 'a', 'supersymmetric', 'con... | [-0.13132139518332314, 0.1570048270268287, 0.016051187938321908, 0.09988700147737867, -0.10012474247175727, -0.21969566864132042, -0.09435346674069132, 0.35879625572698376, -0.18749189228606475, -0.2115400187985998, 0.09387730273031171, -0.29498252687458454, -0.21974947786247226, 0.1771668818923579, -0.0899738165235120... |
710.2454 | Two positivity conjectures for Kerov polynomials | Kerov polynomials express the normalized characters of irreducible
representations of the symmetric group, evaluated on a cycle, as polynomials in
the free cumulants of the associated Young diagram. We present two positivity
conjectures for their coefficients. The latter are stronger than the positivity
conjecture of... | math.CO math.RT | kerov polynomials express the normalized characters of irreducible representations of the symmetric group evaluated on a cycle as polynomials in the free cumulants of the associated young diagram we present two positivity conjectures for their coefficients the latter are stronger than the positivity conjecture of kerov... | [['kerov', 'polynomials', 'express', 'the', 'normalized', 'characters', 'of', 'irreducible', 'representations', 'of', 'the', 'symmetric', 'group', 'evaluated', 'on', 'a', 'cycle', 'as', 'polynomials', 'in', 'the', 'free', 'cumulants', 'of', 'the', 'associated', 'young', 'diagram', 'we', 'present', 'two', 'positivity', ... | [-0.20714255319718194, 0.1219136520364317, -0.10698763924479789, 0.0926328628152913, -0.05857063001211809, -0.08642557174993717, -0.012233870241752997, 0.30164700024286095, -0.24807513322757216, -0.2166087269326862, 0.1049307985302555, -0.24324446230917712, -0.14710895622111098, 0.19107360449828664, -0.0779481516124642... |
710.2455 | Superfluid turbulence and pulsar glitch statistics | Experimental evidence is reviewed for the existence of superfluid turbulence
in a differentially rotating, spherical shell at high Reynolds numbers
($\Rey\gsim 10^3$), such as the outer core of a neutron star. It is shown that
torque variability increases with $\Rey$, suggesting that glitch activity in
radio pulsars ... | astro-ph | experimental evidence is reviewed for the existence of superfluid turbulence in a differentially rotating spherical shell at high reynolds numbers reygsim 103 such as the outer core of a neutron star it is shown that torque variability increases with rey suggesting that glitch activity in radio pulsars may be a functio... | [['experimental', 'evidence', 'is', 'reviewed', 'for', 'the', 'existence', 'of', 'superfluid', 'turbulence', 'in', 'a', 'differentially', 'rotating', 'spherical', 'shell', 'at', 'high', 'reynolds', 'numbers', 'reygsim', '103', 'such', 'as', 'the', 'outer', 'core', 'of', 'a', 'neutron', 'star', 'it', 'is', 'shown', 'tha... | [-0.12343745624012728, 0.23934662689100064, -0.03382366707748068, 0.127920947336067, -0.05640495711538408, -0.09246399689702288, 0.04306868825935655, 0.33178338379227734, -0.1594622858489553, -0.34647298049152137, 0.05814522217094366, -0.311351257065932, 0.01099622996139621, 0.2641408922620088, -0.00481055453022395, -0... |
710.2456 | Localization of elastic deformation in strongly anisotropic, porous,
linear materials with periodic microstructures: exact solutions and dilute
expansions | Exact solutions are derived for the problem of a two-dimensional, infinitely
anisotropic, linear-elastic medium containing a periodic lattice of voids. The
matrix material possesses either one infinitely soft, or one infinitely hard
loading direction, which induces localized (singular) field configurations. The
effec... | cond-mat.mtrl-sci | exact solutions are derived for the problem of a twodimensional infinitely anisotropic linearelastic medium containing a periodic lattice of voids the matrix material possesses either one infinitely soft or one infinitely hard loading direction which induces localized singular field configurations the effective elastic... | [['exact', 'solutions', 'are', 'derived', 'for', 'the', 'problem', 'of', 'a', 'twodimensional', 'infinitely', 'anisotropic', 'linearelastic', 'medium', 'containing', 'a', 'periodic', 'lattice', 'of', 'voids', 'the', 'matrix', 'material', 'possesses', 'either', 'one', 'infinitely', 'soft', 'or', 'one', 'infinitely', 'ha... | [-0.1222090051041044, 0.16444670739849318, -0.08226638375906486, 0.03160895708629599, -0.04190928204728903, -0.09806828757110458, -0.017514775660289014, 0.3761919727611462, -0.2770329216813931, -0.2498133149507437, 0.12811901611541618, -0.30218497564978647, -0.1449491359721619, 0.17731664616039536, 0.028427967973578498... |
710.2457 | Multiple point principle as a mechanism for the suppression of FCNC and
CP--violation phenomena in the 2HDM | We argue that multiple point principle (MPP) can be used to ensure CP
conservation and the absence of flavour changing neutral currents within the
two Higgs doublet model (2HDM). We also discuss Higgs phenomenology in the MPP
inspired 2HDM.
| hep-ph | we argue that multiple point principle mpp can be used to ensure cp conservation and the absence of flavour changing neutral currents within the two higgs doublet model 2hdm we also discuss higgs phenomenology in the mpp inspired 2hdm | [['we', 'argue', 'that', 'multiple', 'point', 'principle', 'mpp', 'can', 'be', 'used', 'to', 'ensure', 'cp', 'conservation', 'and', 'the', 'absence', 'of', 'flavour', 'changing', 'neutral', 'currents', 'within', 'the', 'two', 'higgs', 'doublet', 'model', '2hdm', 'we', 'also', 'discuss', 'higgs', 'phenomenology', 'in', ... | [-0.13616017107732403, 0.21866020182959545, 0.01331741482210465, 0.2267586339312868, -0.12209527466732722, -0.2894680740263982, 0.0619601268046655, 0.3224928887226643, -0.24885757176730877, -0.2855607252090405, 0.010824907699432701, -0.17257449688771978, -0.06560612078278492, 0.02196066534648148, -0.007060510303395299,... |
710.2458 | Indirect Searches for Dark Matter with AMS-02 | AMS-02 is a multi-purpose spectrometer with superconducting magnet, and is
designed for 3 years of data taking aboard the International Space Station. Its
high performance regarding particle identification and energy measurement will
allow performing indirect searches for dark matter (DM) in different channels
simult... | astro-ph | ams02 is a multipurpose spectrometer with superconducting magnet and is designed for 3 years of data taking aboard the international space station its high performance regarding particle identification and energy measurement will allow performing indirect searches for dark matter dm in different channels simultaneously... | [['ams02', 'is', 'a', 'multipurpose', 'spectrometer', 'with', 'superconducting', 'magnet', 'and', 'is', 'designed', 'for', '3', 'years', 'of', 'data', 'taking', 'aboard', 'the', 'international', 'space', 'station', 'its', 'high', 'performance', 'regarding', 'particle', 'identification', 'and', 'energy', 'measurement', ... | [-0.0985953259868456, 0.2194657097570598, -0.10446162237420532, 0.12783707930779487, -0.13042237689974262, -0.16798436123987331, 0.013461518010088042, 0.36330852989910867, -0.2417847505387138, -0.4128639211914703, 0.01934311088053601, -0.3301388441572735, 0.026650303865180296, 0.22839915064190897, 0.029663879935647928,... |
710.2459 | The average kinetic energy density of Cooper pairs above $T_c$ in ${\rm
YBa_2Cu_3O_{7-x}}$, ${\rm Bi_2Sr_2CaCu_2O_{8+\delta}}$, and ${\rm Nb}$ | We have obtained isofield curves for the square root of the average kinetic
energy density of the superconducting state for three single crystals of
underdoped $YBa_2Cu_3O_{7-x}$, an optimally doped single crystal of
$Bi_2Sr_2CaCu_2O_{8+\delta}$, and Nb. These curves, determined from isofield
magnetization versus tem... | cond-mat.supr-con cond-mat.str-el | we have obtained isofield curves for the square root of the average kinetic energy density of the superconducting state for three single crystals of underdoped yba_2cu_3o_7x an optimally doped single crystal of bi_2sr_2cacu_2o_8delta and nb these curves determined from isofield magnetization versus temperature measurem... | [['we', 'have', 'obtained', 'isofield', 'curves', 'for', 'the', 'square', 'root', 'of', 'the', 'average', 'kinetic', 'energy', 'density', 'of', 'the', 'superconducting', 'state', 'for', 'three', 'single', 'crystals', 'of', 'underdoped', 'yba_2cu_3o_7x', 'an', 'optimally', 'doped', 'single', 'crystal', 'of', 'bi_2sr_2ca... | [-0.1597247640495242, 0.20331009855141313, -0.04501435101760187, 0.022886279317411197, 0.0004133242343006463, -0.126546337499401, 0.1595830731950272, 0.33100569289948406, -0.22670875814604177, -0.2950323735856874, 0.008339935511580786, -0.390828769247251, -0.021632090039636898, 0.2584734872497361, 0.06070495668755865, ... |
710.246 | On the uniqueness for the spatially homogeneous Boltzmann equation with
a strong angular singularity | We prove an inequality on the Wasserstein distance with quadratic cost
between two solutions of the spatially homogeneous Boltzmann equation without
angular cutoff, from which we deduce some uniqueness results. In particular, we
obtain a local (in time) well-posedness result in the case of (possibly very)
soft potent... | math.AP | we prove an inequality on the wasserstein distance with quadratic cost between two solutions of the spatially homogeneous boltzmann equation without angular cutoff from which we deduce some uniqueness results in particular we obtain a local in time wellposedness result in the case of possibly very soft potentials a glo... | [['we', 'prove', 'an', 'inequality', 'on', 'the', 'wasserstein', 'distance', 'with', 'quadratic', 'cost', 'between', 'two', 'solutions', 'of', 'the', 'spatially', 'homogeneous', 'boltzmann', 'equation', 'without', 'angular', 'cutoff', 'from', 'which', 'we', 'deduce', 'some', 'uniqueness', 'results', 'in', 'particular',... | [-0.11563075117790478, 0.06447461667983959, -0.13033514971966328, 0.08178295000451054, -0.07902886221300055, -0.13225616763710327, 0.009735492567626246, 0.3578650109145952, -0.30715961022761423, -0.26033532635673234, 0.0903398816699864, -0.2542328447849233, -0.12467114083414925, 0.19620591934527393, -0.0591357466427312... |
710.2461 | The Luminosity Function of X-ray Selected Active Galactic Nuclei:
Evolution of Supermassive Black Holes at High Redshift | We present a measure of the hard (2-8 keV) X-ray luminosity function (XLF) of
Active Galactic Nuclei up to z~5. At high redshifts, the wide area coverage of
the Chandra Multiwavength Project is crucial to detect rare and luminous (Lx >
10^44 erg s^-1) AGN. The inclusion of samples from deeper published surveys,
such ... | astro-ph | we present a measure of the hard 28 kev xray luminosity function xlf of active galactic nuclei up to z5 at high redshifts the wide area coverage of the chandra multiwavength project is crucial to detect rare and luminous lx 1044 erg s1 agn the inclusion of samples from deeper published surveys such as the chandra deep ... | [['we', 'present', 'a', 'measure', 'of', 'the', 'hard', '28', 'kev', 'xray', 'luminosity', 'function', 'xlf', 'of', 'active', 'galactic', 'nuclei', 'up', 'to', 'z5', 'at', 'high', 'redshifts', 'the', 'wide', 'area', 'coverage', 'of', 'the', 'chandra', 'multiwavength', 'project', 'is', 'crucial', 'to', 'detect', 'rare',... | [-0.027055881961700834, 0.09090121136222251, -0.028310440236964496, 0.15290355342494877, -0.07510132209063158, -0.04174226310351514, 0.09407202605052589, 0.4826777181951911, -0.10406827170299948, -0.3732978923126211, 0.04784936012492835, -0.3637451990279601, 0.04937653811225573, 0.224367349952999, 0.005412630503769833,... |
710.2462 | Two-fluid model of the truncated Euler Equations | A phenomenological two-fluid model of the (time-reversible)
spectrally-truncated 3D Euler equation is proposed. The thermalized small
scales are first shown to be quasi-normal. The effective viscosity and thermal
diffusion are then determined, using EDQNM closure and Monte-Carlo numerical
computations. Finally, the m... | physics.flu-dyn | a phenomenological twofluid model of the timereversible spectrallytruncated 3d euler equation is proposed the thermalized small scales are first shown to be quasinormal the effective viscosity and thermal diffusion are then determined using edqnm closure and montecarlo numerical computations finally the model is valida... | [['a', 'phenomenological', 'twofluid', 'model', 'of', 'the', 'timereversible', 'spectrallytruncated', '3d', 'euler', 'equation', 'is', 'proposed', 'the', 'thermalized', 'small', 'scales', 'are', 'first', 'shown', 'to', 'be', 'quasinormal', 'the', 'effective', 'viscosity', 'and', 'thermal', 'diffusion', 'are', 'then', '... | [-0.10237369987174004, 0.12778078313567676, -0.14704635682262182, 0.06925041744086359, -0.07974664024576279, -0.1423275503579394, -0.0901680467775025, 0.27431350119877607, -0.3034139185744737, -0.2406875482660585, 0.08882365015701257, -0.2619604554659288, -0.1167713773736198, 0.18343837535108573, 0.05091248874668963, 0... |
710.2463 | Random close packing of granular matter | We propose an interpretation of the random close packing of granular
materials as a phase transition, and discuss the possibility of experimental
verification.
| cond-mat.soft cond-mat.stat-mech | we propose an interpretation of the random close packing of granular materials as a phase transition and discuss the possibility of experimental verification | [['we', 'propose', 'an', 'interpretation', 'of', 'the', 'random', 'close', 'packing', 'of', 'granular', 'materials', 'as', 'a', 'phase', 'transition', 'and', 'discuss', 'the', 'possibility', 'of', 'experimental', 'verification']] | [-0.16415874528415178, 0.2058958864989741, -0.090971691371954, -0.01626000974489295, -0.03915440274969391, -0.09564631681322404, 0.1403300088384877, 0.3580846546784691, -0.25925015884896985, -0.2934369484529547, 0.10638078425646476, -0.2620449959826858, -0.20854140947694363, 0.11375811048175978, -0.044526983173969, 0.1... |
710.2464 | The 26 year-long X-ray light curve and the X-ray spectrum of the BL Lac
Object 1E 1207.9+3945 in its brightest state | We studied the temporal and spectral evolution of the synchrotron emission
from the high energy peaked BL Lac object 1E 1207.9+3945. Two recent
observations have been performed by the XMM-Newton and Swift satellites; we
carried out X-ray spectral analysis for both of them, and photometry in
optical-ultraviolet filter... | astro-ph | we studied the temporal and spectral evolution of the synchrotron emission from the high energy peaked bl lac object 1e 120793945 two recent observations have been performed by the xmmnewton and swift satellites we carried out xray spectral analysis for both of them and photometry in opticalultraviolet filters for the ... | [['we', 'studied', 'the', 'temporal', 'and', 'spectral', 'evolution', 'of', 'the', 'synchrotron', 'emission', 'from', 'the', 'high', 'energy', 'peaked', 'bl', 'lac', 'object', '1e', '120793945', 'two', 'recent', 'observations', 'have', 'been', 'performed', 'by', 'the', 'xmmnewton', 'and', 'swift', 'satellites', 'we', '... | [-0.04625573997540274, 0.08850023804205613, -0.10449323875005716, 0.12671460345065078, -0.09488547431448331, -0.11709090522400892, 0.07925420926812177, 0.47956122418579, -0.20260525689675257, -0.3882865813990625, 0.09849114227287759, -0.35297760224113095, 0.02893204786277448, 0.24655575218270176, -0.018086888637536994,... |
710.2465 | A geometric construction for fractal sets and related linear operators | A way to add an extra dimension is briefly discussed.
| math.CA | a way to add an extra dimension is briefly discussed | [['a', 'way', 'to', 'add', 'an', 'extra', 'dimension', 'is', 'briefly', 'discussed']] | [-0.1454069759696722, 0.18376894627144794, -0.03725124299526215, 0.15386928381631151, -0.1628725770395249, -0.24740571598522365, -0.008947497606277466, 0.36320770867168906, -0.2699346859008074, -0.20162151623517274, 0.12465763185173273, -0.2695213398896158, -0.19880231767892836, 0.12175249420106411, -0.1515700186602771... |
710.2466 | On the dynamics of (left) orderable groups | We study left orderable groups by using dynamical methods. We apply these
techniques to study the space of orderings of these groups. We show for
instance that for the case of (non-Abelian) free groups, this space is
homeomorphic to the Cantor set. We also study the case of braid groups (for
which the space of orderi... | math.GR math.DS | we study left orderable groups by using dynamical methods we apply these techniques to study the space of orderings of these groups we show for instance that for the case of nonabelian free groups this space is homeomorphic to the cantor set we also study the case of braid groups for which the space of orderings has is... | [['we', 'study', 'left', 'orderable', 'groups', 'by', 'using', 'dynamical', 'methods', 'we', 'apply', 'these', 'techniques', 'to', 'study', 'the', 'space', 'of', 'orderings', 'of', 'these', 'groups', 'we', 'show', 'for', 'instance', 'that', 'for', 'the', 'case', 'of', 'nonabelian', 'free', 'groups', 'this', 'space', 'i... | [-0.14783127398761076, 0.11375720332287988, -0.09017510209493687, 0.07156550471135632, -0.09118252640120059, -0.05317731189136785, 0.07201488466637436, 0.37474725606729425, -0.3067002040899803, -0.226151998498625, 0.11341616579235714, -0.28784075449438434, -0.14610549755324828, 0.16421560962384166, -0.1288469936002359,... |
710.2467 | Track-Based Particle Flow | One of the most important aspects of detector development for the ILC is a
good jet energy resolution sigma_E/E. To achieve the goal of high precision
measurements sigma_E/E = 0.30/sqrt(E(GeV)} is proposed. The particle flow
approach together with highly granular calorimeters is able to reach this goal.
This paper pr... | physics.ins-det physics.data-an | one of the most important aspects of detector development for the ilc is a good jet energy resolution sigma_ee to achieve the goal of high precision measurements sigma_ee 030sqrtegev is proposed the particle flow approach together with highly granular calorimeters is able to reach this goal this paper presents a new pa... | [['one', 'of', 'the', 'most', 'important', 'aspects', 'of', 'detector', 'development', 'for', 'the', 'ilc', 'is', 'a', 'good', 'jet', 'energy', 'resolution', 'sigma_ee', 'to', 'achieve', 'the', 'goal', 'of', 'high', 'precision', 'measurements', 'sigma_ee', '030sqrtegev', 'is', 'proposed', 'the', 'particle', 'flow', 'ap... | [-0.05869744987795492, 0.10169438776475462, -0.11802326732423979, 0.01947345295709304, -0.07402082887030655, -0.14723524084774317, -0.0628467287925713, 0.3729220853223429, -0.17758990913272726, -0.3733355012032893, 0.04898587696544536, -0.294003113862369, -0.025048211507208935, 0.2248218790869918, -0.05325792065833683,... |
710.2468 | Statistics in the Landscape of Intersecting Brane Models | An approach towards a statistical survey of four dimensional supersymmetric
vacua in the string theory landscape is described and illustrated with three
examples of ensembles of intersecting D-brane models. The question whether it
is conceivable to make predictions based on statistical distributions is
discussed. Esp... | hep-th | an approach towards a statistical survey of four dimensional supersymmetric vacua in the string theory landscape is described and illustrated with three examples of ensembles of intersecting dbrane models the question whether it is conceivable to make predictions based on statistical distributions is discussed especial... | [['an', 'approach', 'towards', 'a', 'statistical', 'survey', 'of', 'four', 'dimensional', 'supersymmetric', 'vacua', 'in', 'the', 'string', 'theory', 'landscape', 'is', 'described', 'and', 'illustrated', 'with', 'three', 'examples', 'of', 'ensembles', 'of', 'intersecting', 'dbrane', 'models', 'the', 'question', 'whethe... | [-0.09807365520119474, 0.1480323047979656, -0.09564827205976109, 0.18858126911044412, -0.01363170697571492, -0.19985338713514147, -0.00614435509204042, 0.3550581161247252, -0.19510368954438667, -0.3106533442502962, 0.06650759695194565, -0.3074298317985633, -0.1376956484474048, 0.15965855774445484, -0.04569904504914321,... |
710.2469 | CP violation and final state interactions in B --> K pi pi decays | Effects of CP violation and of final state interactions between pairs of
pseudoscalar mesons are studied in three-body B+, B-, B0 and antiB0 decays into
K pi pi. An alternative approach to the isobar model for three-body B decays is
proposed. It is based on the QCD factorization approximation and the knowledge
of the... | hep-ph | effects of cp violation and of final state interactions between pairs of pseudoscalar mesons are studied in threebody b b b0 and antib0 decays into k pi pi an alternative approach to the isobar model for threebody b decays is proposed it is based on the qcd factorization approximation and the knowledge of the mesonmeso... | [['effects', 'of', 'cp', 'violation', 'and', 'of', 'final', 'state', 'interactions', 'between', 'pairs', 'of', 'pseudoscalar', 'mesons', 'are', 'studied', 'in', 'threebody', 'b', 'b', 'b0', 'and', 'antib0', 'decays', 'into', 'k', 'pi', 'pi', 'an', 'alternative', 'approach', 'to', 'the', 'isobar', 'model', 'for', 'three... | [-0.09716327512553365, 0.2616105817789331, -0.06830924988300796, 0.10637519007556023, -0.06856924052694886, -0.14549341467832486, 0.1366104250617956, 0.2630579810677551, -0.18507114497900712, -0.2196589856753199, -0.08456614472001321, -0.35828849929201556, -0.015551956381472781, 0.09816661220791889, 0.14576313194386134... |
710.247 | Lattice Approach to Light Scalars | I report on lattice QCD calculations that study the properties of the a0 and
f0 mesons.
| hep-lat | i report on lattice qcd calculations that study the properties of the a0 and f0 mesons | [['i', 'report', 'on', 'lattice', 'qcd', 'calculations', 'that', 'study', 'the', 'properties', 'of', 'the', 'a0', 'and', 'f0', 'mesons']] | [-0.12391679873690009, 0.18541280075442046, -0.10501901112729684, 0.019549561955500394, -0.01617572200484574, -0.0934236696921289, 0.12159591284580529, 0.41261759772896767, -0.13173213065601885, -0.07665301393717527, 0.02832755062263459, -0.36163593316450715, -0.06614479434210807, 0.06157560150313657, 0.162059381487779... |
710.2471 | On the effective charge of hydrophobic polyelectrolytes | In this paper we analyze the behavior of hydrophobic polyelectrolytes. It has
been proposed that this system adopts a pearl-necklace structure reminiscent of
the Rayleigh instability of a charged droplet. Using a Poisson-Boltzmann
approach, we calculate the counterion distribution around a given pearl
assuming the la... | cond-mat.soft | in this paper we analyze the behavior of hydrophobic polyelectrolytes it has been proposed that this system adopts a pearlnecklace structure reminiscent of the rayleigh instability of a charged droplet using a poissonboltzmann approach we calculate the counterion distribution around a given pearl assuming the latter to... | [['in', 'this', 'paper', 'we', 'analyze', 'the', 'behavior', 'of', 'hydrophobic', 'polyelectrolytes', 'it', 'has', 'been', 'proposed', 'that', 'this', 'system', 'adopts', 'a', 'pearlnecklace', 'structure', 'reminiscent', 'of', 'the', 'rayleigh', 'instability', 'of', 'a', 'charged', 'droplet', 'using', 'a', 'poissonbolt... | [-0.08239913787608882, 0.09239979830427884, -0.1190117285628845, 0.03617383060276273, -0.030530895584741154, -0.09445360389764647, 0.0777384348408747, 0.30476774529109263, -0.18082406885842248, -0.3439758490385102, -0.01620029159590837, -0.2865647300596712, -0.1766704335926218, 0.13969863175943092, -0.07129955354675248... |
710.2472 | EW NLO corrections to pair production of top-squarks at the LHC | Presented are complete electroweak (EW) corrections at ${\cal
O}(\alpha\alpha_{\mathrm s}^{\mathrm 2})$ to top-squark pair production at the
Large Hadron Collider (LHC) within the framework of the Minimal Supersymmetric
Standard Model (MSSM). At this order, effects from the interference of EW and
QCD contributions ha... | hep-ph | presented are complete electroweak ew corrections at cal oalphaalpha_mathrm smathrm 2 to topsquark pair production at the large hadron collider lhc within the framework of the minimal supersymmetric standard model mssm at this order effects from the interference of ew and qcd contributions have to be taken into account... | [['presented', 'are', 'complete', 'electroweak', 'ew', 'corrections', 'at', 'cal', 'oalphaalpha_mathrm', 'smathrm', '2', 'to', 'topsquark', 'pair', 'production', 'at', 'the', 'large', 'hadron', 'collider', 'lhc', 'within', 'the', 'framework', 'of', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'at', ... | [-0.02637324377281379, 0.24092810244381993, -0.06361032368709581, 0.18689106203928071, -0.009875732164570614, -0.13818348127437896, -0.00985598337801197, 0.31687870221448283, -0.19969066234800634, -0.25888438534604596, -0.008306930612336514, -0.33619104159547936, 0.07834627970911656, 0.08293916123235433, 0.077834559613... |
710.2473 | How does gas cool in DM halos? | In order to study the process of cooling in dark-matter (DM) halos and assess
how well simple models can represent it, we run a set of radiative SPH
hydrodynamical simulations of isolated halos, with gas sitting initially in
hydrostatic equilibrium within Navarro-Frenk-White (NFW) potential wells. [...]
After having ... | astro-ph | in order to study the process of cooling in darkmatter dm halos and assess how well simple models can represent it we run a set of radiative sph hydrodynamical simulations of isolated halos with gas sitting initially in hydrostatic equilibrium within navarrofrenkwhite nfw potential wells after having assessed the numer... | [['in', 'order', 'to', 'study', 'the', 'process', 'of', 'cooling', 'in', 'darkmatter', 'dm', 'halos', 'and', 'assess', 'how', 'well', 'simple', 'models', 'can', 'represent', 'it', 'we', 'run', 'a', 'set', 'of', 'radiative', 'sph', 'hydrodynamical', 'simulations', 'of', 'isolated', 'halos', 'with', 'gas', 'sitting', 'in... | [-0.04512265604400724, 0.12614477431984097, -0.0726602331787848, 0.07244397701296464, 0.00881000883735769, -0.07525222236455119, 0.04468054781493471, 0.36114576649473645, -0.1980153127604694, -0.36936630100581974, 0.08369060637727183, -0.261885127381754, 0.010997507991938722, 0.20556124232959516, 0.007389926805647169, ... |
710.2474 | Thermodynamical properties of hairy black holes in n spacetimes
dimensions | The issue concerning the existence of exact black hole solutions in presence
of non vanishing cosmological constant and scalar fields is reconsidered. With
regard to this, in investigating no-hair theorem violations, exact solutions of
gravity having as a source an interacting and conformally coupled scalar field
are... | hep-th | the issue concerning the existence of exact black hole solutions in presence of non vanishing cosmological constant and scalar fields is reconsidered with regard to this in investigating nohair theorem violations exact solutions of gravity having as a source an interacting and conformally coupled scalar field are revis... | [['the', 'issue', 'concerning', 'the', 'existence', 'of', 'exact', 'black', 'hole', 'solutions', 'in', 'presence', 'of', 'non', 'vanishing', 'cosmological', 'constant', 'and', 'scalar', 'fields', 'is', 'reconsidered', 'with', 'regard', 'to', 'this', 'in', 'investigating', 'nohair', 'theorem', 'violations', 'exact', 'so... | [-0.2106094490422794, 0.09791050878176177, -0.03465798984836327, 0.14737956251640374, -0.0819935570654114, -0.2280464779972779, -0.06772506419632039, 0.2810506153998248, -0.15091644614683777, -0.2585648366091825, 0.13640409624439487, -0.33067170795304385, -0.06430491086702501, 0.14674341668155086, -0.0532516392492009, ... |
710.2475 | Fast X-ray Oscillations During Magnetar Flares | The giant flares produced by highly magnetized neutron stars, "magnetars,"
are the brightest sources of high energy radiation outside our solar system.
Serendipitous observations with NASA's Rossi X-ray Timing Explorer (RXTE) of
the two most recent flares resulted in the discovery of high frequency
oscillations in th... | astro-ph | the giant flares produced by highly magnetized neutron stars magnetars are the brightest sources of high energy radiation outside our solar system serendipitous observations with nasas rossi xray timing explorer rxte of the two most recent flares resulted in the discovery of high frequency oscillations in their xray fl... | [['the', 'giant', 'flares', 'produced', 'by', 'highly', 'magnetized', 'neutron', 'stars', 'magnetars', 'are', 'the', 'brightest', 'sources', 'of', 'high', 'energy', 'radiation', 'outside', 'our', 'solar', 'system', 'serendipitous', 'observations', 'with', 'nasas', 'rossi', 'xray', 'timing', 'explorer', 'rxte', 'of', 't... | [-0.09563710492209725, 0.24498331251256014, -0.0243693964055054, 0.10232241909494097, -0.18882301470862245, -0.0009943777124204163, 0.08141656572939301, 0.3613222728500951, -0.1835812978844053, -0.40765704573044237, 0.1083402002749488, -0.3743894463229292, -0.016193440965956676, 0.28794526866250586, -0.0382977450125903... |
710.2476 | Effect of charge modulation in (LaVO3)m(SrVO3)n superlattices on the
insulator-metal transition | A series of epitaxial (LaVO3)6m(SrVO3)m superlattices having the same nominal
composition as La6/7Sr1/7VO3, a Mott-Hubbard insulator, were grown with
pulsed-laser deposition on [001]-oriented SrTiO3 substrates, and their
superlattice period was varied. When m=1, the insulating resistivity of
bulk-like La6/7Sr1/7VO3 i... | cond-mat.mtrl-sci cond-mat.str-el | a series of epitaxial lavo36msrvo3m superlattices having the same nominal composition as la67sr17vo3 a motthubbard insulator were grown with pulsedlaser deposition on 001oriented srtio3 substrates and their superlattice period was varied when m1 the insulating resistivity of bulklike la67sr17vo3 is obtained however an ... | [['a', 'series', 'of', 'epitaxial', 'lavo36msrvo3m', 'superlattices', 'having', 'the', 'same', 'nominal', 'composition', 'as', 'la67sr17vo3', 'a', 'motthubbard', 'insulator', 'were', 'grown', 'with', 'pulsedlaser', 'deposition', 'on', '001oriented', 'srtio3', 'substrates', 'and', 'their', 'superlattice', 'period', 'was... | [-0.15374670294369316, 0.24134497566210683, 0.007616972861936889, -0.05842335319919205, 0.02285449539700134, -0.183787224169534, 0.1249775294992295, 0.49543261020393164, -0.2451257546391379, -0.3273860484945004, 0.008456941012160055, -0.342811244816243, -0.10104730513438091, 0.179344513023702, -0.013861704855686524, 0.... |
710.2477 | Supersymmetric LHC phenomenology without a light Higgs boson | After a brief discussion of the mass of the Higgs in supersymmetry, I
introduce \lambdaSUSY, a model with an extra chiral singlet superfield in
addition to the MSSM field content. The key features of the model are: the
superpotential W=\lambda S H_d H_u with a large coupling \lambda and the
resulting lightest Higgs w... | hep-ph | after a brief discussion of the mass of the higgs in supersymmetry i introduce lambdasusy a model with an extra chiral singlet superfield in addition to the mssm field content the key features of the model are the superpotential wlambda s h_d h_u with a large coupling lambda and the resulting lightest higgs with mass a... | [['after', 'a', 'brief', 'discussion', 'of', 'the', 'mass', 'of', 'the', 'higgs', 'in', 'supersymmetry', 'i', 'introduce', 'lambdasusy', 'a', 'model', 'with', 'an', 'extra', 'chiral', 'singlet', 'superfield', 'in', 'addition', 'to', 'the', 'mssm', 'field', 'content', 'the', 'key', 'features', 'of', 'the', 'model', 'are... | [-0.11058275381186872, 0.28287890699598545, -0.009297474632772166, 0.13848842394124883, -0.0974695265000121, -0.19669668072457897, -0.03168525848160969, 0.29134368867707555, -0.19247104241146465, -0.27394060957705957, 0.029339036403297124, -0.28537758286477305, -0.02795246218362551, 0.05618012653077754, -0.008771486161... |
710.2478 | Nonmonotonic energy harvesting efficiency in biased exciton chains | We theoretically study the efficiency of energy harvesting in linear exciton
chains with an energy bias, where the initial excitation is taking place at the
high-energy end of the chain and the energy is harvested (trapped) at the other
end. The efficiency is characterized by means of the average time for the
exciton... | cond-mat.dis-nn cond-mat.mtrl-sci | we theoretically study the efficiency of energy harvesting in linear exciton chains with an energy bias where the initial excitation is taking place at the highenergy end of the chain and the energy is harvested trapped at the other end the efficiency is characterized by means of the average time for the exciton to be ... | [['we', 'theoretically', 'study', 'the', 'efficiency', 'of', 'energy', 'harvesting', 'in', 'linear', 'exciton', 'chains', 'with', 'an', 'energy', 'bias', 'where', 'the', 'initial', 'excitation', 'is', 'taking', 'place', 'at', 'the', 'highenergy', 'end', 'of', 'the', 'chain', 'and', 'the', 'energy', 'is', 'harvested', '... | [-0.14112246989602584, 0.18034849176818055, -0.0408910829945408, 0.08416219910686003, -0.004133210579389112, -0.14315664270605416, 0.07460775999030336, 0.3702304160638534, -0.29124731820155964, -0.2654438697574462, 0.03519385856108126, -0.2953452697132734, -0.07249601821890696, 0.17622814336766865, 0.04524694008014581,... |
710.2479 | Collisional stability of fermionic Feshbach molecules | Using a Feshbach resonance, we create ultracold fermionic molecules starting
from a Bose-Fermi atom gas mixture. The resulting mixture of atoms and weakly
bound molecules provides a rich system for studying few-body collisions because
of the variety of atomic collision partners for molecules; either bosonic,
fermioni... | cond-mat.other | using a feshbach resonance we create ultracold fermionic molecules starting from a bosefermi atom gas mixture the resulting mixture of atoms and weakly bound molecules provides a rich system for studying fewbody collisions because of the variety of atomic collision partners for molecules either bosonic fermionic or dis... | [['using', 'a', 'feshbach', 'resonance', 'we', 'create', 'ultracold', 'fermionic', 'molecules', 'starting', 'from', 'a', 'bosefermi', 'atom', 'gas', 'mixture', 'the', 'resulting', 'mixture', 'of', 'atoms', 'and', 'weakly', 'bound', 'molecules', 'provides', 'a', 'rich', 'system', 'for', 'studying', 'fewbody', 'collision... | [-0.11829838940018286, 0.2787080120211572, -0.05061154218202227, 0.06562185193950917, 0.05037999473344744, -0.197596834909715, 0.08264829743695393, 0.3454647392369388, -0.23392597620448705, -0.2533745008489389, -0.0734414574546279, -0.30601802561301317, -0.009786826393598418, 0.12859406917921026, 0.11578408502607365, 0... |
710.248 | Singularities of Brill-Noether loci for vector bundles on a curve | In this paper we consider the singularities of the varieties parameterizing
stable vector bundles of fixed rank and degree with sections on a smooth curve
of genus at least two. In particular, we extend results of Y. Laszlo, and of
the second author, regarding the singularities of generalized theta divisors.
| math.AG | in this paper we consider the singularities of the varieties parameterizing stable vector bundles of fixed rank and degree with sections on a smooth curve of genus at least two in particular we extend results of y laszlo and of the second author regarding the singularities of generalized theta divisors | [['in', 'this', 'paper', 'we', 'consider', 'the', 'singularities', 'of', 'the', 'varieties', 'parameterizing', 'stable', 'vector', 'bundles', 'of', 'fixed', 'rank', 'and', 'degree', 'with', 'sections', 'on', 'a', 'smooth', 'curve', 'of', 'genus', 'at', 'least', 'two', 'in', 'particular', 'we', 'extend', 'results', 'of'... | [-0.21655527201946825, 0.042706440560286864, -0.09378489595837891, 0.03442300117341802, -0.04030991879757494, -0.14718627429567277, 0.015452468560542911, 0.30326005777344106, -0.25807285994291307, -0.17378488708287476, 0.07543770786840469, -0.2841274927742779, -0.16630498901940882, 0.17505510874092578, -0.1537289700657... |
710.2481 | Stellar populations in the bulges of S0s and the formation of S0
galaxies | The stellar populations in the bulges of S0s, together with the galaxies'
dynamics, masses and globular clusters, contain very interesting clues about
their formation. I present here recent evidence suggesting that S0s are the
descendants of fading spirals whose star formation ceased.
| astro-ph | the stellar populations in the bulges of s0s together with the galaxies dynamics masses and globular clusters contain very interesting clues about their formation i present here recent evidence suggesting that s0s are the descendants of fading spirals whose star formation ceased | [['the', 'stellar', 'populations', 'in', 'the', 'bulges', 'of', 's0s', 'together', 'with', 'the', 'galaxies', 'dynamics', 'masses', 'and', 'globular', 'clusters', 'contain', 'very', 'interesting', 'clues', 'about', 'their', 'formation', 'i', 'present', 'here', 'recent', 'evidence', 'suggesting', 'that', 's0s', 'are', '... | [-0.10430846456438303, 0.127463738389668, -0.1371989692783072, 0.2031050824249784, -0.11279932967764103, -0.011374900516654764, 0.021412265827945833, 0.4696008459265743, -0.056020391306706836, -0.3439309013386567, 0.04303885864127161, -0.25157516600475427, -0.13527526209751764, 0.12529764459690168, -0.04439373796672693... |
710.2482 | Can LHC Test the See-Saw Mechanism? | We discuss the prospects for detecting right-handed neutrinos which are
introduced in the see-saw mechanism at future colliders. This requires a very
accurate cancellation between contributions from different right-handed
neutrinos to the light neutrino mass matrix. We search for possible symmetries
behind this cance... | hep-ph | we discuss the prospects for detecting righthanded neutrinos which are introduced in the seesaw mechanism at future colliders this requires a very accurate cancellation between contributions from different righthanded neutrinos to the light neutrino mass matrix we search for possible symmetries behind this cancellation... | [['we', 'discuss', 'the', 'prospects', 'for', 'detecting', 'righthanded', 'neutrinos', 'which', 'are', 'introduced', 'in', 'the', 'seesaw', 'mechanism', 'at', 'future', 'colliders', 'this', 'requires', 'a', 'very', 'accurate', 'cancellation', 'between', 'contributions', 'from', 'different', 'righthanded', 'neutrinos', ... | [-0.10779115688499241, 0.3299817806287181, -0.004357662109569425, 0.22914266287060897, -0.09464817423196066, -0.17611068306224686, 0.004298899972456552, 0.33379730756084125, -0.2471424949000634, -0.32940568578473867, 0.04908950541257149, -0.2788519987304296, -0.06147919444178808, 0.1801394900018793, 0.04128637487689654... |
710.2483 | On the arithmetical rank of a special class of minimal varieties | We study the arithmetical ranks and the cohomological dimensions of an
infinite class of Cohen-Macaulay varieties of minimal degree. Among these we
find, on the one hand, infinitely many set-theoretic complete intersections, on
the other hand examples where the arithmetical rank is arbitrarily greater than
the codime... | math.AC math.AG | we study the arithmetical ranks and the cohomological dimensions of an infinite class of cohenmacaulay varieties of minimal degree among these we find on the one hand infinitely many settheoretic complete intersections on the other hand examples where the arithmetical rank is arbitrarily greater than the codimension | [['we', 'study', 'the', 'arithmetical', 'ranks', 'and', 'the', 'cohomological', 'dimensions', 'of', 'an', 'infinite', 'class', 'of', 'cohenmacaulay', 'varieties', 'of', 'minimal', 'degree', 'among', 'these', 'we', 'find', 'on', 'the', 'one', 'hand', 'infinitely', 'many', 'settheoretic', 'complete', 'intersections', 'on... | [-0.18019135532147706, 0.058050674359385976, -0.027955114881091928, 0.11321879393530097, -0.08081817785476117, -0.19236730156030427, -0.03834739875325814, 0.28045116480875837, -0.2625693448601251, -0.2062322204694786, 0.13197108770799923, -0.32631951237612583, -0.12172325567758464, 0.21244222528122841, -0.1179297421278... |
710.2484 | Cosmological implications of the Higgs mass measurement | We assume the validity of the Standard Model up to an arbitrary high-energy
scale and discuss what information on the early stages of the Universe can be
extracted from a measurement of the Higgs mass. For Mh < 130 GeV, the Higgs
potential can develop an instability at large field values. From the absence of
excessiv... | hep-ph astro-ph hep-th | we assume the validity of the standard model up to an arbitrary highenergy scale and discuss what information on the early stages of the universe can be extracted from a measurement of the higgs mass for mh 130 gev the higgs potential can develop an instability at large field values from the absence of excessive therma... | [['we', 'assume', 'the', 'validity', 'of', 'the', 'standard', 'model', 'up', 'to', 'an', 'arbitrary', 'highenergy', 'scale', 'and', 'discuss', 'what', 'information', 'on', 'the', 'early', 'stages', 'of', 'the', 'universe', 'can', 'be', 'extracted', 'from', 'a', 'measurement', 'of', 'the', 'higgs', 'mass', 'for', 'mh', ... | [-0.1056165943844452, 0.2317956586710799, -0.10735565999928633, 0.12524781356482406, -0.05371409909560361, -0.12948393774499814, -0.005209400083130881, 0.27869437990304313, -0.24959535803515775, -0.3141389007279493, 0.08204659479917366, -0.22224434291392398, -0.07459356421188519, 0.16789562470544983, 0.0120008629005319... |
710.2485 | RHIC Low-Energy Challenges and Plans | There is significant interest in RHIC heavy ion collisions at
$\sqrt{s_{NN}}=$5--50 GeV, motivated by a search for the QCD phase transition
critical point. The lowest energies for this search are well below the nominal
RHIC gold injection collision energy of $\sqrt{s_{NN}}=19.6$ GeV. There are
several operations chal... | physics.acc-ph | there is significant interest in rhic heavy ion collisions at sqrts_nn550 gev motivated by a search for the qcd phase transition critical point the lowest energies for this search are well below the nominal rhic gold injection collision energy of sqrts_nn196 gev there are several operations challenges at rhic in this r... | [['there', 'is', 'significant', 'interest', 'in', 'rhic', 'heavy', 'ion', 'collisions', 'at', 'sqrts_nn550', 'gev', 'motivated', 'by', 'a', 'search', 'for', 'the', 'qcd', 'phase', 'transition', 'critical', 'point', 'the', 'lowest', 'energies', 'for', 'this', 'search', 'are', 'well', 'below', 'the', 'nominal', 'rhic', '... | [-0.07288858552561386, 0.22763377404036492, -0.0621678309637661, 0.08179933705097554, 0.02200046818654396, -0.13967656046642285, 0.04462044949790365, 0.40959183565880125, -0.21223691397003439, -0.3533487173679628, 0.04326437003175287, -0.34880893768154475, 0.08363415556714723, 0.23571844934730937, 0.02691865362423031, ... |
710.2486 | Measuring Fine Tuning In Supersymmetry | The solution to fine tuning is one of the principal motivations for
supersymmetry. However constraints on the parameter space of the Minimal
Supersymmetric Standard Model (MSSM) suggest it may also require fine tuning
(although to a much lesser extent). To compare this tuning with different
extensions of the Standard... | hep-ph | the solution to fine tuning is one of the principal motivations for supersymmetry however constraints on the parameter space of the minimal supersymmetric standard model mssm suggest it may also require fine tuning although to a much lesser extent to compare this tuning with different extensions of the standard model i... | [['the', 'solution', 'to', 'fine', 'tuning', 'is', 'one', 'of', 'the', 'principal', 'motivations', 'for', 'supersymmetry', 'however', 'constraints', 'on', 'the', 'parameter', 'space', 'of', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'suggest', 'it', 'may', 'also', 'require', 'fine', 'tuning', 'alt... | [-0.03391395627113525, 0.08177998024757471, -0.05656993479351513, 0.13789664816188937, -0.1273130332507814, -0.1958262846649935, 0.027066002367064357, 0.401143088999864, -0.23090830251264075, -0.34861449761956464, 0.12056009717222575, -0.23636648512911052, -0.1297774134654901, 0.18937530306963404, -0.08087680367558885,... |
710.2487 | Quantum Shared Broadcasting | A generalization of quantum broadcasting protocol is presented. Here the goal
is to copy an unknown input state into two subsystems which partially overlap.
We show that the possibility of implementing these protocols strongly depends
upon the overlap among the subsystems. Conditions for approximated shared
broadcast... | quant-ph | a generalization of quantum broadcasting protocol is presented here the goal is to copy an unknown input state into two subsystems which partially overlap we show that the possibility of implementing these protocols strongly depends upon the overlap among the subsystems conditions for approximated shared broadcasting a... | [['a', 'generalization', 'of', 'quantum', 'broadcasting', 'protocol', 'is', 'presented', 'here', 'the', 'goal', 'is', 'to', 'copy', 'an', 'unknown', 'input', 'state', 'into', 'two', 'subsystems', 'which', 'partially', 'overlap', 'we', 'show', 'that', 'the', 'possibility', 'of', 'implementing', 'these', 'protocols', 'st... | [-0.2144036117339662, 0.18906074893584446, -0.05361870214498291, 0.025903000714606605, 0.0006235378532437608, -0.20752813089832975, 0.08564227677319043, 0.3953158012203251, -0.28741826066592085, -0.2687634519922237, 0.07354768539274421, -0.2442420648682552, -0.13499987180694006, 0.16896416346814172, -0.0792109030589927... |
710.2488 | Submersions and effective descent of etale morphisms | Using the flatification by blow-up result of Raynaud and Gruson, we obtain
new results for submersive and subtrusive morphisms. We show that universally
subtrusive morphisms, and in particular universally open morphisms, are
morphisms of effective descent for the fibered category of etale morphisms. Our
results exten... | math.AG math.AC | using the flatification by blowup result of raynaud and gruson we obtain new results for submersive and subtrusive morphisms we show that universally subtrusive morphisms and in particular universally open morphisms are morphisms of effective descent for the fibered category of etale morphisms our results extend and su... | [['using', 'the', 'flatification', 'by', 'blowup', 'result', 'of', 'raynaud', 'and', 'gruson', 'we', 'obtain', 'new', 'results', 'for', 'submersive', 'and', 'subtrusive', 'morphisms', 'we', 'show', 'that', 'universally', 'subtrusive', 'morphisms', 'and', 'in', 'particular', 'universally', 'open', 'morphisms', 'are', 'm... | [-0.128237549255469, 0.01587121594431145, -0.08636456322357325, 0.1272187655459025, -0.076911685988307, -0.1633098200761846, -0.0024686297135693685, 0.3465800290927291, -0.40236781553498335, -0.2027955132403544, 0.08254797127530245, -0.22056103833019733, -0.12664168813664997, 0.2588976878805884, -0.27302987591496536, -... |
710.2489 | Moments of nucleon distribution amplitudes from irreducible three-quark
operators | Semi-exclusive and exclusive processes are becoming more and more important
in high energy physics since they are excellently suited to study the internal
hadronic structure. To analyze such processes the knowledge of the hadron
distribution amplitudes, which are universal for different reactions, is
essential. Only ... | hep-lat | semiexclusive and exclusive processes are becoming more and more important in high energy physics since they are excellently suited to study the internal hadronic structure to analyze such processes the knowledge of the hadron distribution amplitudes which are universal for different reactions is essential only rather ... | [['semiexclusive', 'and', 'exclusive', 'processes', 'are', 'becoming', 'more', 'and', 'more', 'important', 'in', 'high', 'energy', 'physics', 'since', 'they', 'are', 'excellently', 'suited', 'to', 'study', 'the', 'internal', 'hadronic', 'structure', 'to', 'analyze', 'such', 'processes', 'the', 'knowledge', 'of', 'the',... | [-0.0797246265052367, 0.2320519303872941, -0.13433188589049444, 0.13083737674394563, -0.08393278609240247, -0.10244749034078972, 0.04733852808844418, 0.4069694311748589, -0.17313841951019582, -0.2560012945244389, 0.058934054385510186, -0.2763386302447367, -0.09052946584058866, 0.14794588120383842, 0.04737903586684561, ... |
710.249 | Dimensional Reduction Applied to Non-Supersymmetric Theories | We consider regularisation of a Yang-Mills theory by Dimensional Reduction
(DRED). In particular, the anomalous dimensions of fermion masses and gauge
coupling are computed to four-loop order. We put special emphasis on the
treatment of evanescent couplings which appear when DRED is applied to
non-supersymmetric theo... | hep-th | we consider regularisation of a yangmills theory by dimensional reduction dred in particular the anomalous dimensions of fermion masses and gauge coupling are computed to fourloop order we put special emphasis on the treatment of evanescent couplings which appear when dred is applied to nonsupersymmetric theories we hi... | [['we', 'consider', 'regularisation', 'of', 'a', 'yangmills', 'theory', 'by', 'dimensional', 'reduction', 'dred', 'in', 'particular', 'the', 'anomalous', 'dimensions', 'of', 'fermion', 'masses', 'and', 'gauge', 'coupling', 'are', 'computed', 'to', 'fourloop', 'order', 'we', 'put', 'special', 'emphasis', 'on', 'the', 't... | [-0.14694004469783978, 0.1736884231446311, -0.017721586488187314, 0.11183594983012882, -0.06837130091153085, -0.15642764108488336, 0.006020646789693274, 0.33888590466231105, -0.12430043944623322, -0.2510441023623571, 0.06023986667569261, -0.2706455141014885, -0.18794602287234738, 0.11714805423689541, -0.033915646001696... |
710.2491 | The Rapid Outbursting Star GM Cep: An EX-or in Tr 37? | We present optical, IR and millimeter observations of the solar-type star
13-277, also known as GM Cep, in the 4 Myr-old cluster Tr 37. GM Cep
experiences rapid magnitude variations of more than 2 mag at optical
wavelengths. We explore the causes of the variability, which seem to be
dominated by strong increases in t... | astro-ph | we present optical ir and millimeter observations of the solartype star 13277 also known as gm cep in the 4 myrold cluster tr 37 gm cep experiences rapid magnitude variations of more than 2 mag at optical wavelengths we explore the causes of the variability which seem to be dominated by strong increases in the accretio... | [['we', 'present', 'optical', 'ir', 'and', 'millimeter', 'observations', 'of', 'the', 'solartype', 'star', '13277', 'also', 'known', 'as', 'gm', 'cep', 'in', 'the', '4', 'myrold', 'cluster', 'tr', '37', 'gm', 'cep', 'experiences', 'rapid', 'magnitude', 'variations', 'of', 'more', 'than', '2', 'mag', 'at', 'optical', 'w... | [-0.12111556631551013, 0.1622589602715002, -0.043464375440171864, 0.10764651334736168, -0.1066344463260575, -0.11663968441715031, 0.09003301322864334, 0.4306569431510127, -0.1746807472213646, -0.3280075358098033, 0.12171459341064424, -0.2258899494150431, -0.03271643272688929, 0.18762042210730226, -0.08783765291683844, ... |
710.2492 | O(a^2) cutoff effects in Wilson fermion simulations | We show that the size of the O(a^2) flavour violating cutoff artifacts that
have been found to affect the value of the neutral pion mass in simulations
with maximally twisted Wilson fermions is controlled by a continuum QCD
quantity that is fairly large and is determined by the dynamical mechanism of
spontaneous chir... | hep-lat | we show that the size of the oa2 flavour violating cutoff artifacts that have been found to affect the value of the neutral pion mass in simulations with maximally twisted wilson fermions is controlled by a continuum qcd quantity that is fairly large and is determined by the dynamical mechanism of spontaneous chiral sy... | [['we', 'show', 'that', 'the', 'size', 'of', 'the', 'oa2', 'flavour', 'violating', 'cutoff', 'artifacts', 'that', 'have', 'been', 'found', 'to', 'affect', 'the', 'value', 'of', 'the', 'neutral', 'pion', 'mass', 'in', 'simulations', 'with', 'maximally', 'twisted', 'wilson', 'fermions', 'is', 'controlled', 'by', 'a', 'co... | [-0.11133133752635964, 0.2802188745416377, -0.08217136760282776, 0.10148476451716346, -0.045594577782827876, -0.11599852569988402, 0.051988094192727104, 0.36235870440369067, -0.1927446491935331, -0.2784487422393716, 0.07613783279717293, -0.2813945631618085, -0.060620877160893184, 0.11769779919565695, -0.014368444798595... |
710.2493 | Indirect dark matter searches with H.E.S.S | The annihilations of WIMPs produce high energy gamma-rays in the final state.
These high energy gamma-rays may be detected by IACTs such as the H.E.S.S.
array of Imaging Atmospheric Cherenkov telescopes. Besides the popular targets
such as the Galactic Center or galaxy clusters such as VIRGO, dwarf spheroidal
galaxie... | astro-ph | the annihilations of wimps produce high energy gammarays in the final state these high energy gammarays may be detected by iacts such as the hess array of imaging atmospheric cherenkov telescopes besides the popular targets such as the galactic center or galaxy clusters such as virgo dwarf spheroidal galaxies are privi... | [['the', 'annihilations', 'of', 'wimps', 'produce', 'high', 'energy', 'gammarays', 'in', 'the', 'final', 'state', 'these', 'high', 'energy', 'gammarays', 'may', 'be', 'detected', 'by', 'iacts', 'such', 'as', 'the', 'hess', 'array', 'of', 'imaging', 'atmospheric', 'cherenkov', 'telescopes', 'besides', 'the', 'popular', ... | [-0.06665892750067913, 0.16479490671082642, -0.07998216301806409, 0.21528872735992385, -0.16537370427330542, -0.05769582838682389, -0.08313456760650431, 0.3807608951341266, -0.13489192176213557, -0.41815679039616416, -0.009404040538895599, -0.35419933647952145, 0.026427049730921647, 0.22249575256730034, 0.0430103360639... |
710.2494 | Soft diffraction at the LHC: a partonic interpretation | We present a `new generation' model for high energy proton-proton `soft'
interactions. It allows for a full set of multi-Pomeron vertices, as well as
including multichannel eikonal scattering. It describes the behaviour of the
proton-proton total, sigma(total), and elastic dsigma(el)/dt, cross sections
together with ... | hep-ph | we present a new generation model for high energy protonproton soft interactions it allows for a full set of multipomeron vertices as well as including multichannel eikonal scattering it describes the behaviour of the protonproton total sigmatotal and elastic dsigmaeldt cross sections together with those for low and hi... | [['we', 'present', 'a', 'new', 'generation', 'model', 'for', 'high', 'energy', 'protonproton', 'soft', 'interactions', 'it', 'allows', 'for', 'a', 'full', 'set', 'of', 'multipomeron', 'vertices', 'as', 'well', 'as', 'including', 'multichannel', 'eikonal', 'scattering', 'it', 'describes', 'the', 'behaviour', 'of', 'the'... | [-0.05760559791575789, 0.146472470675037, -0.07361623198786915, 0.15892099059830583, -0.05256976938176462, -0.0774656839624239, 0.00781446641365833, 0.34444649105562886, -0.2070183131035746, -0.3186589520315037, -0.023791528166518274, -0.36595182352680505, -0.03585415176828118, 0.15427905570250006, 0.05168142005910768,... |
710.2495 | A Continuity Theorem for Stinespring's Dilation | We show a continuity theorem for Stinespring's dilation: two completely
positive maps between arbitrary C*-algebras are close in cb-norm iff we can
find corresponding dilations that are close in operator norm. The proof
establishes the equivalence of the cb-norm distance and the Bures distance for
completely positive... | quant-ph math-ph math.MP math.OA | we show a continuity theorem for stinesprings dilation two completely positive maps between arbitrary calgebras are close in cbnorm iff we can find corresponding dilations that are close in operator norm the proof establishes the equivalence of the cbnorm distance and the bures distance for completely positive maps we ... | [['we', 'show', 'a', 'continuity', 'theorem', 'for', 'stinesprings', 'dilation', 'two', 'completely', 'positive', 'maps', 'between', 'arbitrary', 'calgebras', 'are', 'close', 'in', 'cbnorm', 'iff', 'we', 'can', 'find', 'corresponding', 'dilations', 'that', 'are', 'close', 'in', 'operator', 'norm', 'the', 'proof', 'esta... | [-0.14383421609610586, 0.1432487334220371, -0.08919011595727559, 0.14230461352105653, -0.011589258310518094, -0.17832465470668726, -0.00749745148225754, 0.4025078574528119, -0.3593245953587549, -0.16778987276068488, 0.10719276620823491, -0.3321969036977472, -0.17340826545010454, 0.17702889031664068, -0.1342388195418087... |
710.2496 | Regression estimation from an individual stable sequence | We consider univariate regression estimation from an individual (non-random)
sequence $(x_1,y_1),(x_2,y_2), ... \in \real \times \real$, which is stable in
the sense that for each interval $A \subseteq \real$, (i) the limiting relative
frequency of $A$ under $x_1, x_2, ...$ is governed by an unknown probability
distr... | math.PR cs.IT math.IT math.ST stat.TH | we consider univariate regression estimation from an individual nonrandom sequence x_1y_1x_2y_2 in real times real which is stable in the sense that for each interval a subseteq real i the limiting relative frequency of a under x_1 x_2 is governed by an unknown probability distribution mu and ii the limiting average of... | [['we', 'consider', 'univariate', 'regression', 'estimation', 'from', 'an', 'individual', 'nonrandom', 'sequence', 'x_1y_1x_2y_2', 'in', 'real', 'times', 'real', 'which', 'is', 'stable', 'in', 'the', 'sense', 'that', 'for', 'each', 'interval', 'a', 'subseteq', 'real', 'i', 'the', 'limiting', 'relative', 'frequency', 'o... | [-0.12975327960440527, 0.11771315524318246, -0.04007971300837278, 0.04757848215342543, 0.0019215146789089744, -0.19685550557524467, 0.034596822460513287, 0.41652913577229583, -0.28141499623256244, -0.18951099944119684, 0.11230767355144224, -0.28240625467776453, -0.14654491813978393, 0.19634179852827882, -0.120924786986... |
710.2497 | A Categorical Construction of Ultrafilters | Ultrafilters are useful mathematical objects having applications in
nonstandard analysis, Ramsey theory, Boolean algebra, topology, and other areas
of mathematics. In this note, we provide a categorical construction of
ultrafilters in terms of the inverse limit of an inverse family of finite
partitions; this is an el... | math.CT math.GM math.GN | ultrafilters are useful mathematical objects having applications in nonstandard analysis ramsey theory boolean algebra topology and other areas of mathematics in this note we provide a categorical construction of ultrafilters in terms of the inverse limit of an inverse family of finite partitions this is an elementary ... | [['ultrafilters', 'are', 'useful', 'mathematical', 'objects', 'having', 'applications', 'in', 'nonstandard', 'analysis', 'ramsey', 'theory', 'boolean', 'algebra', 'topology', 'and', 'other', 'areas', 'of', 'mathematics', 'in', 'this', 'note', 'we', 'provide', 'a', 'categorical', 'construction', 'of', 'ultrafilters', 'i... | [-0.07995274664859313, 0.10370653967500501, -0.11087276693433523, 0.14021937802396212, -0.133729681901231, -0.06349082467951686, 0.054063421968257405, 0.3155796232230559, -0.3287751336355467, -0.2442292440116305, 0.11145836921452822, -0.23802674616072672, -0.17012796722229798, 0.19806580952796582, -0.1918164628016687, ... |
710.2498 | Scaling and low energy constants in lattice QCD with N_f=2 maximally
twisted Wilson quarks | We report on the scaling of basic hadronic observables in lattice QCD with
N_f=2 maximally twisted Wilson dynamical quarks. We give preliminary results
for some of the Gasser-Leutwyler low energy constants, the chiral condensate
and the average mass of u and d quarks.
| hep-lat | we report on the scaling of basic hadronic observables in lattice qcd with n_f2 maximally twisted wilson dynamical quarks we give preliminary results for some of the gasserleutwyler low energy constants the chiral condensate and the average mass of u and d quarks | [['we', 'report', 'on', 'the', 'scaling', 'of', 'basic', 'hadronic', 'observables', 'in', 'lattice', 'qcd', 'with', 'n_f2', 'maximally', 'twisted', 'wilson', 'dynamical', 'quarks', 'we', 'give', 'preliminary', 'results', 'for', 'some', 'of', 'the', 'gasserleutwyler', 'low', 'energy', 'constants', 'the', 'chiral', 'cond... | [-0.15380200955930146, 0.3510634074485752, -0.08723726250274583, 0.060412697667299314, -0.0018196989468103925, -0.08687201150162362, 0.10812229637143224, 0.37993480698313825, -0.11388571809998951, -0.20115865754006906, 0.024049766218224758, -0.3013726741422054, -0.014708866062032621, 0.07452592446447112, 0.052642731689... |
710.2499 | Dynamical instability of the XY spiral state of ferromagnetic
condensates | We calculate the spectrum of collective excitations of the XY spiral state
prepared adiabatically or suddenly from a uniform ferromagnetic F=1 condensate.
For spiral wavevectors past a critical value, spin wave excitation energies
become imaginary indicating a dynamical instability. We construct phase
diagrams as fun... | cond-mat.other | we calculate the spectrum of collective excitations of the xy spiral state prepared adiabatically or suddenly from a uniform ferromagnetic f1 condensate for spiral wavevectors past a critical value spin wave excitation energies become imaginary indicating a dynamical instability we construct phase diagrams as functions... | [['we', 'calculate', 'the', 'spectrum', 'of', 'collective', 'excitations', 'of', 'the', 'xy', 'spiral', 'state', 'prepared', 'adiabatically', 'or', 'suddenly', 'from', 'a', 'uniform', 'ferromagnetic', 'f1', 'condensate', 'for', 'spiral', 'wavevectors', 'past', 'a', 'critical', 'value', 'spin', 'wave', 'excitation', 'en... | [-0.2730170988764327, 0.28326612392153877, -0.10975053581373337, 0.07820984830435079, -0.06920447883861086, -0.1072972053326129, 0.04434340366592201, 0.3795935007242056, -0.23236555465532896, -0.1959883845814217, -0.03048979782929214, -0.28873940729177916, -0.05164392719206472, 0.14046472871156696, 0.2043239968793037, ... |
710.25 | Density estimation from an individual numerical sequence | This paper considers estimation of a univariate density from an individual
numerical sequence. It is assumed that (i) the limiting relative frequencies of
the numerical sequence are governed by an unknown density, and (ii) there is a
known upper bound for the variation of the density on an increasing sequence of
inte... | math.PR cs.IT math.IT math.ST stat.TH | this paper considers estimation of a univariate density from an individual numerical sequence it is assumed that i the limiting relative frequencies of the numerical sequence are governed by an unknown density and ii there is a known upper bound for the variation of the density on an increasing sequence of intervals a ... | [['this', 'paper', 'considers', 'estimation', 'of', 'a', 'univariate', 'density', 'from', 'an', 'individual', 'numerical', 'sequence', 'it', 'is', 'assumed', 'that', 'i', 'the', 'limiting', 'relative', 'frequencies', 'of', 'the', 'numerical', 'sequence', 'are', 'governed', 'by', 'an', 'unknown', 'density', 'and', 'ii',... | [-0.11371828811799946, 0.08726233602219904, -0.06372432049829513, 0.049599876219872385, 0.00015493780981911266, -0.14235703064047772, 0.02838810800028074, 0.40582214742291556, -0.24452237047902917, -0.2666342275308283, 0.12956208684962525, -0.2464059390552828, -0.16080966198047542, 0.20483853738329819, -0.1194395321704... |
710.2501 | nuMSM and its experimental tests | $\nu$MSM is a minimal renormalizable extension of the Standard Model by right
handed neutrinos. This model explains the neutrino oscillations and provides a
candidate for the Dark Matter and a mechanism of baryon number generation in
the Early Universe. We discuss here existing constraints on the model and
possible c... | hep-ph | numsm is a minimal renormalizable extension of the standard model by right handed neutrinos this model explains the neutrino oscillations and provides a candidate for the dark matter and a mechanism of baryon number generation in the early universe we discuss here existing constraints on the model and possible conseque... | [['numsm', 'is', 'a', 'minimal', 'renormalizable', 'extension', 'of', 'the', 'standard', 'model', 'by', 'right', 'handed', 'neutrinos', 'this', 'model', 'explains', 'the', 'neutrino', 'oscillations', 'and', 'provides', 'a', 'candidate', 'for', 'the', 'dark', 'matter', 'and', 'a', 'mechanism', 'of', 'baryon', 'number', ... | [-0.10527661216699265, 0.20599984636699611, -0.03996186768636108, 0.20191158818250352, -0.13145187842574987, -0.1301664752462371, 0.06273597292602062, 0.2566543332978406, -0.21447282707826656, -0.32792731757191096, 0.055262512559155846, -0.27740634718740526, -0.07268662968311798, 0.18648534648713064, 0.0462221305775032... |
710.2502 | Search for rare b-meson decays at CDF | We report on the search for $B^0_s\to\mu^+\mu^-$, $B^0_d\to\mu^+\mu^-$ decays
and $b\to s \mu^+\mu^-$ transitions in exclusive decays of B mesons using the
CDF II detector at the Fermilab Tevatron Collider. Using 2 fb$^{-1}$ of Run II
data we find upper limits on the branching fractions
$\mathcal{B}(B^0_s\to\mu^+\mu^... | hep-ex | we report on the search for b0_stomumu b0_dtomumu decays and bto s mumu transitions in exclusive decays of b mesons using the cdf ii detector at the fermilab tevatron collider using 2 fb1 of run ii data we find upper limits on the branching fractions mathcalbb0_stomumu58times 108 and mathcalbb0_dtomumu18times 108 at 95... | [['we', 'report', 'on', 'the', 'search', 'for', 'b0_stomumu', 'b0_dtomumu', 'decays', 'and', 'bto', 's', 'mumu', 'transitions', 'in', 'exclusive', 'decays', 'of', 'b', 'mesons', 'using', 'the', 'cdf', 'ii', 'detector', 'at', 'the', 'fermilab', 'tevatron', 'collider', 'using', '2', 'fb1', 'of', 'run', 'ii', 'data', 'we'... | [-0.04145929189312651, 0.22652922140112447, 0.01255668845763545, 0.0931884346552837, 0.006384714311103762, -0.12702801848911208, 0.22943001097056692, 0.23814634170475196, -0.06356044317147246, -0.30778688923628245, 0.013027420812171458, -0.44007383277754725, 0.1747490818163863, 0.14234929921588413, 0.15691545878157573,... |
710.2503 | On the mass formula and Wigner and curvature energy terms | The efficiency of different mass formulas derived from the liquid drop model
including or not the curvature energy, the Wigner term and different powers of
the relative neutron excess $I$ has been determined by a least square fitting
procedure to the experimental atomic masses assuming a constant
R$_{0,charge}$/A$^{1... | nucl-ex | the efficiency of different mass formulas derived from the liquid drop model including or not the curvature energy the wigner term and different powers of the relative neutron excess i has been determined by a least square fitting procedure to the experimental atomic masses assuming a constant r_0chargea13 ratio the wi... | [['the', 'efficiency', 'of', 'different', 'mass', 'formulas', 'derived', 'from', 'the', 'liquid', 'drop', 'model', 'including', 'or', 'not', 'the', 'curvature', 'energy', 'the', 'wigner', 'term', 'and', 'different', 'powers', 'of', 'the', 'relative', 'neutron', 'excess', 'i', 'has', 'been', 'determined', 'by', 'a', 'le... | [-0.07285533820758436, 0.15691660952265604, -0.07999746127533588, 0.08847031285894094, -0.011070748796285416, -0.1156312895098489, 0.07465112779178831, 0.3309361805567647, -0.22469187804525442, -0.3704080802531415, 0.03291135560260108, -0.28993793717115235, 0.011221160681106814, 0.16321791233817615, -0.0083312203058463... |
710.2504 | Electronic band structure and exchange coupling constants in ACr2X4
spinels | We present the results of band structure calculations for ACr2X4 (A=Zn, Cd,
Hg and X=O, S, Se) spinels. Effective exchange coupling constants between Cr
spins are determined by fitting the energy of spin spirals to a classical
Heisenberg model. The calculations reproduce the change of the sign of the
dominant nearest... | cond-mat.other cond-mat.str-el | we present the results of band structure calculations for acr2x4 azn cd hg and xo s se spinels effective exchange coupling constants between cr spins are determined by fitting the energy of spin spirals to a classical heisenberg model the calculations reproduce the change of the sign of the dominant nearestneighbor exc... | [['we', 'present', 'the', 'results', 'of', 'band', 'structure', 'calculations', 'for', 'acr2x4', 'azn', 'cd', 'hg', 'and', 'xo', 's', 'se', 'spinels', 'effective', 'exchange', 'coupling', 'constants', 'between', 'cr', 'spins', 'are', 'determined', 'by', 'fitting', 'the', 'energy', 'of', 'spin', 'spirals', 'to', 'a', 'c... | [-0.1516980124774893, 0.16976433303245328, 0.059802830808502086, 0.10234248924324839, -0.051359989997152175, -0.18793961293155664, 0.07256198931508316, 0.4311432395680029, -0.26094520388201614, -0.27678576551881606, -0.04124748410626513, -0.37502549200883656, -0.07954803234917832, 0.13233631502523957, 0.139756931877527... |
710.2505 | Generic Trace Semantics via Coinduction | Trace semantics has been defined for various kinds of state-based systems,
notably with different forms of branching such as non-determinism vs.
probability. In this paper we claim to identify one underlying mathematical
structure behind these "trace semantics," namely coinduction in a Kleisli
category. This claim is... | cs.LO | trace semantics has been defined for various kinds of statebased systems notably with different forms of branching such as nondeterminism vs probability in this paper we claim to identify one underlying mathematical structure behind these trace semantics namely coinduction in a kleisli category this claim is based on o... | [['trace', 'semantics', 'has', 'been', 'defined', 'for', 'various', 'kinds', 'of', 'statebased', 'systems', 'notably', 'with', 'different', 'forms', 'of', 'branching', 'such', 'as', 'nondeterminism', 'vs', 'probability', 'in', 'this', 'paper', 'we', 'claim', 'to', 'identify', 'one', 'underlying', 'mathematical', 'struc... | [-0.09661683246233958, 0.023046443873139203, -0.12896337432852178, 0.11520404968295975, -0.12554748396577084, -0.09444473519627201, 0.040949403766844944, 0.37124590391881374, -0.374103713886845, -0.23562516218966298, 0.07199448997689933, -0.16127894862898087, -0.12636278941410414, 0.15354404457142218, -0.18759982753953... |
710.2506 | Stochastic Integrals and Evolution Equations with Gaussian Random Fields | The paper studies stochastic integration with respect to Gaussian processes
and fields. It is more convenient to work with a field than a process: by
definition, a field is a collection of stochastic integrals for a class of
deterministic integrands. The problem is then to extend the definition to
random integrands. ... | math.PR math.AP | the paper studies stochastic integration with respect to gaussian processes and fields it is more convenient to work with a field than a process by definition a field is a collection of stochastic integrals for a class of deterministic integrands the problem is then to extend the definition to random integrands an orth... | [['the', 'paper', 'studies', 'stochastic', 'integration', 'with', 'respect', 'to', 'gaussian', 'processes', 'and', 'fields', 'it', 'is', 'more', 'convenient', 'to', 'work', 'with', 'a', 'field', 'than', 'a', 'process', 'by', 'definition', 'a', 'field', 'is', 'a', 'collection', 'of', 'stochastic', 'integrals', 'for', 'a... | [-0.11576213968883091, 0.10180170246912744, -0.1110378969864812, 0.07676214799069062, -0.1151246763111577, -0.07166546475034484, 0.02936346351153656, 0.349286170845682, -0.29454149228466814, -0.2165066918482319, 0.11512076950147132, -0.2282434607719356, -0.1954704143784263, 0.22854651128950199, -0.0684405797476734, 0.0... |
710.2507 | Stochastic suspensions of heavy particles | Turbulent suspensions of heavy particles in incompressible flows have gained
much attention in recent years. A large amount of work focused on the impact
that the inertia and the dissipative dynamics of the particles have on their
dynamical and statistical properties. Substantial progress followed from the
study of s... | nlin.CD cond-mat.stat-mech physics.flu-dyn | turbulent suspensions of heavy particles in incompressible flows have gained much attention in recent years a large amount of work focused on the impact that the inertia and the dissipative dynamics of the particles have on their dynamical and statistical properties substantial progress followed from the study of suspe... | [['turbulent', 'suspensions', 'of', 'heavy', 'particles', 'in', 'incompressible', 'flows', 'have', 'gained', 'much', 'attention', 'in', 'recent', 'years', 'a', 'large', 'amount', 'of', 'work', 'focused', 'on', 'the', 'impact', 'that', 'the', 'inertia', 'and', 'the', 'dissipative', 'dynamics', 'of', 'the', 'particles', ... | [-0.1095409591454871, 0.15360094985745273, -0.10017102373061343, 0.0330911039889447, -0.02659419136072852, -0.06900432864707835, -0.028872194763937452, 0.3241734459876404, -0.2398126895508146, -0.2819218861173337, 0.056873160483157645, -0.26462069543198363, -0.13794357383070405, 0.20523411244881062, -0.0528638808666701... |
710.2508 | Right-Chiral Sneutrino LSP in mSUGRA: Event characteristics of NLSP at
the LHC | We study a supersymmetric scenario where the lighter tau-sneutrino is the
lightest supersymmetric particle, while the lighter stau-state is the next
lightest. Such a scenario can be motivated within the framework of minimal
supergravity, with just the addition of a right-chiral neutrino superfield.
Such a spectrum le... | hep-ph | we study a supersymmetric scenario where the lighter tausneutrino is the lightest supersymmetric particle while the lighter staustate is the next lightest such a scenario can be motivated within the framework of minimal supergravity with just the addition of a rightchiral neutrino superfield such a spectrum leads to ra... | [['we', 'study', 'a', 'supersymmetric', 'scenario', 'where', 'the', 'lighter', 'tausneutrino', 'is', 'the', 'lightest', 'supersymmetric', 'particle', 'while', 'the', 'lighter', 'staustate', 'is', 'the', 'next', 'lightest', 'such', 'a', 'scenario', 'can', 'be', 'motivated', 'within', 'the', 'framework', 'of', 'minimal',... | [-0.059019843900188954, 0.25662139878783485, -0.0563347303575956, 0.16396493815337446, -0.06908917425218786, -0.17548462925571026, -0.001060783502295392, 0.30753639049477655, -0.22108467695957953, -0.29808369040775046, 0.06580739823229943, -0.2944838776907856, -0.038991806180317806, 0.15184038854780432, -0.020869447252... |
710.2509 | Locally Compact Objects in Exact Categories | We identify two categories of locally compact objects on an exact category A.
They correspond to the well-known constructions of the Beilinson category lim A
and the Kato category k(A). We study their mutual relations and compare the two
constructions. We prove that lim A is an exact category, which gives to this
cat... | math.CT math.KT | we identify two categories of locally compact objects on an exact category a they correspond to the wellknown constructions of the beilinson category lim a and the kato category ka we study their mutual relations and compare the two constructions we prove that lim a is an exact category which gives to this category a v... | [['we', 'identify', 'two', 'categories', 'of', 'locally', 'compact', 'objects', 'on', 'an', 'exact', 'category', 'a', 'they', 'correspond', 'to', 'the', 'wellknown', 'constructions', 'of', 'the', 'beilinson', 'category', 'lim', 'a', 'and', 'the', 'kato', 'category', 'ka', 'we', 'study', 'their', 'mutual', 'relations', ... | [-0.13891681486692947, 0.002551597255878111, -0.0812595433428183, 0.13394815128189153, -0.08849729262451586, -0.11984752296493986, 0.008537439211534385, 0.39490248301090336, -0.370221829540335, -0.20687358545410073, 0.08557868577762802, -0.20631684588952962, -0.11957688795195685, 0.23109314329603797, -0.195147960136334... |
710.251 | Intracellular microrheology of motile Amoeba proteus | The motility of motile Amoeba proteus was examined using the technique of
passive particle tracking microrheology, with the aid of newly-developed
particle tracking software, a fast digital camera and an optical microscope. We
tracked large numbers of endogeneous particles in the amoebae, which displayed
subdiffusive... | cond-mat.soft q-bio.CB | the motility of motile amoeba proteus was examined using the technique of passive particle tracking microrheology with the aid of newlydeveloped particle tracking software a fast digital camera and an optical microscope we tracked large numbers of endogeneous particles in the amoebae which displayed subdiffusive motion... | [['the', 'motility', 'of', 'motile', 'amoeba', 'proteus', 'was', 'examined', 'using', 'the', 'technique', 'of', 'passive', 'particle', 'tracking', 'microrheology', 'with', 'the', 'aid', 'of', 'newlydeveloped', 'particle', 'tracking', 'software', 'a', 'fast', 'digital', 'camera', 'and', 'an', 'optical', 'microscope', 'w... | [-0.14082085476299497, 0.2101412814477155, -0.10665794992365124, -0.015123545474702174, -0.027829051196998234, -0.14678100358535787, -0.062166366117109156, 0.3608906812456198, -0.29998884970310186, -0.24660218228932423, 0.04368725372975261, -0.26126081546734475, -0.17221409212457153, 0.18016108458935534, -0.06279246721... |
710.2511 | Thermal effects in exciton harvesting in biased one-dimensional systems | The study of energy harvesting in chain-like structures is important due to
its relevance to a variety of interesting physical systems. Harvesting is
understood as the combination of exciton transport through intra-band exciton
relaxation (via scattering on phonon modes) and subsequent quenching by a trap.
Previously... | cond-mat.dis-nn cond-mat.mtrl-sci | the study of energy harvesting in chainlike structures is important due to its relevance to a variety of interesting physical systems harvesting is understood as the combination of exciton transport through intraband exciton relaxation via scattering on phonon modes and subsequent quenching by a trap previously we have... | [['the', 'study', 'of', 'energy', 'harvesting', 'in', 'chainlike', 'structures', 'is', 'important', 'due', 'to', 'its', 'relevance', 'to', 'a', 'variety', 'of', 'interesting', 'physical', 'systems', 'harvesting', 'is', 'understood', 'as', 'the', 'combination', 'of', 'exciton', 'transport', 'through', 'intraband', 'exci... | [-0.14630267275112732, 0.18523503605060146, -0.05479202351333307, 0.057412824066497184, -0.026870502502008873, -0.15531914849166892, 0.05016419014282292, 0.42166798638312947, -0.27790835757124505, -0.28036256927797304, 0.04718039550789399, -0.25186780441435985, -0.13725015753464373, 0.219744990957614, 0.008484803527397... |
710.2512 | Monodromy transform approach in the theory of integrable reductions of
Einstein's field equations and some applications | A brief sketch of the formulation of the monodromy transform approach and
corresponding integral equation methods as well as of various applications of
this approach for solution of integrable symmetry reductions of Einstein's
field equations is presented.
| gr-qc | a brief sketch of the formulation of the monodromy transform approach and corresponding integral equation methods as well as of various applications of this approach for solution of integrable symmetry reductions of einsteins field equations is presented | [['a', 'brief', 'sketch', 'of', 'the', 'formulation', 'of', 'the', 'monodromy', 'transform', 'approach', 'and', 'corresponding', 'integral', 'equation', 'methods', 'as', 'well', 'as', 'of', 'various', 'applications', 'of', 'this', 'approach', 'for', 'solution', 'of', 'integrable', 'symmetry', 'reductions', 'of', 'einst... | [-0.10545558593160398, -0.026498217355913005, -0.13850900367204402, 0.0763131252716522, -0.11534703335397549, -0.12015611875953304, -0.06748987301378637, 0.2699014278682503, -0.2922159617615713, -0.31062859759942907, 0.16876721935900482, -0.24950436965839282, -0.23362841145009608, 0.22462087332560504, -0.05708099969637... |
710.2513 | Structural dependence of robustness and load tolerance in scale-free
networks | The structure of complex networks in previous research has been widely
described as scale-free networks generated by the preferential attachment
model. However, the preferential attachment model does not take into account
the detailed topological property observed in real networks. Here we propose
the models of scale... | cond-mat.dis-nn | the structure of complex networks in previous research has been widely described as scalefree networks generated by the preferential attachment model however the preferential attachment model does not take into account the detailed topological property observed in real networks here we propose the models of scalefree n... | [['the', 'structure', 'of', 'complex', 'networks', 'in', 'previous', 'research', 'has', 'been', 'widely', 'described', 'as', 'scalefree', 'networks', 'generated', 'by', 'the', 'preferential', 'attachment', 'model', 'however', 'the', 'preferential', 'attachment', 'model', 'does', 'not', 'take', 'into', 'account', 'the',... | [-0.14342007206287236, 0.12489722207841017, -0.025933193671517075, 0.09300010040557632, -0.03290173965506256, -0.23735415521077813, 0.035221329300353925, 0.4448058009186449, -0.25843887082786143, -0.27407069656377037, 0.03690272399884028, -0.2699839883852595, -0.305797726501684, 0.10229591122285152, -0.0781790169693219... |
710.2514 | A possible source of spin-polarized electrons: The inert
graphene/Ni(111) system | We report on an investigation of spin-polarized secondary electron emission
from the chemically inert system: graphene/Ni(111). An ordered passivated
graphene layer (monolayer of graphite, MG) was formed on Ni(111) surface via
cracking of propylene gas. The spin-polarization of the secondary electrons
obtained from t... | cond-mat.mtrl-sci | we report on an investigation of spinpolarized secondary electron emission from the chemically inert system grapheneni111 an ordered passivated graphene layer monolayer of graphite mg was formed on ni111 surface via cracking of propylene gas the spinpolarization of the secondary electrons obtained from this system upon... | [['we', 'report', 'on', 'an', 'investigation', 'of', 'spinpolarized', 'secondary', 'electron', 'emission', 'from', 'the', 'chemically', 'inert', 'system', 'grapheneni111', 'an', 'ordered', 'passivated', 'graphene', 'layer', 'monolayer', 'of', 'graphite', 'mg', 'was', 'formed', 'on', 'ni111', 'surface', 'via', 'cracking... | [-0.08100263504853832, 0.1801342923615514, -0.02273660748985342, -0.017445741552034055, 0.03981137275695801, -0.19572374255883254, 0.12414837915408002, 0.4344448156824166, -0.25647763890976255, -0.3053596557371996, -0.06507858860475774, -0.36333370979198, -0.0613150172020224, 0.1912684604096946, -0.0010219554850746963,... |
710.2515 | Superposition of fields of two Reissner - Nordstrom sources | In this paper we present a 5-parametric family of static asymptotically flat
solutions for the superposed gravitational and electromagnetic fields of two
Reissner-Nordstr\"om sources with arbitrary parameters -- masses, charges and
separating distance. A procedure for solving of the linear singular integral
equation ... | gr-qc | in this paper we present a 5parametric family of static asymptotically flat solutions for the superposed gravitational and electromagnetic fields of two reissnernordstrom sources with arbitrary parameters masses charges and separating distance a procedure for solving of the linear singular integral equation form of the... | [['in', 'this', 'paper', 'we', 'present', 'a', '5parametric', 'family', 'of', 'static', 'asymptotically', 'flat', 'solutions', 'for', 'the', 'superposed', 'gravitational', 'and', 'electromagnetic', 'fields', 'of', 'two', 'reissnernordstrom', 'sources', 'with', 'arbitrary', 'parameters', 'masses', 'charges', 'and', 'sep... | [-0.19856304471225789, 0.06637290341313928, -0.09478546337729009, 0.06102142288194348, -0.07426392748796691, -0.12770246864723353, -0.013786299899220467, 0.2897475225307668, -0.19387984092657765, -0.2529654981131898, 0.10412820433654511, -0.2925932701677084, -0.1051022769495224, 0.17240363292900535, -0.0128150132523539... |
710.2516 | Are there compact heavy four-quark bound states? | We present an exact method to study four-quark systems based on the
hyperspherical harmonics formalism. We apply it to several physical systems of
interest containing two heavy and two light quarks using different quark-quark
potentials. Our conclusions mark the boundaries for the possible existence of
compact, non-m... | hep-ph hep-ex nucl-th | we present an exact method to study fourquark systems based on the hyperspherical harmonics formalism we apply it to several physical systems of interest containing two heavy and two light quarks using different quarkquark potentials our conclusions mark the boundaries for the possible existence of compact nonmolecular... | [['we', 'present', 'an', 'exact', 'method', 'to', 'study', 'fourquark', 'systems', 'based', 'on', 'the', 'hyperspherical', 'harmonics', 'formalism', 'we', 'apply', 'it', 'to', 'several', 'physical', 'systems', 'of', 'interest', 'containing', 'two', 'heavy', 'and', 'two', 'light', 'quarks', 'using', 'different', 'quarkq... | [-0.11866264385445154, 0.21623922749302651, -0.14893630058230722, 0.11117965866099386, -0.01918822799480575, -0.14810820537044064, 0.05496926121961544, 0.32334777410416043, -0.16265952889533603, -0.21276725500493365, -0.03038019459174179, -0.27712859192534406, -0.05349164526526104, 0.12026147303335807, 0.06609185334356... |
710.2517 | Gluon Saturation and Black Hole Criticality | We discuss the recent proposal in hep-th/0611312 where it was shown that the
critical anomalous dimension associated to the onset of non-linear effects in
the high energy limit of QCD coincides with the critical exponent governing the
radius of the black hole formed in the spherically symmetric collapse of a
massless... | hep-th | we discuss the recent proposal in hepth0611312 where it was shown that the critical anomalous dimension associated to the onset of nonlinear effects in the high energy limit of qcd coincides with the critical exponent governing the radius of the black hole formed in the spherically symmetric collapse of a massless scal... | [['we', 'discuss', 'the', 'recent', 'proposal', 'in', 'hepth0611312', 'where', 'it', 'was', 'shown', 'that', 'the', 'critical', 'anomalous', 'dimension', 'associated', 'to', 'the', 'onset', 'of', 'nonlinear', 'effects', 'in', 'the', 'high', 'energy', 'limit', 'of', 'qcd', 'coincides', 'with', 'the', 'critical', 'expone... | [-0.159050118977281, 0.16870976098694077, -0.10055563285512696, 0.058421157809023405, -0.0428008145934559, -0.09272206311737348, -0.015558082082560916, 0.2839648713098657, -0.2020055980708702, -0.22863559874432876, 0.05322944231881039, -0.2613683382917504, -0.13729297847459024, 0.12669601578517517, 0.001018258220869767... |
710.2518 | Variations of the high-level Balmer line spectrum of the helium-strong
star Sigma Orionis E | Using the high-level Balmer lines and continuum, we trace the density
structure of two magnetospheric disk segments of the prototypical Bp star sigma
Ori E (B2p) as these segments occult portions of the star during the rotational
cycle. High-resolution spectra of the Balmer lines >H9 and Balmer edge were
obtained on ... | astro-ph | using the highlevel balmer lines and continuum we trace the density structure of two magnetospheric disk segments of the prototypical bp star sigma ori e b2p as these segments occult portions of the star during the rotational cycle highresolution spectra of the balmer lines h9 and balmer edge were obtained on seven nig... | [['using', 'the', 'highlevel', 'balmer', 'lines', 'and', 'continuum', 'we', 'trace', 'the', 'density', 'structure', 'of', 'two', 'magnetospheric', 'disk', 'segments', 'of', 'the', 'prototypical', 'bp', 'star', 'sigma', 'ori', 'e', 'b2p', 'as', 'these', 'segments', 'occult', 'portions', 'of', 'the', 'star', 'during', 't... | [-0.08098718858804532, 0.11992827854019676, -0.04256441562674604, 0.06607847859517538, -0.031013823651771685, -0.08618289147699743, 0.0594015731006866, 0.4562522705742403, -0.20634043474394576, -0.3475125890213793, 0.08257162976787685, -0.3085384668810363, -0.03837734198152207, 0.18343468049026437, -0.04648898505952377... |
710.2519 | Using $K^0\pi^-\to\pi^-$ transitions to compute $K\to(\pi\pi)_{I=0}$
decay amplitudes at NLO in the chiral expansion | It is proposed to compute matrix elements for the (unphysical) $K^0\pi^-\to
\pi^-$ transition to determine the next-to-leading order low energy constants
of the weak chiral Lagrangian. This allows us to evaluate $K\to(\pi\pi)_{I=0}$
decay amplitudes at this level of precision. This approach has several
significant ad... | hep-lat | it is proposed to compute matrix elements for the unphysical k0pito pi transition to determine the nexttoleading order low energy constants of the weak chiral lagrangian this allows us to evaluate ktopipi_i0 decay amplitudes at this level of precision this approach has several significant advantages over the use of kto... | [['it', 'is', 'proposed', 'to', 'compute', 'matrix', 'elements', 'for', 'the', 'unphysical', 'k0pito', 'pi', 'transition', 'to', 'determine', 'the', 'nexttoleading', 'order', 'low', 'energy', 'constants', 'of', 'the', 'weak', 'chiral', 'lagrangian', 'this', 'allows', 'us', 'to', 'evaluate', 'ktopipi_i0', 'decay', 'ampl... | [-0.11444416129222465, 0.14751588591625767, -0.07895877748905193, 0.07350943554266696, -0.08918128770569132, -0.07169747367382996, 0.10251932771551231, 0.32521523008980446, -0.22077458034942132, -0.28326696281631786, 0.01580699632639095, -0.2872337943780521, -0.10721476628844227, 0.1032984039879271, 0.02802615589092648... |
710.252 | The equation of state with nonzero chemical potential for 2+1 flavors | We present results for the QCD equation of state with nonzero chemical
potential using the Taylor expansion method with terms up to sixth order in the
expansion. Our calculations are performed on asqtad 2+1 quark flavor lattices
at $N_t=4$.
| hep-lat | we present results for the qcd equation of state with nonzero chemical potential using the taylor expansion method with terms up to sixth order in the expansion our calculations are performed on asqtad 21 quark flavor lattices at n_t4 | [['we', 'present', 'results', 'for', 'the', 'qcd', 'equation', 'of', 'state', 'with', 'nonzero', 'chemical', 'potential', 'using', 'the', 'taylor', 'expansion', 'method', 'with', 'terms', 'up', 'to', 'sixth', 'order', 'in', 'the', 'expansion', 'our', 'calculations', 'are', 'performed', 'on', 'asqtad', '21', 'quark', 'f... | [-0.06317904541412225, 0.16939970429461354, -0.11069182556074782, -0.041698017181494296, -0.02379456711694216, -0.011306739340607937, 0.1034040752117737, 0.3713502039034397, -0.1419854390506561, -0.2665144627292951, 0.08916747428846951, -0.3292068897340542, -0.024736212709775336, 0.09856639235901336, 0.1440747301691235... |
710.2521 | A formula for the coincidence Reidemeister trace of selfmaps on bouquets
of circles | We give a formula for the coincidence Reidemeister trace of selfmaps on
bouquets of circles in terms of the Fox calculus. Our formula reduces the
problem of computing the coincidence Reidemeister trace to the problem of
distinguishing doubly twisted conjugacy classes in free groups.
| math.GN math.AT | we give a formula for the coincidence reidemeister trace of selfmaps on bouquets of circles in terms of the fox calculus our formula reduces the problem of computing the coincidence reidemeister trace to the problem of distinguishing doubly twisted conjugacy classes in free groups | [['we', 'give', 'a', 'formula', 'for', 'the', 'coincidence', 'reidemeister', 'trace', 'of', 'selfmaps', 'on', 'bouquets', 'of', 'circles', 'in', 'terms', 'of', 'the', 'fox', 'calculus', 'our', 'formula', 'reduces', 'the', 'problem', 'of', 'computing', 'the', 'coincidence', 'reidemeister', 'trace', 'to', 'the', 'problem... | [-0.1991079728203741, 0.05097713209265335, -0.06344982893841172, 0.12336956832388585, -0.09300131621685895, -0.08307606956540523, 0.06200620598710058, 0.27144883725453506, -0.3163225640627471, -0.33018352489241143, 0.03845957925395024, -0.28582132641564717, -0.0764255687403916, 0.1986688363619826, -0.16109011438675225,... |
710.2522 | Unconventional interaction between vortices in a polarized Fermi gas | Recently, a homogeneous superfluid state with a single gapless Fermi surface
was predicted to be the ground state of an ultracold Fermi gas with spin
population imbalance in the regime of molecular Bose-Einstein condensation. We
study vortices in this novel state using a symmetry-based effective field
theory, which c... | cond-mat.supr-con cond-mat.other | recently a homogeneous superfluid state with a single gapless fermi surface was predicted to be the ground state of an ultracold fermi gas with spin population imbalance in the regime of molecular boseeinstein condensation we study vortices in this novel state using a symmetrybased effective field theory which captures... | [['recently', 'a', 'homogeneous', 'superfluid', 'state', 'with', 'a', 'single', 'gapless', 'fermi', 'surface', 'was', 'predicted', 'to', 'be', 'the', 'ground', 'state', 'of', 'an', 'ultracold', 'fermi', 'gas', 'with', 'spin', 'population', 'imbalance', 'in', 'the', 'regime', 'of', 'molecular', 'boseeinstein', 'condensa... | [-0.18275382848371713, 0.2501221879567437, -0.089665235350288, 0.09870296878191089, -0.03057983133139767, -0.16691629749297493, 0.06750653990065932, 0.2908245977229638, -0.257462583563016, -0.26169243640659345, -0.049760339132946176, -0.30330297254521205, -0.12159954459134575, 0.13092925350687795, 0.0567151147204672, 0... |
710.2523 | An analysis of the abstracts presented at the annual meetings of the
Society for Neuroscience from 2001 to 2006 | We extracted and processed abstract data from the SFN annual meeting
abstracts during the period 2001-2006, using techniques and software from
natural language processing, database management, and data visualization and
analysis. An important first step in the process was the application of data
cleaning and disambig... | physics.data-an q-bio.NC | we extracted and processed abstract data from the sfn annual meeting abstracts during the period 20012006 using techniques and software from natural language processing database management and data visualization and analysis an important first step in the process was the application of data cleaning and disambiguation ... | [['we', 'extracted', 'and', 'processed', 'abstract', 'data', 'from', 'the', 'sfn', 'annual', 'meeting', 'abstracts', 'during', 'the', 'period', '20012006', 'using', 'techniques', 'and', 'software', 'from', 'natural', 'language', 'processing', 'database', 'management', 'and', 'data', 'visualization', 'and', 'analysis', ... | [-0.0687173812989118, 0.0445701758215578, -0.046631658078267184, 0.04819613648945666, -0.09098397261593216, -0.07002985100638505, 0.062108454305202676, 0.3700490293883965, -0.23100323847756954, -0.3720617709237986, 0.12312059047904125, -0.32495804230668857, -0.1500921642548158, 0.2024802049758471, -0.11677298045833595,... |
710.2524 | Neutrino time travel | We discuss causality properties of extra-dimensional theories allowing for
effectively superluminal bulk shortcuts. Such shortcuts for sterile neutrinos
have been discussed as a solution to the puzzling LSND and MiniBooNE neutrino
oscillation results. We focus here on the sub-category of asymmetrically warped
brane s... | hep-ph | we discuss causality properties of extradimensional theories allowing for effectively superluminal bulk shortcuts such shortcuts for sterile neutrinos have been discussed as a solution to the puzzling lsnd and miniboone neutrino oscillation results we focus here on the subcategory of asymmetrically warped brane spaceti... | [['we', 'discuss', 'causality', 'properties', 'of', 'extradimensional', 'theories', 'allowing', 'for', 'effectively', 'superluminal', 'bulk', 'shortcuts', 'such', 'shortcuts', 'for', 'sterile', 'neutrinos', 'have', 'been', 'discussed', 'as', 'a', 'solution', 'to', 'the', 'puzzling', 'lsnd', 'and', 'miniboone', 'neutrin... | [-0.14190499792712624, 0.2652110907751439, -0.06346101140122065, 0.18264994643670454, -0.13493475112854764, -0.2308291384866566, 0.027839565846897018, 0.3425559319262759, -0.1992268453278903, -0.2885307443610738, 0.050616956238760454, -0.2709596853551528, -0.09405070012749246, 0.17689434648229835, -0.08560622809454799,... |
710.2525 | Lepton Flavor Violation at the LHC | In supersymmetric scenarios, the seesaw mechanism involving heavy
right-handed neutrinos implies sizable lepton flavor violation (LFV) in the
slepton sector. We discuss the potential of detecting LFV processes at the LHC
in mSUGRA+seesaw scenarios and for general mixing in either the left- or
right-handed slepton sec... | hep-ph | in supersymmetric scenarios the seesaw mechanism involving heavy righthanded neutrinos implies sizable lepton flavor violation lfv in the slepton sector we discuss the potential of detecting lfv processes at the lhc in msugraseesaw scenarios and for general mixing in either the left or righthanded slepton sector the re... | [['in', 'supersymmetric', 'scenarios', 'the', 'seesaw', 'mechanism', 'involving', 'heavy', 'righthanded', 'neutrinos', 'implies', 'sizable', 'lepton', 'flavor', 'violation', 'lfv', 'in', 'the', 'slepton', 'sector', 'we', 'discuss', 'the', 'potential', 'of', 'detecting', 'lfv', 'processes', 'at', 'the', 'lhc', 'in', 'ms... | [-0.11451705304595332, 0.38607332957132406, 0.10283476507756859, 0.27216551583260296, -0.059245598254104456, -0.26277298405766486, 0.07480966746807098, 0.27423683684319256, -0.2360881634367009, -0.22202590256929397, 0.004985211316185693, -0.3349901855768015, 0.021067855511015903, 0.10052453083141397, 0.0856569692453679... |
710.2526 | Angle dependent quasiparticle weights in correlated metals | The variation in the quasiparticle weight $Z$ on moving around the fermi
surface in correlated metals is studied theoretically. Our primary example is a
heavy Fermi liquid treated within the standard hybridization mean field theory.
The most dramatic variation in the quasiparticle weight happens in situations
where t... | cond-mat.str-el | the variation in the quasiparticle weight z on moving around the fermi surface in correlated metals is studied theoretically our primary example is a heavy fermi liquid treated within the standard hybridization mean field theory the most dramatic variation in the quasiparticle weight happens in situations where the hyb... | [['the', 'variation', 'in', 'the', 'quasiparticle', 'weight', 'z', 'on', 'moving', 'around', 'the', 'fermi', 'surface', 'in', 'correlated', 'metals', 'is', 'studied', 'theoretically', 'our', 'primary', 'example', 'is', 'a', 'heavy', 'fermi', 'liquid', 'treated', 'within', 'the', 'standard', 'hybridization', 'mean', 'fi... | [-0.17475763480895415, 0.23443845582331937, -0.05190206683264711, 0.11714410288139987, -0.028922079311600193, -0.1472311888773663, 0.09182656958280579, 0.36455102774720544, -0.27007261831805895, -0.242834471572095, -0.02879227316066718, -0.3380782374371894, -0.11995603898778939, 0.1553699974767649, -0.02990390759898732... |
710.2527 | Equilibrium Properties of Mixtures of Bosons and Fermions | Partial Quantum Nearest Neighbor Probability Density Functions (PQNNPDF's)
are formulated for the purpose of determining the behavior of quantum mixed
systems in equilibrium in a manner analogous to that provided for classical
multi-component systems. Developments in partial quantum m-tuplet distribution
functions, a... | cond-mat.stat-mech cond-mat.mtrl-sci | partial quantum nearest neighbor probability density functions pqnnpdfs are formulated for the purpose of determining the behavior of quantum mixed systems in equilibrium in a manner analogous to that provided for classical multicomponent systems developments in partial quantum mtuplet distribution functions a generali... | [['partial', 'quantum', 'nearest', 'neighbor', 'probability', 'density', 'functions', 'pqnnpdfs', 'are', 'formulated', 'for', 'the', 'purpose', 'of', 'determining', 'the', 'behavior', 'of', 'quantum', 'mixed', 'systems', 'in', 'equilibrium', 'in', 'a', 'manner', 'analogous', 'to', 'that', 'provided', 'for', 'classical'... | [-0.12375490194798522, 0.1351775022387655, -0.05979726799821432, 0.07695944410485042, 0.010466892338168304, -0.13937910371748483, 0.012825175544939341, 0.3255723115073237, -0.2568949087959739, -0.20241831557668613, 0.06702355518463207, -0.27920017083200205, -0.13362657261880495, 0.19087834975195933, 0.00428040989930123... |
710.2528 | Chern-Simons Modified General Relativity: Conserved charges | We construct the conserved charges (mass and angular momentum) of the
Chern-Simons modified General Relativity in asymptotically flat and Anti-de
Sitter (AdS) spacetimes. Our definition is based on background Killing
symmetries and reduces to the known expressions in the proper limits.
| gr-qc astro-ph hep-th | we construct the conserved charges mass and angular momentum of the chernsimons modified general relativity in asymptotically flat and antide sitter ads spacetimes our definition is based on background killing symmetries and reduces to the known expressions in the proper limits | [['we', 'construct', 'the', 'conserved', 'charges', 'mass', 'and', 'angular', 'momentum', 'of', 'the', 'chernsimons', 'modified', 'general', 'relativity', 'in', 'asymptotically', 'flat', 'and', 'antide', 'sitter', 'ads', 'spacetimes', 'our', 'definition', 'is', 'based', 'on', 'background', 'killing', 'symmetries', 'and... | [-0.16400768153551148, 0.16290953185227586, -0.07556012511344218, 0.13528554342834778, -0.17262270917161937, -0.11228628606512779, -0.05961674651721629, 0.2995462859526458, -0.061023876014188294, -0.25370843684380284, 0.0395884300893025, -0.2704071298968501, -0.09811801377047853, 0.10965203834561313, -0.119958978259890... |
710.2529 | Heuristic decomposition of cones in molecular conformational space | In a previous work arXiv:physics/0611108v2, it was shown that the volume
spanned by a molecular system in its conformational space can be effectively
bounded by a polyhedral cone, this cone is described by means of a simple
combinatorial formula. On the other hand it was constructed a transversal graph
structure enco... | physics.comp-ph | in a previous work arxivphysics0611108v2 it was shown that the volume spanned by a molecular system in its conformational space can be effectively bounded by a polyhedral cone this cone is described by means of a simple combinatorial formula on the other hand it was constructed a transversal graph structure encoding th... | [['in', 'a', 'previous', 'work', 'arxivphysics0611108v2', 'it', 'was', 'shown', 'that', 'the', 'volume', 'spanned', 'by', 'a', 'molecular', 'system', 'in', 'its', 'conformational', 'space', 'can', 'be', 'effectively', 'bounded', 'by', 'a', 'polyhedral', 'cone', 'this', 'cone', 'is', 'described', 'by', 'means', 'of', 'a... | [-0.11398103873073795, 0.14108072126226634, -0.11542194012130044, 0.07483857166329302, -0.0940689133653014, -0.10825592867511603, 0.04481091126607558, 0.36518917866435247, -0.32594707664390354, -0.27351726434126344, 0.11349936625584192, -0.23689884527288763, -0.17047374399820553, 0.2035186700138849, -0.0562243853682488... |
710.253 | Smectic ordering in athermal systems of rod-like triblock copolymers | The phase behavior of the system of parallel rigid triblock copolymers is
examined using the second-virial density functional theory. The triblock
particle consists of two identical infinitely thin hard rods of finite lengths
on the opposite ends of one central hard cylinder with nonzero length and
diameter. Stabilit... | cond-mat.soft cond-mat.mtrl-sci | the phase behavior of the system of parallel rigid triblock copolymers is examined using the secondvirial density functional theory the triblock particle consists of two identical infinitely thin hard rods of finite lengths on the opposite ends of one central hard cylinder with nonzero length and diameter stability ana... | [['the', 'phase', 'behavior', 'of', 'the', 'system', 'of', 'parallel', 'rigid', 'triblock', 'copolymers', 'is', 'examined', 'using', 'the', 'secondvirial', 'density', 'functional', 'theory', 'the', 'triblock', 'particle', 'consists', 'of', 'two', 'identical', 'infinitely', 'thin', 'hard', 'rods', 'of', 'finite', 'lengt... | [-0.21031859342686154, 0.2577884791136691, -0.06208444955391866, -0.013587521873837844, -0.012887643739073114, -0.16527844902805305, -0.001793055764089028, 0.39097813402838777, -0.27701526426244527, -0.24500092541319177, 0.09634918317368085, -0.27856178082751504, -0.08145811017038244, 0.09598705062685027, 0.03361749215... |
710.2531 | Lens space surgeries and L-space homology spheres | We describe necessary and sufficient conditions for a knot in an L-space to
have an L-space homology sphere surgery. We use these conditions to reformulate
a conjecture of Berge about which knots in S^3 admit lens space surgeries.
| math.GT | we describe necessary and sufficient conditions for a knot in an lspace to have an lspace homology sphere surgery we use these conditions to reformulate a conjecture of berge about which knots in s3 admit lens space surgeries | [['we', 'describe', 'necessary', 'and', 'sufficient', 'conditions', 'for', 'a', 'knot', 'in', 'an', 'lspace', 'to', 'have', 'an', 'lspace', 'homology', 'sphere', 'surgery', 'we', 'use', 'these', 'conditions', 'to', 'reformulate', 'a', 'conjecture', 'of', 'berge', 'about', 'which', 'knots', 'in', 's3', 'admit', 'lens', ... | [-0.2944983093950309, 0.005881570580593114, -0.1954894511176175, 0.1474167274213151, -0.16148488099784836, -0.21825733633809968, -0.04756417801285064, 0.433693029084488, -0.20838006066256448, -0.31630202372999566, 0.14543388753908834, -0.16080198375091545, -0.2246556862159387, 0.17204514082129063, -0.24924362681217885,... |
710.2532 | Sleeping on the Job: Energy-Efficient Broadcast for Radio Networks | We address the problem of minimizing power consumption when performing
reliable broadcast on a radio network under the following popular model. Each
node in the network is located on a point in a two dimensional grid, and
whenever a node sends a message, all awake nodes within distance r receive the
message. In the b... | cs.DS | we address the problem of minimizing power consumption when performing reliable broadcast on a radio network under the following popular model each node in the network is located on a point in a two dimensional grid and whenever a node sends a message all awake nodes within distance r receive the message in the broadca... | [['we', 'address', 'the', 'problem', 'of', 'minimizing', 'power', 'consumption', 'when', 'performing', 'reliable', 'broadcast', 'on', 'a', 'radio', 'network', 'under', 'the', 'following', 'popular', 'model', 'each', 'node', 'in', 'the', 'network', 'is', 'located', 'on', 'a', 'point', 'in', 'a', 'two', 'dimensional', 'g... | [-0.20702362418608758, 0.07437693580623768, -0.037167842097544264, -0.0028865310068854092, -0.056122654497406436, -0.24351832347026872, 0.18736562813092686, 0.3705651853143156, -0.2867788559094849, -0.3085732375901542, 0.09021263127252882, -0.3120593251750886, -0.11164530817476556, 0.11756465533442349, -0.1149761375185... |
710.2533 | Modularity-Maximizing Network Communities via Mathematical Programming | In many networks, it is of great interest to identify "communities",
unusually densely knit groups of individuals. Such communities often shed light
on the function of the networks or underlying properties of the individuals.
Recently, Newman suggested "modularity" as a natural measure of the quality of
a network par... | physics.data-an | in many networks it is of great interest to identify communities unusually densely knit groups of individuals such communities often shed light on the function of the networks or underlying properties of the individuals recently newman suggested modularity as a natural measure of the quality of a network partitioning i... | [['in', 'many', 'networks', 'it', 'is', 'of', 'great', 'interest', 'to', 'identify', 'communities', 'unusually', 'densely', 'knit', 'groups', 'of', 'individuals', 'such', 'communities', 'often', 'shed', 'light', 'on', 'the', 'function', 'of', 'the', 'networks', 'or', 'underlying', 'properties', 'of', 'the', 'individual... | [-0.0944854687586485, -0.013929937934997062, -0.11012357791928067, 0.09804134527009657, -0.09709301577690481, -0.1584812545767239, 0.0753869691999915, 0.3927091473544186, -0.2700912809443914, -0.3522118425726975, 0.10693718857642538, -0.25525827405032364, -0.20937227431700609, 0.19734409350150434, -0.04625387528159825,... |
710.2534 | On Torsion Fields in Higher Derivative Quantum Gravity | We consider axial torsion fields which appear in higher derivative quantum
gravity. It is shown, in general, that the torsion field possesses states with
two spins, one and zero, with different masses. The first-order formulation of
torsion fields is performed. Projection operators extracting pure spin and mass
state... | gr-qc hep-th | we consider axial torsion fields which appear in higher derivative quantum gravity it is shown in general that the torsion field possesses states with two spins one and zero with different masses the firstorder formulation of torsion fields is performed projection operators extracting pure spin and mass states are give... | [['we', 'consider', 'axial', 'torsion', 'fields', 'which', 'appear', 'in', 'higher', 'derivative', 'quantum', 'gravity', 'it', 'is', 'shown', 'in', 'general', 'that', 'the', 'torsion', 'field', 'possesses', 'states', 'with', 'two', 'spins', 'one', 'and', 'zero', 'with', 'different', 'masses', 'the', 'firstorder', 'form... | [-0.23384885265444277, 0.20755656514401463, -0.06352774399221578, 0.060606353678105566, -0.10041105779237114, -0.11324178272942928, -0.12712801024793985, 0.3225342556834221, -0.2156044677302072, -0.2858798233368857, 0.023420995817022314, -0.24435935710260476, -0.12743920951404356, 0.10557070153299719, 0.035674454263326... |
710.2535 | O'Raifeartaigh models with spontaneous R-symmetry breaking | O'Raifeartaigh models with general R-charge assignments can have vacua where
both supersymmetry and R-symmetry are spontaneously broken. Most of these vacua
are metastable because the potential shows a runaway behaviour. We explain the
relation between runaway directions and R-symmetry.
| hep-th | oraifeartaigh models with general rcharge assignments can have vacua where both supersymmetry and rsymmetry are spontaneously broken most of these vacua are metastable because the potential shows a runaway behaviour we explain the relation between runaway directions and rsymmetry | [['oraifeartaigh', 'models', 'with', 'general', 'rcharge', 'assignments', 'can', 'have', 'vacua', 'where', 'both', 'supersymmetry', 'and', 'rsymmetry', 'are', 'spontaneously', 'broken', 'most', 'of', 'these', 'vacua', 'are', 'metastable', 'because', 'the', 'potential', 'shows', 'a', 'runaway', 'behaviour', 'we', 'expla... | [-0.16193494546967438, 0.2654458273154421, -0.05814226550790362, 0.16199554617588335, -0.09705617515226969, -0.24786783756019595, 0.02611169732438448, 0.3995962219360547, -0.13421964740010503, -0.3198131747925893, 0.09896486877010037, -0.2635658265163119, -0.12225257103832868, 0.002055289271550301, -0.06195386119473439... |
710.2536 | Isoperimetric regions in spherical cones and Yamabe constants of
$M\times S^1$ | Given closed Riemannian manifold $(M^n, g)$ of positive Ricci curvature
$Ricci(g) \geq (n-1)g$ we study isoperimetric regions on the spherical cone
over $M$. When $g$ is Einstein we use this to compute the Yamabe constant of
$(M \times {\bf R}, g + dt^2)$ and so to obtain lower bounds for the Yamabe
invariant of $M\t... | math.DG | given closed riemannian manifold mn g of positive ricci curvature riccig geq n1g we study isoperimetric regions on the spherical cone over m when g is einstein we use this to compute the yamabe constant of m times bf r g dt2 and so to obtain lower bounds for the yamabe invariant of mtimes s1 | [['given', 'closed', 'riemannian', 'manifold', 'mn', 'g', 'of', 'positive', 'ricci', 'curvature', 'riccig', 'geq', 'n1g', 'we', 'study', 'isoperimetric', 'regions', 'on', 'the', 'spherical', 'cone', 'over', 'm', 'when', 'g', 'is', 'einstein', 'we', 'use', 'this', 'to', 'compute', 'the', 'yamabe', 'constant', 'of', 'm',... | [-0.2713724050916872, 0.06948851815969595, -0.015139778302806729, 0.024920011536692672, -0.12710176257170597, -0.21501180656113714, -0.06884006983688418, 0.38050220892676767, -0.19403178592757234, -0.282012495932714, 0.10557729214921875, -0.28900188225198464, -0.08865424845683968, 0.11426161647826996, -0.09796438740570... |
710.2537 | Spookytechnology and Society | New technologies based on the exploitation of so-called "second order"
quantum phenomena - such as quantum entanglement - deserve a public-friendly,
rational, and sexy name. Spookytechnology is that unifying term. From
historical and motivational perspectives, this name has greater value than the
many variations of q... | physics.pop-ph cond-mat.mtrl-sci physics.soc-ph quant-ph | new technologies based on the exploitation of socalled second order quantum phenomena such as quantum entanglement deserve a publicfriendly rational and sexy name spookytechnology is that unifying term from historical and motivational perspectives this name has greater value than the many variations of quantum this and... | [['new', 'technologies', 'based', 'on', 'the', 'exploitation', 'of', 'socalled', 'second', 'order', 'quantum', 'phenomena', 'such', 'as', 'quantum', 'entanglement', 'deserve', 'a', 'publicfriendly', 'rational', 'and', 'sexy', 'name', 'spookytechnology', 'is', 'that', 'unifying', 'term', 'from', 'historical', 'and', 'mo... | [-0.08560312234718974, 0.1307401271769777, -0.09612992249215797, 0.04854516353104069, -0.10048652095914197, -0.13988162983544802, 0.038752208412915934, 0.2817789209948387, -0.24844556073852195, -0.2898318042862229, 0.13785191522401874, -0.25667661246067536, -0.20491946182058504, 0.24967881853687382, -0.0699290901005345... |
710.2538 | Detectability of CMB tensor B modes via delensing with weak lensing
galaxy surveys | We analyze the possibility of delensing CMB polarization maps using
foreground weak lensing (WL) information. We build an estimator of the CMB
lensing potential out of optimally combined projected potential estimators to
different source redshift bins. Our estimator is most sensitive to the redshift
depth of the WL s... | astro-ph | we analyze the possibility of delensing cmb polarization maps using foreground weak lensing wl information we build an estimator of the cmb lensing potential out of optimally combined projected potential estimators to different source redshift bins our estimator is most sensitive to the redshift depth of the wl survey ... | [['we', 'analyze', 'the', 'possibility', 'of', 'delensing', 'cmb', 'polarization', 'maps', 'using', 'foreground', 'weak', 'lensing', 'wl', 'information', 'we', 'build', 'an', 'estimator', 'of', 'the', 'cmb', 'lensing', 'potential', 'out', 'of', 'optimally', 'combined', 'projected', 'potential', 'estimators', 'to', 'dif... | [-0.06826609499716702, 0.05211639991847243, -0.06937385682697193, 0.09972448693498825, -0.07965876170648978, -0.09100512630650953, 0.016029375239024656, 0.38808494705993396, -0.23748298395971337, -0.3021327107285078, 0.059144862644517654, -0.347031131600782, -0.05922149687987537, 0.2288210754690226, -0.0125546420064683... |
710.2539 | Low energy effective theory on a regularized brane in 6D gauged chiral
supergravity | We derive the low energy effective theory on a brane in six-dimensional
chiral supergravity. The conical 3-brane singularities are resolved by
introducing cylindrical codimension one 4-branes whose interiors are capped by
a regular spacetime. The effective theory is described by the Brans-Dicke (BD)
theory with the B... | hep-th astro-ph gr-qc | we derive the low energy effective theory on a brane in sixdimensional chiral supergravity the conical 3brane singularities are resolved by introducing cylindrical codimension one 4branes whose interiors are capped by a regular spacetime the effective theory is described by the bransdicke bd theory with the bd paramete... | [['we', 'derive', 'the', 'low', 'energy', 'effective', 'theory', 'on', 'a', 'brane', 'in', 'sixdimensional', 'chiral', 'supergravity', 'the', 'conical', '3brane', 'singularities', 'are', 'resolved', 'by', 'introducing', 'cylindrical', 'codimension', 'one', '4branes', 'whose', 'interiors', 'are', 'capped', 'by', 'a', 'r... | [-0.14085570529946503, 0.1343665585226444, -0.09126798483359036, 0.07485225950163235, -0.09263287620096644, -0.1415792927460594, -0.01631778631850171, 0.28841016153062415, -0.23245635609664778, -0.26008768548962435, 0.09266080251797354, -0.2347307074972353, -0.16077995502289283, 0.11129756293902991, -0.0592219506742785... |
710.254 | Modulated Perturbations from Instant Preheating after new Ekpyrosis | We present a mechanism to transfer the spectrum of perturbations in a scalar
isocurvature field $\xi$ onto the matter content in the radiation era via
modulated, instant preheating after ekpyrosis. In this setup, $\xi$ determines
the coupling constant relevant for the decay of a preheat matter field into
Fermions. Th... | hep-th astro-ph | we present a mechanism to transfer the spectrum of perturbations in a scalar isocurvature field xi onto the matter content in the radiation era via modulated instant preheating after ekpyrosis in this setup xi determines the coupling constant relevant for the decay of a preheat matter field into fermions the resulting ... | [['we', 'present', 'a', 'mechanism', 'to', 'transfer', 'the', 'spectrum', 'of', 'perturbations', 'in', 'a', 'scalar', 'isocurvature', 'field', 'xi', 'onto', 'the', 'matter', 'content', 'in', 'the', 'radiation', 'era', 'via', 'modulated', 'instant', 'preheating', 'after', 'ekpyrosis', 'in', 'this', 'setup', 'xi', 'deter... | [-0.13658315454043274, 0.21236751740798354, -0.1379009001528877, 0.11996805192792269, -0.0968815072259882, -0.16992798928383804, -0.01284756317696594, 0.33157555254622856, -0.24708533143877917, -0.2657087041794905, 0.08507545158738129, -0.22851854800185384, -0.11646562345749399, 0.1846931916307549, -0.00853411833434338... |
710.2541 | Toward Empirical Constraints on the Global Redshifted 21 cm Brightness
Temperature During the Epoch of Reionization | Preliminary results are presented from a simple, single-antenna experiment
designed to measure the all-sky radio spectrum between 100 and 200 MHz. The
system used an internal comparison-switching scheme to reduce non-smooth
instrumental contaminants in the measured spectrum to 75 mK. From the
observations, we place a... | astro-ph | preliminary results are presented from a simple singleantenna experiment designed to measure the allsky radio spectrum between 100 and 200 mhz the system used an internal comparisonswitching scheme to reduce nonsmooth instrumental contaminants in the measured spectrum to 75 mk from the observations we place an initial ... | [['preliminary', 'results', 'are', 'presented', 'from', 'a', 'simple', 'singleantenna', 'experiment', 'designed', 'to', 'measure', 'the', 'allsky', 'radio', 'spectrum', 'between', '100', 'and', '200', 'mhz', 'the', 'system', 'used', 'an', 'internal', 'comparisonswitching', 'scheme', 'to', 'reduce', 'nonsmooth', 'instru... | [-0.03509984574316499, 0.15054418752887824, -0.04150638142600656, 0.06287409477204514, -0.0629575395096953, -0.09483655964096005, 0.0743861505152801, 0.41424629784977207, -0.22570370639889287, -0.3491119856587969, 0.06880132743390277, -0.29102219831771575, 0.020664881388298594, 0.18726927952912564, 0.001385031914553390... |
710.2542 | Probing clumpy stellar winds with a neutron star | INTEGRAL, the European Space Agency's gamma-ray observatory, tripled the
number of super-giant high-mass X-ray binaries (sgHMXB) known in the Galaxy by
revealing absorbed and fast transient (SFXT) systems. In these sources,
quantitative constraints on the wind clumping of the massive stars could be
obtained from the ... | astro-ph | integral the european space agencys gammaray observatory tripled the number of supergiant highmass xray binaries sghmxb known in the galaxy by revealing absorbed and fast transient sfxt systems in these sources quantitative constraints on the wind clumping of the massive stars could be obtained from the study of the ha... | [['integral', 'the', 'european', 'space', 'agencys', 'gammaray', 'observatory', 'tripled', 'the', 'number', 'of', 'supergiant', 'highmass', 'xray', 'binaries', 'sghmxb', 'known', 'in', 'the', 'galaxy', 'by', 'revealing', 'absorbed', 'and', 'fast', 'transient', 'sfxt', 'systems', 'in', 'these', 'sources', 'quantitative'... | [-0.12745354450307786, 0.16419997951506, -0.04769886032874255, 0.15303021050395296, -0.10344054006824369, -0.062953837255114, 0.04649915786729635, 0.44153854129345793, -0.13303804953619347, -0.37540662568675254, 0.08645892396544744, -0.3167405095588612, 0.006258587266539077, 0.24563705751084183, -0.018819152769681654, ... |
710.2543 | Dynamics of Magnetized Spherical Accretion Flows | Transonic accretion flow with self-consistent treatment of random magnetic
field is presented.
| astro-ph | transonic accretion flow with selfconsistent treatment of random magnetic field is presented | [['transonic', 'accretion', 'flow', 'with', 'selfconsistent', 'treatment', 'of', 'random', 'magnetic', 'field', 'is', 'presented']] | [-0.21721458186705908, 0.17755107674747705, -0.0576305917929858, -0.03331159613056419, -0.12847344189261398, -0.1293270861109098, -0.10761309104661147, 0.41588179022073746, -0.17068744031712413, -0.280667538754642, 0.01649176678620279, -0.17079969712843499, 0.0340449915577968, 0.18431358660260835, -0.010637401137501001... |
710.2544 | Chern class identities from tadpole matching in type IIB and F-theory | In light of Sen's weak coupling limit of F-theory as a type IIB orientifold,
the compatibility of the tadpole conditions leads to a non-trivial identity
relating the Euler characteristics of an elliptically fibered Calabi-Yau
fourfold and of certain related surfaces. We present the physical argument
leading to the id... | hep-th math.AG | in light of sens weak coupling limit of ftheory as a type iib orientifold the compatibility of the tadpole conditions leads to a nontrivial identity relating the euler characteristics of an elliptically fibered calabiyau fourfold and of certain related surfaces we present the physical argument leading to the identity a... | [['in', 'light', 'of', 'sens', 'weak', 'coupling', 'limit', 'of', 'ftheory', 'as', 'a', 'type', 'iib', 'orientifold', 'the', 'compatibility', 'of', 'the', 'tadpole', 'conditions', 'leads', 'to', 'a', 'nontrivial', 'identity', 'relating', 'the', 'euler', 'characteristics', 'of', 'an', 'elliptically', 'fibered', 'calabiy... | [-0.19778672037524433, 0.04569756368261129, -0.12338457490299262, 0.14228621738798478, -0.11120540491195724, -0.17698136428858038, 0.0005322704422652867, 0.25435732261222954, -0.25100920351185635, -0.2392652262111797, 0.11719801755746814, -0.21436820867520093, -0.18674792289380837, 0.189308030664726, -0.157935644673439... |
710.2545 | A Freiman-type theorem for locally compact abelian groups | We prove a Freiman-type theorem for locally compact abelian groups. If A is a
subset of a locally compact abelian group with Haar measure m and m(nA) <
n^dm(A) for all n>d log d then we describe A in a way which is tight up to
logarithmic factors in d.
| math.CA math.NT | we prove a freimantype theorem for locally compact abelian groups if a is a subset of a locally compact abelian group with haar measure m and mna ndma for all nd log d then we describe a in a way which is tight up to logarithmic factors in d | [['we', 'prove', 'a', 'freimantype', 'theorem', 'for', 'locally', 'compact', 'abelian', 'groups', 'if', 'a', 'is', 'a', 'subset', 'of', 'a', 'locally', 'compact', 'abelian', 'group', 'with', 'haar', 'measure', 'm', 'and', 'mna', 'ndma', 'for', 'all', 'nd', 'log', 'd', 'then', 'we', 'describe', 'a', 'in', 'a', 'way', 'w... | [-0.16235293308272958, 0.137309534358792, -0.12707411928568035, 0.07025785432294167, -0.05748832724445189, -0.16092606915238625, 0.10498466703878269, 0.39654809213243425, -0.2548502629894453, -0.1958821136310386, 0.07289177685258134, -0.27555048015589517, -0.09991188442412142, 0.1993583548416306, -0.0985621192958206, -... |
710.2546 | Micromagnetic Simulations of Ferromagnetic Rings | Thin nanomagnetic rings have generated interest for fundamental studies of
magnetization reversal and also for their potential in various applications,
particularly as magnetic memories. They are a rare example of a geometry in
which an analytical solution for the rate of thermally induced magnetic
reversal has been ... | cond-mat.mes-hall cond-mat.other | thin nanomagnetic rings have generated interest for fundamental studies of magnetization reversal and also for their potential in various applications particularly as magnetic memories they are a rare example of a geometry in which an analytical solution for the rate of thermally induced magnetic reversal has been dete... | [['thin', 'nanomagnetic', 'rings', 'have', 'generated', 'interest', 'for', 'fundamental', 'studies', 'of', 'magnetization', 'reversal', 'and', 'also', 'for', 'their', 'potential', 'in', 'various', 'applications', 'particularly', 'as', 'magnetic', 'memories', 'they', 'are', 'a', 'rare', 'example', 'of', 'a', 'geometry',... | [-0.17411312962611836, 0.16501061362834016, -0.057111669690798846, 0.04586623451642452, -0.032853414815279744, -0.12846231728251423, 0.006578205229203787, 0.3992473941116083, -0.2651540987884566, -0.29801809496336407, 0.11138864129165849, -0.2355961960049406, -0.10306256075630024, 0.23694591344664653, 0.031095096282660... |
710.2547 | Topological defects and equation of state of gluon plasma | We show that the degrees of freedom associated with magnetic monopole- and
vortexlike gluonic configurations make a strong contribution to the anomaly of
the energy-momentum tensor of Yang-Mills theory in the deconfinement phase
immediately above the critical temperature. As is well known in
zero-temperature Yang-Mil... | hep-lat hep-ph hep-th | we show that the degrees of freedom associated with magnetic monopole and vortexlike gluonic configurations make a strong contribution to the anomaly of the energymomentum tensor of yangmills theory in the deconfinement phase immediately above the critical temperature as is well known in zerotemperature yangmills theor... | [['we', 'show', 'that', 'the', 'degrees', 'of', 'freedom', 'associated', 'with', 'magnetic', 'monopole', 'and', 'vortexlike', 'gluonic', 'configurations', 'make', 'a', 'strong', 'contribution', 'to', 'the', 'anomaly', 'of', 'the', 'energymomentum', 'tensor', 'of', 'yangmills', 'theory', 'in', 'the', 'deconfinement', 'p... | [-0.18915064543218232, 0.29059813322388744, -0.07269688392931706, 0.09478082324581055, -0.06301402665748454, -0.06284204133242222, 0.001898609808332628, 0.35605362119466655, -0.15326445005686568, -0.23950398409978882, 0.05731996944944125, -0.3024362866388689, -0.1466532466693385, 0.04443434378740811, 0.0398533342055755... |
710.2548 | Measurement of the inclusive B_s^0 -> X^+ l^- \nu semileptonic decay
branching fraction | Inclusive semileptonic B_s^0 -> X^+ l^- \nu decays are studied for the first
time using a 23.6 fb^{-1} data sample collected on the Y(5S) resonance with the
Belle detector at the KEKB asymmetric energy e^+ e^- collider. These decays are
identified by the means of a lepton accompanied by a same-sign D_s^+ meson
origin... | hep-ex | inclusive semileptonic b_s0 x l nu decays are studied for the first time using a 236 fb1 data sample collected on the y5s resonance with the belle detector at the kekb asymmetric energy e e collider these decays are identified by the means of a lepton accompanied by a samesign d_s meson originating from the other b_s0 ... | [['inclusive', 'semileptonic', 'b_s0', 'x', 'l', 'nu', 'decays', 'are', 'studied', 'for', 'the', 'first', 'time', 'using', 'a', '236', 'fb1', 'data', 'sample', 'collected', 'on', 'the', 'y5s', 'resonance', 'with', 'the', 'belle', 'detector', 'at', 'the', 'kekb', 'asymmetric', 'energy', 'e', 'e', 'collider', 'these', 'd... | [-0.09812889179442934, 0.27751112603076084, -0.002349946110289756, 0.08865455433166003, 0.02127831121073748, -0.1738893550449634, 0.12049690128126128, 0.26107333156817814, -0.1593844375868396, -0.2925933132902151, -0.06919328360231518, -0.47334560820817706, 0.17138689461853204, 0.1586521216573542, 0.1037966469567784, 0... |
710.2549 | Congruences among modular forms on U(2,2) and the Bloch-Kato conjecture | Let k be a positive integer divisible by 4, l>k a prime, and f an elliptic
cuspidal eigenform of weight k-1, level 4, and non-trivial character. Let
\rho_f be the l-adic Galois representation attached to f. In this paper we
provide evidence for the Bloch-Kato conjecture for a twist of the adjoint motif
of \rho_f in t... | math.NT math.RT | let k be a positive integer divisible by 4 lk a prime and f an elliptic cuspidal eigenform of weight k1 level 4 and nontrivial character let rho_f be the ladic galois representation attached to f in this paper we provide evidence for the blochkato conjecture for a twist of the adjoint motif of rho_f in the following wa... | [['let', 'k', 'be', 'a', 'positive', 'integer', 'divisible', 'by', '4', 'lk', 'a', 'prime', 'and', 'f', 'an', 'elliptic', 'cuspidal', 'eigenform', 'of', 'weight', 'k1', 'level', '4', 'and', 'nontrivial', 'character', 'let', 'rho_f', 'be', 'the', 'ladic', 'galois', 'representation', 'attached', 'to', 'f', 'in', 'this', ... | [-0.23777837847018432, 0.07326324365516176, -0.17175246276695963, 0.0004065625351512621, -0.11718747798438696, -0.15604138382526875, -0.02217173876657321, 0.2820178269290588, -0.33685754348432095, -0.2264847159467664, 0.023459228900962994, -0.24362617512528692, -0.12162534613326244, 0.18438358756739803, -0.098683484535... |
710.255 | The lightest neutralino in the MNSSM | We examine the allowed mass range of the lightest neutralino within the
Minimal Non--minimal Supersymmetric Standard Model. Being absolutely stable if
R-parity is conserved this lightest neutralino is a candidate for the dark
matter of the universe. We establish the theoretical upper bound on the
lightest neutralino ... | hep-ph | we examine the allowed mass range of the lightest neutralino within the minimal nonminimal supersymmetric standard model being absolutely stable if rparity is conserved this lightest neutralino is a candidate for the dark matter of the universe we establish the theoretical upper bound on the lightest neutralino mass an... | [['we', 'examine', 'the', 'allowed', 'mass', 'range', 'of', 'the', 'lightest', 'neutralino', 'within', 'the', 'minimal', 'nonminimal', 'supersymmetric', 'standard', 'model', 'being', 'absolutely', 'stable', 'if', 'rparity', 'is', 'conserved', 'this', 'lightest', 'neutralino', 'is', 'a', 'candidate', 'for', 'the', 'dark... | [-0.11109100937444184, 0.24731758532314935, -0.03454980067908764, 0.24918934815962399, -0.09314799360332213, -0.1483626327992949, 0.04051723314179461, 0.2734883695915674, -0.17507235346628086, -0.33912377644862446, 0.025240881721921533, -0.245269767690583, 0.08251115894277714, 0.10180691813625994, 0.012785277591319755,... |
710.2551 | On general flux backgrounds with localized sources | We derive new consistency conditions for string compactifications with
generic fluxes (RR, NSNS, geometrical) and localized sources (D-branes,
NS-branes, KK-monopoles). The constraints are all related by string dualities
and share a common origin in M-theory. We also find new sources of
instabilities. We discuss the ... | hep-th | we derive new consistency conditions for string compactifications with generic fluxes rr nsns geometrical and localized sources dbranes nsbranes kkmonopoles the constraints are all related by string dualities and share a common origin in mtheory we also find new sources of instabilities we discuss the importance of the... | [['we', 'derive', 'new', 'consistency', 'conditions', 'for', 'string', 'compactifications', 'with', 'generic', 'fluxes', 'rr', 'nsns', 'geometrical', 'and', 'localized', 'sources', 'dbranes', 'nsbranes', 'kkmonopoles', 'the', 'constraints', 'are', 'all', 'related', 'by', 'string', 'dualities', 'and', 'share', 'a', 'com... | [-0.17018235622403713, 0.13030446498439863, -0.04894995207969959, 0.21372807311037412, -0.08779972698181294, -0.13564268698056156, 0.06029565236889399, 0.317258673089628, -0.1533699129600651, -0.2715390207819067, 0.11934778976003424, -0.24965293675374525, -0.13872938356720485, 0.1509309224390353, -0.09659955981545723, ... |
710.2552 | Simultaneous Estimation of Time Delays and Quasar Structure | We expand our Bayesian Monte Carlo method for analyzing the light curves of
gravitationally lensed quasars to simultaneously estimate time delays and
quasar structure including their mutual uncertainties. We apply the method to
HE1104-1805 and QJ0158-4325, two doubly-imaged quasars with microlensing and
intrinsic var... | astro-ph | we expand our bayesian monte carlo method for analyzing the light curves of gravitationally lensed quasars to simultaneously estimate time delays and quasar structure including their mutual uncertainties we apply the method to he11041805 and qj01584325 two doublyimaged quasars with microlensing and intrinsic variabilit... | [['we', 'expand', 'our', 'bayesian', 'monte', 'carlo', 'method', 'for', 'analyzing', 'the', 'light', 'curves', 'of', 'gravitationally', 'lensed', 'quasars', 'to', 'simultaneously', 'estimate', 'time', 'delays', 'and', 'quasar', 'structure', 'including', 'their', 'mutual', 'uncertainties', 'we', 'apply', 'the', 'method'... | [-0.06435513256808682, 0.09537988375391691, -0.05117137460770356, 0.09993969844823193, -0.062419802611393314, -0.10597430567647662, 0.049758250453329135, 0.45536330985205786, -0.1848974943221096, -0.3589441009774624, 0.09203141679209957, -0.3100318735119917, 0.03337750247690917, 0.2056861060386103, -0.06183732689298209... |
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