id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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710.1653 | Superhumps and flickering in V1316 Cygni | We present analysis and results of a coordinated CCD photometry campaign to
observe the 2006 June superoutburst of the cataclysmic variable V1316 Cyg
involving 8 longitudinally-distributed observers. The outburst peaked at
magnitude 15.03 on June 10, declined at a rate of 0.14 mag/day, lasted 11 days
and had an ampli... | astro-ph | we present analysis and results of a coordinated ccd photometry campaign to observe the 2006 june superoutburst of the cataclysmic variable v1316 cyg involving 8 longitudinallydistributed observers the outburst peaked at magnitude 1503 on june 10 declined at a rate of 014 magday lasted 11 days and had an amplitude abov... | [['we', 'present', 'analysis', 'and', 'results', 'of', 'a', 'coordinated', 'ccd', 'photometry', 'campaign', 'to', 'observe', 'the', '2006', 'june', 'superoutburst', 'of', 'the', 'cataclysmic', 'variable', 'v1316', 'cyg', 'involving', '8', 'longitudinallydistributed', 'observers', 'the', 'outburst', 'peaked', 'at', 'mag... | [-0.12311043061449059, 0.18951884920584608, -0.11509355996005656, 0.0336719817576176, -0.06177417530065394, -0.14263866821432977, 0.1341296599254877, 0.356635350766249, -0.18096637080103015, -0.32822725956844273, 0.11966553906450508, -0.32782892780217193, -0.09490283304982662, 0.1965617288722459, -0.12483546098777863, ... |
710.1654 | GOODS 850-5 -- A z>4 Galaxy Discovered in the Submillimeter? | We report an SMA interferometric identification of a bright submillimeter
source, GOODS 850-5. This source is one of the brightest 850 um sources in the
GOODS-N but is extremely faint at all other wavelengths. It is not detected in
the GOODS HST ACS images and only shows a weak 2 sigma signal at 1.4 GHz. It is
detect... | astro-ph | we report an sma interferometric identification of a bright submillimeter source goods 8505 this source is one of the brightest 850 um sources in the goodsn but is extremely faint at all other wavelengths it is not detected in the goods hst acs images and only shows a weak 2 sigma signal at 14 ghz it is detected in the... | [['we', 'report', 'an', 'sma', 'interferometric', 'identification', 'of', 'a', 'bright', 'submillimeter', 'source', 'goods', '8505', 'this', 'source', 'is', 'one', 'of', 'the', 'brightest', '850', 'um', 'sources', 'in', 'the', 'goodsn', 'but', 'is', 'extremely', 'faint', 'at', 'all', 'other', 'wavelengths', 'it', 'is',... | [-0.0610502952427425, 0.07086069696905473, -0.06453654998318946, 0.0675448672833575, -0.12411179586482096, -0.130718891454385, 0.03553444671474318, 0.5437378227869247, -0.1251965499324526, -0.3210842615251053, 0.12051994283188214, -0.31246398555540894, -0.047856181295231934, 0.16312166578829923, -0.021961640821091158, ... |
710.1655 | Toward a precise determination of Tc with 2+1 flavors of quarks | We present a status report on a new high statistics study of the high
temperature transition in full QCD at zero chemical potential. Our simulations
use both improved asqtad and p4 staggered quarks on lattices with a temporal
extent N_t = 8 and light quark masses approximately one tenth the strange quark
mass. In thi... | hep-lat | we present a status report on a new high statistics study of the high temperature transition in full qcd at zero chemical potential our simulations use both improved asqtad and p4 staggered quarks on lattices with a temporal extent n_t 8 and light quark masses approximately one tenth the strange quark mass in this repo... | [['we', 'present', 'a', 'status', 'report', 'on', 'a', 'new', 'high', 'statistics', 'study', 'of', 'the', 'high', 'temperature', 'transition', 'in', 'full', 'qcd', 'at', 'zero', 'chemical', 'potential', 'our', 'simulations', 'use', 'both', 'improved', 'asqtad', 'and', 'p4', 'staggered', 'quarks', 'on', 'lattices', 'wit... | [-0.09440223097660672, 0.1563806169758643, -0.11841858396524782, 0.03609088309914679, -0.011613097553653223, -0.06773429659094561, 0.14762935473013097, 0.3704007770362738, -0.14610754542035964, -0.3254092608553332, 0.08895501167710602, -0.2926864003477333, -0.024826985725142935, 0.15666354718609704, 0.0316811260423279,... |
710.1656 | Heavy deformed nuclei in the shell model Monte Carlo method | We extend the shell model Monte Carlo approach to heavy deformed nuclei using
a new proton-neutron formalism. The low excitation energies of such nuclei
necessitate calculations at low temperatures for which a stabilization method
is implemented in the canonical ensemble. We apply the method to study a well
deformed ... | nucl-th | we extend the shell model monte carlo approach to heavy deformed nuclei using a new protonneutron formalism the low excitation energies of such nuclei necessitate calculations at low temperatures for which a stabilization method is implemented in the canonical ensemble we apply the method to study a well deformed raree... | [['we', 'extend', 'the', 'shell', 'model', 'monte', 'carlo', 'approach', 'to', 'heavy', 'deformed', 'nuclei', 'using', 'a', 'new', 'protonneutron', 'formalism', 'the', 'low', 'excitation', 'energies', 'of', 'such', 'nuclei', 'necessitate', 'calculations', 'at', 'low', 'temperatures', 'for', 'which', 'a', 'stabilization... | [-0.004097019853846481, 0.14744827355413387, -0.09434592871693895, 0.14052923976754148, 0.05524428755743429, -0.09301320615923032, 0.04788133690599352, 0.3936797538617005, -0.1753833013237454, -0.2962885532062501, -0.05132883824990131, -0.2961669575655833, -0.053697597398422656, 0.13129342557028092, 0.05819334233092377... |
710.1657 | Manipulating Biopolymer Dynamics by Anisotropic Nanoconfinement | How the geometry of nano-sized confinement affects dynamics of biomaterials
is interesting yet poorly understood. An elucidation of structural details upon
nano-sized confinement may benefit manufacturing pharmaceuticals in biomaterial
sciences and medicine. The behavior of biopolymers in nano-sized confinement is
in... | physics.bio-ph | how the geometry of nanosized confinement affects dynamics of biomaterials is interesting yet poorly understood an elucidation of structural details upon nanosized confinement may benefit manufacturing pharmaceuticals in biomaterial sciences and medicine the behavior of biopolymers in nanosized confinement is investiga... | [['how', 'the', 'geometry', 'of', 'nanosized', 'confinement', 'affects', 'dynamics', 'of', 'biomaterials', 'is', 'interesting', 'yet', 'poorly', 'understood', 'an', 'elucidation', 'of', 'structural', 'details', 'upon', 'nanosized', 'confinement', 'may', 'benefit', 'manufacturing', 'pharmaceuticals', 'in', 'biomaterial'... | [-0.10180541508335379, 0.18814450138609484, -0.07986798716498719, 0.05912931849748167, -0.027088608595565142, -0.09101552024038674, 0.01321809250305617, 0.41519243354278224, -0.2811773204893172, -0.29354762306977666, 0.03874857248944951, -0.2254503305021283, -0.2280448207541579, 0.15622581325935184, -0.0616032416151175... |
710.1658 | Comment on GL(2,R) geometry of 4th order ODEs | We describe 4th order ODEs satisfying two contact invariant conditions of
Bryant in terms of the Ricci tensor of a certain gl(2,R) valued connection. We
also provide nonhomogeneous examples of such ODEs.
| math.DG | we describe 4th order odes satisfying two contact invariant conditions of bryant in terms of the ricci tensor of a certain gl2r valued connection we also provide nonhomogeneous examples of such odes | [['we', 'describe', '4th', 'order', 'odes', 'satisfying', 'two', 'contact', 'invariant', 'conditions', 'of', 'bryant', 'in', 'terms', 'of', 'the', 'ricci', 'tensor', 'of', 'a', 'certain', 'gl2r', 'valued', 'connection', 'we', 'also', 'provide', 'nonhomogeneous', 'examples', 'of', 'such', 'odes']] | [-0.2859811119851656, 0.07534535398008302, -0.04808053973829374, 0.06862364613334648, -0.14657042739418102, -0.1537480510160094, -0.13110607751877978, 0.30820562364533544, -0.2534944022190757, -0.23183747206348926, 0.13081117490582983, -0.2574172696331516, -0.2417672664159909, 0.12243650620803237, -0.056921160910860635... |
710.1659 | Kraus decomposition for chaotic environments including time-dependent
subsystem Hamiltonians | We derive an exact and explicit Kraus decomposition for the reduced density
of a quantum system simultaneously interacting with time-dependent external
fields and a chaotic environment of thermodynamic dimension. We test the
accuracy of the Kraus decomposition against exact numerical results for a CNOT
gate performed... | quant-ph | we derive an exact and explicit kraus decomposition for the reduced density of a quantum system simultaneously interacting with timedependent external fields and a chaotic environment of thermodynamic dimension we test the accuracy of the kraus decomposition against exact numerical results for a cnot gate performed on ... | [['we', 'derive', 'an', 'exact', 'and', 'explicit', 'kraus', 'decomposition', 'for', 'the', 'reduced', 'density', 'of', 'a', 'quantum', 'system', 'simultaneously', 'interacting', 'with', 'timedependent', 'external', 'fields', 'and', 'a', 'chaotic', 'environment', 'of', 'thermodynamic', 'dimension', 'we', 'test', 'the',... | [-0.2052985124189306, 0.1342316515892398, -0.05128095063657777, 0.0505872146648078, 0.051361251024630024, -0.22056665176500542, 0.09791846717456104, 0.3535063064631981, -0.16303107118221452, -0.29702071359733473, 0.05584502180509672, -0.24082567989574494, -0.09358015084462995, 0.2189916965608309, -0.00966619051413963, ... |
710.166 | Sharing lattices throughout the world: an ILDG status report | The international lattice data grid, a system for sharing gauge configuration
files throughout the world, is operational for the most part. I give a status
report, give some pointers on accessing lattice files, and highlight some of
the available gauge configurations.
| hep-lat | the international lattice data grid a system for sharing gauge configuration files throughout the world is operational for the most part i give a status report give some pointers on accessing lattice files and highlight some of the available gauge configurations | [['the', 'international', 'lattice', 'data', 'grid', 'a', 'system', 'for', 'sharing', 'gauge', 'configuration', 'files', 'throughout', 'the', 'world', 'is', 'operational', 'for', 'the', 'most', 'part', 'i', 'give', 'a', 'status', 'report', 'give', 'some', 'pointers', 'on', 'accessing', 'lattice', 'files', 'and', 'highl... | [-0.21625708007230993, 0.10006979580332594, -0.04010514382886269, 0.042899433901056466, -0.10606718699379665, -0.18365282824308407, 0.08417002752809445, 0.3564440274565685, -0.19489878173292866, -0.2868850110325871, 0.19186870581129703, -0.31513995291074604, -0.03714685937071719, 0.14462580232704966, -0.042640142733367... |
710.1661 | General Theory of the Quantum Kicked Rotator. I | This is the first of a series of two papers. We discuss some basic problems
of the quantum kicked rotator (QKR) and review some important results in the
literature. We point out the flaws in the inverse Cayley transform method to
prove dynamic localization. When $\tau/2\pi$, where $\tau$ is the kick period,
is very c... | nlin.CD | this is the first of a series of two papers we discuss some basic problems of the quantum kicked rotator qkr and review some important results in the literature we point out the flaws in the inverse cayley transform method to prove dynamic localization when tau2pi where tau is the kick period is very close to a rationa... | [['this', 'is', 'the', 'first', 'of', 'a', 'series', 'of', 'two', 'papers', 'we', 'discuss', 'some', 'basic', 'problems', 'of', 'the', 'quantum', 'kicked', 'rotator', 'qkr', 'and', 'review', 'some', 'important', 'results', 'in', 'the', 'literature', 'we', 'point', 'out', 'the', 'flaws', 'in', 'the', 'inverse', 'cayley'... | [-0.14160499439193783, 0.10990298656344583, -0.07306280404075303, 0.09981067019213118, -0.05996180134719576, -0.14859600377861748, 0.03939581751050851, 0.3743444446643645, -0.2854345593950711, -0.2287083316530863, 0.1264497865155466, -0.28062157131154725, -0.218251426005736, 0.24201938675832935, -0.052921068939295685, ... |
710.1662 | The Exact Renormalization Group -- renormalization theory revisited -- | We overview the entire renormalization theory, both perturbative and
non-perturbative, by the method of the exact renormalization group (ERG). We
emphasize particularly on the perturbative application of the ERG to the phi4
theory and QED in the four dimensional euclidean space.
| hep-th | we overview the entire renormalization theory both perturbative and nonperturbative by the method of the exact renormalization group erg we emphasize particularly on the perturbative application of the erg to the phi4 theory and qed in the four dimensional euclidean space | [['we', 'overview', 'the', 'entire', 'renormalization', 'theory', 'both', 'perturbative', 'and', 'nonperturbative', 'by', 'the', 'method', 'of', 'the', 'exact', 'renormalization', 'group', 'erg', 'we', 'emphasize', 'particularly', 'on', 'the', 'perturbative', 'application', 'of', 'the', 'erg', 'to', 'the', 'phi4', 'the... | [-0.11840686142989774, 0.12073803670340921, -0.09331513958892262, 0.1426309845978167, -0.051649104054199486, -0.03039385042176014, 0.02838670691225405, 0.37111024458597347, -0.14503392917899097, -0.24105645207938078, 0.07264044279766428, -0.29581277925384847, -0.1384544830496718, 0.17868977348978926, 0.0286383279258521... |
710.1663 | Modeling Phase-resolved Observations of the Surfaces of Magnetic Neutron
Stars | Recent observations by XMM-Newton detected rotational pulsations in the total
brightness and spectrum of several neutron stars. To properly interpret the
data, accurate modeling of neutron star emission is necessary. Detailed
analysis of the shape and strength of the rotational variations allows a
measurement of the ... | astro-ph | recent observations by xmmnewton detected rotational pulsations in the total brightness and spectrum of several neutron stars to properly interpret the data accurate modeling of neutron star emission is necessary detailed analysis of the shape and strength of the rotational variations allows a measurement of the surfac... | [['recent', 'observations', 'by', 'xmmnewton', 'detected', 'rotational', 'pulsations', 'in', 'the', 'total', 'brightness', 'and', 'spectrum', 'of', 'several', 'neutron', 'stars', 'to', 'properly', 'interpret', 'the', 'data', 'accurate', 'modeling', 'of', 'neutron', 'star', 'emission', 'is', 'necessary', 'detailed', 'an... | [-0.09554765210486948, 0.10219986866771553, -0.09437911542287718, 0.0891768506905161, -0.12768208464452377, -0.038284269040256426, 0.06006904091676309, 0.3872023830966403, -0.19428762753644455, -0.3598177280946402, 0.10242485018170555, -0.28811300244478844, -0.05137211602414027, 0.24905257142381743, -0.0220582771289628... |
710.1664 | On the 2-typical de Rham-Witt complex | In this paper we introduce the 2-typical de Rham-Witt complex for arbitrary
commutative, unital rings and log-rings. We describe this complex for the rings
\Z and \Z_{(2)}, for the log-ring (\Z_{(2)},M) with the canonical
log-structure, and we describe its behaviour under polynomial extensions. In an
appendix we also... | math.KT math.NT | in this paper we introduce the 2typical de rhamwitt complex for arbitrary commutative unital rings and logrings we describe this complex for the rings z and z_2 for the logring z_2m with the canonical logstructure and we describe its behaviour under polynomial extensions in an appendix we also describe the ptypical de ... | [['in', 'this', 'paper', 'we', 'introduce', 'the', '2typical', 'de', 'rhamwitt', 'complex', 'for', 'arbitrary', 'commutative', 'unital', 'rings', 'and', 'logrings', 'we', 'describe', 'this', 'complex', 'for', 'the', 'rings', 'z', 'and', 'z_2', 'for', 'the', 'logring', 'z_2m', 'with', 'the', 'canonical', 'logstructure',... | [-0.19829377183182673, 0.06595625480536414, -0.09889742246066982, 0.09986375297250395, -0.05483806190313771, -0.134459530452097, -0.1134236016543582, 0.3404498952356252, -0.3075571940873157, -0.16712840743870896, 0.052286291067403824, -0.18618339245969598, -0.18955000621181997, 0.16429744530469179, -0.11743281954391437... |
710.1665 | Duality between random trap and barrier models | We discuss the physical consequences of a duality between two models with
quenched disorder, in which particles propagate in one dimension among random
traps or across random barriers. We derive an exact relation between their
diffusion fronts at fixed disorder, and deduce from this that their
disorder-averaged diffu... | cond-mat.stat-mech cond-mat.dis-nn | we discuss the physical consequences of a duality between two models with quenched disorder in which particles propagate in one dimension among random traps or across random barriers we derive an exact relation between their diffusion fronts at fixed disorder and deduce from this that their disorderaveraged diffusion f... | [['we', 'discuss', 'the', 'physical', 'consequences', 'of', 'a', 'duality', 'between', 'two', 'models', 'with', 'quenched', 'disorder', 'in', 'which', 'particles', 'propagate', 'in', 'one', 'dimension', 'among', 'random', 'traps', 'or', 'across', 'random', 'barriers', 'we', 'derive', 'an', 'exact', 'relation', 'between... | [-0.10289692980518868, 0.21840140079083814, -0.08790481661792932, 0.12344779332877721, 0.019824817866021985, -0.1562939276702182, 0.06932619989438113, 0.39237488700120254, -0.3171283760795716, -0.2511112884899905, 0.04228828789606734, -0.28162678217428716, -0.16822633411746127, 0.14251374639570713, 0.031992401391657634... |
710.1666 | The role of Stellar Feedback in the formation of galactic disks and
bulges in a LCDM Universe | Although supernova explosions and stellar winds happens at scales bellow 100
pc, they affect the interstellar medium(ISM) and galaxy formation. We use
cosmological N-body+Hydrodynamics simulations of galaxy formation, as well as
simulations of the ISM to study the effect of stellar feedback on galactic
scales. Stella... | astro-ph | although supernova explosions and stellar winds happens at scales bellow 100 pc they affect the interstellar mediumism and galaxy formation we use cosmological nbodyhydrodynamics simulations of galaxy formation as well as simulations of the ism to study the effect of stellar feedback on galactic scales stellar feedback... | [['although', 'supernova', 'explosions', 'and', 'stellar', 'winds', 'happens', 'at', 'scales', 'bellow', '100', 'pc', 'they', 'affect', 'the', 'interstellar', 'mediumism', 'and', 'galaxy', 'formation', 'we', 'use', 'cosmological', 'nbodyhydrodynamics', 'simulations', 'of', 'galaxy', 'formation', 'as', 'well', 'as', 'si... | [-0.05397596599174325, 0.11426946054818435, -0.060425670504882616, 0.12689579342706844, -0.11293115248656148, -0.026251968260125054, 0.003800627664773614, 0.39784969260486275, -0.19397176003695785, -0.38504943863807856, 0.051908660254284894, -0.25756101885979826, 0.020588525473237872, 0.1949707647493285, -0.01195622289... |
710.1667 | Consistence of a GL(3,R) gauge formulation for topological massive
gravity | We include a Chern-Simons term in a GL(3,R) gauge formulation of gravity with
a cosmological contribution in 2+1 dimension and we explore consistence showing
that excitations must be causal and standard topological massive gravity is
recovered from this type of construction at the torsionless limit.
| gr-qc | we include a chernsimons term in a gl3r gauge formulation of gravity with a cosmological contribution in 21 dimension and we explore consistence showing that excitations must be causal and standard topological massive gravity is recovered from this type of construction at the torsionless limit | [['we', 'include', 'a', 'chernsimons', 'term', 'in', 'a', 'gl3r', 'gauge', 'formulation', 'of', 'gravity', 'with', 'a', 'cosmological', 'contribution', 'in', '21', 'dimension', 'and', 'we', 'explore', 'consistence', 'showing', 'that', 'excitations', 'must', 'be', 'causal', 'and', 'standard', 'topological', 'massive', '... | [-0.16414867556757398, 0.14882779493927956, -0.09730165382433269, 0.09662227628545629, -0.10104695880371663, -0.14400817450756828, -0.01197646852168772, 0.2477578161077367, -0.1850076284673479, -0.2755752115510404, 0.08187112950512933, -0.26747078059448137, -0.18098080816368262, 0.09661029105385145, -0.0879032001209755... |
710.1668 | Direct Detection of Non-Chiral Dark Matter | Direct detection experiments rule out fermion dark matter that is a chiral
representation of the electroweak gauge group. Non-chiral real, complex and
singlet representations, however, provide viable fermion dark matter
candidates. Although any one of these candidates will be virtually impossible
to detect at the LHC... | hep-ph | direct detection experiments rule out fermion dark matter that is a chiral representation of the electroweak gauge group nonchiral real complex and singlet representations however provide viable fermion dark matter candidates although any one of these candidates will be virtually impossible to detect at the lhc it is s... | [['direct', 'detection', 'experiments', 'rule', 'out', 'fermion', 'dark', 'matter', 'that', 'is', 'a', 'chiral', 'representation', 'of', 'the', 'electroweak', 'gauge', 'group', 'nonchiral', 'real', 'complex', 'and', 'singlet', 'representations', 'however', 'provide', 'viable', 'fermion', 'dark', 'matter', 'candidates',... | [-0.1419526305158925, 0.24542771506532401, -0.08226280176075317, 0.11817464867282702, -0.1540500317544987, -0.19165961982475388, 0.0023910876483335133, 0.36502881504987417, -0.20446578154002715, -0.2844284817777923, 0.04993761405593863, -0.2659228125597998, -0.04609372374759606, 0.13511061883526065, 0.08768922280879658... |
710.1669 | Mordell-Lang and Skolem-Mahler-Lech theorems for endomorphisms of
semiabelian varieties | Using the Skolem-Mahler-Lech theorem, we prove a dynamical Mordell-Lang
conjecture for semiabelian varieties.
| math.NT math.AG | using the skolemmahlerlech theorem we prove a dynamical mordelllang conjecture for semiabelian varieties | [['using', 'the', 'skolemmahlerlech', 'theorem', 'we', 'prove', 'a', 'dynamical', 'mordelllang', 'conjecture', 'for', 'semiabelian', 'varieties']] | [-0.2906729275217423, -0.017303028645423744, -0.2926723945599336, 0.20032594123711953, -0.05565549977696859, -0.22427871329888988, 0.016556996350678112, 0.14280161454987067, -0.3290736451745033, -0.11169508042243811, 0.054778554261876986, -0.09110054343294066, -0.1721391282402552, 0.29216894708000696, -0.28517391324902... |
710.167 | Fermion Production in Strong Magnetic Field and its Astrophysical
Implications | We calculate the effective potential of a strong magnetic field induced by
fermions with anomalous magnetic moments which couple to the electromagnetic
field in the form of the Pauli interaction. For a uniform magnetic field, we
find the explicit form of the effective potential. It is found that the
non-vanishing ima... | hep-th | we calculate the effective potential of a strong magnetic field induced by fermions with anomalous magnetic moments which couple to the electromagnetic field in the form of the pauli interaction for a uniform magnetic field we find the explicit form of the effective potential it is found that the nonvanishing imaginary... | [['we', 'calculate', 'the', 'effective', 'potential', 'of', 'a', 'strong', 'magnetic', 'field', 'induced', 'by', 'fermions', 'with', 'anomalous', 'magnetic', 'moments', 'which', 'couple', 'to', 'the', 'electromagnetic', 'field', 'in', 'the', 'form', 'of', 'the', 'pauli', 'interaction', 'for', 'a', 'uniform', 'magnetic'... | [-0.20140556494486245, 0.20128592137565754, -0.05806060402161058, 0.1076663806275439, -0.10297035341534544, -0.06590249255463919, -0.01622184109463192, 0.3392494784668088, -0.2349425828002174, -0.29495642136487943, 0.042394029255271616, -0.2318870323819711, -0.15243317310369628, 0.19948341860709823, 0.07870029644931063... |
710.1671 | Jet isomorphism for conformal geometry | Jet isomorphism theorems for conformal geometry are discussed. A new proof of
the jet isomorphism theorem for odd-dimensional conformal geometry is outlined,
using an ambient realization of the conformal deformation complex. An infinite
order ambient lift for conformal densities in the case in which harmonic
extensio... | math.DG | jet isomorphism theorems for conformal geometry are discussed a new proof of the jet isomorphism theorem for odddimensional conformal geometry is outlined using an ambient realization of the conformal deformation complex an infinite order ambient lift for conformal densities in the case in which harmonic extension is o... | [['jet', 'isomorphism', 'theorems', 'for', 'conformal', 'geometry', 'are', 'discussed', 'a', 'new', 'proof', 'of', 'the', 'jet', 'isomorphism', 'theorem', 'for', 'odddimensional', 'conformal', 'geometry', 'is', 'outlined', 'using', 'an', 'ambient', 'realization', 'of', 'the', 'conformal', 'deformation', 'complex', 'an'... | [-0.15804478699622088, 0.13932356005255453, -0.08127529653784347, 0.08880271288655596, -0.11091431921781743, -0.1527815213401432, -0.1254305459865152, 0.3454071097586253, -0.2307288626795762, -0.20700775663534257, 0.11293087264025355, -0.19122554740728173, -0.13386694022313986, 0.1846973392857264, -0.08912777481919588,... |
710.1672 | A Kaluza-Klein Model with Spontaneous Symmetry Breaking: Light-Particle
Effective Action and its Compactification Scale Dependence | We investigate decoupling of heavy Kaluza-Klein modes in an Abelian Higgs
model with space-time topologies $\mathbb{R}^{3,1} \times S^{1}$ and
$\mathbb{R}^{3,1} \times S^{1}/\mathbb{Z}_{2}$. After integrating out heavy KK
modes we find the effective action for the zero mode fields. We find that in
the $\mathbb{R}^{3,... | hep-th | we investigate decoupling of heavy kaluzaklein modes in an abelian higgs model with spacetime topologies mathbbr31 times s1 and mathbbr31 times s1mathbbz_2 after integrating out heavy kk modes we find the effective action for the zero mode fields we find that in the mathbbr31 times s1 topology the heavy modes do not de... | [['we', 'investigate', 'decoupling', 'of', 'heavy', 'kaluzaklein', 'modes', 'in', 'an', 'abelian', 'higgs', 'model', 'with', 'spacetime', 'topologies', 'mathbbr31', 'times', 's1', 'and', 'mathbbr31', 'times', 's1mathbbz_2', 'after', 'integrating', 'out', 'heavy', 'kk', 'modes', 'we', 'find', 'the', 'effective', 'action... | [-0.17563589406108804, 0.24482192364263256, -0.06077070352330338, 0.10126717489674775, -0.0824852778438867, -0.12939513465880736, 0.026137210586512083, 0.3318443532225501, -0.21362307290655735, -0.27963347244735814, 0.09700198287282547, -0.2789334405824775, -0.09183910645742799, 0.11209086728513284, -0.0277871259331732... |
710.1673 | Conformal SO(2,4) Transformations of the One-Cusp Wilson Loop Surface | By applying the conformal SO(2,4) transformations to the elementary one-cusp
Wilson loop surface we construct various two-cusp and four-cusp Wilson loop
surface configurations in AdS_5 and demonstrate that they solve the string
equations of the Nambu-Goto string action. The conformal boosts of the basic
four-cusp Wil... | hep-th | by applying the conformal so24 transformations to the elementary onecusp wilson loop surface we construct various twocusp and fourcusp wilson loop surface configurations in ads_5 and demonstrate that they solve the string equations of the nambugoto string action the conformal boosts of the basic fourcusp wilson loop su... | [['by', 'applying', 'the', 'conformal', 'so24', 'transformations', 'to', 'the', 'elementary', 'onecusp', 'wilson', 'loop', 'surface', 'we', 'construct', 'various', 'twocusp', 'and', 'fourcusp', 'wilson', 'loop', 'surface', 'configurations', 'in', 'ads_5', 'and', 'demonstrate', 'that', 'they', 'solve', 'the', 'string', ... | [-0.13035209018101052, 0.19792141094122354, -0.06478832724288379, 0.12625294223018899, -0.05129243703786193, -0.15603891139418433, -0.017118402115046616, 0.37211336708832077, -0.19750310573726892, -0.2261485679688432, 0.1134200910909851, -0.27908263434996694, -0.16269328835968314, 0.13979341370258025, -0.09294517164504... |
710.1674 | Interference of surface plasmon polaritions controlled by the phase of
incident light | Interference patterns of surface plasmon polaritons(SPPs) are observed in the
extraordinary optical transmission through subwavelength holes in optically
thick metal plate. It is found that the phase of incident light can be
transferred to SPPs. We can control the destructive and constructive
interference of SPPs by ... | physics.optics | interference patterns of surface plasmon polaritonsspps are observed in the extraordinary optical transmission through subwavelength holes in optically thick metal plate it is found that the phase of incident light can be transferred to spps we can control the destructive and constructive interference of spps by modula... | [['interference', 'patterns', 'of', 'surface', 'plasmon', 'polaritonsspps', 'are', 'observed', 'in', 'the', 'extraordinary', 'optical', 'transmission', 'through', 'subwavelength', 'holes', 'in', 'optically', 'thick', 'metal', 'plate', 'it', 'is', 'found', 'that', 'the', 'phase', 'of', 'incident', 'light', 'can', 'be', ... | [-0.22225854928061986, 0.25685397207012606, -0.1550881081364221, 0.049360321157210924, -0.06510235322639346, -0.1905477149153335, 0.04975397736416198, 0.5077860562079068, -0.25027120899822974, -0.342488385808085, -0.04750311378868193, -0.3141155476850044, -0.15597321157757607, 0.19402853089074293, -0.02028613811125979,... |
710.1675 | Is the cosmological "constant" a nonlocal quantum residue of
discreteness of the causal set type? | The evidence for an accelerating Hubble expansion appears to have confirmed
the heuristic prediction, from causal set theory, of a fluctuating and
``ever-present'' cosmological term in the Einstein equations. A more concrete
phenomenological model incorporating this prediction has been devised and
tested, but it rema... | gr-qc astro-ph hep-th | the evidence for an accelerating hubble expansion appears to have confirmed the heuristic prediction from causal set theory of a fluctuating and everpresent cosmological term in the einstein equations a more concrete phenomenological model incorporating this prediction has been devised and tested but it remains incompl... | [['the', 'evidence', 'for', 'an', 'accelerating', 'hubble', 'expansion', 'appears', 'to', 'have', 'confirmed', 'the', 'heuristic', 'prediction', 'from', 'causal', 'set', 'theory', 'of', 'a', 'fluctuating', 'and', 'everpresent', 'cosmological', 'term', 'in', 'the', 'einstein', 'equations', 'a', 'more', 'concrete', 'phen... | [-0.09080599141945582, 0.07917370942572409, -0.11961576845046253, 0.11176684254502517, -0.1444514843545133, -0.14968702934622283, 0.004954912615264015, 0.33538697248384836, -0.2205055733361552, -0.279204802910587, 0.11080268425528982, -0.2543373917034196, -0.15340296046868448, 0.1766192449384459, -0.045429395737066385,... |
710.1676 | Electric Transport Properties of the p53 Gene and the Effects of Point
Mutations | In this work, charge transport (CT) properties of the p53 gene are
numerically studied by the transfer matrix method, and using either single or
double strand effective tight-binding models. A statistical analysis of the
consequences of known p53 point mutations on CT features is performed. It is
found that in contra... | q-bio.GN | in this work charge transport ct properties of the p53 gene are numerically studied by the transfer matrix method and using either single or double strand effective tightbinding models a statistical analysis of the consequences of known p53 point mutations on ct features is performed it is found that in contrast to oth... | [['in', 'this', 'work', 'charge', 'transport', 'ct', 'properties', 'of', 'the', 'p53', 'gene', 'are', 'numerically', 'studied', 'by', 'the', 'transfer', 'matrix', 'method', 'and', 'using', 'either', 'single', 'or', 'double', 'strand', 'effective', 'tightbinding', 'models', 'a', 'statistical', 'analysis', 'of', 'the', '... | [-0.058185045501320726, 0.08720935204522297, -0.04258751468215552, 0.1219242436086966, 0.004650352957348029, -0.14514725778976248, 0.08584215439493871, 0.3682278168698152, -0.26619384274818003, -0.25414678230881693, 0.03692888947100275, -0.2613021918055084, -0.25308496709913014, 0.1841233321129241, -0.05729580404650834... |
710.1677 | A Search for 6.7 GHz Methanol Masers in M33 | We report the negative results from a search for 6.7 GHz methanol masers in
the nearby spiral galaxy M33. We observed 14 GMCs in the central 4 kpc of the
Galaxy, and found 3 sigma upper limits to the flux density of ~9 mJy in
spectral channels having a velocity width of 0.069 km/s. By velocity shifting
and combining ... | astro-ph | we report the negative results from a search for 67 ghz methanol masers in the nearby spiral galaxy m33 we observed 14 gmcs in the central 4 kpc of the galaxy and found 3 sigma upper limits to the flux density of 9 mjy in spectral channels having a velocity width of 0069 kms by velocity shifting and combining the spect... | [['we', 'report', 'the', 'negative', 'results', 'from', 'a', 'search', 'for', '67', 'ghz', 'methanol', 'masers', 'in', 'the', 'nearby', 'spiral', 'galaxy', 'm33', 'we', 'observed', '14', 'gmcs', 'in', 'the', 'central', '4', 'kpc', 'of', 'the', 'galaxy', 'and', 'found', '3', 'sigma', 'upper', 'limits', 'to', 'the', 'flu... | [-0.08230470820788795, 0.07227601623260364, -0.04208091162701151, 0.06694337637111572, -0.07285132783520688, -0.04694733438916059, 0.10503591665191882, 0.4169006260223131, -0.12399930209216814, -0.34765825291344926, 0.035112560051775696, -0.2595298713378942, -0.002128240158920413, 0.20225639051910657, 0.007897496560532... |
710.1678 | Resolving the Formation of Protogalaxies. II. Central Gravitational
Collapse | Numerous cosmological hydrodynamic studies have addressed the formation of
galaxies. Here we choose to study the first stages of galaxy formation,
including non-equilibrium atomic primordial gas cooling, gravity and
hydrodynamics. Using initial conditions appropriate for the concordance
cosmological model of structur... | astro-ph | numerous cosmological hydrodynamic studies have addressed the formation of galaxies here we choose to study the first stages of galaxy formation including nonequilibrium atomic primordial gas cooling gravity and hydrodynamics using initial conditions appropriate for the concordance cosmological model of structure forma... | [['numerous', 'cosmological', 'hydrodynamic', 'studies', 'have', 'addressed', 'the', 'formation', 'of', 'galaxies', 'here', 'we', 'choose', 'to', 'study', 'the', 'first', 'stages', 'of', 'galaxy', 'formation', 'including', 'nonequilibrium', 'atomic', 'primordial', 'gas', 'cooling', 'gravity', 'and', 'hydrodynamics', 'u... | [-0.12079490054762501, 0.16399305622825752, -0.05131157000308199, 0.1155753479760826, -0.018742165543296517, -0.04321111086292646, -0.026785626942616197, 0.34136127680540085, -0.19408168729663414, -0.33988868513269654, 0.04642700308827285, -0.24435547864602053, 0.014677135037508473, 0.16723642195459104, 0.0458619784846... |
710.1679 | On computations of Hurwitz-Hodge integrals | We describe a method to compute Hurwitz-Hodge integrals.
| math.AG math.SG | we describe a method to compute hurwitzhodge integrals | [['we', 'describe', 'a', 'method', 'to', 'compute', 'hurwitzhodge', 'integrals']] | [-0.16183123737573624, -0.052442997111938894, -0.20266099367290735, 0.1952240839600563, -0.10850010113790631, -0.039308581210207194, 0.05109299346804619, 0.4101442899554968, -0.27859799936413765, -0.205934954341501, 0.037245600193273276, -0.23632067069411278, -0.2712330278009176, 0.24233943689614534, -0.109172337106429... |
710.168 | On vacuum structures of N = 2 LSUSY QED equivalent to N = 2 NLSUSY model | The vacuum structure of N = 2 linear supersymmetry (LSUSY) invariant QED,
which is equivalent to N = 2 nonlinear supersymmetry (NLSUSY) model, is studied
explicitly in two dimensional space-time (d = 2). Two different isometries
SO(1,3) and SO(3,1) appear for the vacuum field configuration corresponding to
the variou... | hep-th | the vacuum structure of n 2 linear supersymmetry lsusy invariant qed which is equivalent to n 2 nonlinear supersymmetry nlsusy model is studied explicitly in two dimensional spacetime d 2 two different isometries so13 and so31 appear for the vacuum field configuration corresponding to the various parameter regions two ... | [['the', 'vacuum', 'structure', 'of', 'n', '2', 'linear', 'supersymmetry', 'lsusy', 'invariant', 'qed', 'which', 'is', 'equivalent', 'to', 'n', '2', 'nonlinear', 'supersymmetry', 'nlsusy', 'model', 'is', 'studied', 'explicitly', 'in', 'two', 'dimensional', 'spacetime', 'd', '2', 'two', 'different', 'isometries', 'so13'... | [-0.19519127825716218, 0.27526987676576126, -0.003741616220826185, 0.14329055028256812, -0.075177487368867, -0.2363348792821757, -0.11187461318484948, 0.3504183187002414, -0.20368817205369277, -0.29671842375414836, 0.10431406888835083, -0.20229806353975283, -0.08158634629063799, 0.01330061890123608, 0.01674068012231911... |
710.1681 | Tree FCNC and non-unitarity of CKM matrix | We discuss possible signatures of the tree level FCNC, which results from the
non-unitarity of CKM matrix. We first define the unitaity step-by-step, and
possible test of the non-unitaity through the 4-value-KM parametrization. We,
then, show how the phase angle of the unitary triangle would change in case of
the vec... | hep-ph | we discuss possible signatures of the tree level fcnc which results from the nonunitarity of ckm matrix we first define the unitaity stepbystep and possible test of the nonunitaity through the 4valuekm parametrization we then show how the phase angle of the unitary triangle would change in case of the vectorlike down q... | [['we', 'discuss', 'possible', 'signatures', 'of', 'the', 'tree', 'level', 'fcnc', 'which', 'results', 'from', 'the', 'nonunitarity', 'of', 'ckm', 'matrix', 'we', 'first', 'define', 'the', 'unitaity', 'stepbystep', 'and', 'possible', 'test', 'of', 'the', 'nonunitaity', 'through', 'the', '4valuekm', 'parametrization', '... | [-0.08829137584608462, 0.22372877800242147, -0.040206499552975096, 0.09716291808419758, -0.09365730737853381, -0.12407488363613892, 0.17724306696456754, 0.3321738350722525, -0.29590214675085413, -0.25580324593465775, 0.06297383199206605, -0.26607577628197354, -0.15716464719217685, 0.09711566049372777, 0.035607784352679... |
710.1682 | Constraining the parameters of binary systems through time-dependent
light deflection | A theory is derived relating the configuration of the cores of active
galaxies, specifically candidates for presumed super-massive black hole
binaries (SMBHBs), to time-dependent changes in images of those galaxies. Three
deflection quantities, resulting from the monopole term, mass quadrupole term,
and spin dipole t... | gr-qc | a theory is derived relating the configuration of the cores of active galaxies specifically candidates for presumed supermassive black hole binaries smbhbs to timedependent changes in images of those galaxies three deflection quantities resulting from the monopole term mass quadrupole term and spin dipole term of the c... | [['a', 'theory', 'is', 'derived', 'relating', 'the', 'configuration', 'of', 'the', 'cores', 'of', 'active', 'galaxies', 'specifically', 'candidates', 'for', 'presumed', 'supermassive', 'black', 'hole', 'binaries', 'smbhbs', 'to', 'timedependent', 'changes', 'in', 'images', 'of', 'those', 'galaxies', 'three', 'deflectio... | [-0.09058658771927615, 0.08998978559107504, -0.05078920028417518, 0.1187231881746189, -0.07537163935168728, -0.08872952520144745, 0.025531483212130536, 0.37368237944483235, -0.15663721182040477, -0.3660498188988289, 0.07229453514293327, -0.25321330224866406, -0.09728123412851505, 0.2651078346381454, -0.0544724662118313... |
710.1683 | Biases in the Gravitational Lens Population Induced by Halo and Galaxy
Triaxiality | The lensing cross section of triaxial halos depends on the relative
orientation between a halo's principal axes and its line of sight.
Consequently, a lensing subsample of randomly oriented halos is not, in
general,randomly oriented. Using an isothermal mass model for the lensing
galaxies and their host halos, we sho... | astro-ph | the lensing cross section of triaxial halos depends on the relative orientation between a halos principal axes and its line of sight consequently a lensing subsample of randomly oriented halos is not in generalrandomly oriented using an isothermal mass model for the lensing galaxies and their host halos we show that th... | [['the', 'lensing', 'cross', 'section', 'of', 'triaxial', 'halos', 'depends', 'on', 'the', 'relative', 'orientation', 'between', 'a', 'halos', 'principal', 'axes', 'and', 'its', 'line', 'of', 'sight', 'consequently', 'a', 'lensing', 'subsample', 'of', 'randomly', 'oriented', 'halos', 'is', 'not', 'in', 'generalrandomly... | [-0.14398451644275462, 0.09275664384721188, -0.0826148452127681, 0.09256935238783412, -0.09820192259422598, -0.023963741620723657, -0.01070525844981097, 0.44859920414214466, -0.15923255535071706, -0.3545046715155483, -0.0013895039714344921, -0.28379167444047765, -0.02759494609106083, 0.1697434777316742, 0.0250448189802... |
710.1684 | Comments on gluon 6-point scattering amplitudes in N=4 SYM at strong
coupling | We use the AdS/CFT prescription of Alday and Maldacena \cite{am} to analyze
gluon 6-point scattering amplitudes at strong coupling in ${\cal N}=4$ SYM. By
cutting and gluing we obtain AdS 6-point amplitudes that contain extra boundary
conditions and come close to matching the field theory results. We interpret
them a... | hep-th | we use the adscft prescription of alday and maldacena citeam to analyze gluon 6point scattering amplitudes at strong coupling in cal n4 sym by cutting and gluing we obtain ads 6point amplitudes that contain extra boundary conditions and come close to matching the field theory results we interpret them as parts of the f... | [['we', 'use', 'the', 'adscft', 'prescription', 'of', 'alday', 'and', 'maldacena', 'citeam', 'to', 'analyze', 'gluon', '6point', 'scattering', 'amplitudes', 'at', 'strong', 'coupling', 'in', 'cal', 'n4', 'sym', 'by', 'cutting', 'and', 'gluing', 'we', 'obtain', 'ads', '6point', 'amplitudes', 'that', 'contain', 'extra', ... | [-0.15476471682079138, 0.16218441421786944, -0.09668190874780218, 0.1622220294177532, -0.06358872277041276, -0.09654083378302554, 0.032933500741298, 0.36146658783157665, -0.13689945479234059, -0.2483264600361387, 0.07862308384074519, -0.2975794291123748, -0.17830407332628964, 0.09958289310336113, -0.029804122758408387,... |
710.1685 | Natural scale of cosmological constant in seesaw mechanism with broken
SUSY | The cosmological constant is inherently determined by the scale of breaking
down supersymmetry in the mechanism of seesaw fluctuations of two
vacuum-states.
| hep-th gr-qc hep-ph | the cosmological constant is inherently determined by the scale of breaking down supersymmetry in the mechanism of seesaw fluctuations of two vacuumstates | [['the', 'cosmological', 'constant', 'is', 'inherently', 'determined', 'by', 'the', 'scale', 'of', 'breaking', 'down', 'supersymmetry', 'in', 'the', 'mechanism', 'of', 'seesaw', 'fluctuations', 'of', 'two', 'vacuumstates']] | [-0.21146572336909317, 0.29710072314455394, -0.005525302585391771, 0.17673674086663163, -0.0814228274282955, -0.1614086394796946, -0.013931312199149812, 0.2761619020076025, -0.32428766574178425, -0.3292271246512731, 0.13434336504655048, -0.1747909113321276, -0.03873893547625769, 0.06657865537064415, 0.06517493627255871... |
710.1686 | Electronic functionalization of the surface of organic semiconductors
with self-assembled monolayers | Molecular self-assembly has been extensively used for surface modification of
metals and oxides for a variety of applications, including molecular and
organic electronics. One of the goals of this research is to learn how the
electronic properties of these surfaces can be modified by self-assembled
monolayers (SAM). ... | cond-mat.mtrl-sci | molecular selfassembly has been extensively used for surface modification of metals and oxides for a variety of applications including molecular and organic electronics one of the goals of this research is to learn how the electronic properties of these surfaces can be modified by selfassembled monolayers sam here we d... | [['molecular', 'selfassembly', 'has', 'been', 'extensively', 'used', 'for', 'surface', 'modification', 'of', 'metals', 'and', 'oxides', 'for', 'a', 'variety', 'of', 'applications', 'including', 'molecular', 'and', 'organic', 'electronics', 'one', 'of', 'the', 'goals', 'of', 'this', 'research', 'is', 'to', 'learn', 'how... | [-0.10904887167555166, 0.1632421846174466, -0.016071131180335835, -0.030339216157544133, -0.0003023358862619938, -0.14123827110260453, 0.041908482456275986, 0.42131201165058174, -0.2375204452972223, -0.2961695879334357, 0.028530520240055035, -0.28510913508376334, -0.17034966279695765, 0.2198604816377799, -0.00782087030... |
710.1687 | Statistically interacting quasiparticles in Ising chains | The exclusion statistics of two complementary sets of quasiparticles,
generated from opposite ends of the spectrum, are identified for Ising chains
with spin s=1/2,1. In the s=1/2 case the two sets are antiferromagnetic domain
walls (solitons) and ferromagnetic domains (strings). In the s=1 case they are
soliton pair... | cond-mat.stat-mech | the exclusion statistics of two complementary sets of quasiparticles generated from opposite ends of the spectrum are identified for ising chains with spin s121 in the s12 case the two sets are antiferromagnetic domain walls solitons and ferromagnetic domains strings in the s1 case they are soliton pairs and nested str... | [['the', 'exclusion', 'statistics', 'of', 'two', 'complementary', 'sets', 'of', 'quasiparticles', 'generated', 'from', 'opposite', 'ends', 'of', 'the', 'spectrum', 'are', 'identified', 'for', 'ising', 'chains', 'with', 'spin', 's121', 'in', 'the', 's12', 'case', 'the', 'two', 'sets', 'are', 'antiferromagnetic', 'domain... | [-0.21428886712544082, 0.18315668238057314, -0.014567478480258663, 0.09839961829665729, 0.00013313869529060627, -0.16994533696407943, 0.01754503190290722, 0.4034582293580139, -0.214155735055867, -0.20725119799547093, 0.10007081274172953, -0.38101840210392285, 0.00022978786575166802, 0.17438895802019702, 0.0913448205223... |
710.1688 | Adaptive estimation of linear functionals by model selection | We propose an estimation procedure for linear functionals based on Gaussian
model selection techniques. We show that the procedure is adaptive, and we give
a non asymptotic oracle inequality for the risk of the selected estimator with
respect to the $\mathbb{L}_p$ loss. An application to the problem of estimating
a s... | math.ST stat.TH | we propose an estimation procedure for linear functionals based on gaussian model selection techniques we show that the procedure is adaptive and we give a non asymptotic oracle inequality for the risk of the selected estimator with respect to the mathbbl_p loss an application to the problem of estimating a signal or i... | [['we', 'propose', 'an', 'estimation', 'procedure', 'for', 'linear', 'functionals', 'based', 'on', 'gaussian', 'model', 'selection', 'techniques', 'we', 'show', 'that', 'the', 'procedure', 'is', 'adaptive', 'and', 'we', 'give', 'a', 'non', 'asymptotic', 'oracle', 'inequality', 'for', 'the', 'risk', 'of', 'the', 'select... | [-0.07265003282015049, -0.011770670956932933, -0.13821648034943446, 0.08137947958358194, -0.03422319378319477, -0.13723369087979553, 0.08658492585111942, 0.3942532980082823, -0.2602344025222082, -0.25385136581035256, 0.1560824503678651, -0.27362737083984984, -0.1397649075462675, 0.23227469182928048, -0.1332738508972975... |
710.1689 | Formation and Growth of Nanowire | The kinetics of main physical processes controlling the growth of nanowires
(NW) via evolution pass " vapor-liquid-solid" is considered. The roles of the
thermodynamics and kinetics of cluster nucleation in the initial stage of NW
formation are studied. Approximate expressions for NW length are obtained in
one-dimens... | cond-mat.mtrl-sci | the kinetics of main physical processes controlling the growth of nanowires nw via evolution pass vaporliquidsolid is considered the roles of the thermodynamics and kinetics of cluster nucleation in the initial stage of nw formation are studied approximate expressions for nw length are obtained in onedimensional approx... | [['the', 'kinetics', 'of', 'main', 'physical', 'processes', 'controlling', 'the', 'growth', 'of', 'nanowires', 'nw', 'via', 'evolution', 'pass', 'vaporliquidsolid', 'is', 'considered', 'the', 'roles', 'of', 'the', 'thermodynamics', 'and', 'kinetics', 'of', 'cluster', 'nucleation', 'in', 'the', 'initial', 'stage', 'of',... | [-0.1124788242453579, 0.14510964037930613, -0.022461443258229123, -0.008289261191572634, 0.023427498262746118, -0.09263813972312918, 0.03336399833681763, 0.4003277241442633, -0.25554397508942633, -0.25843875883247264, 0.057590139480257624, -0.27961401216765885, -0.06365233389360289, 0.19679586226821585, 0.0697716152375... |
710.169 | Inference in nonparametric current status models with covariates | In interval censored models with current status observations, the variables
are indicators of the presence of individuals on observation intervals and
covariates. When several individuals share the same observation interval, a
simple procedure provides new estimators for the distribution of the
observation times and ... | math.ST stat.TH | in interval censored models with current status observations the variables are indicators of the presence of individuals on observation intervals and covariates when several individuals share the same observation interval a simple procedure provides new estimators for the distribution of the observation times and their... | [['in', 'interval', 'censored', 'models', 'with', 'current', 'status', 'observations', 'the', 'variables', 'are', 'indicators', 'of', 'the', 'presence', 'of', 'individuals', 'on', 'observation', 'intervals', 'and', 'covariates', 'when', 'several', 'individuals', 'share', 'the', 'same', 'observation', 'interval', 'a', '... | [-0.12497259430630608, 0.10613989870627086, -0.0776141956123675, 0.11378531922521286, -0.044653735903286654, -0.1447230266667036, 0.1043457557368742, 0.4316756243189407, -0.19636682899625496, -0.31263716995369556, 0.13086653033238943, -0.3033832340869446, -0.06485587197659147, 0.1989922186056542, -0.06482242758190909, ... |
710.1691 | UCDs - more massive than allowed? | Dynamical mass estimates of ultra-compact dwarfs galaxies and massive
globular clusters in the Fornax and Virgo clusters and around the giant
elliptical Cen A have revealed some surprising results: 1) above about 10^6
M_sun the mass-to-light (M/L) ratio increases with the objects' mass; 2) some
UCDs/massive GCs show ... | astro-ph | dynamical mass estimates of ultracompact dwarfs galaxies and massive globular clusters in the fornax and virgo clusters and around the giant elliptical cen a have revealed some surprising results 1 above about 106 m_sun the masstolight ml ratio increases with the objects mass 2 some ucdsmassive gcs show high ml values ... | [['dynamical', 'mass', 'estimates', 'of', 'ultracompact', 'dwarfs', 'galaxies', 'and', 'massive', 'globular', 'clusters', 'in', 'the', 'fornax', 'and', 'virgo', 'clusters', 'and', 'around', 'the', 'giant', 'elliptical', 'cen', 'a', 'have', 'revealed', 'some', 'surprising', 'results', '1', 'above', 'about', '106', 'm_su... | [-0.06837126366603612, 0.09350823500532318, -0.05886629239910028, 0.1737126919134012, -0.11470917573791337, -0.05393044064773924, 0.07210416037546978, 0.4334286654198712, -0.06421969267116352, -0.416912099278786, -0.011321863557466052, -0.3052745200608942, -0.07206277307546274, 0.20648510990960692, -0.06337149111046032... |
710.1692 | Rates of asymptotic regularity for Halpern iterations of nonexpansive
mappings | In this paper we obtain new effective results on the Halpern iterations of
nonexpansive mappings using methods from mathematical logic or, more
specifically, proof-theoretic techniques. We give effective rates of asymptotic
regularity for the Halpern iterations of nonexpansive self-mappings of nonempty
convex sets in... | math.FA math.LO | in this paper we obtain new effective results on the halpern iterations of nonexpansive mappings using methods from mathematical logic or more specifically prooftheoretic techniques we give effective rates of asymptotic regularity for the halpern iterations of nonexpansive selfmappings of nonempty convex sets in normed... | [['in', 'this', 'paper', 'we', 'obtain', 'new', 'effective', 'results', 'on', 'the', 'halpern', 'iterations', 'of', 'nonexpansive', 'mappings', 'using', 'methods', 'from', 'mathematical', 'logic', 'or', 'more', 'specifically', 'prooftheoretic', 'techniques', 'we', 'give', 'effective', 'rates', 'of', 'asymptotic', 'regu... | [-0.1103347681419109, 0.020553690154985007, -0.10548965213820338, 0.11926699811333998, -0.08770533486838555, -0.12249023052087675, 0.12776606473360314, 0.31915691278926617, -0.2645144513808191, -0.19476326189922272, 0.1259249610545036, -0.27468327213622007, -0.1409207798141223, 0.21483001143335262, -0.19411000767205325... |
710.1693 | Connecting B_d and B_s decays through QCD factorisation and flavour
symmetries | We analyse B_{d,s} -> K(*)0 K(*)0 modes within the SM, relating them in a
controlled way through SU(3)-flavour symmetry and QCD-improved factorisation.
We propose a set of sum rules for such penguin-mediated decays to constrain
some CKM angles. We determine B_s -> KK branching ratios and CP-asymmetries as
functions o... | hep-ph | we analyse b_ds k0 k0 modes within the sm relating them in a controlled way through su3flavour symmetry and qcdimproved factorisation we propose a set of sum rules for such penguinmediated decays to constrain some ckm angles we determine b_s kk branching ratios and cpasymmetries as functions of a_dirb_d k0 bark0 applyi... | [['we', 'analyse', 'b_ds', 'k0', 'k0', 'modes', 'within', 'the', 'sm', 'relating', 'them', 'in', 'a', 'controlled', 'way', 'through', 'su3flavour', 'symmetry', 'and', 'qcdimproved', 'factorisation', 'we', 'propose', 'a', 'set', 'of', 'sum', 'rules', 'for', 'such', 'penguinmediated', 'decays', 'to', 'constrain', 'some',... | [-0.12033925834893763, 0.24777362237114514, -0.07408361622035059, 0.12737646226340266, -0.10772146310295853, -0.1750607739077575, 0.1753317252532996, 0.29968194888710087, -0.26950749474118896, -0.18227487965139436, -0.02331517358942986, -0.3009503764837091, -0.0448053042585058, 0.07910542661296342, 0.06069395467708471,... |
710.1694 | An efficient modulation scheme for dual beam polarimetry | An eight stage balanced modulation scheme for dual beam polarimetry is
presented in this paper. The four Stokes parameters are weighted equally in all
the eight stages of modulation resulting in total polarimetric efficiency of
unity. The gain table error inherent in dual beam system is reduced by using
the well know... | astro-ph | an eight stage balanced modulation scheme for dual beam polarimetry is presented in this paper the four stokes parameters are weighted equally in all the eight stages of modulation resulting in total polarimetric efficiency of unity the gain table error inherent in dual beam system is reduced by using the well known be... | [['an', 'eight', 'stage', 'balanced', 'modulation', 'scheme', 'for', 'dual', 'beam', 'polarimetry', 'is', 'presented', 'in', 'this', 'paper', 'the', 'four', 'stokes', 'parameters', 'are', 'weighted', 'equally', 'in', 'all', 'the', 'eight', 'stages', 'of', 'modulation', 'resulting', 'in', 'total', 'polarimetric', 'effic... | [-0.1302400981677937, 0.12037311864751121, -0.0390570024947072, 0.0016750698064954407, -0.058471536419043936, -0.14449986231000145, 0.006364183539214234, 0.4219250963639696, -0.2249734577957262, -0.3457496303076647, 0.10910677880866035, -0.22295229755291324, -0.07221538472214245, 0.24927617148274467, -0.070177251639574... |
710.1695 | On the large-scale angular distribution of short-Gamma ray bursts | We investigate the large-scale angular distribution of the short-Gamma ray
bursts (SGRBs) from BATSE experiment, using a new coordinates-free method. The
analyses performed take into account the angular correlations induced by the
non-uniform sky exposure during the experiment, and the uncertainty in the
measured ang... | astro-ph | we investigate the largescale angular distribution of the shortgamma ray bursts sgrbs from batse experiment using a new coordinatesfree method the analyses performed take into account the angular correlations induced by the nonuniform sky exposure during the experiment and the uncertainty in the measured angular coordi... | [['we', 'investigate', 'the', 'largescale', 'angular', 'distribution', 'of', 'the', 'shortgamma', 'ray', 'bursts', 'sgrbs', 'from', 'batse', 'experiment', 'using', 'a', 'new', 'coordinatesfree', 'method', 'the', 'analyses', 'performed', 'take', 'into', 'account', 'the', 'angular', 'correlations', 'induced', 'by', 'the'... | [-0.08677793809442551, 0.13581909599877265, -0.10170316324847473, 0.18135926195997865, -0.05548049247061664, -0.02729414101061109, 0.022464148419026237, 0.40961102597028404, -0.2559618057755681, -0.3587800476385595, 0.04854141722218581, -0.35010907183553985, -0.04945378580021781, 0.22564973300262414, 0.0404983517689654... |
710.1696 | pi-pi and pi-K scatterings in three-flavour resummed chiral perturbation
theory | The (light but not-so-light) strange quark may play a special role in the
low-energy dynamics of QCD. The presence of strange quark pairs in the sea may
have a significant impact of the pattern of chiral symmetry breaking : in
particular large differences can occur between the chiral limits of two and
three massless ... | hep-ph | the light but notsolight strange quark may play a special role in the lowenergy dynamics of qcd the presence of strange quark pairs in the sea may have a significant impact of the pattern of chiral symmetry breaking in particular large differences can occur between the chiral limits of two and three massless flavours i... | [['the', 'light', 'but', 'notsolight', 'strange', 'quark', 'may', 'play', 'a', 'special', 'role', 'in', 'the', 'lowenergy', 'dynamics', 'of', 'qcd', 'the', 'presence', 'of', 'strange', 'quark', 'pairs', 'in', 'the', 'sea', 'may', 'have', 'a', 'significant', 'impact', 'of', 'the', 'pattern', 'of', 'chiral', 'symmetry', ... | [-0.153138681810144, 0.23855882515673035, -0.12666156601902664, 0.10692765934676943, -0.08751314622152723, -0.09870738020636362, 0.05500069605798255, 0.3246541127061345, -0.20841283741075609, -0.27655135830706457, 0.04934443689594677, -0.31532665634314705, -0.10528654859093475, 0.09307097164337855, -0.01125930986363219... |
710.1697 | Lifetime of OH masers at the tip of the asymptotic giant branch | Context: A large fraction of otherwise similar asymptotic giant branch stars
(AGB) do not show OH maser emission. As shown recently, a restricted lifetime
may give a natural explanation as to why only part of any sample emits maser
emission at a given epoch.
Aims: We wish to probe the lifetime of 1612 MHz OH masers... | astro-ph | context a large fraction of otherwise similar asymptotic giant branch stars agb do not show oh maser emission as shown recently a restricted lifetime may give a natural explanation as to why only part of any sample emits maser emission at a given epoch aims we wish to probe the lifetime of 1612 mhz oh masers in circums... | [['context', 'a', 'large', 'fraction', 'of', 'otherwise', 'similar', 'asymptotic', 'giant', 'branch', 'stars', 'agb', 'do', 'not', 'show', 'oh', 'maser', 'emission', 'as', 'shown', 'recently', 'a', 'restricted', 'lifetime', 'may', 'give', 'a', 'natural', 'explanation', 'as', 'to', 'why', 'only', 'part', 'of', 'any', 's... | [-0.07345991664944942, 0.13930021609721632, -0.03313069925564578, 0.07184718772320291, -0.1316604162342741, -0.05179944661009194, 0.09303670747489748, 0.45335651435073737, -0.12261106719566761, -0.34543964758746876, 0.04342967192944939, -0.24978979117116012, 0.007836940060343361, 0.12984858955306627, -0.085418154180344... |
710.1698 | Neutron scattering study of magnetic ordering and excitations in the
ternary rare-earth diborocarbide Ce^{11}B_2C_2 | Neutron scattering experiments have been performed on the ternary rare-earth
diborocarbide Ce$^{11}$B$_2$C$_2$. The powder diffraction experiment confirms
formation of a long-range magnetic order at $T_{\rm N} = 7.3$ K, where a
sinusoidally modulated structure is realized with the modulation vector ${\bm
q} = [0.167(... | cond-mat.str-el cond-mat.mtrl-sci | neutron scattering experiments have been performed on the ternary rareearth diborocarbide ce11b_2c_2 the powder diffraction experiment confirms formation of a longrange magnetic order at t_rm n 73 k where a sinusoidally modulated structure is realized with the modulation vector bm q 01673 01673 01143 inelastic excitati... | [['neutron', 'scattering', 'experiments', 'have', 'been', 'performed', 'on', 'the', 'ternary', 'rareearth', 'diborocarbide', 'ce11b_2c_2', 'the', 'powder', 'diffraction', 'experiment', 'confirms', 'formation', 'of', 'a', 'longrange', 'magnetic', 'order', 'at', 't_rm', 'n', '73', 'k', 'where', 'a', 'sinusoidally', 'modu... | [-0.16166718558468404, 0.29604901256895955, -0.0007849181882075725, 0.08765735499515769, -0.006205621741208879, -0.12386492509995738, 0.09845847431720504, 0.3689569282345474, -0.22837822145271686, -0.28641392124155834, -0.08839999531966544, -0.40972023704840294, -0.026078356661263014, 0.09975059707423732, 0.13037881198... |
710.1699 | Finitely generated lattice-ordered groups with soluble word problem | William W. Boone and Graham Higman proved that a finitely generated group has
soluble word problem if and only if it can be embedded in a simple group that
can be embedded in a finitely presented group. We prove the exact analogue for
lattice-ordered groups: Theorem: A finitely generated lattice-ordered group has
sol... | math.GR math.LO | william w boone and graham higman proved that a finitely generated group has soluble word problem if and only if it can be embedded in a simple group that can be embedded in a finitely presented group we prove the exact analogue for latticeordered groups theorem a finitely generated latticeordered group has soluble wor... | [['william', 'w', 'boone', 'and', 'graham', 'higman', 'proved', 'that', 'a', 'finitely', 'generated', 'group', 'has', 'soluble', 'word', 'problem', 'if', 'and', 'only', 'if', 'it', 'can', 'be', 'embedded', 'in', 'a', 'simple', 'group', 'that', 'can', 'be', 'embedded', 'in', 'a', 'finitely', 'presented', 'group', 'we', ... | [-0.10721715969830445, 0.14300269574618818, -0.17422353005343952, 0.07722816401228462, -0.11961524380543798, -0.184825296960195, -0.006869428685491847, 0.42626721253522587, -0.3849481504948176, -0.20319932893149018, 0.14821240618421705, -0.25402986853546705, -0.1348639993745949, 0.2513871358265889, -0.18461155556334355... |
710.17 | The Spatially Closed Universe | The general world model for homogeneous and isotropic universe has been
roposed. For this purpose, we introduce a global and fiducial system of
reference (world reference frame) constructed on a 5-dimensional space-time
that is embedding the universe, and define the line element as the separation
between two neighbor... | astro-ph | the general world model for homogeneous and isotropic universe has been roposed for this purpose we introduce a global and fiducial system of reference world reference frame constructed on a 5dimensional spacetime that is embedding the universe and define the line element as the separation between two neighboring event... | [['the', 'general', 'world', 'model', 'for', 'homogeneous', 'and', 'isotropic', 'universe', 'has', 'been', 'roposed', 'for', 'this', 'purpose', 'we', 'introduce', 'a', 'global', 'and', 'fiducial', 'system', 'of', 'reference', 'world', 'reference', 'frame', 'constructed', 'on', 'a', '5dimensional', 'spacetime', 'that', ... | [-0.12131726094133531, 0.14068976308960743, -0.09735675490379368, 0.08579079037644315, -0.06311655441747495, -0.10424561125109903, -0.03910547918381376, 0.3855764603776926, -0.2135402041521889, -0.2895766419781096, 0.0652890395722352, -0.26395281615787775, -0.04525308615907475, 0.16218452371993206, -0.02962322375123794... |
710.1701 | Exponential Families and MaxEnt Calculations for Entropy Measures of
Statistical Physics | For a wide range of entropy measures, easy calculation of equilibria is
possible using a principle of Game Theoretical Equilibrium related to Jaynes
Maximum Entropy Principle. This follows previous work of the author and relates
to works of Naudts and, partly, Abe and Bagci.
| cond-mat.stat-mech | for a wide range of entropy measures easy calculation of equilibria is possible using a principle of game theoretical equilibrium related to jaynes maximum entropy principle this follows previous work of the author and relates to works of naudts and partly abe and bagci | [['for', 'a', 'wide', 'range', 'of', 'entropy', 'measures', 'easy', 'calculation', 'of', 'equilibria', 'is', 'possible', 'using', 'a', 'principle', 'of', 'game', 'theoretical', 'equilibrium', 'related', 'to', 'jaynes', 'maximum', 'entropy', 'principle', 'this', 'follows', 'previous', 'work', 'of', 'the', 'author', 'and... | [-0.07928836481137709, 0.07417509701124138, -0.1568227648227052, 0.05977624735202302, -0.06962073865261945, -0.1579438241156326, 0.1383252646139061, 0.2640522833574902, -0.25524924880697986, -0.32957251285287464, 0.048945272304329344, -0.2748689641964368, -0.09535049797374416, 0.16689972736110742, -0.19146016887812453,... |
710.1702 | Formation of solitons in atomic Bose-Einstein condensates by dark-state
adiabatic passage | We propose a new method of creating solitons in elongated Bose-Einstein
Condensates (BECs) by sweeping three laser beams through the BEC. If one of the
beams is in the first order (TEM10) Hermite-Gaussian mode, its amplitude has a
transversal phase slip which can be transferred to the atoms creating a
soliton. Using ... | cond-mat.soft quant-ph | we propose a new method of creating solitons in elongated boseeinstein condensates becs by sweeping three laser beams through the bec if one of the beams is in the first order tem10 hermitegaussian mode its amplitude has a transversal phase slip which can be transferred to the atoms creating a soliton using this method... | [['we', 'propose', 'a', 'new', 'method', 'of', 'creating', 'solitons', 'in', 'elongated', 'boseeinstein', 'condensates', 'becs', 'by', 'sweeping', 'three', 'laser', 'beams', 'through', 'the', 'bec', 'if', 'one', 'of', 'the', 'beams', 'is', 'in', 'the', 'first', 'order', 'tem10', 'hermitegaussian', 'mode', 'its', 'ampli... | [-0.1358787640470186, 0.18163781956867958, -0.11062997434954576, 0.04058435436800062, -0.08881675885096799, -0.161814721217909, -0.0006300600026014859, 0.40449353608840366, -0.27948506630775405, -0.26237227952266795, 0.05683160506991473, -0.24094572797527905, -0.10027220970723869, 0.20016838787398036, 0.028720192395423... |
710.1703 | The BMV experiment : a novel apparatus to study the propagation of light
in a transverse magnetic field | In this paper, we describe in detail the BMV (Bir\'efringence Magn\'etique du
Vide) experiment, a novel apparatus to study the propagation of light in a
transverse magnetic field. It is based on a very high finesse Fabry-Perot
cavity and on pulsed magnets specially designed for this purpose. We justify
our technical ... | physics.optics hep-ex | in this paper we describe in detail the bmv birefringence magnetique du vide experiment a novel apparatus to study the propagation of light in a transverse magnetic field it is based on a very high finesse fabryperot cavity and on pulsed magnets specially designed for this purpose we justify our technical choices and w... | [['in', 'this', 'paper', 'we', 'describe', 'in', 'detail', 'the', 'bmv', 'birefringence', 'magnetique', 'du', 'vide', 'experiment', 'a', 'novel', 'apparatus', 'to', 'study', 'the', 'propagation', 'of', 'light', 'in', 'a', 'transverse', 'magnetic', 'field', 'it', 'is', 'based', 'on', 'a', 'very', 'high', 'finesse', 'fab... | [-0.14169864907162263, 0.10738326854382953, -0.10527677222465476, 0.02989731006285486, -0.09523926464219888, -0.11427331583108753, 0.007018987756843368, 0.42694166315098603, -0.16566301084822044, -0.28350895290883876, 0.0851113033577955, -0.21751554617658259, -0.15722339109828073, 0.2301554259068022, -0.104314341923842... |
710.1704 | A giant controllable gap in the optical spectrum of a semiconductor
laser subject to intense feedback with rotated polarization | A semiconductor laser subject to delayed optical feedback is investigated in
the limit of extremely intense feedback power. In a range of feedback
polarization rotation angles the emission spectra of the laser reveal a giant
gap with width of more than a terahertz. The position of the gap and its width
are shown to b... | physics.optics | a semiconductor laser subject to delayed optical feedback is investigated in the limit of extremely intense feedback power in a range of feedback polarization rotation angles the emission spectra of the laser reveal a giant gap with width of more than a terahertz the position of the gap and its width are shown to be re... | [['a', 'semiconductor', 'laser', 'subject', 'to', 'delayed', 'optical', 'feedback', 'is', 'investigated', 'in', 'the', 'limit', 'of', 'extremely', 'intense', 'feedback', 'power', 'in', 'a', 'range', 'of', 'feedback', 'polarization', 'rotation', 'angles', 'the', 'emission', 'spectra', 'of', 'the', 'laser', 'reveal', 'a'... | [-0.16211743421918073, 0.13931337293761317, -0.07605195611249656, 0.008473527630849275, -0.06345651273149996, -0.11005288691958412, 0.083787731413031, 0.49842438772320746, -0.24295032491208984, -0.3181151772500016, 0.04245468706649262, -0.23684731036191806, -0.10836864610901102, 0.27305417372263036, -0.0063016126805450... |
710.1705 | Dimensionality and morphology of particle and bubble clusters in
turbulent flow | We conduct numerical experiments to investigate the spatial clustering of
particles and bubbles in simulations of homogeneous and isotropic turbulence.
Varying the Stokes parameter and the densities, striking differences in the
clustering of the particles can be observed. To quantify these visual findings
we use the ... | nlin.CD physics.flu-dyn | we conduct numerical experiments to investigate the spatial clustering of particles and bubbles in simulations of homogeneous and isotropic turbulence varying the stokes parameter and the densities striking differences in the clustering of the particles can be observed to quantify these visual findings we use the kapla... | [['we', 'conduct', 'numerical', 'experiments', 'to', 'investigate', 'the', 'spatial', 'clustering', 'of', 'particles', 'and', 'bubbles', 'in', 'simulations', 'of', 'homogeneous', 'and', 'isotropic', 'turbulence', 'varying', 'the', 'stokes', 'parameter', 'and', 'the', 'densities', 'striking', 'differences', 'in', 'the',... | [-0.08027740084294316, 0.11905084196096245, -0.13840212423698922, 0.09786173427138327, -0.026944055398280136, -0.06175431546437516, -0.0012418053548976864, 0.34791068452803386, -0.26076025825069216, -0.34691052918317, 0.048326814856051836, -0.28427915789713176, -0.09000324036904497, 0.1160822848754402, 0.00577804324724... |
710.1706 | Relativistic calculations of the lifetimes and hyperfine structure
constants in $^{67}$Zn$^{+}$ | This work presents accurate {\it ab initio} determination of the magnetic
dipole (M1) and electric quadrupole (E2) hyperfine structure constants for the
ground and a few low-lying excited states in $^{67}$Zn$^{+}$, which is one of
the interesting systems in fundamental physics. The coupled-cluster (CC) theory
within ... | physics.atom-ph | this work presents accurate it ab initio determination of the magnetic dipole m1 and electric quadrupole e2 hyperfine structure constants for the ground and a few lowlying excited states in 67zn which is one of the interesting systems in fundamental physics the coupledcluster cc theory within the relativistic framework... | [['this', 'work', 'presents', 'accurate', 'it', 'ab', 'initio', 'determination', 'of', 'the', 'magnetic', 'dipole', 'm1', 'and', 'electric', 'quadrupole', 'e2', 'hyperfine', 'structure', 'constants', 'for', 'the', 'ground', 'and', 'a', 'few', 'lowlying', 'excited', 'states', 'in', '67zn', 'which', 'is', 'one', 'of', 't... | [-0.11233321693725884, 0.17066992598335706, -0.02770936258861588, 0.11887621545314754, 0.010581780385109596, -0.1047990267570303, 0.023348299097657826, 0.38334524836736145, -0.2077175017265189, -0.3244951600251995, -3.449451523246588e-05, -0.29774731524392134, -0.08310792887695478, 0.1573842048636396, 0.090180209279491... |
710.1707 | M-theory branes and their interactions | In recent years there has been some progress in understanding how one might
model the interactions of branes in M-theory despite not having a fundamental
perturbative description. The goal of this review is to describe different
approaches to M-theory branes and their interactions. This includes: a review
of M-theory... | hep-th | in recent years there has been some progress in understanding how one might model the interactions of branes in mtheory despite not having a fundamental perturbative description the goal of this review is to describe different approaches to mtheory branes and their interactions this includes a review of mtheory branes ... | [['in', 'recent', 'years', 'there', 'has', 'been', 'some', 'progress', 'in', 'understanding', 'how', 'one', 'might', 'model', 'the', 'interactions', 'of', 'branes', 'in', 'mtheory', 'despite', 'not', 'having', 'a', 'fundamental', 'perturbative', 'description', 'the', 'goal', 'of', 'this', 'review', 'is', 'to', 'describ... | [-0.133928192716636, 0.10513164750771241, -0.1029148869670331, 0.0853517461460858, -0.13212447785877027, -0.1356410629827571, 0.0023633912833554024, 0.3292042384070627, -0.18400434521811732, -0.2947218251215775, 0.09318444055107454, -0.31258373627481, -0.18396290866762735, 0.12236190718870736, -0.1381050188387378, 0.01... |
710.1708 | Variable Modified Chaplygin Gas and Accelerating Universe | In this letter, I have proposed a model of variable modified Chaplygin gas
and shown its role in accelerating phase of the universe. I have shown that the
equation of state of this model is valid from the radiation era to quiessence
model. The graphical representations of statefinder parameters characterize
different... | gr-qc | in this letter i have proposed a model of variable modified chaplygin gas and shown its role in accelerating phase of the universe i have shown that the equation of state of this model is valid from the radiation era to quiessence model the graphical representations of statefinder parameters characterize different phas... | [['in', 'this', 'letter', 'i', 'have', 'proposed', 'a', 'model', 'of', 'variable', 'modified', 'chaplygin', 'gas', 'and', 'shown', 'its', 'role', 'in', 'accelerating', 'phase', 'of', 'the', 'universe', 'i', 'have', 'shown', 'that', 'the', 'equation', 'of', 'state', 'of', 'this', 'model', 'is', 'valid', 'from', 'the', '... | [-0.09745363972181065, 0.09569596675043898, -0.12658494577479007, 0.03068300025753065, -0.03178857160565346, -0.11754385577931778, -0.025035009705531065, 0.3077860427533846, -0.24079526610561272, -0.2665094572828332, 0.03658207502640061, -0.23537390167588618, -0.13515479587637055, 0.1507043892886045, -0.014890662046955... |
710.1709 | Transport in Magnetic Nanoparticles Super-Lattices : Coulomb Blockade,
Hysteresis and Magnetic Field Induced Switching | We report on magnetotransport measurements on millimetric super-lattices of
Co-Fe nanoparticles surrounded by an organic layer. At low temperature, the
transition between the Coulomb blockade and the conductive regime becomes
abrupt and hysteretic. The transition between both regime can be induced by a
magnetic field... | cond-mat.mtrl-sci | we report on magnetotransport measurements on millimetric superlattices of cofe nanoparticles surrounded by an organic layer at low temperature the transition between the coulomb blockade and the conductive regime becomes abrupt and hysteretic the transition between both regime can be induced by a magnetic field leadin... | [['we', 'report', 'on', 'magnetotransport', 'measurements', 'on', 'millimetric', 'superlattices', 'of', 'cofe', 'nanoparticles', 'surrounded', 'by', 'an', 'organic', 'layer', 'at', 'low', 'temperature', 'the', 'transition', 'between', 'the', 'coulomb', 'blockade', 'and', 'the', 'conductive', 'regime', 'becomes', 'abrup... | [-0.21459609483204345, 0.2822379632539677, -0.0007559782551491962, -0.039121329240665276, -0.027235552485046142, -0.16853485506794907, 0.13017022104605155, 0.3769670227213818, -0.2465616870781078, -0.37935868478106227, -0.019948044884949924, -0.3453005961854668, -0.1603289810831056, 0.2058396706576733, 0.05348963945665... |
710.171 | Distributed Order Calculus: an Operator-Theoretic Interpretation | Within the functional calculi of Bochner-Phillips and Hirsch, we describe the
operators of distributed order differentiation and integration as functions of
the classical differentiation and integration operators respectively.
| math-ph math.FA math.MP | within the functional calculi of bochnerphillips and hirsch we describe the operators of distributed order differentiation and integration as functions of the classical differentiation and integration operators respectively | [['within', 'the', 'functional', 'calculi', 'of', 'bochnerphillips', 'and', 'hirsch', 'we', 'describe', 'the', 'operators', 'of', 'distributed', 'order', 'differentiation', 'and', 'integration', 'as', 'functions', 'of', 'the', 'classical', 'differentiation', 'and', 'integration', 'operators', 'respectively']] | [-0.1287179578960474, 0.04537921147753617, -0.042143183519198955, 0.0999073859836374, -0.019869932987993316, -0.005916524678468704, 0.05975145715222295, 0.33601153402456213, -0.294134915673307, -0.24132624747497694, 0.14911023464602685, -0.27541101397946477, -0.18207125405647925, 0.13848308427259326, -0.050895164163583... |
710.1711 | Excited State Spectroscopy in the Lattice Gross-Neveu Model | We present preliminary results of an excited state spectroscopy calculation
in the 2-d lattice Gross-Neveu model. We address the construction of suitable
interpolators for the variational method and their overlap with excitations. We
comment on the role of the eigenvectors as a tool for matching scattering
states on ... | hep-lat | we present preliminary results of an excited state spectroscopy calculation in the 2d lattice grossneveu model we address the construction of suitable interpolators for the variational method and their overlap with excitations we comment on the role of the eigenvectors as a tool for matching scattering states on lattic... | [['we', 'present', 'preliminary', 'results', 'of', 'an', 'excited', 'state', 'spectroscopy', 'calculation', 'in', 'the', '2d', 'lattice', 'grossneveu', 'model', 'we', 'address', 'the', 'construction', 'of', 'suitable', 'interpolators', 'for', 'the', 'variational', 'method', 'and', 'their', 'overlap', 'with', 'excitatio... | [-0.07859607169834468, 0.13574179045463097, -0.07186656390639165, 0.0684807286150037, -0.012818551407410549, -0.06667240861749563, 0.07678363277451493, 0.41234593838453293, -0.18449192221921223, -0.2523573593308146, 0.09461895320698833, -0.31789202046974635, -0.14242768628397384, 0.15617403104596844, 0.0590266532515390... |
710.1712 | Exact results for quench dynamics and defect production in a
two-dimensional model | We show that for a d-dimensional model in which a quench with a rate
\tau^{-1} takes the system across a d-m dimensional critical surface, the
defect density scales as n \sim 1/\tau^{m\nu/(z\nu +1)}, where \nu and z are
the correlation length and dynamical critical exponents characterizing the
critical surface. We ex... | cond-mat.stat-mech cond-mat.str-el | we show that for a ddimensional model in which a quench with a rate tau1 takes the system across a dm dimensional critical surface the defect density scales as n sim 1taumnuznu 1 where nu and z are the correlation length and dynamical critical exponents characterizing the critical surface we explicitly demonstrate that... | [['we', 'show', 'that', 'for', 'a', 'ddimensional', 'model', 'in', 'which', 'a', 'quench', 'with', 'a', 'rate', 'tau1', 'takes', 'the', 'system', 'across', 'a', 'dm', 'dimensional', 'critical', 'surface', 'the', 'defect', 'density', 'scales', 'as', 'n', 'sim', '1taumnuznu', '1', 'where', 'nu', 'and', 'z', 'are', 'the',... | [-0.12654022107045482, 0.1351335833543681, -0.09001919312529194, 0.08266583424925045, 0.036734570572785674, -0.16198887078439617, 0.03292937862383907, 0.3372579760571435, -0.24172634252536934, -0.26808925960393787, 0.06339069859924934, -0.2819988399707866, -0.19231388162939078, 0.21571458864604456, 0.08312426327085755,... |
710.1713 | An update in monopole condensation in two-flavour Adjoint QCD | QCD with fermions in the adjoint representation (aQCD) is a model for which a
deconfinement and a chiral phase transition take place at different
temperatures. In this work, we present a study of the deconfinement transition
in the dual superconductor picture based on the evaluation of an operator which
carries magne... | hep-lat | qcd with fermions in the adjoint representation aqcd is a model for which a deconfinement and a chiral phase transition take place at different temperatures in this work we present a study of the deconfinement transition in the dual superconductor picture based on the evaluation of an operator which carries magnetic ch... | [['qcd', 'with', 'fermions', 'in', 'the', 'adjoint', 'representation', 'aqcd', 'is', 'a', 'model', 'for', 'which', 'a', 'deconfinement', 'and', 'a', 'chiral', 'phase', 'transition', 'take', 'place', 'at', 'different', 'temperatures', 'in', 'this', 'work', 'we', 'present', 'a', 'study', 'of', 'the', 'deconfinement', 'tr... | [-0.13456311216803937, 0.21352738871050375, -0.09552778874171301, 0.05199869135304273, -0.05701851255251366, -0.05089279916589555, 0.07995244288066565, 0.34741360665235704, -0.15659344489844426, -0.2389292266870876, 0.05597132081685823, -0.29405140850322264, -0.1469781593265898, 0.053889767192213715, 0.0577317896000679... |
710.1714 | Layered Phase Investigations | The extra dimensional defects that are introduced to generate the lattice
chiral zero modes are not simply a computational trick, but have interesting
physical consequences. After reviewing what is known about the layered phase
they can generate, I argue how it is possible to simulate Yang-Mills theories
with reduced... | hep-lat | the extra dimensional defects that are introduced to generate the lattice chiral zero modes are not simply a computational trick but have interesting physical consequences after reviewing what is known about the layered phase they can generate i argue how it is possible to simulate yangmills theories with reduced syste... | [['the', 'extra', 'dimensional', 'defects', 'that', 'are', 'introduced', 'to', 'generate', 'the', 'lattice', 'chiral', 'zero', 'modes', 'are', 'not', 'simply', 'a', 'computational', 'trick', 'but', 'have', 'interesting', 'physical', 'consequences', 'after', 'reviewing', 'what', 'is', 'known', 'about', 'the', 'layered',... | [-0.1043086095870582, 0.2505864075878087, -0.10292595581096761, 0.11967490370015559, -0.12167215163764708, -0.16998343848322026, 0.04319425915395293, 0.3845492691787727, -0.2737334735266974, -0.2805081336923382, 0.11882223809987087, -0.27203254629036083, -0.2110438204185544, 0.11662990249255124, -0.09012809405377244, -... |
710.1715 | FUV Spectroscopy of the sdOB Primary of the Eclipsing Binary System AA
Dor | AA Dor is an eclipsing, close, post common-envelope binary (PCEB). We present
a detailed spectral analysis of its sdOB primary star based on observations
obtained with the Far Ultraviolet Spectroscopic Explorer (FUSE). Due to a
strong contamination by interstellar absorption, we had to model both, the
stellar spectru... | astro-ph | aa dor is an eclipsing close post commonenvelope binary pceb we present a detailed spectral analysis of its sdob primary star based on observations obtained with the far ultraviolet spectroscopic explorer fuse due to a strong contamination by interstellar absorption we had to model both the stellar spectrum as well as ... | [['aa', 'dor', 'is', 'an', 'eclipsing', 'close', 'post', 'commonenvelope', 'binary', 'pceb', 'we', 'present', 'a', 'detailed', 'spectral', 'analysis', 'of', 'its', 'sdob', 'primary', 'star', 'based', 'on', 'observations', 'obtained', 'with', 'the', 'far', 'ultraviolet', 'spectroscopic', 'explorer', 'fuse', 'due', 'to',... | [-0.008812706278903144, 0.05590216144441261, -0.047180660059010344, 0.07904616498022474, -0.140816999652556, -0.0883338198664465, 0.07924121545261836, 0.4787355484707015, -0.1737556609192065, -0.34672938392364555, 0.051099001714361034, -0.32831368651241066, -0.08079804297106291, 0.14911951289312647, -0.0548054560885897... |
710.1716 | Information and entropy in quantum Brownian motion: Thermodynamic
entropy versus von Neumann entropy | We compare the thermodynamic entropy of a quantum Brownian oscillator derived
from the partition function of the subsystem with the von Neumann entropy of
its reduced density matrix. At low temperatures we find deviations between
these two entropies which are due to the fact that the Brownian particle and
its environ... | quant-ph | we compare the thermodynamic entropy of a quantum brownian oscillator derived from the partition function of the subsystem with the von neumann entropy of its reduced density matrix at low temperatures we find deviations between these two entropies which are due to the fact that the brownian particle and its environmen... | [['we', 'compare', 'the', 'thermodynamic', 'entropy', 'of', 'a', 'quantum', 'brownian', 'oscillator', 'derived', 'from', 'the', 'partition', 'function', 'of', 'the', 'subsystem', 'with', 'the', 'von', 'neumann', 'entropy', 'of', 'its', 'reduced', 'density', 'matrix', 'at', 'low', 'temperatures', 'we', 'find', 'deviatio... | [-0.07803035849925652, 0.1525120739864188, -0.102992267743434, 0.06993580916495894, 0.03380028775552668, -0.1476466692433322, 0.053591663365863185, 0.32535611931985664, -0.2814199384652399, -0.2503500660601002, 0.10893128044097133, -0.35367891747224073, -0.1108919405503579, 0.20697928017370842, -0.040215568066204105, 0... |
710.1717 | Error correction in ensemble registers for quantum repeaters and quantum
computers | We propose to use a collective excitation blockade mechanism to identify
errors that occur due to disturbances of single atoms in ensemble quantum
registers where qubits are stored in the collective population of different
internal atomic states. A simple error correction procedure and a simple
decoherence-free encod... | quant-ph | we propose to use a collective excitation blockade mechanism to identify errors that occur due to disturbances of single atoms in ensemble quantum registers where qubits are stored in the collective population of different internal atomic states a simple error correction procedure and a simple decoherencefree encoding ... | [['we', 'propose', 'to', 'use', 'a', 'collective', 'excitation', 'blockade', 'mechanism', 'to', 'identify', 'errors', 'that', 'occur', 'due', 'to', 'disturbances', 'of', 'single', 'atoms', 'in', 'ensemble', 'quantum', 'registers', 'where', 'qubits', 'are', 'stored', 'in', 'the', 'collective', 'population', 'of', 'diffe... | [-0.1627244693937443, 0.27284023230421844, -0.001016147340000686, 0.06493437034472571, 0.06203699278471581, -0.2242547488392536, 0.13309795482447212, 0.4230912844887224, -0.24353266321122646, -0.28476382447880205, -0.06619766067074201, -0.24713874380972425, -0.06333491079888101, 0.12945721443679373, -0.0553353606423331... |
710.1718 | Measuring the accretion rate and kinetic luminosity functions of
supermassive black holes | We derive accretion rate functions (ARFs) and kinetic luminosity functions
(KLF) for jet-launching supermassive black holes. The accretion rate as well as
the kinetic power of an active galaxy is estimated from the radio emission of
the jet. For compact low-power jets, we use the core radio emission while the
jet pow... | astro-ph | we derive accretion rate functions arfs and kinetic luminosity functions klf for jetlaunching supermassive black holes the accretion rate as well as the kinetic power of an active galaxy is estimated from the radio emission of the jet for compact lowpower jets we use the core radio emission while the jet power of highp... | [['we', 'derive', 'accretion', 'rate', 'functions', 'arfs', 'and', 'kinetic', 'luminosity', 'functions', 'klf', 'for', 'jetlaunching', 'supermassive', 'black', 'holes', 'the', 'accretion', 'rate', 'as', 'well', 'as', 'the', 'kinetic', 'power', 'of', 'an', 'active', 'galaxy', 'is', 'estimated', 'from', 'the', 'radio', '... | [-0.045902151299111696, 0.08678202762746137, -0.05358678202879564, 0.17734091656853507, -0.11685847543793071, -0.08249893654418651, 0.015948421404879523, 0.4348081997759528, -0.1748970162940104, -0.3188112053140324, 0.05303662081118018, -0.2912096603874886, 0.0075256865491418416, 0.24723467065943358, -0.007418806682780... |
710.1719 | A remark on Fano 4-folds having (3,1)-type extremal contractions | Let X be the blow-up of a smooth projective 4-fold Y along a smooth curve C
and let E be the exceptional divisor. Assume that X is a Fano manifold and has
an elementary extremal contraction $\phi: X \to Z$ of (3,1)-type such that E is
$\phi$-ample (recall that a contraction map for a 4-fold is called (3,1)-type
if th... | math.AG | let x be the blowup of a smooth projective 4fold y along a smooth curve c and let e be the exceptional divisor assume that x is a fano manifold and has an elementary extremal contraction phi x to z of 31type such that e is phiample recall that a contraction map for a 4fold is called 31type if the exceptional locus is a... | [['let', 'x', 'be', 'the', 'blowup', 'of', 'a', 'smooth', 'projective', '4fold', 'y', 'along', 'a', 'smooth', 'curve', 'c', 'and', 'let', 'e', 'be', 'the', 'exceptional', 'divisor', 'assume', 'that', 'x', 'is', 'a', 'fano', 'manifold', 'and', 'has', 'an', 'elementary', 'extremal', 'contraction', 'phi', 'x', 'to', 'z', ... | [-0.24095474764149874, 0.04596640640514298, -0.17686594713558543, -0.007418210897470844, -0.09193070740141768, -0.2364281934309513, 0.00432997103780508, 0.3907137848040525, -0.32604493471258816, -0.11464220008991183, 0.08232004230624025, -0.3032643090477808, -0.13225554811651818, 0.19339167917434602, -0.178529147866201... |
710.172 | Meson mass spectrum at finite temperature and density in the strong
coupling limit of lattice QCD for color SU(3) | We investigate the meson mass spectrum in the strong coupling limit of
lattice QCD with one species of staggered fermion for the SU(N_c) color gauge
group, including N_c=3. We analytically derive meson masses as functions of
temperature and chemical potential via chiral condensates. We show that meson
masses quickly ... | hep-lat nucl-th | we investigate the meson mass spectrum in the strong coupling limit of lattice qcd with one species of staggered fermion for the sun_c color gauge group including n_c3 we analytically derive meson masses as functions of temperature and chemical potential via chiral condensates we show that meson masses quickly decrease... | [['we', 'investigate', 'the', 'meson', 'mass', 'spectrum', 'in', 'the', 'strong', 'coupling', 'limit', 'of', 'lattice', 'qcd', 'with', 'one', 'species', 'of', 'staggered', 'fermion', 'for', 'the', 'sun_c', 'color', 'gauge', 'group', 'including', 'n_c3', 'we', 'analytically', 'derive', 'meson', 'masses', 'as', 'function... | [-0.09933368170459289, 0.2898745866114041, -0.07158966131100897, 0.06979924307961483, -0.028573387127835304, -0.11978406716661993, 0.1274505156907253, 0.3834168001776561, -0.16367082733268035, -0.2279299132496817, -0.002469938119247672, -0.2899570140925789, -0.04567837644208339, 0.0373580202285666, 0.0956819377533975, ... |
710.1721 | Quantum advantages in classically defined tasks | We analyze classically defined games for which a quantum team has an
advantage over any classical team. The quantum team has a clear advantage in
games in which the players of each team are separated in space and the quantum
team can use unusually strong correlations of the Einstein-Podolsky-Rosen (EPR)
type. We pres... | quant-ph | we analyze classically defined games for which a quantum team has an advantage over any classical team the quantum team has a clear advantage in games in which the players of each team are separated in space and the quantum team can use unusually strong correlations of the einsteinpodolskyrosen epr type we present an e... | [['we', 'analyze', 'classically', 'defined', 'games', 'for', 'which', 'a', 'quantum', 'team', 'has', 'an', 'advantage', 'over', 'any', 'classical', 'team', 'the', 'quantum', 'team', 'has', 'a', 'clear', 'advantage', 'in', 'games', 'in', 'which', 'the', 'players', 'of', 'each', 'team', 'are', 'separated', 'in', 'space',... | [-0.13462578516919166, 0.06899699922238749, -0.1732871860666718, 0.08021369128901926, -0.04653886974685722, -0.21855345929765868, 0.029194575537177216, 0.38492818192268413, -0.22353288108610692, -0.30872949466316235, 0.036591656451087654, -0.26718295304777306, -0.13725586238110232, 0.14281202987250355, -0.0819879034792... |
710.1722 | Precision electroweak calculation of the production of a high
transverse-momentum lepton pair at hadron colliders | We present a detailed study of the production of a high transverse-momentum
lepton pair at hadron colliders, which includes the exact O(alpha) electroweak
corrections properly matched with leading logarithmic effects due to multiple
photon emission, as required by the experiments at the Fermilab Tevatron and
the CERN... | hep-ph | we present a detailed study of the production of a high transversemomentum lepton pair at hadron colliders which includes the exact oalpha electroweak corrections properly matched with leading logarithmic effects due to multiple photon emission as required by the experiments at the fermilab tevatron and the cern lhc nu... | [['we', 'present', 'a', 'detailed', 'study', 'of', 'the', 'production', 'of', 'a', 'high', 'transversemomentum', 'lepton', 'pair', 'at', 'hadron', 'colliders', 'which', 'includes', 'the', 'exact', 'oalpha', 'electroweak', 'corrections', 'properly', 'matched', 'with', 'leading', 'logarithmic', 'effects', 'due', 'to', 'm... | [-0.051189141035018884, 0.19926612531445675, -0.07353981417893875, 0.15167160973727672, -0.006774861367465165, -0.09797866507261595, -0.02892781132293033, 0.3259865006615148, -0.15862318467096898, -0.24446802890141967, 0.016042141075872006, -0.3590640397360701, 0.055825423769897124, 0.16202497109770775, 0.1005628980299... |
710.1723 | Electronic inter-tube transfer in double-wall carbon nanotubes with
impurities | Inter-tube conductance of double-wall carbon nanotubes with impurities is
numerically studied. Its length dependence for various impurities is scaled by
a mean-free path. The inter-tube conductance exhibits drastic linear increase
with the tube length and takes a maximum around at the localization length. The
maximum... | cond-mat.mes-hall | intertube conductance of doublewall carbon nanotubes with impurities is numerically studied its length dependence for various impurities is scaled by a meanfree path the intertube conductance exhibits drastic linear increase with the tube length and takes a maximum around at the localization length the maximum conducta... | [['intertube', 'conductance', 'of', 'doublewall', 'carbon', 'nanotubes', 'with', 'impurities', 'is', 'numerically', 'studied', 'its', 'length', 'dependence', 'for', 'various', 'impurities', 'is', 'scaled', 'by', 'a', 'meanfree', 'path', 'the', 'intertube', 'conductance', 'exhibits', 'drastic', 'linear', 'increase', 'wi... | [-0.21507927958133086, 0.2761836263860734, -0.01398135581985116, 0.014106341670618727, 0.029623458864835073, -0.19361766722610105, 0.026992564252138418, 0.38977014976290036, -0.27768023055538815, -0.2553447807242848, -0.05810789321109934, -0.3856722750824015, -0.11318731532467283, 0.20030753296044357, 0.006228198842057... |
710.1724 | Optimal Covariant Measurement of Momentum on a Half Line in Quantum
Mechanics | We cannot perform the projective measurement of a momentum on a half line
since it is not an observable. Nevertheless, we would like to obtain some
physical information of the momentum on a half line. We define an optimality
for measurement as minimizing the variance between an inferred outcome of the
measured system... | quant-ph | we cannot perform the projective measurement of a momentum on a half line since it is not an observable nevertheless we would like to obtain some physical information of the momentum on a half line we define an optimality for measurement as minimizing the variance between an inferred outcome of the measured system befo... | [['we', 'can', 'not', 'perform', 'the', 'projective', 'measurement', 'of', 'a', 'momentum', 'on', 'a', 'half', 'line', 'since', 'it', 'is', 'not', 'an', 'observable', 'nevertheless', 'we', 'would', 'like', 'to', 'obtain', 'some', 'physical', 'information', 'of', 'the', 'momentum', 'on', 'a', 'half', 'line', 'we', 'defi... | [-0.12528049524165005, 0.10850306895682574, -0.08468464402584759, 0.07612771628422695, -0.07162573249107855, -0.11698002015966122, 0.07405638777253795, 0.36240893197845825, -0.250267446843873, -0.2602615029739639, 0.11060784576586419, -0.2601099177749336, -0.053188304331130774, 0.19822173383575437, -0.04119442788986889... |
710.1725 | Pseudoscalar Flavor-Singlet Physics with Staggered Fermions | Accurately calculating the mass of flavor-singlet meson states from numerical
lattice simulations is an important milestone for lattice QCD. Careful
measurement of the full pseudoscalar flavor-singlet propagator is also a
crucial step in understanding the dynamics of the fermion sea on the lattice,
in particular for ... | hep-lat | accurately calculating the mass of flavorsinglet meson states from numerical lattice simulations is an important milestone for lattice qcd careful measurement of the full pseudoscalar flavorsinglet propagator is also a crucial step in understanding the dynamics of the fermion sea on the lattice in particular for potent... | [['accurately', 'calculating', 'the', 'mass', 'of', 'flavorsinglet', 'meson', 'states', 'from', 'numerical', 'lattice', 'simulations', 'is', 'an', 'important', 'milestone', 'for', 'lattice', 'qcd', 'careful', 'measurement', 'of', 'the', 'full', 'pseudoscalar', 'flavorsinglet', 'propagator', 'is', 'also', 'a', 'crucial'... | [-0.09365058988102792, 0.2949456337907274, -0.11983568991683884, 0.08309744554571807, -0.043649651731053986, -0.08978725000310482, 0.07374392142576844, 0.3556978400727665, -0.1138674640154213, -0.21876568758837234, 0.036709989320463786, -0.2995663554476643, -0.09281353238268675, 0.10888615986447275, 0.09755572077047861... |
710.1726 | Interior of Nonuniform Black Strings | We consider nonuniform black strings inside their event horizon. We present
numerical evidence, that the singularity touches the horizon as the horizon
topology changing transition is reached.
| hep-th gr-qc | we consider nonuniform black strings inside their event horizon we present numerical evidence that the singularity touches the horizon as the horizon topology changing transition is reached | [['we', 'consider', 'nonuniform', 'black', 'strings', 'inside', 'their', 'event', 'horizon', 'we', 'present', 'numerical', 'evidence', 'that', 'the', 'singularity', 'touches', 'the', 'horizon', 'as', 'the', 'horizon', 'topology', 'changing', 'transition', 'is', 'reached']] | [-0.25885758286824934, 0.12154359749897763, -0.1103781872704901, 0.16281077837036853, -0.13893584037820497, -0.12187991525839877, 0.07272457941090343, 0.3705517822807586, -0.22819533861345714, -0.23401484376302473, 0.21943841308907228, -0.3547903502153026, -0.0738991342002043, 0.09273886473642455, -0.05939626666130843,... |
710.1727 | The Centre of M83 | Stellar kinematics show no evidence of hidden mass concentrations at the
centre of M83. We show the clearest evidence yet of an age gradient along the
starburst arc and interpret the arc to have formed from orbital motion away
from a starforming region in the dust lane.
| astro-ph | stellar kinematics show no evidence of hidden mass concentrations at the centre of m83 we show the clearest evidence yet of an age gradient along the starburst arc and interpret the arc to have formed from orbital motion away from a starforming region in the dust lane | [['stellar', 'kinematics', 'show', 'no', 'evidence', 'of', 'hidden', 'mass', 'concentrations', 'at', 'the', 'centre', 'of', 'm83', 'we', 'show', 'the', 'clearest', 'evidence', 'yet', 'of', 'an', 'age', 'gradient', 'along', 'the', 'starburst', 'arc', 'and', 'interpret', 'the', 'arc', 'to', 'have', 'formed', 'from', 'orb... | [-0.06747869034594994, 0.06678218492882654, -0.12617839343766582, 0.09332859617202206, -0.04394528626444492, 0.007670260797393449, 0.060058004856902235, 0.4981770027191081, -0.2079192525211801, -0.3121183216373654, 0.03551072924288901, -0.253911430491729, -0.02681604431981736, 0.1546572864729356, -0.020056455421504228,... |
710.1728 | Prospects of Forward Energy Flow and Low-x Physics at the LHC | The LHC will soon provide proton-proton collisions at the unprecedented
center of mass energy, $\sqrt{s}=$14 TeV. This not only allows us to probe new
regions of high-$p_T$ physics, but also low-$x$ and forward physics. A
selection of potential measurements are described to outline the prospects for
low-$x$ and forwa... | hep-ph | the lhc will soon provide protonproton collisions at the unprecedented center of mass energy sqrts14 tev this not only allows us to probe new regions of highp_t physics but also lowx and forward physics a selection of potential measurements are described to outline the prospects for lowx and forward physics in the atla... | [['the', 'lhc', 'will', 'soon', 'provide', 'protonproton', 'collisions', 'at', 'the', 'unprecedented', 'center', 'of', 'mass', 'energy', 'sqrts14', 'tev', 'this', 'not', 'only', 'allows', 'us', 'to', 'probe', 'new', 'regions', 'of', 'highp_t', 'physics', 'but', 'also', 'lowx', 'and', 'forward', 'physics', 'a', 'selecti... | [0.003488686293010311, 0.21452691900575982, -0.18850426603879394, 0.1925766986598068, -0.12639552351601166, -0.1685820365693934, -0.01638468501061715, 0.31605069769610616, -0.23587612409530015, -0.3444765418655528, 0.012083439740496848, -0.35350693891187207, 0.10763248319512811, 0.19993841086096806, 0.07079204110878295... |
710.1729 | The Grounds For Time Dependent Market Potentials From Dealers' Dynamics | We apply the potential force estimation method to artificial time series of
market price produced by a deterministic dealer model. We find that dealers'
feedback of linear prediction of market price based on the latest mean price
changes plays the central role in the market's potential force. When markets
are dominat... | q-fin.GN physics.data-an physics.soc-ph | we apply the potential force estimation method to artificial time series of market price produced by a deterministic dealer model we find that dealers feedback of linear prediction of market price based on the latest mean price changes plays the central role in the markets potential force when markets are dominated by ... | [['we', 'apply', 'the', 'potential', 'force', 'estimation', 'method', 'to', 'artificial', 'time', 'series', 'of', 'market', 'price', 'produced', 'by', 'a', 'deterministic', 'dealer', 'model', 'we', 'find', 'that', 'dealers', 'feedback', 'of', 'linear', 'prediction', 'of', 'market', 'price', 'based', 'on', 'the', 'lates... | [-0.140412900928561, 0.09167354201821432, -0.10090774345875092, 0.09133593063189151, -0.08334516768330989, -0.18702602854049574, 0.10296107546987701, 0.38317232492239506, -0.2942574766196617, -0.26847045432954825, 0.07092554311822998, -0.3229491290802213, -0.18126549398245878, 0.18016471404722598, -0.057610971469604345... |
710.173 | Building Blue Stragglers with Stellar Collisions | The evolution of stellar collision products in cluster simulations has
usually been modelled using simplified prescriptions. Such prescriptions either
replace the collision product with an (evolved) main sequence star, or assume
that the collision product was completely mixed during the collision.
It is known from ... | astro-ph | the evolution of stellar collision products in cluster simulations has usually been modelled using simplified prescriptions such prescriptions either replace the collision product with an evolved main sequence star or assume that the collision product was completely mixed during the collision it is known from hydrodyna... | [['the', 'evolution', 'of', 'stellar', 'collision', 'products', 'in', 'cluster', 'simulations', 'has', 'usually', 'been', 'modelled', 'using', 'simplified', 'prescriptions', 'such', 'prescriptions', 'either', 'replace', 'the', 'collision', 'product', 'with', 'an', 'evolved', 'main', 'sequence', 'star', 'or', 'assume', ... | [-0.041264565077144655, 0.1621998040880135, -0.13518434966914356, 0.08514287887723185, -0.016764553431421518, -0.049702941253781316, -0.08974194796523079, 0.41976177202537657, -0.23174551576375962, -0.30144165418110785, 0.11255490662646479, -0.24284635730087756, -0.03880173145327717, 0.15384857172844932, -0.02104040760... |
710.1731 | A near-infrared interferometric survey of debris disk stars. I. Probing
the hot dust content around epsilon Eridani and tau Ceti with CHARA/FLUOR | We probed the first 3AU around tau Ceti and epsilon Eridani with the CHARA
array (Mt Wilson, USA) in order to gauge the 2micron excess flux emanating from
possible hot dust grains in the debris disks and to also resolve the stellar
photospheres. High precision visibility amplitude measurements were performed
with the... | astro-ph | we probed the first 3au around tau ceti and epsilon eridani with the chara array mt wilson usa in order to gauge the 2micron excess flux emanating from possible hot dust grains in the debris disks and to also resolve the stellar photospheres high precision visibility amplitude measurements were performed with the fluor... | [['we', 'probed', 'the', 'first', '3au', 'around', 'tau', 'ceti', 'and', 'epsilon', 'eridani', 'with', 'the', 'chara', 'array', 'mt', 'wilson', 'usa', 'in', 'order', 'to', 'gauge', 'the', '2micron', 'excess', 'flux', 'emanating', 'from', 'possible', 'hot', 'dust', 'grains', 'in', 'the', 'debris', 'disks', 'and', 'to', ... | [-0.06964991891436512, 0.12680231589623267, -0.06567416533168095, 0.06375925813730039, -0.09021473573860324, -0.0991025936891674, 0.038617584327463796, 0.40813391436677193, -0.1944709901169214, -0.38322777263147145, 0.06554346599235335, -0.33112653232334804, 0.03407803386047211, 0.1624288338501477, -0.06780706281036449... |
710.1732 | On the structure of the constraint algebra for systems whose gauge
transformations depend on higher order time derivatives of the gauge
parameters | The dynamical systems invariant under gauge transformations with higher order
time derivatives of the gauge parameter are considered from the Hamiltonian
point of view. We investigate the consequences of the basic requirements that
the constraints on the one hand and the Hamiltonian and constraints on the
other hand ... | hep-th | the dynamical systems invariant under gauge transformations with higher order time derivatives of the gauge parameter are considered from the hamiltonian point of view we investigate the consequences of the basic requirements that the constraints on the one hand and the hamiltonian and constraints on the other hand for... | [['the', 'dynamical', 'systems', 'invariant', 'under', 'gauge', 'transformations', 'with', 'higher', 'order', 'time', 'derivatives', 'of', 'the', 'gauge', 'parameter', 'are', 'considered', 'from', 'the', 'hamiltonian', 'point', 'of', 'view', 'we', 'investigate', 'the', 'consequences', 'of', 'the', 'basic', 'requirement... | [-0.19011830974041538, 0.11378299336716094, -0.09651758223224212, 0.08042314167387839, -0.12833258841077194, -0.14117988628533887, 0.004622728776131921, 0.31072107505272417, -0.29029880050460205, -0.2851949856233071, 0.14595290740287645, -0.23930602493312428, -0.16182196021819598, 0.18648576839169598, -0.03320090111468... |
710.1733 | Diffraction at the Tevatron | This article contains a summary of the recent results in diffractive physics
at the Tevatron. Results from the CDF diffraction program include the single
diffractive to non-diffractive ratio in dijet events, observation of exclusive
$e^+e^-$ production via two-photon exchange, hints of exclusive $\gamma\gamma$
produc... | hep-ex | this article contains a summary of the recent results in diffractive physics at the tevatron results from the cdf diffraction program include the single diffractive to nondiffractive ratio in dijet events observation of exclusive ee production via twophoton exchange hints of exclusive gammagamma production via double p... | [['this', 'article', 'contains', 'a', 'summary', 'of', 'the', 'recent', 'results', 'in', 'diffractive', 'physics', 'at', 'the', 'tevatron', 'results', 'from', 'the', 'cdf', 'diffraction', 'program', 'include', 'the', 'single', 'diffractive', 'to', 'nondiffractive', 'ratio', 'in', 'dijet', 'events', 'observation', 'of',... | [-0.03869235506982938, 0.1791948047171551, -0.15197676788594522, 0.13663572645172067, -0.0753005466819422, -0.09283728581177045, 0.06537913043715365, 0.3141101793679473, -0.22713415403786588, -0.21403745861647472, -0.054334593238309026, -0.37905003069198295, -0.004462043454947128, 0.17737763746456586, 0.098614280992378... |
710.1734 | When Stars Collide | When two stars collide and merge they form a new star that can stand out
against the background population in a starcluster as a blue straggler. In so
called collision runaways many stars can merge and may form a very massive star
that eventually forms an intermediate mass blackhole. We have performed
detailed evolut... | astro-ph | when two stars collide and merge they form a new star that can stand out against the background population in a starcluster as a blue straggler in so called collision runaways many stars can merge and may form a very massive star that eventually forms an intermediate mass blackhole we have performed detailed evolution ... | [['when', 'two', 'stars', 'collide', 'and', 'merge', 'they', 'form', 'a', 'new', 'star', 'that', 'can', 'stand', 'out', 'against', 'the', 'background', 'population', 'in', 'a', 'starcluster', 'as', 'a', 'blue', 'straggler', 'in', 'so', 'called', 'collision', 'runaways', 'many', 'stars', 'can', 'merge', 'and', 'may', 'f... | [-0.06566967591978945, 0.2065779610678841, -0.12719149566633073, 0.17120548960991908, -0.1154127890162321, -0.04512382769403425, 0.08200808836940073, 0.37702461635811374, -0.12914889633890475, -0.34511589887447086, 0.005576340021221555, -0.30388821604418326, 0.0020326736618068303, 0.1881323393060918, -0.062942731320052... |
710.1735 | Static black hole solutions with a self interacting conformally coupled
scalar field | We study static, spherically symmetric black hole solutions of the Einstein
equations with a positive cosmological constant and a conformally coupled self
interacting scalar field. Exact solutions for this model found by
Mart{\'\i}nez, Troncoso, and Zanelli, (MTZ), were subsequently shown to be
unstable under linear ... | hep-th gr-qc | we study static spherically symmetric black hole solutions of the einstein equations with a positive cosmological constant and a conformally coupled self interacting scalar field exact solutions for this model found by martinez troncoso and zanelli mtz were subsequently shown to be unstable under linear perturbations w... | [['we', 'study', 'static', 'spherically', 'symmetric', 'black', 'hole', 'solutions', 'of', 'the', 'einstein', 'equations', 'with', 'a', 'positive', 'cosmological', 'constant', 'and', 'a', 'conformally', 'coupled', 'self', 'interacting', 'scalar', 'field', 'exact', 'solutions', 'for', 'this', 'model', 'found', 'by', 'ma... | [-0.1924975836886099, 0.0864026446757541, -0.10565791744738817, 0.09779970708619565, -0.0944052752904379, -0.158606952157779, -0.039978047291813895, 0.2928359315861972, -0.17625240576214707, -0.23398092987899405, 0.15818462786428894, -0.28374893851697636, -0.1052965147402854, 0.16122197769641972, -0.019484312023194388,... |
710.1736 | Phonon Driven Nonlinear Electrical Behavior in Molecular Devices | Electronic transport in a model molecular device coupled to local phonon
modes is theoretically analyzed. The method allows for obtaining an accurate
approximation of the system's quantum state irrespective of the electron and
phonon energy scales. Nonlinear electrical features emerge from the calculated
current-volt... | cond-mat.mes-hall | electronic transport in a model molecular device coupled to local phonon modes is theoretically analyzed the method allows for obtaining an accurate approximation of the systems quantum state irrespective of the electron and phonon energy scales nonlinear electrical features emerge from the calculated currentvoltage ch... | [['electronic', 'transport', 'in', 'a', 'model', 'molecular', 'device', 'coupled', 'to', 'local', 'phonon', 'modes', 'is', 'theoretically', 'analyzed', 'the', 'method', 'allows', 'for', 'obtaining', 'an', 'accurate', 'approximation', 'of', 'the', 'systems', 'quantum', 'state', 'irrespective', 'of', 'the', 'electron', '... | [-0.16532296826442083, 0.13591533418298543, -0.1078838308279713, 0.05526476895902306, 0.0002907123416662216, -0.150173296580712, 0.062754311679552, 0.31164554170022407, -0.3006958085174362, -0.27170522880818077, -0.02961996541979412, -0.31033063742351563, -0.1366543307652076, 0.212851838938271, 0.05754684452588359, 0.0... |
710.1737 | A number filter for matter-waves | In current Bose-Einstein condensate experiments, the shot-to-shot variation
of atom number fluctuates up to 10%. In here, we present a procedure to
suppress such fluctuations by using a nonlinear p-pi-pbar matter wave
interferometer for a Bose-Einstein condensate with two internal states and a
high beam-splitter asym... | quant-ph | in current boseeinstein condensate experiments the shottoshot variation of atom number fluctuates up to 10 in here we present a procedure to suppress such fluctuations by using a nonlinear ppipbar matter wave interferometer for a boseeinstein condensate with two internal states and a high beamsplitter asymmetry p pbar ... | [['in', 'current', 'boseeinstein', 'condensate', 'experiments', 'the', 'shottoshot', 'variation', 'of', 'atom', 'number', 'fluctuates', 'up', 'to', '10', 'in', 'here', 'we', 'present', 'a', 'procedure', 'to', 'suppress', 'such', 'fluctuations', 'by', 'using', 'a', 'nonlinear', 'ppipbar', 'matter', 'wave', 'interferomet... | [-0.14010389373396281, 0.2186167587565307, -0.06828263718174932, 0.08124418187897975, 0.006309235445511194, -0.1447156106788711, 0.04736389124185353, 0.32361237465599435, -0.23590123643063837, -0.30276408122369536, 0.0011162866441601956, -0.31394612934026456, -0.087058244847957, 0.14979529282779513, 0.00873232856795283... |
710.1738 | Modified f(R) gravity unifying R^m inflation with \LambdaCDM epoch | We consider modified $f(R)$ gravity which may unify $R^m$ early-time
inflation with late-time $\Lambda$CDM epoch. It is shown that such model passes
the local tests (Newton law, stability of Earth-like gravitational solution,
very heavy mass for additional scalar degree of freedom) and suggests the
realistic alternat... | hep-th astro-ph gr-qc | we consider modified fr gravity which may unify rm earlytime inflation with latetime lambdacdm epoch it is shown that such model passes the local tests newton law stability of earthlike gravitational solution very heavy mass for additional scalar degree of freedom and suggests the realistic alternative for general rela... | [['we', 'consider', 'modified', 'fr', 'gravity', 'which', 'may', 'unify', 'rm', 'earlytime', 'inflation', 'with', 'latetime', 'lambdacdm', 'epoch', 'it', 'is', 'shown', 'that', 'such', 'model', 'passes', 'the', 'local', 'tests', 'newton', 'law', 'stability', 'of', 'earthlike', 'gravitational', 'solution', 'very', 'heav... | [-0.15715822574178068, 0.09872869099878395, -0.12919442779384555, 0.18207851528228883, -0.1509338214372595, -0.24020836749114097, -0.12522136393235997, 0.28841778548279157, -0.19685909654945136, -0.3098216671884681, 0.04144267047910641, -0.2043186278237651, -0.1075136320044597, 0.17930138231022283, -0.01748507470668604... |
710.1739 | Lagrangian statistics in forced two-dimensional turbulence | We report on simulations of two-dimensional turbulence in the inverse energy
cascade regime. Focusing on the statistics of Lagrangian tracer particles,
scaling behavior of the probability density functions of velocity fluctuations
is investigated. The results are compared to the three-dimensional case. In
particular ... | physics.flu-dyn | we report on simulations of twodimensional turbulence in the inverse energy cascade regime focusing on the statistics of lagrangian tracer particles scaling behavior of the probability density functions of velocity fluctuations is investigated the results are compared to the threedimensional case in particular an analy... | [['we', 'report', 'on', 'simulations', 'of', 'twodimensional', 'turbulence', 'in', 'the', 'inverse', 'energy', 'cascade', 'regime', 'focusing', 'on', 'the', 'statistics', 'of', 'lagrangian', 'tracer', 'particles', 'scaling', 'behavior', 'of', 'the', 'probability', 'density', 'functions', 'of', 'velocity', 'fluctuations... | [-0.152264185704246, 0.1565779287226748, -0.12292501471196134, 0.08419085420943033, 0.03080748575907874, -0.03359777308125273, -0.029677987452147597, 0.31857988141836174, -0.22860211000429936, -0.27063219986452036, 0.027722729492023677, -0.3271736831639905, -0.11960567390344229, 0.1946249800363937, 0.042791186310477125... |
710.174 | A regularity and compactness theory for immersed stable minimal
hypersurfaces of multiplicity at most 2 | We prove that a stable minimal hypersurface of an open ball having a singular
set of locally finite codimension 2 Hausdorff measure which is weakly close to
a multiplicity 2 hyperplane is a 2-valued C^{1, alpha} graph in the interior.
Applications including a compactness theorem for a class of immersed stable
minimal... | math.DG | we prove that a stable minimal hypersurface of an open ball having a singular set of locally finite codimension 2 hausdorff measure which is weakly close to a multiplicity 2 hyperplane is a 2valued c1 alpha graph in the interior applications including a compactness theorem for a class of immersed stable minimal hypersu... | [['we', 'prove', 'that', 'a', 'stable', 'minimal', 'hypersurface', 'of', 'an', 'open', 'ball', 'having', 'a', 'singular', 'set', 'of', 'locally', 'finite', 'codimension', '2', 'hausdorff', 'measure', 'which', 'is', 'weakly', 'close', 'to', 'a', 'multiplicity', '2', 'hyperplane', 'is', 'a', '2valued', 'c1', 'alpha', 'gr... | [-0.1733071538220559, 0.10713153435769657, -0.06386350840330124, 0.1087253076539907, -0.0371313229635624, -0.16744630276225508, -0.018902060482650994, 0.3121754209777074, -0.25343019273132084, -0.15152888654598168, 0.14864347507412146, -0.29311345665316496, -0.07403535369001994, 0.17534456017560193, -0.1715702392027846... |
710.1741 | Semileptonic D-decays and Lattice QCD | We explore four different strategies to extract the D-meson semileptonic
decay form factors from the Green functions computed in QCD numerically on the
lattice. From our numerical tests we find that two such strategies, based on
the use of double ratios of 3-point correlation functions, lead to an
appreciable reducti... | hep-lat hep-ph | we explore four different strategies to extract the dmeson semileptonic decay form factors from the green functions computed in qcd numerically on the lattice from our numerical tests we find that two such strategies based on the use of double ratios of 3point correlation functions lead to an appreciable reduction of s... | [['we', 'explore', 'four', 'different', 'strategies', 'to', 'extract', 'the', 'dmeson', 'semileptonic', 'decay', 'form', 'factors', 'from', 'the', 'green', 'functions', 'computed', 'in', 'qcd', 'numerically', 'on', 'the', 'lattice', 'from', 'our', 'numerical', 'tests', 'we', 'find', 'that', 'two', 'such', 'strategies',... | [-0.06460244529256501, 0.1368423740444921, -0.07427522868935749, 0.09163752614914142, -0.02613323184507947, -0.056587280859191395, 0.08762550134615031, 0.3699739542549726, -0.2287457177665123, -0.22727912119061677, 0.07870749865548167, -0.29982204454922184, -0.12058629853814148, 0.17585171964595614, 0.04175442885895519... |
710.1742 | Neutrino Mass Matrix from Seesaw Mechanism with Heavy Majorana Neutrino
Subject to Texture Zero and Invariant Under a Cyclic Permutation | We evaluate the predictive power of the neutrino mass matrices arising from
seesaw mechanism with heavy Majorana mass matrices subject to texture zero and
satisfy a cyclic permutation invariant form to the solar neutrino mixing
phenomena. From eight possible patterns of heavy Majorana neutrino mass matrix,
we found t... | hep-ph | we evaluate the predictive power of the neutrino mass matrices arising from seesaw mechanism with heavy majorana mass matrices subject to texture zero and satisfy a cyclic permutation invariant form to the solar neutrino mixing phenomena from eight possible patterns of heavy majorana neutrino mass matrix we found that ... | [['we', 'evaluate', 'the', 'predictive', 'power', 'of', 'the', 'neutrino', 'mass', 'matrices', 'arising', 'from', 'seesaw', 'mechanism', 'with', 'heavy', 'majorana', 'mass', 'matrices', 'subject', 'to', 'texture', 'zero', 'and', 'satisfy', 'a', 'cyclic', 'permutation', 'invariant', 'form', 'to', 'the', 'solar', 'neutri... | [-0.13196627250138976, 0.36484115738957906, 0.0022325323263106688, 0.2046255762728684, -0.050437870059060315, -0.19764306556037947, 0.0384743476082405, 0.31930546995813713, -0.2319426193437858, -0.29490751084195427, 0.048127718569335294, -0.27507062570179164, -0.0902501546765027, 0.13932218137260985, 0.0091037670507618... |
710.1743 | Non-Statistical gamma Rays from Fragments | Polarization mechanism by Strutinsky-Denisov gives rise to the electric
dipole radiation from fragments. Its probability calculated within the LDM
turns out to be ~3.5x10-2 per fission. The radiation occurs during
thermolization of the post-rupture deformation energy of the fragments, but
before the neutron emission.... | quant-ph | polarization mechanism by strutinskydenisov gives rise to the electric dipole radiation from fragments its probability calculated within the ldm turns out to be 35x102 per fission the radiation occurs during thermolization of the postrupture deformation energy of the fragments but before the neutron emission | [['polarization', 'mechanism', 'by', 'strutinskydenisov', 'gives', 'rise', 'to', 'the', 'electric', 'dipole', 'radiation', 'from', 'fragments', 'its', 'probability', 'calculated', 'within', 'the', 'ldm', 'turns', 'out', 'to', 'be', '35x102', 'per', 'fission', 'the', 'radiation', 'occurs', 'during', 'thermolization', 'o... | [-0.05170584108564071, 0.22994624532293528, -0.11564451771555469, 0.10424216575920582, -0.0009556211531162262, -0.04084555340232328, 0.06436453629285097, 0.3393148539587855, -0.2896621782332659, -0.3113219408551231, -0.055668219737708566, -0.2720091727562249, 0.027501252270303665, 0.17083200202323495, 0.032743741496233... |
710.1744 | Quantum problem solving as simultaneous computation | I provide an alternative way of seeing quantum computation. First, I describe
an idealized classical problem solving machine that, thanks to a many body
interaction, reversibly and nondeterministically produces the solution of the
problem under the simultaneous influence of all the problem constraints. This
requires ... | quant-ph | i provide an alternative way of seeing quantum computation first i describe an idealized classical problem solving machine that thanks to a many body interaction reversibly and nondeterministically produces the solution of the problem under the simultaneous influence of all the problem constraints this requires a perfe... | [['i', 'provide', 'an', 'alternative', 'way', 'of', 'seeing', 'quantum', 'computation', 'first', 'i', 'describe', 'an', 'idealized', 'classical', 'problem', 'solving', 'machine', 'that', 'thanks', 'to', 'a', 'many', 'body', 'interaction', 'reversibly', 'and', 'nondeterministically', 'produces', 'the', 'solution', 'of',... | [-0.11743350116742982, 0.08921533382834039, -0.10637772879459792, 0.013797915423185462, -0.05725960805908673, -0.12750723977469736, 0.04776791360022293, 0.2944967544306484, -0.34265582508304054, -0.304001276012924, 0.09915298986817814, -0.2565593194030225, -0.11374833612495826, 0.1953304603188816, -0.05433548841690127,... |
710.1745 | The GBT350 Survey of the Northern Galactic Plane for Radio Pulsars and
Transients | Using the Green Bank Telescope (GBT) and Pulsar Spigot at 350MHz, we have
surveyed the Northern Galactic Plane for pulsars and radio transients. This
survey covers roughly 1000 square degrees of sky within 75 deg < l < 165 deg
and |b| < 5.5 deg, a region of the Galactic Plane inaccessible to both the
Parkes and Areci... | astro-ph | using the green bank telescope gbt and pulsar spigot at 350mhz we have surveyed the northern galactic plane for pulsars and radio transients this survey covers roughly 1000 square degrees of sky within 75 deg l 165 deg and b 55 deg a region of the galactic plane inaccessible to both the parkes and arecibo multibeam sur... | [['using', 'the', 'green', 'bank', 'telescope', 'gbt', 'and', 'pulsar', 'spigot', 'at', '350mhz', 'we', 'have', 'surveyed', 'the', 'northern', 'galactic', 'plane', 'for', 'pulsars', 'and', 'radio', 'transients', 'this', 'survey', 'covers', 'roughly', '1000', 'square', 'degrees', 'of', 'sky', 'within', '75', 'deg', 'l',... | [-0.136642954852407, 0.09497527129727826, 0.0010372274868210318, 0.07005386201286769, -0.16005849112350976, -0.04597771086139224, 0.11166953787042369, 0.3774776264063774, -0.18222619397177672, -0.37119427270266, 0.13458319794091206, -0.3261252732456772, -0.059098166822936504, 0.2801291772454817, -0.0017611535545501117,... |
710.1746 | Field Theory on Nonanticommutative Superspace | We discuss a deformation of the Hopf algebra of supersymmetry (SUSY)
transformations based on a special choice of twist. As usual, algebra itself
remains unchanged, but the comultiplication changes. This leads to the deformed
Leibniz rule for SUSY transformations. Superfields are elements of the algebra
of functions ... | hep-th | we discuss a deformation of the hopf algebra of supersymmetry susy transformations based on a special choice of twist as usual algebra itself remains unchanged but the comultiplication changes this leads to the deformed leibniz rule for susy transformations superfields are elements of the algebra of functions of the us... | [['we', 'discuss', 'a', 'deformation', 'of', 'the', 'hopf', 'algebra', 'of', 'supersymmetry', 'susy', 'transformations', 'based', 'on', 'a', 'special', 'choice', 'of', 'twist', 'as', 'usual', 'algebra', 'itself', 'remains', 'unchanged', 'but', 'the', 'comultiplication', 'changes', 'this', 'leads', 'to', 'the', 'deforme... | [-0.1672036662110654, 0.1415483517896222, -0.06468270545744377, 0.04653962588484359, -0.13991644154100313, -0.11810241383196705, -0.04359188861436332, 0.3469707147906656, -0.28559552108079356, -0.19934074579150943, 0.1226411549060646, -0.2100049915095872, -0.17141803094874258, 0.11582991889799418, -0.12397059924715785,... |
710.1747 | Manifold and metric in numerical solution of the quasi-static
electromagnetic boundary value problems | Classical vector analysis is the predominant formalism used by engineers of
computational electromagnetism, despite the fact that manifold as a theoretical
concept has existed for a century. This paper discusses the benefits of
manifolds over the traditional approach in practical problems of modelling.
With a structu... | math-ph math.MP | classical vector analysis is the predominant formalism used by engineers of computational electromagnetism despite the fact that manifold as a theoretical concept has existed for a century this paper discusses the benefits of manifolds over the traditional approach in practical problems of modelling with a structural a... | [['classical', 'vector', 'analysis', 'is', 'the', 'predominant', 'formalism', 'used', 'by', 'engineers', 'of', 'computational', 'electromagnetism', 'despite', 'the', 'fact', 'that', 'manifold', 'as', 'a', 'theoretical', 'concept', 'has', 'existed', 'for', 'a', 'century', 'this', 'paper', 'discusses', 'the', 'benefits',... | [-0.09495731807117791, 0.007308236482602201, -0.076465998403728, 0.03987044412642717, -0.1297615496539756, -0.11866700990909809, -0.017951411507582588, 0.34527810624751604, -0.294667299464345, -0.3194827408970971, 0.10188378193660787, -0.2281569621182586, -0.22667170827227986, 0.23136784761874496, -0.11178746594263142,... |
710.1748 | One-loop corrections to three-body leptonic chargino decays | We calculate full one-loop corrections to the genuine three-body decays of
the light chargino \chi_1^\pm to \chi^0_1 l^\pm \nu in the Minimal
Supersymmetric Standard Model. We find that the corrections to the decay width
can be of the order of a few percent. We show also how radiative corrections
affect energy and an... | hep-ph | we calculate full oneloop corrections to the genuine threebody decays of the light chargino chi_1pm to chi0_1 lpm nu in the minimal supersymmetric standard model we find that the corrections to the decay width can be of the order of a few percent we show also how radiative corrections affect energy and angular distribu... | [['we', 'calculate', 'full', 'oneloop', 'corrections', 'to', 'the', 'genuine', 'threebody', 'decays', 'of', 'the', 'light', 'chargino', 'chi_1pm', 'to', 'chi0_1', 'lpm', 'nu', 'in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'we', 'find', 'that', 'the', 'corrections', 'to', 'the', 'decay', 'width', 'can',... | [-0.034052563293291066, 0.22593574834473687, -0.05439960915627408, 0.2299823604267219, -0.0313898435119411, -0.11599941210468011, 0.05340883700409904, 0.29013574018207344, -0.2438937110087738, -0.28427542147130286, -0.025406695944497938, -0.3616217467291602, 0.0015330330693516239, 0.13108669666589462, 0.047173897880290... |
710.1749 | On the frequency and temperature dependence of the conductivity | We obtain the frequency and temperature dependence of the conductivity for
(disordered) solids, where the temperature dependence is defined in terms of
the related thermodynamic state function in exponential (or power law, etc.)
forms. The model is applied to n-type Si with various donor and acceptor
impurities and s... | cond-mat.mtrl-sci | we obtain the frequency and temperature dependence of the conductivity for disordered solids where the temperature dependence is defined in terms of the related thermodynamic state function in exponential or power law etc forms the model is applied to ntype si with various donor and acceptor impurities and several conc... | [['we', 'obtain', 'the', 'frequency', 'and', 'temperature', 'dependence', 'of', 'the', 'conductivity', 'for', 'disordered', 'solids', 'where', 'the', 'temperature', 'dependence', 'is', 'defined', 'in', 'terms', 'of', 'the', 'related', 'thermodynamic', 'state', 'function', 'in', 'exponential', 'or', 'power', 'law', 'etc... | [-0.07109908767544278, 0.21175159456594506, -0.011716945891881861, 0.004722314286216094, 0.040706693228879355, -0.16757348503508582, 0.051895940267458196, 0.37437223770269534, -0.2512970647388479, -0.31685563860597404, 0.048765205562387295, -0.3743547451477952, -0.07108525299501219, 0.18763185009678326, 0.0343182542838... |
710.175 | 3000 % high-field magnetoresistance in super-lattices of CoFe
nanoparticles | We report on magnetotransport measurements on millimetre-large super-lattices
of CoFe nanoparticles surrounded by an organic layer. Electrical properties are
typical of Coulomb blockade in three dimensional arrays of nanoparticles. A
large high-field magnetoresistance, reaching up to 3000 %, is measured between
1.8 a... | cond-mat.mtrl-sci | we report on magnetotransport measurements on millimetrelarge superlattices of cofe nanoparticles surrounded by an organic layer electrical properties are typical of coulomb blockade in three dimensional arrays of nanoparticles a large highfield magnetoresistance reaching up to 3000 is measured between 18 and 10 k this... | [['we', 'report', 'on', 'magnetotransport', 'measurements', 'on', 'millimetrelarge', 'superlattices', 'of', 'cofe', 'nanoparticles', 'surrounded', 'by', 'an', 'organic', 'layer', 'electrical', 'properties', 'are', 'typical', 'of', 'coulomb', 'blockade', 'in', 'three', 'dimensional', 'arrays', 'of', 'nanoparticles', 'a'... | [-0.2110057084927368, 0.2312680035362351, 0.03697999279227173, -0.03707162506282003, -0.009000566561314228, -0.14231279015279652, 0.06722330535239164, 0.4046064183573451, -0.22485430934057946, -0.3673472050904182, -0.001610282087584206, -0.36613836342860995, -0.10588800689417935, 0.21697010390721916, 0.0551914629738843... |
710.1751 | Effective string theory description of the interface free energy | We compare the predictions of the Nambu-Goto effective string model with a
set of high precision Monte Carlo results for interfaces with periodic boundary
conditions in the 3D Ising model. We compute the free energy in the covariant
gauge exactly, up to the inclusion of the Liouville mode. The perturbative
expansion ... | hep-lat | we compare the predictions of the nambugoto effective string model with a set of high precision monte carlo results for interfaces with periodic boundary conditions in the 3d ising model we compute the free energy in the covariant gauge exactly up to the inclusion of the liouville mode the perturbative expansion of thi... | [['we', 'compare', 'the', 'predictions', 'of', 'the', 'nambugoto', 'effective', 'string', 'model', 'with', 'a', 'set', 'of', 'high', 'precision', 'monte', 'carlo', 'results', 'for', 'interfaces', 'with', 'periodic', 'boundary', 'conditions', 'in', 'the', '3d', 'ising', 'model', 'we', 'compute', 'the', 'free', 'energy',... | [-0.10193976092977022, 0.13790094831548855, -0.07866871183883982, 0.09546516045467951, -0.03472511059918766, -0.11447356143371618, 0.03149974156109369, 0.3348275574081274, -0.21211713769736823, -0.31766429663557244, 0.09032005196330642, -0.26337917420048135, -0.11158682183953035, 0.1498875248158934, 0.00519215347349127... |
710.1752 | The formation and evolution of very massive stars in dense stellar
systems | The early evolution of dense stellar systems is governed by massive single
star and binary evolution. Core collapse of dense massive star clusters can
lead to the formation of very massive objects through stellar collisions
($M\geq$ 1000 \msun). Stellar wind mass loss determines the evolution and final
fate of these ... | astro-ph | the early evolution of dense stellar systems is governed by massive single star and binary evolution core collapse of dense massive star clusters can lead to the formation of very massive objects through stellar collisions mgeq 1000 msun stellar wind mass loss determines the evolution and final fate of these objects an... | [['the', 'early', 'evolution', 'of', 'dense', 'stellar', 'systems', 'is', 'governed', 'by', 'massive', 'single', 'star', 'and', 'binary', 'evolution', 'core', 'collapse', 'of', 'dense', 'massive', 'star', 'clusters', 'can', 'lead', 'to', 'the', 'formation', 'of', 'very', 'massive', 'objects', 'through', 'stellar', 'col... | [-0.09558014116450915, 0.15545599711893449, -0.06000477798946508, 0.14567208883020874, -0.10052000846050374, -0.0685427188873291, 0.037394511757405755, 0.36907060180267653, -0.13107816008085463, -0.3869848957935935, 0.054682787996557326, -0.21604610098627944, -0.05887682615039385, 0.18999535743185408, -0.03815636353744... |
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