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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706.2114 | Rigid Limit in N=2 Supergravity and Weak-Gravity Conjecture | We analyze the coupled N=2 supergravity and Yang-Mills system using
holomorphy, near the rigid limit where the former decouples from the latter. We
find that there appears generically a new mass scale around g M_{pl} where g is
the gauge coupling constant and M_{pl} is the Planck scale. This is in accord
with the wea... | hep-th | we analyze the coupled n2 supergravity and yangmills system using holomorphy near the rigid limit where the former decouples from the latter we find that there appears generically a new mass scale around g m_pl where g is the gauge coupling constant and m_pl is the planck scale this is in accord with the weakgravity co... | [['we', 'analyze', 'the', 'coupled', 'n2', 'supergravity', 'and', 'yangmills', 'system', 'using', 'holomorphy', 'near', 'the', 'rigid', 'limit', 'where', 'the', 'former', 'decouples', 'from', 'the', 'latter', 'we', 'find', 'that', 'there', 'appears', 'generically', 'a', 'new', 'mass', 'scale', 'around', 'g', 'm_pl', 'w... | [-0.15180862550875424, 0.1945206444282588, -0.06409319914952927, 0.04895894759573747, -0.07938675968781919, -0.13770458995477874, -0.031272976805544084, 0.2647427192863983, -0.215371160239384, -0.28581523779477624, 0.0879911497295079, -0.2693356352801611, -0.16402682400547672, 0.09121393774812286, -0.03900956580843273,... |
706.2115 | RNA polymerase motors on DNA track: effects of traffic congestion on RNA
synthesis | RNA polymerase (RNAP) is an enzyme that synthesizes a messenger RNA (mRNA)
strand which is complementary to a single-stranded DNA template. From the
perspective of physicists, an RNAP is a molecular motor that utilizes chemical
energy input to move along the track formed by a ssDNA. In some circumstances,
which are d... | physics.bio-ph q-bio.GN | rna polymerase rnap is an enzyme that synthesizes a messenger rna mrna strand which is complementary to a singlestranded dna template from the perspective of physicists an rnap is a molecular motor that utilizes chemical energy input to move along the track formed by a ssdna in some circumstances which are described in... | [['rna', 'polymerase', 'rnap', 'is', 'an', 'enzyme', 'that', 'synthesizes', 'a', 'messenger', 'rna', 'mrna', 'strand', 'which', 'is', 'complementary', 'to', 'a', 'singlestranded', 'dna', 'template', 'from', 'the', 'perspective', 'of', 'physicists', 'an', 'rnap', 'is', 'a', 'molecular', 'motor', 'that', 'utilizes', 'che... | [-0.11742684832731394, 0.1734835434136375, -0.05313882126353031, 0.048694061109873316, -0.019727141050809235, -0.14178747364964622, 0.09926782654647952, 0.38979516862808955, -0.2991808942965502, -0.32095878107814924, -0.00852484201059054, -0.24288079338031132, -0.18743525294190239, 0.16182530072473605, -0.0776806365582... |
706.2116 | Linear precision for parametric patches | We give a precise mathematical formulation for the notions of a parametric
patch and linear precision, and establish their elementary properties. We
relate linear precision to the geometry of a particular linear projection,
giving necessary (and quite restrictive) conditions for a patch to possess
linear precision. A... | math.AG | we give a precise mathematical formulation for the notions of a parametric patch and linear precision and establish their elementary properties we relate linear precision to the geometry of a particular linear projection giving necessary and quite restrictive conditions for a patch to possess linear precision a main fo... | [['we', 'give', 'a', 'precise', 'mathematical', 'formulation', 'for', 'the', 'notions', 'of', 'a', 'parametric', 'patch', 'and', 'linear', 'precision', 'and', 'establish', 'their', 'elementary', 'properties', 'we', 'relate', 'linear', 'precision', 'to', 'the', 'geometry', 'of', 'a', 'particular', 'linear', 'projection'... | [-0.09011722171992481, 0.012507833597015277, -0.11808564158800607, 0.12393640205220571, -0.11838821062130557, -0.18911645488778703, 0.01841945530820603, 0.35520912470974936, -0.3222134769023788, -0.2533992800609183, 0.13796858093810102, -0.19953130023275442, -0.14396979153280312, 0.18854569331264107, -0.125018500326915... |
706.2117 | Novel Master Formula for Twist-3 Soft-Gluon-Pole Mechanism to Single
Transverse-Spin Asymmetry | We prove that twist-3 soft-gluon-pole (SGP) cross section for single spin
asymmetries is determined by a certain ``primordial'' twist-2 cross section up
to kinematic and color factors in the leading order perturbative QCD. This
unveils universal structure behind the SGP cross sections in a variety of hard
processes, ... | hep-ph | we prove that twist3 softgluonpole sgp cross section for single spin asymmetries is determined by a certain primordial twist2 cross section up to kinematic and color factors in the leading order perturbative qcd this unveils universal structure behind the sgp cross sections in a variety of hard processes and also the s... | [['we', 'prove', 'that', 'twist3', 'softgluonpole', 'sgp', 'cross', 'section', 'for', 'single', 'spin', 'asymmetries', 'is', 'determined', 'by', 'a', 'certain', 'primordial', 'twist2', 'cross', 'section', 'up', 'to', 'kinematic', 'and', 'color', 'factors', 'in', 'the', 'leading', 'order', 'perturbative', 'qcd', 'this',... | [-0.08742803850030641, 0.1654070745524, -0.13278176610795211, 0.13082285184527234, -0.021187577615206947, -0.03197005397060468, -0.016403686876494284, 0.3274323674755133, -0.24482862788195514, -0.18758113640455568, -0.09515040263038232, -0.3302627122243486, -0.02562007171158888, 0.15538996088019172, 0.07017357719168828... |
706.2118 | A method for integral cohomology of posets | We present a method to compute integral cohomology of posets. This toolbox is
applicable as soon as the sub-posets under each object possess certain
structure. This is the case for simplicial complexes and simplex-like posets.
The method is based on homological algebra arguments in the category of
functors and on a s... | math.AT | we present a method to compute integral cohomology of posets this toolbox is applicable as soon as the subposets under each object possess certain structure this is the case for simplicial complexes and simplexlike posets the method is based on homological algebra arguments in the category of functors and on a spectral... | [['we', 'present', 'a', 'method', 'to', 'compute', 'integral', 'cohomology', 'of', 'posets', 'this', 'toolbox', 'is', 'applicable', 'as', 'soon', 'as', 'the', 'subposets', 'under', 'each', 'object', 'possess', 'certain', 'structure', 'this', 'is', 'the', 'case', 'for', 'simplicial', 'complexes', 'and', 'simplexlike', '... | [-0.1227672054903001, 0.04601805011872628, -0.12661061917621924, 0.10722406573783887, -0.10759399463022028, -0.12772677272498126, 0.008078620058073792, 0.38377369525692157, -0.3620870649333923, -0.21522395024814653, 0.12087116581112427, -0.18972313889522627, -0.16240098656866178, 0.17676883341083605, -0.176943919080640... |
706.2119 | Structural properties and optical response of Na clusters in Ne, Ar, and
Kr matrices | We discuss the structural properties and optical response of a small Na
cluster inside rare gas (RG) matrices of Ne, Ar, or Kr atoms. The mixed systems
are described with a hierarchical model, treating the cluster at a quantum
mechanical level and the matrix atoms classically in terms of their positions
and polarizat... | cond-mat.other | we discuss the structural properties and optical response of a small na cluster inside rare gas rg matrices of ne ar or kr atoms the mixed systems are described with a hierarchical model treating the cluster at a quantum mechanical level and the matrix atoms classically in terms of their positions and polarizations we ... | [['we', 'discuss', 'the', 'structural', 'properties', 'and', 'optical', 'response', 'of', 'a', 'small', 'na', 'cluster', 'inside', 'rare', 'gas', 'rg', 'matrices', 'of', 'ne', 'ar', 'or', 'kr', 'atoms', 'the', 'mixed', 'systems', 'are', 'described', 'with', 'a', 'hierarchical', 'model', 'treating', 'the', 'cluster', 'a... | [-0.10300602763955184, 0.18679380254144526, -0.01531350110135563, 0.07525126755769763, 0.037189413455652666, -0.12686860040955983, 0.07707088364155165, 0.3962956845125818, -0.2981102523076665, -0.2913083117301729, 0.0022155932780191464, -0.3129166001274895, -0.11752981465606653, 0.06959007814997337, 0.01897109309109030... |
706.212 | IRAS08281-4850 and IRAS14325-6428: two A-type post-AGB stars with
s-process enrichment | One of the puzzling findings in the study of the chemical evolution of
(post-)AGB stars is why very similar stars (in terms of metallicity, spectral
type, infrared properties, etc...) show a very different photospheric
composition. We aim at extending the still limited sample of s-process enriched
post-AGB stars, in ... | astro-ph | one of the puzzling findings in the study of the chemical evolution of postagb stars is why very similar stars in terms of metallicity spectral type infrared properties etc show a very different photospheric composition we aim at extending the still limited sample of sprocess enriched postagb stars in order to obtain a... | [['one', 'of', 'the', 'puzzling', 'findings', 'in', 'the', 'study', 'of', 'the', 'chemical', 'evolution', 'of', 'postagb', 'stars', 'is', 'why', 'very', 'similar', 'stars', 'in', 'terms', 'of', 'metallicity', 'spectral', 'type', 'infrared', 'properties', 'etc', 'show', 'a', 'very', 'different', 'photospheric', 'composi... | [-0.03125110723118743, 0.11609888205561404, -0.08393453443557888, 0.08569224193174244, -0.09142452492243677, -0.05016852435685418, 0.11710145315020412, 0.43874182318593713, -0.1282635360814469, -0.34404175855772756, 0.027364958778270047, -0.2894159770896848, -0.015172698023810011, 0.15936915972565327, -0.10860464676438... |
706.2121 | Diagonalization and representation results for nonpositive sesquilinear
form measures | We study decompositions of operator measures and more general sesquilinear
form measures $E$ into linear combinations of positive parts, and their
diagonal vector expansions. The underlying philosophy is to represent $E$ as a
trace class valued measure of bounded variation on a new Hilbert space related
to $E$. The c... | math.FA | we study decompositions of operator measures and more general sesquilinear form measures e into linear combinations of positive parts and their diagonal vector expansions the underlying philosophy is to represent e as a trace class valued measure of bounded variation on a new hilbert space related to e the choice of th... | [['we', 'study', 'decompositions', 'of', 'operator', 'measures', 'and', 'more', 'general', 'sesquilinear', 'form', 'measures', 'e', 'into', 'linear', 'combinations', 'of', 'positive', 'parts', 'and', 'their', 'diagonal', 'vector', 'expansions', 'the', 'underlying', 'philosophy', 'is', 'to', 'represent', 'e', 'as', 'a',... | [-0.15044393969399122, 0.10174000003858458, -0.1068121780983255, 0.08589539768415963, -0.17347575177120256, -0.10097823452345933, 0.015100783417944479, 0.340690876616613, -0.35132409113494656, -0.17457700801329523, 0.09891663103502928, -0.25328828936702086, -0.15856052148804256, 0.1661950537958477, -0.06672567658456444... |
706.2122 | Eddy current damping of a moving domain wall: beyond the quasistatic
approximation | In conducting ferromagnetic materials, a moving domain wall induces eddy
currents in the sample which give rise to an effective retarding pressure on
the domain wall. We show here that the pressure is not just proportional to the
instantaneous velocity of the wall, as often assumed in domain wall models, but
depends ... | cond-mat.dis-nn cond-mat.mtrl-sci | in conducting ferromagnetic materials a moving domain wall induces eddy currents in the sample which give rise to an effective retarding pressure on the domain wall we show here that the pressure is not just proportional to the instantaneous velocity of the wall as often assumed in domain wall models but depends on the... | [['in', 'conducting', 'ferromagnetic', 'materials', 'a', 'moving', 'domain', 'wall', 'induces', 'eddy', 'currents', 'in', 'the', 'sample', 'which', 'give', 'rise', 'to', 'an', 'effective', 'retarding', 'pressure', 'on', 'the', 'domain', 'wall', 'we', 'show', 'here', 'that', 'the', 'pressure', 'is', 'not', 'just', 'prop... | [-0.1258638500248229, 0.17117726999417196, -0.08549987966717597, 0.027558515493741685, -0.11237946623250057, -0.04320959784008824, 0.014745243633801135, 0.3653375133463557, -0.27027491132091536, -0.31237874969251844, 0.11096492889561903, -0.2143919991999211, -0.10098691116364901, 0.196675462705459, -0.02133650624340302... |
706.2123 | Extending the abilities of the Minkowski spacetime diagram | A two-dimensional Minkowski spacetime diagram is neatly represented on a
Euclidean ordinary plane. However the Euclidean lengths of the lines on the
diagram do not correspond to the true values of physical quantities in
spacetime, except for those referring to the stationary reference frame. In
order to extend its ab... | physics.gen-ph | a twodimensional minkowski spacetime diagram is neatly represented on a euclidean ordinary plane however the euclidean lengths of the lines on the diagram do not correspond to the true values of physical quantities in spacetime except for those referring to the stationary reference frame in order to extend its abilitie... | [['a', 'twodimensional', 'minkowski', 'spacetime', 'diagram', 'is', 'neatly', 'represented', 'on', 'a', 'euclidean', 'ordinary', 'plane', 'however', 'the', 'euclidean', 'lengths', 'of', 'the', 'lines', 'on', 'the', 'diagram', 'do', 'not', 'correspond', 'to', 'the', 'true', 'values', 'of', 'physical', 'quantities', 'in'... | [-0.1004879482319219, 0.1479759856174177, -0.09292388150392901, 0.09361816753414787, -0.09806395331479348, -0.11348177573905048, 0.050697935717548, 0.3663597940875773, -0.23174123442936034, -0.27761302195824356, 0.05137658576489214, -0.24697323811747002, -0.10869782474994856, 0.18792088029460915, -0.0721848337837544, 0... |
706.2124 | Independent transversals in locally sparse graphs | Let G be a graph with maximum degree \Delta whose vertex set is partitioned
into parts V(G) = V_1 \cup ... \cup V_r. A transversal is a subset of V(G)
containing exactly one vertex from each part V_i. If it is also an independent
set, then we call it an independent transversal. The local degree of G is the
maximum nu... | math.CO | let g be a graph with maximum degree delta whose vertex set is partitioned into parts vg v_1 cup cup v_r a transversal is a subset of vg containing exactly one vertex from each part v_i if it is also an independent set then we call it an independent transversal the local degree of g is the maximum number of neighbors o... | [['let', 'g', 'be', 'a', 'graph', 'with', 'maximum', 'degree', 'delta', 'whose', 'vertex', 'set', 'is', 'partitioned', 'into', 'parts', 'vg', 'v_1', 'cup', 'cup', 'v_r', 'a', 'transversal', 'is', 'a', 'subset', 'of', 'vg', 'containing', 'exactly', 'one', 'vertex', 'from', 'each', 'part', 'v_i', 'if', 'it', 'is', 'also'... | [-0.2084276829283316, 0.14334485785372267, -0.034936853688322826, -0.04809199882591921, -0.08058816698830125, -0.1554856180382258, 0.012662643979298421, 0.36115210105224954, -0.28918601058751014, -0.23050948988728143, 0.038865836997322004, -0.3275043055028808, -0.10767704399128618, 0.1071897381942228, -0.07121648683192... |
706.2125 | Quantized vortices in $^{\bf 4}$He droplets: a quantum Monte Carlo study | We present a diffusion Monte Carlo study of a vortex line excitation attached
to the center of a $^4$He droplet at zero temperature. The vortex energy is
estimated for droplets of increasing number of atoms, from N=70 up to 300
showing a monotonous increase with $N$. The evolution of the core radius and
its associate... | cond-mat.other | we present a diffusion monte carlo study of a vortex line excitation attached to the center of a 4he droplet at zero temperature the vortex energy is estimated for droplets of increasing number of atoms from n70 up to 300 showing a monotonous increase with n the evolution of the core radius and its associated energy th... | [['we', 'present', 'a', 'diffusion', 'monte', 'carlo', 'study', 'of', 'a', 'vortex', 'line', 'excitation', 'attached', 'to', 'the', 'center', 'of', 'a', '4he', 'droplet', 'at', 'zero', 'temperature', 'the', 'vortex', 'energy', 'is', 'estimated', 'for', 'droplets', 'of', 'increasing', 'number', 'of', 'atoms', 'from', 'n... | [-0.11530548456590622, 0.21123516418971122, -0.024667598437517882, 0.01964548100833781, 0.04186683362815529, -0.10373381939250975, 0.0651132041006349, 0.3449044099077582, -0.25750984231941404, -0.33281475156545637, 0.06763470570440404, -0.3418382403999567, 0.033370624070521444, 0.15147861732169987, 0.06155486471951008,... |
706.2126 | Attenuation Regulation as a Term Rewriting System | The classical attenuation regulation of gene expression in bacteria is
considered. We propose to represent the secondary RNA structure in the leader
region of a gene or an operon by a term, and we give a probabilistic term
rewriting system modeling the whole process of such a regulation.
| q-bio.QM | the classical attenuation regulation of gene expression in bacteria is considered we propose to represent the secondary rna structure in the leader region of a gene or an operon by a term and we give a probabilistic term rewriting system modeling the whole process of such a regulation | [['the', 'classical', 'attenuation', 'regulation', 'of', 'gene', 'expression', 'in', 'bacteria', 'is', 'considered', 'we', 'propose', 'to', 'represent', 'the', 'secondary', 'rna', 'structure', 'in', 'the', 'leader', 'region', 'of', 'a', 'gene', 'or', 'an', 'operon', 'by', 'a', 'term', 'and', 'we', 'give', 'a', 'probabi... | [-0.19015027477871627, 0.04002731331547693, -0.02202951326520027, 0.10585473221624397, -0.06721730254745732, -0.1309321215376258, 0.08940089241756748, 0.31197807266532135, -0.31890586763620377, -0.24745608676069727, 0.02300145468082822, -0.22003849392058328, -0.26104816044001683, 0.11857407058414537, -0.107516293564913... |
706.2127 | Enhanced decoherence in the vicinity of a phase transition | We study the decoherence of a spin-1/2 induced by an environment which is on
the verge of a continuous phase transition. We consider spin environments
described by the ferromagnetic and antiferromagnetic Heisenberg models on a
square lattice. As is well known, these two dimensional systems undergo a
continuous phase ... | cond-mat.mes-hall | we study the decoherence of a spin12 induced by an environment which is on the verge of a continuous phase transition we consider spin environments described by the ferromagnetic and antiferromagnetic heisenberg models on a square lattice as is well known these two dimensional systems undergo a continuous phase transit... | [['we', 'study', 'the', 'decoherence', 'of', 'a', 'spin12', 'induced', 'by', 'an', 'environment', 'which', 'is', 'on', 'the', 'verge', 'of', 'a', 'continuous', 'phase', 'transition', 'we', 'consider', 'spin', 'environments', 'described', 'by', 'the', 'ferromagnetic', 'and', 'antiferromagnetic', 'heisenberg', 'models', ... | [-0.1778435068729433, 0.29182815546911883, -0.008728374826531965, 0.04394200802961527, 0.01912181096115303, -0.15019654909383903, 0.05281356467133008, 0.3583815569076145, -0.2557100149287472, -0.2051466166118648, 0.11246377690604807, -0.3078559932922854, -0.07527142345398954, 0.15003335682078472, 0.06688477079049476, 0... |
706.2128 | Stability and Formation of the Resonant System HD 73526 | Based on radial velocity measurements it has been found recently that the two
giant planets detected around the star HD 73526 are in 2:1 resonance. However,
as our numerical integration shows, the derived orbital data for this system
result in chaotic behavior of the giant planets, which is uncommon among the
resonan... | astro-ph | based on radial velocity measurements it has been found recently that the two giant planets detected around the star hd 73526 are in 21 resonance however as our numerical integration shows the derived orbital data for this system result in chaotic behavior of the giant planets which is uncommon among the resonant extra... | [['based', 'on', 'radial', 'velocity', 'measurements', 'it', 'has', 'been', 'found', 'recently', 'that', 'the', 'two', 'giant', 'planets', 'detected', 'around', 'the', 'star', 'hd', '73526', 'are', 'in', '21', 'resonance', 'however', 'as', 'our', 'numerical', 'integration', 'shows', 'the', 'derived', 'orbital', 'data',... | [-0.1819079570358302, 0.081587598227123, -0.0991923609233283, 0.04510976193015906, -0.06593575665053535, -0.10536212272040467, 0.012540657180262373, 0.3328493376797501, -0.17967200832282926, -0.28966462402703597, 0.09804409584575431, -0.261168415503616, -0.14301408185782108, 0.2040157066093401, -0.03421089716374557, 0.... |
706.2129 | Two-twistor Description of Membrane | We describe D=4 twistorial membrane in terms of two twistorial
three-dimensional world volume fields. We start with the D-dimensional p-brane
generalizations of two phase space string formulations: the one with $p+1$
vectorial fourmomenta, and the second with tensorial momenta of $(p+1)$-th
rank. Further we consider ... | hep-th | we describe d4 twistorial membrane in terms of two twistorial threedimensional world volume fields we start with the ddimensional pbrane generalizations of two phase space string formulations the one with p1 vectorial fourmomenta and the second with tensorial momenta of p1th rank further we consider tensionful membrane... | [['we', 'describe', 'd4', 'twistorial', 'membrane', 'in', 'terms', 'of', 'two', 'twistorial', 'threedimensional', 'world', 'volume', 'fields', 'we', 'start', 'with', 'the', 'ddimensional', 'pbrane', 'generalizations', 'of', 'two', 'phase', 'space', 'string', 'formulations', 'the', 'one', 'with', 'p1', 'vectorial', 'fou... | [-0.16199727488697327, 0.17346759361974082, -0.0339984416574271, 0.07280715256479389, -0.10355587853431827, -0.12581162961951198, -0.059899751208487804, 0.3081329985631301, -0.18271155870605668, -0.23454354373941652, 0.05378400455052894, -0.23654719728569523, -0.2199961330287722, 0.13207646588474012, -0.097050321032097... |
706.213 | Progress on neural parton distributions | We give a status report on the determination of a set of parton distributions
based on neural networks. In particular, we summarize the determination of the
nonsinglet quark distribution up to NNLO, we compare it with results obtained
using other approaches, and we discuss its use for a determination of
$\alpha_s$.
| hep-ph | we give a status report on the determination of a set of parton distributions based on neural networks in particular we summarize the determination of the nonsinglet quark distribution up to nnlo we compare it with results obtained using other approaches and we discuss its use for a determination of alpha_s | [['we', 'give', 'a', 'status', 'report', 'on', 'the', 'determination', 'of', 'a', 'set', 'of', 'parton', 'distributions', 'based', 'on', 'neural', 'networks', 'in', 'particular', 'we', 'summarize', 'the', 'determination', 'of', 'the', 'nonsinglet', 'quark', 'distribution', 'up', 'to', 'nnlo', 'we', 'compare', 'it', 'wi... | [-0.05933828646426692, 0.06399038906081342, -0.11895767363774426, 0.03790735296320682, -0.06420780400581219, -0.027380896403509027, 0.09485114099202203, 0.4095121883586341, -0.14498466487024345, -0.25626759720491427, 0.07442455148716987, -0.28713276089333434, -0.06973041816815442, 0.1845010126046106, 0.0122500718845164... |
706.2131 | Parton Distributions for LO Calculations | We present a study of the results obtained combining LO partonic matrix
elements with different orders of partons distributions. These are compared to
the best prediction using NLO for both matrix elements and parton
distributions. The aim is to determine which parton distributions are most
appropriate to use in thos... | hep-ph | we present a study of the results obtained combining lo partonic matrix elements with different orders of partons distributions these are compared to the best prediction using nlo for both matrix elements and parton distributions the aim is to determine which parton distributions are most appropriate to use in those ca... | [['we', 'present', 'a', 'study', 'of', 'the', 'results', 'obtained', 'combining', 'lo', 'partonic', 'matrix', 'elements', 'with', 'different', 'orders', 'of', 'partons', 'distributions', 'these', 'are', 'compared', 'to', 'the', 'best', 'prediction', 'using', 'nlo', 'for', 'both', 'matrix', 'elements', 'and', 'parton', ... | [-0.023738977453314963, 0.17468183554915917, -0.11442505355843884, 0.14254896624738145, -0.024214856711756667, -0.038364760784639254, -0.03184935822220588, 0.46682046530883253, -0.178831481583198, -0.2645908715893273, 0.057368898991334405, -0.3620147175718973, -0.03325679937354577, 0.11105812032833512, 0.01436783880409... |
706.2132 | Neutrino Masses and Mixings from String Theory Instantons | We study possible patterns of neutrino masses and mixings in string models in
which Majorana neutrino masses are generated by a certain class of string
theory instantons recently considered in the literature. These instantons may
generate either directly the dim=5 Weinberg operator or right-handed neutrino
Majorana m... | hep-ph hep-th | we study possible patterns of neutrino masses and mixings in string models in which majorana neutrino masses are generated by a certain class of string theory instantons recently considered in the literature these instantons may generate either directly the dim5 weinberg operator or righthanded neutrino majorana masses... | [['we', 'study', 'possible', 'patterns', 'of', 'neutrino', 'masses', 'and', 'mixings', 'in', 'string', 'models', 'in', 'which', 'majorana', 'neutrino', 'masses', 'are', 'generated', 'by', 'a', 'certain', 'class', 'of', 'string', 'theory', 'instantons', 'recently', 'considered', 'in', 'the', 'literature', 'these', 'inst... | [-0.15834707752762014, 0.36291705369081156, -0.0024030573145186495, 0.22487096519454114, -0.07602673532220267, -0.15316984001389247, 0.04231528485474035, 0.31736138404023406, -0.19624942089667766, -0.25424834495505033, 0.03356254846449563, -0.2676896175716893, -0.12121425101373708, 0.15135822826167727, 0.03000967177736... |
706.2133 | Boson-Fermion pairing in Bose-Fermi mixtures on 1D optical lattices | Boson-fermion pairing is considered in a discrete environment of bosons and
fully spin-polarized fermions, coupled via an attractive Bose-Fermi Hubbard
Hamiltonian in one dimension. The results of the T-matrix approximation for
particles of equal mass and at double half filling are compared with the
results of exact ... | cond-mat.other nucl-th | bosonfermion pairing is considered in a discrete environment of bosons and fully spinpolarized fermions coupled via an attractive bosefermi hubbard hamiltonian in one dimension the results of the tmatrix approximation for particles of equal mass and at double half filling are compared with the results of exact diagonal... | [['bosonfermion', 'pairing', 'is', 'considered', 'in', 'a', 'discrete', 'environment', 'of', 'bosons', 'and', 'fully', 'spinpolarized', 'fermions', 'coupled', 'via', 'an', 'attractive', 'bosefermi', 'hubbard', 'hamiltonian', 'in', 'one', 'dimension', 'the', 'results', 'of', 'the', 'tmatrix', 'approximation', 'for', 'pa... | [-0.1364542591618374, 0.20191285564073447, -0.06250833498583258, 0.125662636319046, 0.01599942178129115, -0.20493827978174928, 0.052177853969624266, 0.3538745934686934, -0.1598020565143088, -0.22279167625432214, -0.006636184601423641, -0.33045311163490015, -0.0826561350938088, 0.17558817913393593, 0.08236225133037402, ... |
706.2134 | Rotational stacking and its electronic effects on graphene films grown
on 4H-SiC$(000\bar{1})$ | We examine the stacking order of multilayer graphene grown on the
SiC$(000\bar{1})$ surface using low-energy electron diffraction and surface
X-ray diffraction. We show that the films contain a high density of rotational
stacking faults caused by three types of rotated graphene: sheets rotated
$30^\circ$ and $\pm 2.2... | cond-mat.mtrl-sci | we examine the stacking order of multilayer graphene grown on the sic000bar1 surface using lowenergy electron diffraction and surface xray diffraction we show that the films contain a high density of rotational stacking faults caused by three types of rotated graphene sheets rotated 30circ and pm 220circ relative to th... | [['we', 'examine', 'the', 'stacking', 'order', 'of', 'multilayer', 'graphene', 'grown', 'on', 'the', 'sic000bar1', 'surface', 'using', 'lowenergy', 'electron', 'diffraction', 'and', 'surface', 'xray', 'diffraction', 'we', 'show', 'that', 'the', 'films', 'contain', 'a', 'high', 'density', 'of', 'rotational', 'stacking',... | [-0.19241266531337584, 0.17199335278876657, -0.02069093560982895, -0.04907803401459075, 0.028207925771961788, -0.14310172304976732, 0.1000331568814415, 0.48880539555102587, -0.30795201818026335, -0.30266970502478735, -0.01579625054780211, -0.34148191374593545, -0.15757100343138777, 0.12551833751370264, 0.05183888236310... |
706.2135 | Universality of the REM for dynamics of mean-field spin glasses | We consider a version of a Glauber dynamics for a p-spin
Sherrington--Kirkpatrick model of a spin glass that can be seen as a time
change of simple random walk on the N-dimensional hypercube. We show that, for
any p>2 and any inverse temperature \beta>0, there exist constants g>0, such
that for all exponential time s... | math.PR cond-mat.dis-nn | we consider a version of a glauber dynamics for a pspin sherringtonkirkpatrick model of a spin glass that can be seen as a time change of simple random walk on the ndimensional hypercube we show that for any p2 and any inverse temperature beta0 there exist constants g0 such that for all exponential time scales expgamma... | [['we', 'consider', 'a', 'version', 'of', 'a', 'glauber', 'dynamics', 'for', 'a', 'pspin', 'sherringtonkirkpatrick', 'model', 'of', 'a', 'spin', 'glass', 'that', 'can', 'be', 'seen', 'as', 'a', 'time', 'change', 'of', 'simple', 'random', 'walk', 'on', 'the', 'ndimensional', 'hypercube', 'we', 'show', 'that', 'for', 'an... | [-0.09155708405137794, 0.2054338316681139, -0.12358596110845019, 0.08451924306220261, -0.013874631989290195, -0.1824361920396746, 0.005892280627761973, 0.384984185302093, -0.28268652128204247, -0.22451761850881521, 0.08584763639623676, -0.2528641227964152, -0.09646225974186569, 0.17024543231954523, -0.00379317709704735... |
706.2136 | Factorization analysis for the fragmentation functions of hadrons
containing a heavy quark | Using methods of effective field theory, a systematic analysis of the
fragmentation functions D_{a/H}(x,m_Q) of a hadron H containing a heavy quark Q
is performed (with a=Q,Q_bar,q,q_bar,g). By integrating out pair production of
virtual and real heavy quarks, the fragmentation functions are matched onto a
single nonp... | hep-ph | using methods of effective field theory a systematic analysis of the fragmentation functions d_ahxm_q of a hadron h containing a heavy quark q is performed with aqq_barqq_barg by integrating out pair production of virtual and real heavy quarks the fragmentation functions are matched onto a single nonperturbative functi... | [['using', 'methods', 'of', 'effective', 'field', 'theory', 'a', 'systematic', 'analysis', 'of', 'the', 'fragmentation', 'functions', 'd_ahxm_q', 'of', 'a', 'hadron', 'h', 'containing', 'a', 'heavy', 'quark', 'q', 'is', 'performed', 'with', 'aqq_barqq_barg', 'by', 'integrating', 'out', 'pair', 'production', 'of', 'virt... | [-0.08221110685248456, 0.19820312411742813, -0.14535039827733495, 0.10008490684781407, -0.018198582363878318, -0.0633679605304712, 0.017463451558954003, 0.35156801406777016, -0.23911605116531806, -0.22440034248233762, 0.01063511372661724, -0.2991913438934177, -0.04124216962875913, 0.12018489718069265, 0.057516759006381... |
706.2137 | The broadband spectrum of Cygnus X-1 | The Black Hole (BH) binary Cygnus X-1 has been observed simultaneously by
INTEGRAL, RXTE, and XMM-Newton for four times in November and December 2004,
when Cyg X-1 became first observable with XMM-Newton. During these observations
the source was found in one of its transitional states between the hard state
and the s... | astro-ph | the black hole bh binary cygnus x1 has been observed simultaneously by integral rxte and xmmnewton for four times in november and december 2004 when cyg x1 became first observable with xmmnewton during these observations the source was found in one of its transitional states between the hard state and the soft state we... | [['the', 'black', 'hole', 'bh', 'binary', 'cygnus', 'x1', 'has', 'been', 'observed', 'simultaneously', 'by', 'integral', 'rxte', 'and', 'xmmnewton', 'for', 'four', 'times', 'in', 'november', 'and', 'december', '2004', 'when', 'cyg', 'x1', 'became', 'first', 'observable', 'with', 'xmmnewton', 'during', 'these', 'observa... | [-0.023884324157644098, 0.09359074054025784, -0.08334417933145084, 0.07912647305895482, -0.10169946560389698, -0.16403234570270386, 0.06606944307248604, 0.4542583881768289, -0.1634384873616803, -0.3670722282416112, 0.10775188708820523, -0.36397054704414317, 0.0031189741839461765, 0.19938297336501581, -0.026697247859661... |
706.2138 | Magnetic patterning of (Ga,Mn)As by hydrogen passivation | We present an original method to magnetically pattern thin layers of
(Ga,Mn)As. It relies on local hydrogen passivation to significantly lower the
hole density, and thereby locally suppress the carrier-mediated ferromagnetic
phase. The sample surface is thus maintained continuous, and the minimal
structure size is of... | cond-mat.mtrl-sci | we present an original method to magnetically pattern thin layers of gamnas it relies on local hydrogen passivation to significantly lower the hole density and thereby locally suppress the carriermediated ferromagnetic phase the sample surface is thus maintained continuous and the minimal structure size is of about 200... | [['we', 'present', 'an', 'original', 'method', 'to', 'magnetically', 'pattern', 'thin', 'layers', 'of', 'gamnas', 'it', 'relies', 'on', 'local', 'hydrogen', 'passivation', 'to', 'significantly', 'lower', 'the', 'hole', 'density', 'and', 'thereby', 'locally', 'suppress', 'the', 'carriermediated', 'ferromagnetic', 'phase... | [-0.08664421672455785, 0.1952411511576828, 0.008029817535382946, -0.041804542887115444, -0.015119294647309111, -0.15780150138477728, 0.07718473817108244, 0.4719715991863845, -0.2910453969862585, -0.3233416145667434, 0.035107451739505205, -0.25784261776815826, -0.01505086275680763, 0.18145334939813104, -0.01849471693631... |
706.2139 | Spectral type dependent rotational braking and strong magnetic flux in
three components of the late-M multiple system LHS 1070 | We show individual high resolution spectra of components A, B, and C of the
nearby late-M type multiple system LHS 1070. Component A is a mid-M star, B and
C are known to have masses at the threshold to brown dwarfs. From our spectra
we measure rotation velocities and the mean magnetic field for all three
components ... | astro-ph | we show individual high resolution spectra of components a b and c of the nearby latem type multiple system lhs 1070 component a is a midm star b and c are known to have masses at the threshold to brown dwarfs from our spectra we measure rotation velocities and the mean magnetic field for all three components individua... | [['we', 'show', 'individual', 'high', 'resolution', 'spectra', 'of', 'components', 'a', 'b', 'and', 'c', 'of', 'the', 'nearby', 'latem', 'type', 'multiple', 'system', 'lhs', '1070', 'component', 'a', 'is', 'a', 'midm', 'star', 'b', 'and', 'c', 'are', 'known', 'to', 'have', 'masses', 'at', 'the', 'threshold', 'to', 'bro... | [-0.15334855172109638, 0.1807546920371952, -0.020495138671722705, 0.06709332691800207, -0.10267917931969094, -0.09046332395009402, 0.04267684972218874, 0.40902913643815425, -0.19999573708348775, -0.35893885451921465, 0.05676114906906808, -0.25006459340437365, -0.02823501161041822, 0.1950434588821931, -0.053574285217387... |
706.214 | Multifractality in stock indexes: Fact or fiction? | Multifractal analysis and extensive statistical tests are performed upon
intraday minutely data within individual trading days for four stock market
indexes (including HSI, SZSC, S&P500, and NASDAQ) to check whether the indexes
(instead of the returns) possess multifractality. We find that the mass
exponent $\tau(q)$... | q-fin.ST physics.soc-ph | multifractal analysis and extensive statistical tests are performed upon intraday minutely data within individual trading days for four stock market indexes including hsi szsc sp500 and nasdaq to check whether the indexes instead of the returns possess multifractality we find that the mass exponent tauq is linear and t... | [['multifractal', 'analysis', 'and', 'extensive', 'statistical', 'tests', 'are', 'performed', 'upon', 'intraday', 'minutely', 'data', 'within', 'individual', 'trading', 'days', 'for', 'four', 'stock', 'market', 'indexes', 'including', 'hsi', 'szsc', 'sp500', 'and', 'nasdaq', 'to', 'check', 'whether', 'the', 'indexes', ... | [-0.06711053691048285, 0.10968322701199501, -0.18249674315684208, 0.17795159693433912, -0.05211483798967213, -0.1456026945004959, 0.0952512187385323, 0.4278430857944607, -0.272027459788588, -0.2908050065478633, 0.17501059797302, -0.388931288891057, -0.13646749514016773, 0.21187216369896242, -0.055662171982025895, 0.022... |
706.2141 | Large deviations and Chernoff bound for certain correlated states on a
spin chain | In this paper we extend the results of Lenci and Rey-Bellet on the large
deviation upper bound of the distribution measures of local Hamiltonians with
respect to a Gibbs state, in the setting of translation-invariant finite-range
interactions. We show that a certain factorization property of the reference
state is su... | math-ph math.MP quant-ph | in this paper we extend the results of lenci and reybellet on the large deviation upper bound of the distribution measures of local hamiltonians with respect to a gibbs state in the setting of translationinvariant finiterange interactions we show that a certain factorization property of the reference state is sufficien... | [['in', 'this', 'paper', 'we', 'extend', 'the', 'results', 'of', 'lenci', 'and', 'reybellet', 'on', 'the', 'large', 'deviation', 'upper', 'bound', 'of', 'the', 'distribution', 'measures', 'of', 'local', 'hamiltonians', 'with', 'respect', 'to', 'a', 'gibbs', 'state', 'in', 'the', 'setting', 'of', 'translationinvariant',... | [-0.10968940762386685, 0.16958805349162448, -0.13014199469233229, 0.12128746783480782, 0.02056180972210837, -0.11940786967787778, 0.046480042939286, 0.3185959500247422, -0.2902176971229809, -0.24598082670479815, 0.08598050784944049, -0.29178902592199546, -0.08572486297326219, 0.1738357869943491, -0.059050980898918526, ... |
706.2142 | Path Integral for Quantum Operations | In this paper we consider a phase space path integral for general
time-dependent quantum operations, not necessarily unitary. We obtain the path
integral for a completely positive quantum operation satisfied Lindblad
equation (quantum Markovian master equation). We consider the path integral for
quantum operation wit... | quant-ph | in this paper we consider a phase space path integral for general timedependent quantum operations not necessarily unitary we obtain the path integral for a completely positive quantum operation satisfied lindblad equation quantum markovian master equation we consider the path integral for quantum operation with a simp... | [['in', 'this', 'paper', 'we', 'consider', 'a', 'phase', 'space', 'path', 'integral', 'for', 'general', 'timedependent', 'quantum', 'operations', 'not', 'necessarily', 'unitary', 'we', 'obtain', 'the', 'path', 'integral', 'for', 'a', 'completely', 'positive', 'quantum', 'operation', 'satisfied', 'lindblad', 'equation',... | [-0.21139397525361606, 0.15967306238123957, -0.10704212863834536, 0.055886215499450206, -0.11154307618889274, -0.19574513481169634, 0.04433600991555699, 0.3688843971764555, -0.31778702504780826, -0.1351216668073012, 0.06845754076850277, -0.20429872531367807, -0.20159892076436353, 0.22172426949350202, -0.090518578677913... |
706.2143 | Single electron-spin memory with a semiconductor quantum dot | We show storage of the circular polarisation of an optical field,
transferring it to the spin-state of an individual electron confined in a
single semiconductor quantum dot. The state is subsequently readout through the
electronically-triggered emission of a single photon. The emitted photon shares
the same polarisat... | quant-ph | we show storage of the circular polarisation of an optical field transferring it to the spinstate of an individual electron confined in a single semiconductor quantum dot the state is subsequently readout through the electronicallytriggered emission of a single photon the emitted photon shares the same polarisation as ... | [['we', 'show', 'storage', 'of', 'the', 'circular', 'polarisation', 'of', 'an', 'optical', 'field', 'transferring', 'it', 'to', 'the', 'spinstate', 'of', 'an', 'individual', 'electron', 'confined', 'in', 'a', 'single', 'semiconductor', 'quantum', 'dot', 'the', 'state', 'is', 'subsequently', 'readout', 'through', 'the',... | [-0.13585017797709809, 0.21867403329341553, -0.03192702934062213, 0.01676148979426257, 0.027897992192275737, -0.17122641480475498, 0.001049228028258246, 0.42204692256584597, -0.27992694159404613, -0.3254005146118697, 0.02373633043333009, -0.28824051294025826, 0.038476550679528314, 0.23157349931013382, 0.036783987133020... |
706.2144 | The role of the cotangent bundle in resolving ideals of fat points in
the plane | We study the connection between the generation of a fat point scheme
supported at general points in the plane and the behaviour of the cotangent
bundle with respect to some rational curves particularly relevant for the
scheme. We put forward two conjectures, giving examples and partial results in
support of them.
| math.AG | we study the connection between the generation of a fat point scheme supported at general points in the plane and the behaviour of the cotangent bundle with respect to some rational curves particularly relevant for the scheme we put forward two conjectures giving examples and partial results in support of them | [['we', 'study', 'the', 'connection', 'between', 'the', 'generation', 'of', 'a', 'fat', 'point', 'scheme', 'supported', 'at', 'general', 'points', 'in', 'the', 'plane', 'and', 'the', 'behaviour', 'of', 'the', 'cotangent', 'bundle', 'with', 'respect', 'to', 'some', 'rational', 'curves', 'particularly', 'relevant', 'for'... | [-0.19370176150080035, 0.010325310030477304, -0.09126001641190812, 0.07227959934914228, -0.09069915948545232, -0.13416506429476774, 0.10564186630368817, 0.378872071703275, -0.2640624479116762, -0.20441339690553242, 0.10221515999029518, -0.28884657308934075, -0.17319544442180618, 0.2638430109284088, -0.05374885666385001... |
706.2145 | Prompt muons in extended air showers | We present results of simulations of a muon content in the air showers
induced by very high energy cosmic rays. Muon energy distributions and muon
densities at ground level are given. We discuss a prompt muon component
generated by decays of charm mesons. The method combines standard Monte Carlo
generators incorporat... | astro-ph | we present results of simulations of a muon content in the air showers induced by very high energy cosmic rays muon energy distributions and muon densities at ground level are given we discuss a prompt muon component generated by decays of charm mesons the method combines standard monte carlo generators incorporated in... | [['we', 'present', 'results', 'of', 'simulations', 'of', 'a', 'muon', 'content', 'in', 'the', 'air', 'showers', 'induced', 'by', 'very', 'high', 'energy', 'cosmic', 'rays', 'muon', 'energy', 'distributions', 'and', 'muon', 'densities', 'at', 'ground', 'level', 'are', 'given', 'we', 'discuss', 'a', 'prompt', 'muon', 'co... | [-0.025353350736681494, 0.30372531329386776, -0.05481840126524349, 0.22127441154612648, 0.012534062077681865, -0.0248134454952613, 0.0012440744152803335, 0.391424962830159, -0.19552583475747415, -0.3121515771734618, -0.05616392553107993, -0.40207342381378813, 0.11865331747779442, 0.17272033485313576, 0.0787551525018868... |
706.2146 | Efficient Multidimensional Data Redistribution for Resizable Parallel
Computations | Traditional parallel schedulers running on cluster supercomputers support
only static scheduling, where the number of processors allocated to an
application remains fixed throughout the execution of the job. This results in
under-utilization of idle system resources thereby decreasing overall system
throughput. In ou... | cs.DC | traditional parallel schedulers running on cluster supercomputers support only static scheduling where the number of processors allocated to an application remains fixed throughout the execution of the job this results in underutilization of idle system resources thereby decreasing overall system throughput in our rese... | [['traditional', 'parallel', 'schedulers', 'running', 'on', 'cluster', 'supercomputers', 'support', 'only', 'static', 'scheduling', 'where', 'the', 'number', 'of', 'processors', 'allocated', 'to', 'an', 'application', 'remains', 'fixed', 'throughout', 'the', 'execution', 'of', 'the', 'job', 'this', 'results', 'in', 'un... | [-0.22455983012212977, 0.10279071755082927, -0.040657150300781, -0.026831600009718886, -0.0754250496201702, -0.2125903195414488, 0.12935162387383234, 0.42365933194348254, -0.29623507748019867, -0.34734026918009125, 0.06993659813043164, -0.237322879183323, -0.07334556077823859, 0.18747727349177257, -0.08504609384395387,... |
706.2147 | Replica Condensation and Tree Decay | We give an intuitive method--using local, cyclic replica symmetry--to isolate
exponential tree decay in truncated (connected) correlations. We give an
expansion and use the symmetry to show that all terms vanish, except those
displaying {\em replica condensation}. The condensation property ensures
exponential tree de... | math-ph hep-th math.MP | we give an intuitive methodusing local cyclic replica symmetryto isolate exponential tree decay in truncated connected correlations we give an expansion and use the symmetry to show that all terms vanish except those displaying em replica condensation the condensation property ensures exponential tree decay we illustra... | [['we', 'give', 'an', 'intuitive', 'methodusing', 'local', 'cyclic', 'replica', 'symmetryto', 'isolate', 'exponential', 'tree', 'decay', 'in', 'truncated', 'connected', 'correlations', 'we', 'give', 'an', 'expansion', 'and', 'use', 'the', 'symmetry', 'to', 'show', 'that', 'all', 'terms', 'vanish', 'except', 'those', 'd... | [-0.1470079253783778, 0.18032473093360965, -0.135571826769806, 0.13268793083946495, -0.062245535806697956, -0.16158299487741554, 0.04961829202742699, 0.36348759710569595, -0.25144753762904337, -0.22457715143613954, 0.07688685107346185, -0.26101607960813183, -0.16411285386763183, 0.14635399682721234, -0.0012966262067065... |
706.2148 | High-harmonic generation in diatomic molecules: a quantum-orbit analysis
of the interference patterns | We perform a detailed analysis of high-order harmonic generation in diatomic
molecules within the strong-field approximation, with emphasis on
quantum-interference effects. Specifically, we investigate how the different
types of electron orbits, involving one or two centers, affect the interference
patterns in the sp... | physics.atom-ph | we perform a detailed analysis of highorder harmonic generation in diatomic molecules within the strongfield approximation with emphasis on quantuminterference effects specifically we investigate how the different types of electron orbits involving one or two centers affect the interference patterns in the spectra we a... | [['we', 'perform', 'a', 'detailed', 'analysis', 'of', 'highorder', 'harmonic', 'generation', 'in', 'diatomic', 'molecules', 'within', 'the', 'strongfield', 'approximation', 'with', 'emphasis', 'on', 'quantuminterference', 'effects', 'specifically', 'we', 'investigate', 'how', 'the', 'different', 'types', 'of', 'electro... | [-0.11723961787234244, 0.16737434558950448, -0.08600181091318548, 0.11850911710448485, -0.014916275052682441, -0.11952476316922102, 0.06705520201930307, 0.3713395129106626, -0.23516155069913058, -0.3116962048107711, 0.06672047242128971, -0.2871644891497186, -0.12937616440947505, 0.18073197595771215, -0.0034489828336029... |
706.2149 | A New Comment on "Experimental Observation of Optical Rotation Generated
in Vacuum by a Magnetic Field" | One of the magneto-optical properties of the mirrors of the Fabry-Perot
cavity used for the experiment is considered as a possible origin of the PVLAS
measurement result.
| hep-ex | one of the magnetooptical properties of the mirrors of the fabryperot cavity used for the experiment is considered as a possible origin of the pvlas measurement result | [['one', 'of', 'the', 'magnetooptical', 'properties', 'of', 'the', 'mirrors', 'of', 'the', 'fabryperot', 'cavity', 'used', 'for', 'the', 'experiment', 'is', 'considered', 'as', 'a', 'possible', 'origin', 'of', 'the', 'pvlas', 'measurement', 'result']] | [-0.12970414254124518, 0.08823039179184923, -0.10286990235801097, 0.014651265879230643, -0.03223461902665871, -0.13950954224155457, 0.024411632959661936, 0.32670567626202546, -0.21163487972484696, -0.2964936769394963, 0.0770631621212319, -0.25237465891297217, -0.08159468267802839, 0.2781232711341646, -0.016836927030925... |
706.215 | The polar ring galaxy AM1934-563 revisited | We report long-slit spectroscopic observations of the dust-lane polar-ring
galaxy AM1934-563 obtained with the Southern African Large Telescope (SALT)
during its performance-verification phase. The observations target the spectral
region of the Ha, [NII] and [SII] emission-lines, but show also deep NaI
stellar absorp... | astro-ph | we report longslit spectroscopic observations of the dustlane polarring galaxy am1934563 obtained with the southern african large telescope salt during its performanceverification phase the observations target the spectral region of the ha nii and sii emissionlines but show also deep nai stellar absorption lines that w... | [['we', 'report', 'longslit', 'spectroscopic', 'observations', 'of', 'the', 'dustlane', 'polarring', 'galaxy', 'am1934563', 'obtained', 'with', 'the', 'southern', 'african', 'large', 'telescope', 'salt', 'during', 'its', 'performanceverification', 'phase', 'the', 'observations', 'target', 'the', 'spectral', 'region', '... | [-0.07510617920724809, 0.05252129107881014, -0.07934828224328802, 0.07653258445269674, -0.09908893531618532, -0.06161398658395281, 0.024250167309235564, 0.44717365951014204, -0.181168666200278, -0.2913916388676907, 0.07524441139544924, -0.26927801970425874, -0.06919638107159079, 0.18324435062888142, -0.0356728589286737... |
706.2151 | Nonlocal Cosmology | We explore nonlocally modified models of gravity, inspired by quantum loop
corrections, as a mechanism for explaining current cosmic acceleration. These
theories enjoy two major advantages: they allow a delayed response to cosmic
events, here the transition from radiation to matter dominance, and they avoid
the usual... | astro-ph gr-qc hep-th | we explore nonlocally modified models of gravity inspired by quantum loop corrections as a mechanism for explaining current cosmic acceleration these theories enjoy two major advantages they allow a delayed response to cosmic events here the transition from radiation to matter dominance and they avoid the usual level o... | [['we', 'explore', 'nonlocally', 'modified', 'models', 'of', 'gravity', 'inspired', 'by', 'quantum', 'loop', 'corrections', 'as', 'a', 'mechanism', 'for', 'explaining', 'current', 'cosmic', 'acceleration', 'these', 'theories', 'enjoy', 'two', 'major', 'advantages', 'they', 'allow', 'a', 'delayed', 'response', 'to', 'co... | [-0.13854726449969937, 0.2129495908780133, -0.06620154672247522, 0.19557805483551313, -0.10887808102895231, -0.16377964870565953, 0.027365764655063258, 0.30882504722651316, -0.29309265334159135, -0.3554891883450396, 0.06399393043179503, -0.2608597929972936, -0.10419265176443493, 0.17811879193519844, -0.0537511751220068... |
706.2152 | On elliptic Dunkl operators | We attach elliptic Dunkl operators to an abelian variety with a finite group
action. This generalizes elliptic Dunkl operators for Weyl groups, defined by
Buchstaber, Felder, and Veselov in 1994. We show that these operators commute,
and use them to define representations from category O of elliptic Cherednik
algebra... | math.QA math.RT | we attach elliptic dunkl operators to an abelian variety with a finite group action this generalizes elliptic dunkl operators for weyl groups defined by buchstaber felder and veselov in 1994 we show that these operators commute and use them to define representations from category o of elliptic cherednik algebras we als... | [['we', 'attach', 'elliptic', 'dunkl', 'operators', 'to', 'an', 'abelian', 'variety', 'with', 'a', 'finite', 'group', 'action', 'this', 'generalizes', 'elliptic', 'dunkl', 'operators', 'for', 'weyl', 'groups', 'defined', 'by', 'buchstaber', 'felder', 'and', 'veselov', 'in', '1994', 'we', 'show', 'that', 'these', 'opera... | [-0.14724258287483222, 0.09836521142666219, -0.08874068387433307, 0.06653268717973215, -0.16555486689624074, -0.17583075962210823, -0.0816485621518903, 0.34392027897977984, -0.3881880519246416, -0.14295489310782838, 0.06418232449070345, -0.3005199406852389, -0.1768289523731385, 0.18525504205956475, -0.22475426154235353... |
706.2153 | Stability of boundary measures | We introduce the boundary measure at scale r of a compact subset of the
n-dimensional Euclidean space. We show how it can be computed for point clouds
and suggest these measures can be used for feature detection. The main
contribution of this work is the proof a quantitative stability theorem for
boundary measures us... | cs.CG math.CA math.MG | we introduce the boundary measure at scale r of a compact subset of the ndimensional euclidean space we show how it can be computed for point clouds and suggest these measures can be used for feature detection the main contribution of this work is the proof a quantitative stability theorem for boundary measures using t... | [['we', 'introduce', 'the', 'boundary', 'measure', 'at', 'scale', 'r', 'of', 'a', 'compact', 'subset', 'of', 'the', 'ndimensional', 'euclidean', 'space', 'we', 'show', 'how', 'it', 'can', 'be', 'computed', 'for', 'point', 'clouds', 'and', 'suggest', 'these', 'measures', 'can', 'be', 'used', 'for', 'feature', 'detection... | [-0.0841584106875134, 0.03820327487399523, -0.18346732780444383, 0.10433943892946873, -0.05120186004573586, -0.0909773255725145, 0.05163257920595379, 0.35400437111912786, -0.2764677509515621, -0.2517697860797246, 0.15450733326289845, -0.2483536981410165, -0.15588103418891458, 0.22568941732932782, -0.10908053460498822, ... |
706.2154 | Vector invariants of a class of pseudo-reflection groups and
multisymmetric syzygies | First and second fundamental theorems are given for polynomial invariants of
a class of pseudo-reflection groups (including the Weyl groups of type $B_n$),
under the assumption that the order of the group is invertible in the base
field. Special case of the result is a finite presentation of the algebra of
multisymme... | math.RT math.AG | first and second fundamental theorems are given for polynomial invariants of a class of pseudoreflection groups including the weyl groups of type b_n under the assumption that the order of the group is invertible in the base field special case of the result is a finite presentation of the algebra of multisymmetric poly... | [['first', 'and', 'second', 'fundamental', 'theorems', 'are', 'given', 'for', 'polynomial', 'invariants', 'of', 'a', 'class', 'of', 'pseudoreflection', 'groups', 'including', 'the', 'weyl', 'groups', 'of', 'type', 'b_n', 'under', 'the', 'assumption', 'that', 'the', 'order', 'of', 'the', 'group', 'is', 'invertible', 'in... | [-0.24202255773554116, 0.08145251834790351, -0.08783956099987815, 0.013526061077994344, -0.0882809484303978, -0.11631529994529526, -0.01862660768490873, 0.2728579150831425, -0.3295334046706557, -0.18100742767197325, 0.12114006252254751, -0.19998355349832164, -0.14474343449048893, 0.21280239995164602, -0.102277868096471... |
706.2155 | Dualheap Selection Algorithm: Efficient, Inherently Parallel and
Somewhat Mysterious | An inherently parallel algorithm is proposed that efficiently performs
selection: finding the K-th largest member of a set of N members. Selection is
a common component of many more complex algorithms and therefore is a widely
studied problem.
Not much is new in the proposed dualheap selection algorithm: the heap d... | cs.DS cs.CC cs.DC | an inherently parallel algorithm is proposed that efficiently performs selection finding the kth largest member of a set of n members selection is a common component of many more complex algorithms and therefore is a widely studied problem not much is new in the proposed dualheap selection algorithm the heap data struc... | [['an', 'inherently', 'parallel', 'algorithm', 'is', 'proposed', 'that', 'efficiently', 'performs', 'selection', 'finding', 'the', 'kth', 'largest', 'member', 'of', 'a', 'set', 'of', 'n', 'members', 'selection', 'is', 'a', 'common', 'component', 'of', 'many', 'more', 'complex', 'algorithms', 'and', 'therefore', 'is', '... | [-0.12197631486008408, 0.0781653646249259, -0.11523795039345733, 0.0567560512631621, -0.1402187673989589, -0.20380217215131383, 0.07966544999041344, 0.3889402616142678, -0.2802443797960121, -0.3400725070921926, 0.10850806297943573, -0.25392296471335185, -0.1138236670693392, 0.16745164089831452, -0.09487760690783108, 0.... |
706.2156 | Direct CP Violation in B Decays | We discuss several aspects of direct CP asymmetries in B decays, which are
very useful in spite of hadronic uncertainties in asymmetry calculations. 1)
Asymmetries in decays to $D^{(*)}K^{(*)}$, $\pi^+\pi^-, \rho^+\rho^-$,
providing precision tests for the CKM phase $\gamma$. 2) Null tests in $B^+\to
J/\psi K^+, \pi^... | hep-ph hep-ex | we discuss several aspects of direct cp asymmetries in b decays which are very useful in spite of hadronic uncertainties in asymmetry calculations 1 asymmetries in decays to dk pipi rhorho providing precision tests for the ckm phase gamma 2 null tests in bto jpsi k pipi0 where a nonzero asymmetry provides evidence for ... | [['we', 'discuss', 'several', 'aspects', 'of', 'direct', 'cp', 'asymmetries', 'in', 'b', 'decays', 'which', 'are', 'very', 'useful', 'in', 'spite', 'of', 'hadronic', 'uncertainties', 'in', 'asymmetry', 'calculations', '1', 'asymmetries', 'in', 'decays', 'to', 'dk', 'pipi', 'rhorho', 'providing', 'precision', 'tests', '... | [-0.14511295307589614, 0.2397364032090358, -0.061630478472975286, 0.14616436878948108, -0.0742261693569953, -0.1711403689711638, 0.13290486819131056, 0.22034336426497803, -0.19745151661336421, -0.1881589110292818, -0.05877617116430369, -0.34955467604829565, 0.011727214130856421, 0.11973641207036764, 0.14515827568652837... |
706.2157 | Viscous spin exchange torque on precessional magnetization in
$(\mathrm{LaMnO}_3)_{2n}/(\mathrm{SrMnO}_3)_{n}$ superlattices | Photoinduced magnetization dynamics is investigated in chemically ordered
$(\mathrm{LaMnO}_3)_{2n}/(\mathrm{SrMnO}_3)_n$ superlattices using the
time-resolved magneto-optic Kerr effect. A monotonic frequency-field dependence
is observed for the $n=1$ superlattice, indicating a single spin population
consistent with a... | cond-mat.mtrl-sci cond-mat.str-el | photoinduced magnetization dynamics is investigated in chemically ordered mathrmlamno_3_2nmathrmsrmno_3_n superlattices using the timeresolved magnetooptic kerr effect a monotonic frequencyfield dependence is observed for the n1 superlattice indicating a single spin population consistent with a homogeneous hole distrib... | [['photoinduced', 'magnetization', 'dynamics', 'is', 'investigated', 'in', 'chemically', 'ordered', 'mathrmlamno_3_2nmathrmsrmno_3_n', 'superlattices', 'using', 'the', 'timeresolved', 'magnetooptic', 'kerr', 'effect', 'a', 'monotonic', 'frequencyfield', 'dependence', 'is', 'observed', 'for', 'the', 'n1', 'superlattice'... | [-0.23802161188683954, 0.22679787791907052, -0.04287330609050591, 0.0407687101151278, -0.048499004458110916, -0.14208901049120418, 0.024977213865796846, 0.40994507179831163, -0.26903179016087697, -0.2879045477069645, -0.018833507002465964, -0.2888919842171382, -0.10338234080209296, 0.19833587761687854, 0.05202645669882... |
706.2158 | Ultra High Energy Cosmic Rays Diffusion in an Expanding Universe | We study the solution of the diffusion equation for Ultra-High Energy Cosmic
Rays in the general case of an expanding universe, comparing it with the well
known Syrovatsky solution obtained in the more restrictive case of a static
universe. The formal comparison of the two solutions with all parameters being
fixed id... | astro-ph | we study the solution of the diffusion equation for ultrahigh energy cosmic rays in the general case of an expanding universe comparing it with the well known syrovatsky solution obtained in the more restrictive case of a static universe the formal comparison of the two solutions with all parameters being fixed identic... | [['we', 'study', 'the', 'solution', 'of', 'the', 'diffusion', 'equation', 'for', 'ultrahigh', 'energy', 'cosmic', 'rays', 'in', 'the', 'general', 'case', 'of', 'an', 'expanding', 'universe', 'comparing', 'it', 'with', 'the', 'well', 'known', 'syrovatsky', 'solution', 'obtained', 'in', 'the', 'more', 'restrictive', 'cas... | [-0.12044435791095667, 0.07877638224979616, -0.06080015916894707, 0.11951790017095239, -0.04473318451588663, -0.08818733931467351, -0.015209291405173846, 0.3407990570801, -0.23626459058788088, -0.30990985323054093, 0.0890620534531384, -0.29934864786143106, -0.06688341893216905, 0.20309274767835936, -0.00420618696241743... |
706.2159 | Continuous input nonlocal games | We present a family of nonlocal games in which the inputs the players receive
are continuous. We study three representative members of the family. For the
first two a team sharing quantum correlations (entanglement) has an advantage
over any team restricted to classical correlations. We conjecture that this is
true f... | quant-ph | we present a family of nonlocal games in which the inputs the players receive are continuous we study three representative members of the family for the first two a team sharing quantum correlations entanglement has an advantage over any team restricted to classical correlations we conjecture that this is true for the ... | [['we', 'present', 'a', 'family', 'of', 'nonlocal', 'games', 'in', 'which', 'the', 'inputs', 'the', 'players', 'receive', 'are', 'continuous', 'we', 'study', 'three', 'representative', 'members', 'of', 'the', 'family', 'for', 'the', 'first', 'two', 'a', 'team', 'sharing', 'quantum', 'correlations', 'entanglement', 'has... | [-0.1561668976604686, 0.07311016969383749, -0.10317177084763929, 0.0600011259064836, -0.05261861373496763, -0.14608826732925945, 0.03338524889421918, 0.3633341296118195, -0.2659589205947468, -0.2864107931569471, 0.06046646849994185, -0.3209272626495399, -0.13463276878820132, 0.14189769172157018, -0.056141310253070065, ... |
706.216 | Minimality in topological groups and Heisenberg type groups | We study relatively minimal subgroups in topological groups. We find, in
particular, some natural relatively minimal subgroups in unipotent groups which
are defined over "good" rings. By "good" rings we mean archimedean absolute
valued (not necessarily associative) division rings. Some of the classical
rings which we... | math.GN math.GR | we study relatively minimal subgroups in topological groups we find in particular some natural relatively minimal subgroups in unipotent groups which are defined over good rings by good rings we mean archimedean absolute valued not necessarily associative division rings some of the classical rings which we consider bes... | [['we', 'study', 'relatively', 'minimal', 'subgroups', 'in', 'topological', 'groups', 'we', 'find', 'in', 'particular', 'some', 'natural', 'relatively', 'minimal', 'subgroups', 'in', 'unipotent', 'groups', 'which', 'are', 'defined', 'over', 'good', 'rings', 'by', 'good', 'rings', 'we', 'mean', 'archimedean', 'absolute'... | [-0.22234221018222441, 0.07658936569175448, -0.07680457803499267, 0.08028800042026328, -0.08091334935771413, -0.09563105246500976, -0.014237464450479272, 0.3971221587194287, -0.3204585424658046, -0.21174285946840263, 0.11437811310745281, -0.20164927624794374, -0.1336555070501853, 0.20742341292550764, -0.163658001617225... |
706.2161 | General Hubbard model for strongly interacting fermions in an optical
lattice and its phase detection | Based on consideration of the system symmetry and its Hilbert space, we show
that strongly interacting fermions in an optical lattice or superlattice can be
generically described by a lattice resonance Hamiltonian. The latter can be
mapped to a general Hubbard model with particle assisted tunneling rates. We
investig... | cond-mat.other cond-mat.supr-con | based on consideration of the system symmetry and its hilbert space we show that strongly interacting fermions in an optical lattice or superlattice can be generically described by a lattice resonance hamiltonian the latter can be mapped to a general hubbard model with particle assisted tunneling rates we investigate t... | [['based', 'on', 'consideration', 'of', 'the', 'system', 'symmetry', 'and', 'its', 'hilbert', 'space', 'we', 'show', 'that', 'strongly', 'interacting', 'fermions', 'in', 'an', 'optical', 'lattice', 'or', 'superlattice', 'can', 'be', 'generically', 'described', 'by', 'a', 'lattice', 'resonance', 'hamiltonian', 'the', 'l... | [-0.14847500258409208, 0.1698551106432144, -0.09504397665516714, 0.06779931370284031, -0.00855383336651296, -0.1942388359404933, 0.06796892873649851, 0.4056179311252042, -0.2807132960349489, -0.2396361810898178, 0.06313577672372457, -0.24472028857032935, -0.16682480196363889, 0.13940358773956935, 0.0009485449369871214,... |
706.2162 | The competition of hydrogen-like and isotropic interactions on polymer
collapse | We investigate a lattice model of polymers where the nearest-neighbour
monomer-monomer interaction strengths differ according to whether the local
configurations have so-called ``hydrogen-like'' formations or not. If the
interaction strengths are all the same then the classical $\theta$-point
collapse transition occu... | cond-mat.soft cond-mat.stat-mech | we investigate a lattice model of polymers where the nearestneighbour monomermonomer interaction strengths differ according to whether the local configurations have socalled hydrogenlike formations or not if the interaction strengths are all the same then the classical thetapoint collapse transition occurs on lowering ... | [['we', 'investigate', 'a', 'lattice', 'model', 'of', 'polymers', 'where', 'the', 'nearestneighbour', 'monomermonomer', 'interaction', 'strengths', 'differ', 'according', 'to', 'whether', 'the', 'local', 'configurations', 'have', 'socalled', 'hydrogenlike', 'formations', 'or', 'not', 'if', 'the', 'interaction', 'streng... | [-0.12885397068457677, 0.22509959685533734, -0.05521499487707236, 0.035822681076954015, -0.026335714457349644, -0.12679700791680565, 0.0655576799220095, 0.38675481618459645, -0.2557963874216916, -0.25224704628085926, 0.07450303305005138, -0.29416012501137123, -0.11755177883638276, 0.12191759230691888, 0.059562541373694... |
706.2163 | Predictions for masses of Xi_b baryons | The recent observation by CDF of Sigma_b^{+-} (uub and ddb) baryons within 2
MeV of the predicted Sigma_b - Lambda_b splitting has provided strong
confirmation for the theoretical approach based on modeling the color hyperfine
interaction. We now apply this approach to predict the masses of the Xi_b
family of baryons... | hep-ph hep-ex | the recent observation by cdf of sigma_b uub and ddb baryons within 2 mev of the predicted sigma_b lambda_b splitting has provided strong confirmation for the theoretical approach based on modeling the color hyperfine interaction we now apply this approach to predict the masses of the xi_b family of baryons with quark ... | [['the', 'recent', 'observation', 'by', 'cdf', 'of', 'sigma_b', 'uub', 'and', 'ddb', 'baryons', 'within', '2', 'mev', 'of', 'the', 'predicted', 'sigma_b', 'lambda_b', 'splitting', 'has', 'provided', 'strong', 'confirmation', 'for', 'the', 'theoretical', 'approach', 'based', 'on', 'modeling', 'the', 'color', 'hyperfine'... | [-0.04074082295927736, 0.18148294894059222, -0.07698431478692563, 0.1206243743740574, -0.024879768627148156, -0.0932062193163869, 0.11547348715140726, 0.3345298898164873, -0.18395259287380786, -0.31983506816215124, -0.01339617945012395, -0.3367499000893009, 0.03969651399583435, 0.09983699326619024, 0.060159310437652665... |
706.2164 | Spitzer Mid-to-Far-Infrared Flux Densities of Distant Galaxies | We study the infrared (IR) properties of high-redshift galaxies using deep
Spitzer 24, 70, and 160 micron data. Our primary interest is to improve the
constraints on the total IR luminosities, L(IR), of these galaxies. We combine
the Spitzer data in the southern Extended Chandra Deep Field with a
K-band-selected gala... | astro-ph | we study the infrared ir properties of highredshift galaxies using deep spitzer 24 70 and 160 micron data our primary interest is to improve the constraints on the total ir luminosities lir of these galaxies we combine the spitzer data in the southern extended chandra deep field with a kbandselected galaxy sample and p... | [['we', 'study', 'the', 'infrared', 'ir', 'properties', 'of', 'highredshift', 'galaxies', 'using', 'deep', 'spitzer', '24', '70', 'and', '160', 'micron', 'data', 'our', 'primary', 'interest', 'is', 'to', 'improve', 'the', 'constraints', 'on', 'the', 'total', 'ir', 'luminosities', 'lir', 'of', 'these', 'galaxies', 'we',... | [0.02013651736643389, 0.13731614999389177, 0.006001226956110329, 0.1133896003645111, -0.014252804452553391, -0.023694543337429687, 0.09843370365966177, 0.4943673534601821, -0.059468425855586836, -0.45374794521240697, 0.04416359023087372, -0.3569240441065374, 0.06523239945329713, 0.16303116094005088, -0.0254095916405102... |
706.2165 | A Research-Based Curriculum for Teaching the Photoelectric Effect | Physics faculty consider the photoelectric effect important, but many
erroneously believe it is easy for students to understand. We have developed
curriculum on this topic including an interactive computer simulation,
interactive lectures with peer instruction, and conceptual and mathematical
homework problems. Our c... | physics.ed-ph | physics faculty consider the photoelectric effect important but many erroneously believe it is easy for students to understand we have developed curriculum on this topic including an interactive computer simulation interactive lectures with peer instruction and conceptual and mathematical homework problems our curricul... | [['physics', 'faculty', 'consider', 'the', 'photoelectric', 'effect', 'important', 'but', 'many', 'erroneously', 'believe', 'it', 'is', 'easy', 'for', 'students', 'to', 'understand', 'we', 'have', 'developed', 'curriculum', 'on', 'this', 'topic', 'including', 'an', 'interactive', 'computer', 'simulation', 'interactive'... | [0.02222366387829383, 0.08703505779567192, -0.11791016932974006, 0.11515736660366373, -0.1944953111759127, -0.1887517710320349, 0.07228343749624502, 0.41051839282594355, -0.21416663819481382, -0.42675755586153663, 0.05923854114208843, -0.27986318481551853, -0.14165696335736624, 0.19836291029983139, -0.13592833096662602... |
706.2166 | Canonical heights and the arithmetic complexity of morphisms on
projective space | Let F and G be morphisms of degree at least 2 from P^N to P^N that are
defined over the algebraic closure of Q. We define the arithmetic distance
d(F,G) between F and G to be the supremum over all algebraic points P of
|h_F(P)-h_G(P)|, where h_F and h_G are the canonical heights associated to the
morphisms F and G, r... | math.NT math.DS | let f and g be morphisms of degree at least 2 from pn to pn that are defined over the algebraic closure of q we define the arithmetic distance dfg between f and g to be the supremum over all algebraic points p of h_fph_gp where h_f and h_g are the canonical heights associated to the morphisms f and g respectively we pr... | [['let', 'f', 'and', 'g', 'be', 'morphisms', 'of', 'degree', 'at', 'least', '2', 'from', 'pn', 'to', 'pn', 'that', 'are', 'defined', 'over', 'the', 'algebraic', 'closure', 'of', 'q', 'we', 'define', 'the', 'arithmetic', 'distance', 'dfg', 'between', 'f', 'and', 'g', 'to', 'be', 'the', 'supremum', 'over', 'all', 'algebr... | [-0.21244615507378015, 0.11368845092167831, -0.0585397517765468, 0.013585087769656038, -0.03579350645469396, -0.13325047117376806, 0.027956974028745876, 0.34694254746274006, -0.3609140063372423, -0.2618337938175449, 0.004112313012812146, -0.2672056692810553, -0.086557648232523, 0.2654539579437729, -0.08107431285645601,... |
706.2167 | Renormalization and Induced Gauge Action on a Noncommutative Space | Field theories on deformed spaces suffer from the IR/UV mxing and
renormalization is generically spoiled. In work with R. Wulkenhaar, one of us
realized a way to cure this desease by adding one more marginal operator. We
review these ideas, show the application to $\phi^3$ models and use heat kernel
expansion methods... | hep-th | field theories on deformed spaces suffer from the iruv mxing and renormalization is generically spoiled in work with r wulkenhaar one of us realized a way to cure this desease by adding one more marginal operator we review these ideas show the application to phi3 models and use heat kernel expansion methods for a scala... | [['field', 'theories', 'on', 'deformed', 'spaces', 'suffer', 'from', 'the', 'iruv', 'mxing', 'and', 'renormalization', 'is', 'generically', 'spoiled', 'in', 'work', 'with', 'r', 'wulkenhaar', 'one', 'of', 'us', 'realized', 'a', 'way', 'to', 'cure', 'this', 'desease', 'by', 'adding', 'one', 'more', 'marginal', 'operator... | [-0.07654008427468528, 0.13926310061132036, -0.09646184616056937, 0.09830155659999167, -0.11998664936316865, -0.16993610435165465, 0.012058078396200602, 0.35884997766198856, -0.22235649711385902, -0.26047048903669096, 0.09288568826824693, -0.25229863108002715, -0.18076821235673768, 0.1612062894373334, -0.08267103976437... |
706.2168 | Models of Neutrino Masses and Mixing | Neutrino physics has entered an era of precision measurements. With these
precise measurements, we may be able to distinguish different models that have
been constructed to explain the small neutrino masses and the large mixing
among them. In this talk, I review some of the existing theoretical models and
their predi... | hep-ph | neutrino physics has entered an era of precision measurements with these precise measurements we may be able to distinguish different models that have been constructed to explain the small neutrino masses and the large mixing among them in this talk i review some of the existing theoretical models and their predictions... | [['neutrino', 'physics', 'has', 'entered', 'an', 'era', 'of', 'precision', 'measurements', 'with', 'these', 'precise', 'measurements', 'we', 'may', 'be', 'able', 'to', 'distinguish', 'different', 'models', 'that', 'have', 'been', 'constructed', 'to', 'explain', 'the', 'small', 'neutrino', 'masses', 'and', 'the', 'large... | [-0.042053743455283066, 0.22784218618336902, -0.0670113983667559, 0.1419299125425621, -0.09283598902186861, -0.16685003585492572, 0.022698528193696228, 0.3545395967171148, -0.2339453329073472, -0.3730612279571317, 0.10664033744682523, -0.30807460351260724, -0.0575166431652313, 0.20947852971342704, -0.020895484903896297... |
706.2169 | Nonarchimedean Green functions and dynamics on projective space | Let F: P^N_K --> P^N_K be a morphism of degree d > 1 defined over a field K
that is algebraically closed and complete with respect to a nonarchimedean
absolute value. We prove that a modified Green function G_F associated to F is
Holder continuous on P^N(K) and that the Fatou set F is equal to the set of
points at wh... | math.NT math.DS | let f pn_k pn_k be a morphism of degree d 1 defined over a field k that is algebraically closed and complete with respect to a nonarchimedean absolute value we prove that a modified green function g_f associated to f is holder continuous on pnk and that the fatou set f is equal to the set of points at which g_f is loca... | [['let', 'f', 'pn_k', 'pn_k', 'be', 'a', 'morphism', 'of', 'degree', 'd', '1', 'defined', 'over', 'a', 'field', 'k', 'that', 'is', 'algebraically', 'closed', 'and', 'complete', 'with', 'respect', 'to', 'a', 'nonarchimedean', 'absolute', 'value', 'we', 'prove', 'that', 'a', 'modified', 'green', 'function', 'g_f', 'assoc... | [-0.23174384999672107, 0.09165054373443127, -0.10470537141087317, -0.0009606794114703329, -0.051630942940833834, -0.13580455766799293, 0.056824012615970365, 0.3629676440086599, -0.34011711535331246, -0.15184920688353426, 0.04034160858642519, -0.3014877422399401, -0.06958323398987963, 0.22345867107195833, -0.08996839411... |
706.217 | Transient jets in V617 Sagittarii | Some of the luminous Compact Binary Supersoft X-Ray sources (CBSS) have shown
indications of jets, also called satellites due to their appearance in the
spectra. In V Sagittae (V Sge) stars, the galactic counterparts of the CBSS,
such features have been reported only for WX Cen. If V Sge stars are indeed the
analogs ... | astro-ph | some of the luminous compact binary supersoft xray sources cbss have shown indications of jets also called satellites due to their appearance in the spectra in v sagittae v sge stars the galactic counterparts of the cbss such features have been reported only for wx cen if v sge stars are indeed the analogs of cbss one ... | [['some', 'of', 'the', 'luminous', 'compact', 'binary', 'supersoft', 'xray', 'sources', 'cbss', 'have', 'shown', 'indications', 'of', 'jets', 'also', 'called', 'satellites', 'due', 'to', 'their', 'appearance', 'in', 'the', 'spectra', 'in', 'v', 'sagittae', 'v', 'sge', 'stars', 'the', 'galactic', 'counterparts', 'of', '... | [-0.08007669964909407, 0.1015036963937363, -0.09148800919523649, 0.08360682792906453, -0.14536613776841764, -0.11935899253301996, 0.05027945130744851, 0.46842862807802466, -0.19516716082618682, -0.3139962892823142, 0.060405871612601914, -0.35371725739126925, -0.0597935178084299, 0.20735940021536167, -0.0639022060641812... |
706.2171 | A multiwavelength study of young massive star forming regions: II. The
dust environment | We present observations of 1.2-mm dust continuum emission, made with the
Swedish ESO Submillimeter Telescope, towards eighteen luminous IRAS point
sources, all with colors typical of compact HII regions and associated with
CS(2-1) emission, thought to be representative of young massive star forming
regions. Emission ... | astro-ph | we present observations of 12mm dust continuum emission made with the swedish eso submillimeter telescope towards eighteen luminous iras point sources all with colors typical of compact hii regions and associated with cs21 emission thought to be representative of young massive star forming regions emission was detected... | [['we', 'present', 'observations', 'of', '12mm', 'dust', 'continuum', 'emission', 'made', 'with', 'the', 'swedish', 'eso', 'submillimeter', 'telescope', 'towards', 'eighteen', 'luminous', 'iras', 'point', 'sources', 'all', 'with', 'colors', 'typical', 'of', 'compact', 'hii', 'regions', 'and', 'associated', 'with', 'cs2... | [-0.055259057400390915, 0.14212436704379697, -0.016490256058724097, 0.03962973225330211, -0.032372692017018645, -0.07258921598624353, 0.009222816706201292, 0.4990068567750899, -0.09098736624409909, -0.3508520668976383, 0.0648314594237993, -0.30958665557818055, 0.007235362828118072, 0.1179781973208443, 0.011577728681303... |
706.2172 | Dijet Azimuthal Correlations in QCD Hard Processes | We study the azimuthal correlation distribution for dijet production in QCD
hard processes. This observable is sensitive to soft and/or collinear emissions
in the back-to-back region, giving rise to single and double logarithms. We
provide resummed predictions to NLL accuracy for both DIS at HERA and hadronic
collisi... | hep-ph | we study the azimuthal correlation distribution for dijet production in qcd hard processes this observable is sensitive to soft andor collinear emissions in the backtoback region giving rise to single and double logarithms we provide resummed predictions to nll accuracy for both dis at hera and hadronic collisions at t... | [['we', 'study', 'the', 'azimuthal', 'correlation', 'distribution', 'for', 'dijet', 'production', 'in', 'qcd', 'hard', 'processes', 'this', 'observable', 'is', 'sensitive', 'to', 'soft', 'andor', 'collinear', 'emissions', 'in', 'the', 'backtoback', 'region', 'giving', 'rise', 'to', 'single', 'and', 'double', 'logarithm... | [-0.04027634116655757, 0.1342405738504303, -0.17538239952597406, 0.22068485055839823, -0.026626095446127075, -0.04458315034336861, -0.019465461970427103, 0.43450688282328265, -0.1707792782915696, -0.2375092564466139, -0.04218330950337282, -0.3855959526112964, 0.07454572130565441, 0.09129219775598857, 0.0823455090571623... |
706.2173 | Theoretical Resolution of Magnetic Reconnection in High Energy Plasmas | The formation of macroscopic reconnected magnetic structures (islands) have
been observed in advanced experiments on weakly collisional, well confined
plasmas while established theories of the drift-tearing modes, which depend
strongly on the electron temperature gradient and can describe the formation of
these struc... | physics.plasm-ph physics.space-ph | the formation of macroscopic reconnected magnetic structures islands have been observed in advanced experiments on weakly collisional well confined plasmas while established theories of the drifttearing modes which depend strongly on the electron temperature gradient and can describe the formation of these structures h... | [['the', 'formation', 'of', 'macroscopic', 'reconnected', 'magnetic', 'structures', 'islands', 'have', 'been', 'observed', 'in', 'advanced', 'experiments', 'on', 'weakly', 'collisional', 'well', 'confined', 'plasmas', 'while', 'established', 'theories', 'of', 'the', 'drifttearing', 'modes', 'which', 'depend', 'strongly... | [-0.16598039313514784, 0.2757839900327892, -0.04168844424051846, 0.07355626814050327, -0.04329591816597868, -0.10449636289594331, -0.032399025480916, 0.33765499179092484, -0.25368808730570713, -0.30410505061196846, 0.05583096566686702, -0.24653575784617626, -0.062289650477440575, 0.19992770223272113, 0.0588781063646509... |
706.2174 | Planets around evolved intermediate-mass stars. I. Two substellar
companions in the open clusters NGC 2423 and NGC 4349 | Context. Many efforts are being made to characterize extrasolar planetary
systems and unveil the fundamental mechanisms of planet formation. An important
aspect of the problem, which remains largely unknown, is to understand how the
planet formation process depends on the mass of the parent star. In particular,
as mo... | astro-ph | context many efforts are being made to characterize extrasolar planetary systems and unveil the fundamental mechanisms of planet formation an important aspect of the problem which remains largely unknown is to understand how the planet formation process depends on the mass of the parent star in particular as most plane... | [['context', 'many', 'efforts', 'are', 'being', 'made', 'to', 'characterize', 'extrasolar', 'planetary', 'systems', 'and', 'unveil', 'the', 'fundamental', 'mechanisms', 'of', 'planet', 'formation', 'an', 'important', 'aspect', 'of', 'the', 'problem', 'which', 'remains', 'largely', 'unknown', 'is', 'to', 'understand', '... | [-0.09799826817589175, 0.1434283916610487, -0.06959379518197642, 0.07297408593050124, -0.15201434913281076, -0.05062372757432362, 0.09549802211932493, 0.36485080088174004, -0.11925864264722569, -0.3973283065345, 0.06698414316892418, -0.29568752215332267, -0.0667177470124982, 0.21342167597246806, -0.10640100459632877, 0... |
706.2175 | A resolution of the K(2)-local sphere at the prime 3 | We develop a framework for displaying the stable homotopy theory of the
sphere, at least after localization at the second Morava K-theory K(2). At the
prime 3, we write the spectrum L_{K(2)S^0 as the inverse limit of a tower of
fibrations with four layers. The successive fibers are of the form E_2^hF where
F is a fin... | math.AT | we develop a framework for displaying the stable homotopy theory of the sphere at least after localization at the second morava ktheory k2 at the prime 3 we write the spectrum l_k2s0 as the inverse limit of a tower of fibrations with four layers the successive fibers are of the form e_2hf where f is a finite subgroup o... | [['we', 'develop', 'a', 'framework', 'for', 'displaying', 'the', 'stable', 'homotopy', 'theory', 'of', 'the', 'sphere', 'at', 'least', 'after', 'localization', 'at', 'the', 'second', 'morava', 'ktheory', 'k2', 'at', 'the', 'prime', '3', 'we', 'write', 'the', 'spectrum', 'l_k2s0', 'as', 'the', 'inverse', 'limit', 'of', ... | [-0.21649065073207022, 0.09798819926381111, -0.11531072867661715, 0.046367882643826304, -0.040337651286274194, -0.15517955809086562, -0.0039055744027718903, 0.30851002762001006, -0.3295978090837598, -0.24598463880270718, 0.10783405950758607, -0.297426458906848, -0.10682654322683811, 0.14346872112713754, -0.107625928772... |
706.2176 | Comments on the breakdown of the Landauer bound for information erasure
in the quantum regime | Upon reviewing the article by Allahverdyan and Nieuwenhuizen in PRE, we
conclude that neither the Landauer principle nor the counterexamples presented
by the authors have any relation (i) to thermodynamics, and (ii) to the
interdependence of nonstatistical quantum physics and thermodynamics.
| quant-ph | upon reviewing the article by allahverdyan and nieuwenhuizen in pre we conclude that neither the landauer principle nor the counterexamples presented by the authors have any relation i to thermodynamics and ii to the interdependence of nonstatistical quantum physics and thermodynamics | [['upon', 'reviewing', 'the', 'article', 'by', 'allahverdyan', 'and', 'nieuwenhuizen', 'in', 'pre', 'we', 'conclude', 'that', 'neither', 'the', 'landauer', 'principle', 'nor', 'the', 'counterexamples', 'presented', 'by', 'the', 'authors', 'have', 'any', 'relation', 'i', 'to', 'thermodynamics', 'and', 'ii', 'to', 'the',... | [-0.05328223974693839, 0.12635617723643053, -0.09974551208249134, 0.07509956295352156, -0.044505345730235936, -0.15889736949522956, 0.13506611282710076, 0.28554995512453524, -0.2071079569187288, -0.3038194690626569, 0.06139067187621372, -0.3120065525901027, -0.16011546624869835, 0.1342017671502218, -0.10279943875786735... |
706.2177 | Physical properties of the noncentrosymmetric superconductor
Mg_10Ir_19B_16 | Specific heat, electrical resistivity, and magnetic susceptibility
measurements on a high quality sample of Mg10Ir19B16 provide a self-consistent
determination of its superconducting properties. They indicate that Mg10Ir19B16
is a type-II superconductor (Tc=4.45K, k(0)=20), with an electron-phonon
coupling constant l... | cond-mat.supr-con | specific heat electrical resistivity and magnetic susceptibility measurements on a high quality sample of mg10ir19b16 provide a selfconsistent determination of its superconducting properties they indicate that mg10ir19b16 is a typeii superconductor tc445k k020 with an electronphonon coupling constant l_ep066 an analysi... | [['specific', 'heat', 'electrical', 'resistivity', 'and', 'magnetic', 'susceptibility', 'measurements', 'on', 'a', 'high', 'quality', 'sample', 'of', 'mg10ir19b16', 'provide', 'a', 'selfconsistent', 'determination', 'of', 'its', 'superconducting', 'properties', 'they', 'indicate', 'that', 'mg10ir19b16', 'is', 'a', 'typ... | [-0.2404541654246194, 0.15847695009579182, -0.026052962323384627, 0.03015267107402906, -0.11062198696932422, -0.20259910907064166, 0.14179073902113096, 0.3969092284994466, -0.22709718077842678, -0.31373259850910734, -0.03958090938228582, -0.3719192534685135, -0.041338177264801095, 0.25336557894146866, 0.102770891426397... |
706.2178 | Exactly solvable interacting vertex models | We introduce and solvev a special family of integrable interacting vertex
models that generalizes the well known six-vertex model. In addition to the
usual nearest-neighbor interactions among the vertices, there exist extra
hard-core interactions among pair of vertices at larger distances.The
associated row-to-row tr... | cond-mat.stat-mech cond-mat.str-el | we introduce and solvev a special family of integrable interacting vertex models that generalizes the well known sixvertex model in addition to the usual nearestneighbor interactions among the vertices there exist extra hardcore interactions among pair of vertices at larger distancesthe associated rowtorow transfer mat... | [['we', 'introduce', 'and', 'solvev', 'a', 'special', 'family', 'of', 'integrable', 'interacting', 'vertex', 'models', 'that', 'generalizes', 'the', 'well', 'known', 'sixvertex', 'model', 'in', 'addition', 'to', 'the', 'usual', 'nearestneighbor', 'interactions', 'among', 'the', 'vertices', 'there', 'exist', 'extra', 'h... | [-0.1519022348726199, 0.19402862484359323, 0.040982393834636865, 0.10772322928227607, -0.05181910235198123, -0.19034144016303367, -0.017341414242257654, 0.349665095854062, -0.253254924343563, -0.24567934890949458, 0.041051241319214345, -0.34948283547085146, -0.15039086254450995, 0.09200459094260072, 0.04002039264276868... |
706.2179 | Backreaction in trans-Planckian cosmology: renormalization, trace
anomaly and selfconsistent solutions | We analyze the semiclassical Einstein equations for quantum scalar fields
satisfying modified dispersion relations. We first discuss in detail the
renormalization procedure based on adiabatic subtraction and dimensional
regularization. We show that, contrary to what expected from power counting
arguments, in 3+1 dime... | gr-qc hep-th | we analyze the semiclassical einstein equations for quantum scalar fields satisfying modified dispersion relations we first discuss in detail the renormalization procedure based on adiabatic subtraction and dimensional regularization we show that contrary to what expected from power counting arguments in 31 dimensions ... | [['we', 'analyze', 'the', 'semiclassical', 'einstein', 'equations', 'for', 'quantum', 'scalar', 'fields', 'satisfying', 'modified', 'dispersion', 'relations', 'we', 'first', 'discuss', 'in', 'detail', 'the', 'renormalization', 'procedure', 'based', 'on', 'adiabatic', 'subtraction', 'and', 'dimensional', 'regularization... | [-0.11379620202255677, 0.1367738736477044, -0.1252383793355763, 0.12643203052153096, -0.08071356546293229, -0.07661361597344432, 0.02012892289498617, 0.31253752541052154, -0.24674011080219627, -0.3009061681247023, 0.04820392988239453, -0.26562469975691133, -0.13110821986290283, 0.17669419180091522, 0.003050547389772861... |
706.218 | The effect of Fe and Ru substitution for Ni on the thermopower in
MgCNi_3 | The intermetallic perovskite MgCNi3 is a superconductor with a Tc=7 K.
Substitution of Fe and Ru for Ni decreases Tc monotonically as the doping
concentration is increased. Here we report thermopower measurements, S(T), on
MgCNi3, MgCNi3-xFex and MgCNi3-xRux. For MgCNi3, the thermopower is negative, -
12.5 mikroV/K, ... | cond-mat.supr-con cond-mat.mtrl-sci | the intermetallic perovskite mgcni3 is a superconductor with a tc7 k substitution of fe and ru for ni decreases tc monotonically as the doping concentration is increased here we report thermopower measurements st on mgcni3 mgcni3xfex and mgcni3xrux for mgcni3 the thermopower is negative 125 mikrovk at 300 k the absolut... | [['the', 'intermetallic', 'perovskite', 'mgcni3', 'is', 'a', 'superconductor', 'with', 'a', 'tc7', 'k', 'substitution', 'of', 'fe', 'and', 'ru', 'for', 'ni', 'decreases', 'tc', 'monotonically', 'as', 'the', 'doping', 'concentration', 'is', 'increased', 'here', 'we', 'report', 'thermopower', 'measurements', 'st', 'on', ... | [-0.14143739277987102, 0.2576464399911888, 0.04930970289237928, -0.021548746741916005, 0.008587716112583223, -0.17404270688431306, 0.16966207267659342, 0.3776173319732934, -0.2631253240335929, -0.3217699244585738, -0.012374962155151655, -0.4624419463308234, -0.02438322520863853, 0.17686163218234452, 0.01866920268890170... |
706.2181 | GZK Photons Above 10 EeV | We calculate the flux of "GZK-photons", namely the flux of photons produced
by extragalactic nucleons through the resonant photoproduction of pions, the so
called GZK effect. This flux depends on the UHECR spectrum on Earth, of the
spectrum of nucleons emitted at the sources, which we characterize by its slope
and ma... | astro-ph | we calculate the flux of gzkphotons namely the flux of photons produced by extragalactic nucleons through the resonant photoproduction of pions the so called gzk effect this flux depends on the uhecr spectrum on earth of the spectrum of nucleons emitted at the sources which we characterize by its slope and maximum ener... | [['we', 'calculate', 'the', 'flux', 'of', 'gzkphotons', 'namely', 'the', 'flux', 'of', 'photons', 'produced', 'by', 'extragalactic', 'nucleons', 'through', 'the', 'resonant', 'photoproduction', 'of', 'pions', 'the', 'so', 'called', 'gzk', 'effect', 'this', 'flux', 'depends', 'on', 'the', 'uhecr', 'spectrum', 'on', 'ear... | [-0.049340002981328665, 0.2844176878739347, -0.01180980285938234, 0.17307407222877633, -0.012148299310962564, 0.0025706500994295057, 0.05620443815993663, 0.3753402521268922, -0.15122407837224106, -0.381877362265213, -0.011517261428422344, -0.3869311938877906, 0.042379962011741906, 0.21131778769084864, 0.053351109894956... |
706.2182 | New AB-Thermonuclear Reactor for Aerospace | There are two main methods of nulcear fusion: inertial confinement fusion
(ICF) and magnetic confinement fusion (MCF). Existing thermonuclear reactors
are very complex, expensive, large, and heavy. They cannot achieve the Lawson
creterion.
The author offers an innovation. ICF has on the inside surface of the
shell-... | physics.gen-ph physics.atom-ph | there are two main methods of nulcear fusion inertial confinement fusion icf and magnetic confinement fusion mcf existing thermonuclear reactors are very complex expensive large and heavy they cannot achieve the lawson creterion the author offers an innovation icf has on the inside surface of the shellshaped combustion... | [['there', 'are', 'two', 'main', 'methods', 'of', 'nulcear', 'fusion', 'inertial', 'confinement', 'fusion', 'icf', 'and', 'magnetic', 'confinement', 'fusion', 'mcf', 'existing', 'thermonuclear', 'reactors', 'are', 'very', 'complex', 'expensive', 'large', 'and', 'heavy', 'they', 'can', 'not', 'achieve', 'the', 'lawson',... | [-0.05208279527503358, 0.18334340324879214, -0.02970343383429324, 0.014460529427363719, -0.058680696990175626, -0.13592437658866746, 0.01011124450283555, 0.38219592124003277, -0.2387576289702284, -0.3158229828409895, 0.07414961208178822, -0.30675898775866134, -0.05512413517131123, 0.22079819482172558, -0.12208304668848... |
706.2183 | Color Screening Melts Quarkonium | We calculate quarkonium spectral functions in a quark-gluon plasma using a
potential model based on full QCD lattice calculations of the free energy of
static quark-antiquark pair. We estimate the binding energy and the thermal
width of different quarkonium states. The estimated upper limit for the
dissociation tempe... | hep-ph | we calculate quarkonium spectral functions in a quarkgluon plasma using a potential model based on full qcd lattice calculations of the free energy of static quarkantiquark pair we estimate the binding energy and the thermal width of different quarkonium states the estimated upper limit for the dissociation temperature... | [['we', 'calculate', 'quarkonium', 'spectral', 'functions', 'in', 'a', 'quarkgluon', 'plasma', 'using', 'a', 'potential', 'model', 'based', 'on', 'full', 'qcd', 'lattice', 'calculations', 'of', 'the', 'free', 'energy', 'of', 'static', 'quarkantiquark', 'pair', 'we', 'estimate', 'the', 'binding', 'energy', 'and', 'the',... | [-0.05464594798178365, 0.2050331130434396, -0.12710328145994473, 0.1597240645205602, 0.01779841072462752, -0.060986118675288505, 0.09340729419205149, 0.3667799322944829, -0.15172801753979617, -0.23969860854795424, -0.018882096070259556, -0.30040992105032427, 0.03256273194772617, 0.15038215811758981, 0.1016166235864857,... |
706.2184 | Mapping Class Groups do not have Kazhdan's Property (T) | We prove that the mapping class group of a closed oriented surface of genus
at least two does not have Kazhdan's property (T).
| math.QA math.GR math.GT | we prove that the mapping class group of a closed oriented surface of genus at least two does not have kazhdans property t | [['we', 'prove', 'that', 'the', 'mapping', 'class', 'group', 'of', 'a', 'closed', 'oriented', 'surface', 'of', 'genus', 'at', 'least', 'two', 'does', 'not', 'have', 'kazhdans', 'property', 't']] | [-0.23111794694610263, 0.1584435962545483, -0.14646494107158936, 0.02199454168262689, -0.12554482520436464, -0.20875344949814936, -0.0026139882190719895, 0.4359304095092027, -0.30213501595932507, -0.22772058609711088, 0.08143469659895029, -0.2591812946712193, -0.10876934989557965, 0.19534453182764674, -0.11102042942429... |
706.2185 | Electron-Electron Interactions in the Vacuum Polarization of Graphene | We discuss the effect of electron-electron interactions on the static
polarization properties of graphene beyond RPA. Divergent self-energy
corrections are naturally absorbed into the renormalized coupling constant
$\alpha$. We find that the lowest order vertex correction, which is the first
non-trivial correlation c... | cond-mat.str-el | we discuss the effect of electronelectron interactions on the static polarization properties of graphene beyond rpa divergent selfenergy corrections are naturally absorbed into the renormalized coupling constant alpha we find that the lowest order vertex correction which is the first nontrivial correlation contribution... | [['we', 'discuss', 'the', 'effect', 'of', 'electronelectron', 'interactions', 'on', 'the', 'static', 'polarization', 'properties', 'of', 'graphene', 'beyond', 'rpa', 'divergent', 'selfenergy', 'corrections', 'are', 'naturally', 'absorbed', 'into', 'the', 'renormalized', 'coupling', 'constant', 'alpha', 'we', 'find', 't... | [-0.154673348589823, 0.19430635835430243, -0.045533492912044296, 0.10127583521179764, -0.038966002536187996, -0.10698855557001946, 0.042848369174795904, 0.33086805794353985, -0.2575984486923894, -0.2826851495518917, -0.044979856379341515, -0.40783580405092457, -0.11506249130385496, 0.07623404408691496, 0.07837851677180... |
706.2186 | Cosmic Acceleration, Dark Energy and Fundamental Physics | A web of interlocking observations has established that the expansion of the
Universe is speeding up and not slowing, revealing the presence of some form of
repulsive gravity. Within the context of general relativity the cause of cosmic
acceleration is a highly elastic (p\sim -rho), very smooth form of energy
called ... | astro-ph gr-qc hep-th | a web of interlocking observations has established that the expansion of the universe is speeding up and not slowing revealing the presence of some form of repulsive gravity within the context of general relativity the cause of cosmic acceleration is a highly elastic psim rho very smooth form of energy called dark ener... | [['a', 'web', 'of', 'interlocking', 'observations', 'has', 'established', 'that', 'the', 'expansion', 'of', 'the', 'universe', 'is', 'speeding', 'up', 'and', 'not', 'slowing', 'revealing', 'the', 'presence', 'of', 'some', 'form', 'of', 'repulsive', 'gravity', 'within', 'the', 'context', 'of', 'general', 'relativity', '... | [-0.12801570164510453, 0.1698113326445942, -0.09473358754716489, 0.16128835910690806, -0.12012507053314829, -0.13671713819190778, -0.023215154560444796, 0.30056211348552175, -0.22171894101927098, -0.3557511114821587, 0.061529982654737185, -0.25286202736036933, -0.06480563560667772, 0.22335630081437083, 0.02073220390340... |
706.2187 | Algebraic charge liquids | High temperature superconductivity emerges in the cuprate compounds upon
changing the electron density of an insulator in which the electron spins are
antiferromagnetically ordered. A key characteristic of the superconductor is
that electrons can be extracted from them at zero energy only if their momenta
take one of... | cond-mat.str-el cond-mat.supr-con | high temperature superconductivity emerges in the cuprate compounds upon changing the electron density of an insulator in which the electron spins are antiferromagnetically ordered a key characteristic of the superconductor is that electrons can be extracted from them at zero energy only if their momenta take one of fo... | [['high', 'temperature', 'superconductivity', 'emerges', 'in', 'the', 'cuprate', 'compounds', 'upon', 'changing', 'the', 'electron', 'density', 'of', 'an', 'insulator', 'in', 'which', 'the', 'electron', 'spins', 'are', 'antiferromagnetically', 'ordered', 'a', 'key', 'characteristic', 'of', 'the', 'superconductor', 'is'... | [-0.16901863457754573, 0.23877788461157418, -0.0908260865032394, 0.07329918114956528, -0.04019263142565475, -0.13807357095411038, 0.08459042753516273, 0.33383019767978034, -0.22413667472936014, -0.30555781936223175, -0.021340772064146214, -0.3623500316874448, -0.05192521290933305, 0.17087575644727815, 0.041278265496307... |
706.2188 | Black Hole Constraints on Varying Fundamental Constants | Here we apply the Generalized Second Law of Thermodynamics and derive upper
limits on the variation in the fundamental constants. The maximum variation in
the electronic charge permitted for black holes accreting and emitting in the
present cosmic microwave background corresponds to a variation in the fine
structure ... | astro-ph gr-qc hep-th | here we apply the generalized second law of thermodynamics and derive upper limits on the variation in the fundamental constants the maximum variation in the electronic charge permitted for black holes accreting and emitting in the present cosmic microwave background corresponds to a variation in the fine structure con... | [['here', 'we', 'apply', 'the', 'generalized', 'second', 'law', 'of', 'thermodynamics', 'and', 'derive', 'upper', 'limits', 'on', 'the', 'variation', 'in', 'the', 'fundamental', 'constants', 'the', 'maximum', 'variation', 'in', 'the', 'electronic', 'charge', 'permitted', 'for', 'black', 'holes', 'accreting', 'and', 'em... | [-0.103950658684319, 0.15494202848949887, 0.004134837622219261, 0.0839143982095188, -0.05741591862541564, -0.06447284118311995, 0.09868624285012087, 0.3346249776337534, -0.21247686933914317, -0.3754609013422135, 0.02170612491999178, -0.3261126212854969, -0.04602289629822716, 0.18998726944072528, -0.027534009190276265, ... |
706.2189 | Effects of Selection and Covariance on X-ray Scaling Relations of Galaxy
Clusters | We explore how the behavior of galaxy cluster scaling relations are affected
by flux-limited selection biases and intrinsic covariance among observable
properties. Our models presume log-normal covariance between luminosity (L) and
temperature (T) at fixed mass (M), centered on evolving, power-law mean
relations as a... | astro-ph | we explore how the behavior of galaxy cluster scaling relations are affected by fluxlimited selection biases and intrinsic covariance among observable properties our models presume lognormal covariance between luminosity l and temperature t at fixed mass m centered on evolving powerlaw mean relations as a function of h... | [['we', 'explore', 'how', 'the', 'behavior', 'of', 'galaxy', 'cluster', 'scaling', 'relations', 'are', 'affected', 'by', 'fluxlimited', 'selection', 'biases', 'and', 'intrinsic', 'covariance', 'among', 'observable', 'properties', 'our', 'models', 'presume', 'lognormal', 'covariance', 'between', 'luminosity', 'l', 'and'... | [-0.03261952571751129, 0.1388383224696642, -0.09072364194378738, 0.17081501550762163, -0.07950856738062875, -0.06540185082403402, 0.06328034594264483, 0.44401132899426643, -0.19573711212874662, -0.37785660169057306, 0.03958200643875546, -0.3474556050233303, -0.041907259196253314, 0.17811676068832316, 0.0131681434990417... |
706.219 | Bipolar spintronics: From spin injection to spin-controlled logic | An impressive success of spintronic applications has been typically realized
in metal-based structures which utilize magnetoresistive effects for
substantial improvements in the performance of computer hard drives and
magnetic random access memories. Correspondingly, the theoretical understanding
of spin-polarized tr... | cond-mat.other | an impressive success of spintronic applications has been typically realized in metalbased structures which utilize magnetoresistive effects for substantial improvements in the performance of computer hard drives and magnetic random access memories correspondingly the theoretical understanding of spinpolarized transpor... | [['an', 'impressive', 'success', 'of', 'spintronic', 'applications', 'has', 'been', 'typically', 'realized', 'in', 'metalbased', 'structures', 'which', 'utilize', 'magnetoresistive', 'effects', 'for', 'substantial', 'improvements', 'in', 'the', 'performance', 'of', 'computer', 'hard', 'drives', 'and', 'magnetic', 'rand... | [-0.17086726850495412, 0.11534280410884463, -0.014004961835655446, 0.05716870172147243, -0.10002918448717428, -0.18091505520536513, 0.03542197013167876, 0.4181215587534947, -0.28031578384239425, -0.3107231671581725, 0.032802991600411606, -0.2609462807997838, -0.1603605321588965, 0.2713601452515957, -0.04167927978602154... |
706.2191 | Phases of Dense Quarks at Large N_c | In the limit of a large number of colors, N_c, we suggest that gauge theories
can exhibit several distinct phases at nonzero temperature and quark density.
Two are familiar: a cold, dilute phase of confined hadrons, where the pressure
is ~ 1, and a hot phase of deconfined quarks and gluons, with pressure ~ N_c^2.
Whe... | hep-ph | in the limit of a large number of colors n_c we suggest that gauge theories can exhibit several distinct phases at nonzero temperature and quark density two are familiar a cold dilute phase of confined hadrons where the pressure is 1 and a hot phase of deconfined quarks and gluons with pressure n_c2 when the quark chem... | [['in', 'the', 'limit', 'of', 'a', 'large', 'number', 'of', 'colors', 'n_c', 'we', 'suggest', 'that', 'gauge', 'theories', 'can', 'exhibit', 'several', 'distinct', 'phases', 'at', 'nonzero', 'temperature', 'and', 'quark', 'density', 'two', 'are', 'familiar', 'a', 'cold', 'dilute', 'phase', 'of', 'confined', 'hadrons', ... | [-0.13812231357306518, 0.38674195180504234, -0.09068032593839156, 0.048881238015751394, -0.0042936454235684655, -0.11741567729612344, 0.09894556677871687, 0.35304433870717794, -0.17903964380887938, -0.24841363139756228, 0.022969649399722143, -0.3114618489553043, -0.02596935105618615, 0.03455796261300887, 0.047690206351... |
706.2192 | Analysis and packaging of radiochemical solar neutrino data. 1. Bayesian
approach | According to current practice, the results of each run of a radiochemical
solar neutrino experiment comprise an estimate of the flux and upper and lower
error estimates. These estimates are derived by a maximum-likelihood procedure
from the times of decay events in the analysis chamber. This procedure has the
followi... | hep-ph astro-ph gr-qc | according to current practice the results of each run of a radiochemical solar neutrino experiment comprise an estimate of the flux and upper and lower error estimates these estimates are derived by a maximumlikelihood procedure from the times of decay events in the analysis chamber this procedure has the following sho... | [['according', 'to', 'current', 'practice', 'the', 'results', 'of', 'each', 'run', 'of', 'a', 'radiochemical', 'solar', 'neutrino', 'experiment', 'comprise', 'an', 'estimate', 'of', 'the', 'flux', 'and', 'upper', 'and', 'lower', 'error', 'estimates', 'these', 'estimates', 'are', 'derived', 'by', 'a', 'maximumlikelihood... | [-0.051041310498424405, 0.09907928295865921, -0.07818032233975827, 0.1119991272707869, -0.03360359659418464, -0.08257945616596511, 0.08615309033609395, 0.3134468005437936, -0.21707859900913068, -0.35115024906716175, 0.1345985590546791, -0.2945522145155285, -0.08202097789118333, 0.24642320425249636, -0.09034395848001753... |
706.2193 | Linear pre-metric electrodynamics and deduction of the light cone | We formulate a general framework for describing the electromagnetic
properties of spacetime. These properties are encoded in the `constitutive
tensor of the vacuum', a quantity analogous to that used in the description of
material media. We give a generally covariant derivation of the Fresnel
equation describing the ... | gr-qc | we formulate a general framework for describing the electromagnetic properties of spacetime these properties are encoded in the constitutive tensor of the vacuum a quantity analogous to that used in the description of material media we give a generally covariant derivation of the fresnel equation describing the local p... | [['we', 'formulate', 'a', 'general', 'framework', 'for', 'describing', 'the', 'electromagnetic', 'properties', 'of', 'spacetime', 'these', 'properties', 'are', 'encoded', 'in', 'the', 'constitutive', 'tensor', 'of', 'the', 'vacuum', 'a', 'quantity', 'analogous', 'to', 'that', 'used', 'in', 'the', 'description', 'of', '... | [-0.15195349143797773, 0.14952724243504117, -0.11821651521376739, 0.06404131954616826, -0.11823588968558318, -0.06815101744596967, -0.04084785605348019, 0.33492440980373195, -0.2865408108191332, -0.22304597134327353, 0.0990716585656628, -0.22296028839849422, -0.2307039191895772, 0.15211306213219042, -0.0140022629132980... |
706.2194 | Nonlinear wave-wave interactions in stratified flows: Direct numerical
simulations | To investigate the formation mechanism of energy spectra of internal waves in
the oceans, direct numerical simulations are performed. The simulations are
based on the reduced dynamical equations of rotating stratified turbulence. In
the reduced dynamical equations only wave modes are retained, and vortices and
horizo... | physics.flu-dyn physics.ao-ph | to investigate the formation mechanism of energy spectra of internal waves in the oceans direct numerical simulations are performed the simulations are based on the reduced dynamical equations of rotating stratified turbulence in the reduced dynamical equations only wave modes are retained and vortices and horizontally... | [['to', 'investigate', 'the', 'formation', 'mechanism', 'of', 'energy', 'spectra', 'of', 'internal', 'waves', 'in', 'the', 'oceans', 'direct', 'numerical', 'simulations', 'are', 'performed', 'the', 'simulations', 'are', 'based', 'on', 'the', 'reduced', 'dynamical', 'equations', 'of', 'rotating', 'stratified', 'turbulen... | [-0.2004547525479012, 0.22040477790674115, -0.06027660489829743, 0.10325029838102392, -0.059420494797068235, -0.007237393606626312, -0.03157699543067074, 0.32100388583014994, -0.2421861727714163, -0.28579085261733156, 0.07227904982414848, -0.2661663387127283, -0.10441341753952457, 0.20613911491231757, 0.071979947474260... |
706.2195 | Updated analysis of NN elastic scattering to 3 GeV | A partial-wave analysis of NN elastic scattering data has been updated to
include a number of recent measurements. Experiments carried out at the Cooler
Synchrotron (COSY) by the EDDA Collaboration have had a significant impact
above 1 GeV. Results are discussed in terms of the partial-wave and
direct-reconstruction ... | nucl-th | a partialwave analysis of nn elastic scattering data has been updated to include a number of recent measurements experiments carried out at the cooler synchrotron cosy by the edda collaboration have had a significant impact above 1 gev results are discussed in terms of the partialwave and directreconstruction amplitude... | [['a', 'partialwave', 'analysis', 'of', 'nn', 'elastic', 'scattering', 'data', 'has', 'been', 'updated', 'to', 'include', 'a', 'number', 'of', 'recent', 'measurements', 'experiments', 'carried', 'out', 'at', 'the', 'cooler', 'synchrotron', 'cosy', 'by', 'the', 'edda', 'collaboration', 'have', 'had', 'a', 'significant',... | [-0.11066873168493523, 0.18429017030297123, -0.1412616702331666, 0.0439427977308948, -0.03716768193593685, -0.06281625210961446, 0.052380617272029535, 0.37571135789473004, -0.12508234932543116, -0.3052285333421636, 0.03944153422638377, -0.3855007042553514, -0.00937635970718049, 0.2196592993320937, 0.0965422326897053, 0... |
706.2196 | Operads of compatible structures and weighted partitions | In this paper we describe operads encoding two different kinds of
compatibility of algebraic structures. We show that there exist decompositions
of these in terms of black and white products and we prove that they are Koszul
for a large class of algebraic structures by using the poset method of B.
Vallette. In partic... | math.AT math.CO | in this paper we describe operads encoding two different kinds of compatibility of algebraic structures we show that there exist decompositions of these in terms of black and white products and we prove that they are koszul for a large class of algebraic structures by using the poset method of b vallette in particular ... | [['in', 'this', 'paper', 'we', 'describe', 'operads', 'encoding', 'two', 'different', 'kinds', 'of', 'compatibility', 'of', 'algebraic', 'structures', 'we', 'show', 'that', 'there', 'exist', 'decompositions', 'of', 'these', 'in', 'terms', 'of', 'black', 'and', 'white', 'products', 'and', 'we', 'prove', 'that', 'they', ... | [-0.17426418721941964, 0.07137722045715367, -0.05086075304342168, 0.1114066732432028, -0.08001946663217885, -0.09750195063783654, -0.038546648952511274, 0.42266459643308607, -0.36688066595899205, -0.2328063319570252, 0.10782244793372228, -0.20250571774584905, -0.23513628896325828, 0.1888005914565708, -0.160863904428801... |
706.2197 | The cycle of interstellar dust in galaxies of different morphological
types | By means of chemical evolution models for galaxies of different morphological
type, we have performed a detailed study of the evolution of the cosmic dust
properties in different environments: the solar neighbourhood, elliptical
galaxies and dwarf irregular galaxies. Starting from the same formalism as
developed by D... | astro-ph | by means of chemical evolution models for galaxies of different morphological type we have performed a detailed study of the evolution of the cosmic dust properties in different environments the solar neighbourhood elliptical galaxies and dwarf irregular galaxies starting from the same formalism as developed by dwek 19... | [['by', 'means', 'of', 'chemical', 'evolution', 'models', 'for', 'galaxies', 'of', 'different', 'morphological', 'type', 'we', 'have', 'performed', 'a', 'detailed', 'study', 'of', 'the', 'evolution', 'of', 'the', 'cosmic', 'dust', 'properties', 'in', 'different', 'environments', 'the', 'solar', 'neighbourhood', 'ellipt... | [-0.0020396747023013755, 0.09462913986635843, -0.09417042369732094, 0.1459018435845681, -0.04916757432777, -0.01170335905768242, 0.016211946752527493, 0.40746212661323056, -0.13772981806757487, -0.33321577836972127, 0.00901146487127233, -0.24935412179054645, -0.046275769757475646, 0.16447669811201693, -0.01628752015440... |
706.2198 | The effect of curvature and topology on membrane hydrodynamics | We study the mobility of extended objects (rods) on a spherical liquid-liquid
interface to show how this quantity is modified in a striking manner by both
the curvature and the topology of the interface. We present theoretical
calculations and experimental measurements of the interfacial fluid velocity
field around a... | cond-mat.soft | we study the mobility of extended objects rods on a spherical liquidliquid interface to show how this quantity is modified in a striking manner by both the curvature and the topology of the interface we present theoretical calculations and experimental measurements of the interfacial fluid velocity field around a movin... | [['we', 'study', 'the', 'mobility', 'of', 'extended', 'objects', 'rods', 'on', 'a', 'spherical', 'liquidliquid', 'interface', 'to', 'show', 'how', 'this', 'quantity', 'is', 'modified', 'in', 'a', 'striking', 'manner', 'by', 'both', 'the', 'curvature', 'and', 'the', 'topology', 'of', 'the', 'interface', 'we', 'present',... | [-0.16470257463657018, 0.1792008334440767, -0.13867845694597775, -0.0127833386503377, -0.043670722174919345, -0.1262999329200575, 0.01357087589663598, 0.3554728667984165, -0.25749346458814243, -0.2988380088767001, 0.05322954183087223, -0.2540032985502655, -0.13888640738390748, 0.13006363270885662, -0.05668807948896553,... |
706.2199 | Carrier-mediated magnetoelectricity in complex oxide heterostructures | While tremendous success has been achieved to date in creating both single
phase and composite magnetoelectric materials, the quintessential
electric-field control of magnetism remains elusive. In this work, we
demonstrate a linear magnetoelectric effect which arises from a novel
carrier-mediated mechanism, and is a ... | cond-mat.mtrl-sci | while tremendous success has been achieved to date in creating both single phase and composite magnetoelectric materials the quintessential electricfield control of magnetism remains elusive in this work we demonstrate a linear magnetoelectric effect which arises from a novel carriermediated mechanism and is a universa... | [['while', 'tremendous', 'success', 'has', 'been', 'achieved', 'to', 'date', 'in', 'creating', 'both', 'single', 'phase', 'and', 'composite', 'magnetoelectric', 'materials', 'the', 'quintessential', 'electricfield', 'control', 'of', 'magnetism', 'remains', 'elusive', 'in', 'this', 'work', 'we', 'demonstrate', 'a', 'lin... | [-0.19169199008377283, 0.11774549852001598, -0.07353495868238231, -0.0072838975030444855, -0.11029612490775313, -0.1345480244357403, 0.08255603322099278, 0.4016832744805362, -0.3036509279462355, -0.2960182468546188, -0.009155829494826379, -0.2574624176078483, -0.2210723795546732, 0.15717168101182896, 0.0143369447850570... |
706.22 | Searching for H->WW(*) and Other Diboson Final States at CDF | We report searches for standard model (SM) Higgs production decaying to WW(*)
and continuum ZZ production in the two charged lepton and two neutrino final
states. The data were collected with the CDF II detector at the Fermilab
Tevatron and correspond to an integrated luminosity of 1.1^fb-1. In order to
separate the ... | hep-ex | we report searches for standard model sm higgs production decaying to ww and continuum zz production in the two charged lepton and two neutrino final states the data were collected with the cdf ii detector at the fermilab tevatron and correspond to an integrated luminosity of 11fb1 in order to separate the processes co... | [['we', 'report', 'searches', 'for', 'standard', 'model', 'sm', 'higgs', 'production', 'decaying', 'to', 'ww', 'and', 'continuum', 'zz', 'production', 'in', 'the', 'two', 'charged', 'lepton', 'and', 'two', 'neutrino', 'final', 'states', 'the', 'data', 'were', 'collected', 'with', 'the', 'cdf', 'ii', 'detector', 'at', '... | [-0.031608231390806305, 0.15347433612581843, -0.03237041888135425, 0.13874900936343365, -0.004827725372726111, -0.13172182305707603, 0.07961772232615429, 0.2838377251001678, -0.12219881724981631, -0.36738184945349645, 0.015653758261205374, -0.41202635651708935, 0.0866157488944344, 0.10561996641763144, 0.093557062334374... |
706.2201 | Spin-waves in a complex magnetic system: nonextensive approach | In this paper we analyze the spin-wave excitations (magnons) of an
inhomogeneous spin system within the Boltzmann-Gibbs framework and then connect
the results with the nonextensive approach (in the sense of Tsallis
statistics). Considering an equivalence between those two frameworks, we could
connect the entropic par... | cond-mat.stat-mech | in this paper we analyze the spinwave excitations magnons of an inhomogeneous spin system within the boltzmanngibbs framework and then connect the results with the nonextensive approach in the sense of tsallis statistics considering an equivalence between those two frameworks we could connect the entropic parameter q w... | [['in', 'this', 'paper', 'we', 'analyze', 'the', 'spinwave', 'excitations', 'magnons', 'of', 'an', 'inhomogeneous', 'spin', 'system', 'within', 'the', 'boltzmanngibbs', 'framework', 'and', 'then', 'connect', 'the', 'results', 'with', 'the', 'nonextensive', 'approach', 'in', 'the', 'sense', 'of', 'tsallis', 'statistics'... | [-0.143120757806556, 0.1687619055006316, -0.14669622969813645, 0.06362602286849563, -0.036039553006718815, -0.06979861661889836, 0.016768196305125264, 0.30372720750931065, -0.3038010785699283, -0.2670184148745121, -0.023384570496426404, -0.33586306472946154, -0.1231163728034038, 0.15965643331506535, -0.0211360793664904... |
706.2202 | New metamaterials with macroscopic behavior outside that of continuum
elastodynamics | Metamaterials are constructed such that, for a narrow range of frequencies,
the momentum density depends on the local displacement gradient, and the stress
depends on the local velocity. In these models the momentum density generally
depends not only on the strain, but also on the local rotation, and the stress
is ge... | math-ph math.MP | metamaterials are constructed such that for a narrow range of frequencies the momentum density depends on the local displacement gradient and the stress depends on the local velocity in these models the momentum density generally depends not only on the strain but also on the local rotation and the stress is generally ... | [['metamaterials', 'are', 'constructed', 'such', 'that', 'for', 'a', 'narrow', 'range', 'of', 'frequencies', 'the', 'momentum', 'density', 'depends', 'on', 'the', 'local', 'displacement', 'gradient', 'and', 'the', 'stress', 'depends', 'on', 'the', 'local', 'velocity', 'in', 'these', 'models', 'the', 'momentum', 'densit... | [-0.15199787522746752, 0.19257416997033244, -0.08613463956862688, -0.003153353334010507, -0.10253580590002596, -0.07447440306602332, -0.02156856539659202, 0.39787084145399815, -0.26316887500266045, -0.24845264182211116, 0.1139317599120729, -0.20168272354819167, -0.13289678245424652, 0.24006285762879997, -0.045216917825... |
706.2203 | Entropy production in high-energy heavy-ion collisions and the
correlation of shear viscosity and thermalization time | We study entropy production in the early stage of high-energy heavy-ion
collisions due to shear viscosity. We employ the second-order theory of
Israel-Stewart with two different stress relaxation times, as appropriate for
strong coupling or for a Boltzmann gas, respectively, and compare the
hydrodynamic evolution. Ba... | nucl-th hep-ph hep-th nucl-ex | we study entropy production in the early stage of highenergy heavyion collisions due to shear viscosity we employ the secondorder theory of israelstewart with two different stress relaxation times as appropriate for strong coupling or for a boltzmann gas respectively and compare the hydrodynamic evolution based on pres... | [['we', 'study', 'entropy', 'production', 'in', 'the', 'early', 'stage', 'of', 'highenergy', 'heavyion', 'collisions', 'due', 'to', 'shear', 'viscosity', 'we', 'employ', 'the', 'secondorder', 'theory', 'of', 'israelstewart', 'with', 'two', 'different', 'stress', 'relaxation', 'times', 'as', 'appropriate', 'for', 'stron... | [-0.12251779832339164, 0.20483119548944084, -0.15695408435867114, 0.0783682776431107, -0.006524385567441457, -0.09890831610532243, -0.011936767544292164, 0.24924425355808325, -0.25137833407845256, -0.26158555672198786, 0.058977066506944724, -0.2863999429244955, -0.004063522120342911, 0.18195957504701996, 0.015681020590... |
706.2204 | Gorenstein Multiple Structures on Smooth Algebraic Varieties | We characterize the Gorenstein nilpotent scheme structures on a smooth
algebraic variety as support, in terms of a duality property of the graded
objects associated to two canonical filtrations.
| math.AG math.AC | we characterize the gorenstein nilpotent scheme structures on a smooth algebraic variety as support in terms of a duality property of the graded objects associated to two canonical filtrations | [['we', 'characterize', 'the', 'gorenstein', 'nilpotent', 'scheme', 'structures', 'on', 'a', 'smooth', 'algebraic', 'variety', 'as', 'support', 'in', 'terms', 'of', 'a', 'duality', 'property', 'of', 'the', 'graded', 'objects', 'associated', 'to', 'two', 'canonical', 'filtrations']] | [-0.2030180031112556, -0.005198342500832574, -0.12334812015038112, 0.12513743360237828, -0.12381749150568042, -0.13179556630423356, -0.06611111406879179, 0.379874913856901, -0.4086834582789191, -0.137366804904465, 0.09775452826830462, -0.16718319919088792, -0.1731854745283209, 0.1974397449400918, -0.22035595292932, -0.... |
706.2205 | Role of resonances in rho^0 -> pi^+ pi^- gamma | We study the effect of the sigma(600) and a_1(1260) resonances in the rho^0
-> pi^+ pi^- gamma decay, within the meson dominance model. Major effects are
driven by the mass and width parameters of the sigma(600), and the usually
neglected contribution of the a_1(1260), although small by itself, may become
sizable thr... | hep-ph | we study the effect of the sigma600 and a_11260 resonances in the rho0 pi pi gamma decay within the meson dominance model major effects are driven by the mass and width parameters of the sigma600 and the usually neglected contribution of the a_11260 although small by itself may become sizable through its interference w... | [['we', 'study', 'the', 'effect', 'of', 'the', 'sigma600', 'and', 'a_11260', 'resonances', 'in', 'the', 'rho0', 'pi', 'pi', 'gamma', 'decay', 'within', 'the', 'meson', 'dominance', 'model', 'major', 'effects', 'are', 'driven', 'by', 'the', 'mass', 'and', 'width', 'parameters', 'of', 'the', 'sigma600', 'and', 'the', 'us... | [-0.14477769460661824, 0.23340717810162595, -0.07854739749351534, 0.11016080670372069, -0.06976810878438648, -0.07121239196961728, 0.09666391519751295, 0.34039668477723534, -0.23217686786203184, -0.25661727432683806, -0.011446962550839532, -0.2770273288990432, -0.0631724548587036, 0.11629166039551182, 0.073793702652225... |
706.2206 | A Case Study of Low-Mass Star Formation | This article synthesizes observational data from an extensive program aimed
toward a comprehensive understanding of star formation in a low-mass
star-forming molecular cloud. New observations and published data spanning from
the centimeter wave band to the near infrared reveal the high and low density
molecular gas, ... | astro-ph | this article synthesizes observational data from an extensive program aimed toward a comprehensive understanding of star formation in a lowmass starforming molecular cloud new observations and published data spanning from the centimeter wave band to the near infrared reveal the high and low density molecular gas dust a... | [['this', 'article', 'synthesizes', 'observational', 'data', 'from', 'an', 'extensive', 'program', 'aimed', 'toward', 'a', 'comprehensive', 'understanding', 'of', 'star', 'formation', 'in', 'a', 'lowmass', 'starforming', 'molecular', 'cloud', 'new', 'observations', 'and', 'published', 'data', 'spanning', 'from', 'the',... | [-0.06929622372757327, 0.057226055629281236, -0.08658068269087037, 0.049169366974998616, -0.08451304049231112, 0.01123478346205545, 0.11012668932462989, 0.41479051394282646, -0.17684938690080396, -0.3624172884232874, 0.059986308704675084, -0.2694099243150426, -0.028959058699602226, 0.1378735491856581, -0.00702008735037... |
706.2207 | Relationship between Hawking radiation from black holes and spontaneous
excitation of atoms | Using the formalism that separates the contributions of vacuum fluctuations
and radiation reaction to the rate of change of the mean atomic energy, we show
that a two-level atom in interaction with a quantum massless scalar field both
in the Hartle-Hawking and Unruh vacuum in a 1+1 dimensional black hole
background s... | hep-th gr-qc | using the formalism that separates the contributions of vacuum fluctuations and radiation reaction to the rate of change of the mean atomic energy we show that a twolevel atom in interaction with a quantum massless scalar field both in the hartlehawking and unruh vacuum in a 11 dimensional black hole background spontan... | [['using', 'the', 'formalism', 'that', 'separates', 'the', 'contributions', 'of', 'vacuum', 'fluctuations', 'and', 'radiation', 'reaction', 'to', 'the', 'rate', 'of', 'change', 'of', 'the', 'mean', 'atomic', 'energy', 'we', 'show', 'that', 'a', 'twolevel', 'atom', 'in', 'interaction', 'with', 'a', 'quantum', 'massless'... | [-0.11913336691454299, 0.21609951988678455, -0.08159018679900087, 0.08064940812793553, -0.011189035401671878, -0.13030513321734533, 0.014300302261763737, 0.3233341482306315, -0.17967064086009155, -0.26218917990519, -6.790662930955078e-05, -0.35164176352506826, -0.04813921148311501, 0.15568659211747532, 0.00100464472347... |
706.2208 | Contractions, deformations and curvature | The role of curvature in relation with Lie algebra contractions of the
pseudo-ortogonal algebras so(p,q) is fully described by considering some
associated symmetrical homogeneous spaces of constant curvature within a
Cayley-Klein framework. We show that a given Lie algebra contraction can be
interpreted geometrically... | math-ph math.MP math.QA | the role of curvature in relation with lie algebra contractions of the pseudoortogonal algebras sopq is fully described by considering some associated symmetrical homogeneous spaces of constant curvature within a cayleyklein framework we show that a given lie algebra contraction can be interpreted geometrically as the ... | [['the', 'role', 'of', 'curvature', 'in', 'relation', 'with', 'lie', 'algebra', 'contractions', 'of', 'the', 'pseudoortogonal', 'algebras', 'sopq', 'is', 'fully', 'described', 'by', 'considering', 'some', 'associated', 'symmetrical', 'homogeneous', 'spaces', 'of', 'constant', 'curvature', 'within', 'a', 'cayleyklein', ... | [-0.15503467654921643, 0.1521544738586807, -0.06308694555694964, 0.10646213585779854, -0.11226722584865617, -0.10412797493635552, -0.08862705619226321, 0.3762715147108051, -0.29687335346792393, -0.1984052892166672, 0.13821399768200168, -0.20416224748556708, -0.17941112088449035, 0.1771774547115127, -0.09942401788265161... |
706.2209 | SU(3) Ghosts with Spin | A new Lorentz-covariant gauge is presented for SU(3). In this gauge, both the
ghosts and the gauge fields in the (4, 5, 6, 7) gauge directions acquire
half-integral spin. As a result, the ghosts in these directions have the
correct relationship between spin and statistics, while the gauge fields have
the incorrect re... | hep-th | a new lorentzcovariant gauge is presented for su3 in this gauge both the ghosts and the gauge fields in the 4 5 6 7 gauge directions acquire halfintegral spin as a result the ghosts in these directions have the correct relationship between spin and statistics while the gauge fields have the incorrect relationship conse... | [['a', 'new', 'lorentzcovariant', 'gauge', 'is', 'presented', 'for', 'su3', 'in', 'this', 'gauge', 'both', 'the', 'ghosts', 'and', 'the', 'gauge', 'fields', 'in', 'the', '4', '5', '6', '7', 'gauge', 'directions', 'acquire', 'halfintegral', 'spin', 'as', 'a', 'result', 'the', 'ghosts', 'in', 'these', 'directions', 'have... | [-0.17659599072661022, 0.2988573833648175, -0.08841888580414257, 0.1357304016496435, -0.09205023203121156, -0.12109305386488535, -0.0045980581234456325, 0.38427322578369355, -0.17218399369612228, -0.3243503993833248, 0.08319195377288804, -0.23834101113072614, -0.10200195169380429, 0.029637849267230044, -0.0039052387262... |
706.221 | A Mathematica script for harmonic oscillator nuclear matrix elements
arising in semileptonic electroweak interactions | Semi-leptonic electroweak interactions in nuclei - such as \beta decay, \mu
capture, charged- and neutral-current neutrino reactions, and electron
scattering - are described by a set of multipole operators carrying definite
parity and angular momentum, obtained by projection from the underlying nuclear
charge and thr... | nucl-th | semileptonic electroweak interactions in nuclei such as beta decay mu capture charged and neutralcurrent neutrino reactions and electron scattering are described by a set of multipole operators carrying definite parity and angular momentum obtained by projection from the underlying nuclear charge and threecurrent opera... | [['semileptonic', 'electroweak', 'interactions', 'in', 'nuclei', 'such', 'as', 'beta', 'decay', 'mu', 'capture', 'charged', 'and', 'neutralcurrent', 'neutrino', 'reactions', 'and', 'electron', 'scattering', 'are', 'described', 'by', 'a', 'set', 'of', 'multipole', 'operators', 'carrying', 'definite', 'parity', 'and', 'a... | [-0.0844067967545925, 0.20524469867268635, -0.03453541123440118, 0.09886296264676275, -0.03333396771063235, -0.08546668352528286, 0.016217686386880814, 0.3526325259172154, -0.23651562380837277, -0.2515697294547863, 0.03504451045000678, -0.29991012023907615, -0.07149604750884464, 0.15717350355953386, 0.06881312762197922... |
706.2211 | Holographic hessence models | We discuss the evolution of holographic hessence model, which satisfies the
holographic principle and can naturally realizes the equation of state crossing
-1. By discussing the evolution of the models in the $w w'$ plane, we find
that, if $c\geq1$, $w_{he}\geq-1$ and $\dot{V}<0$ keep for all time, which are
quintess... | astro-ph | we discuss the evolution of holographic hessence model which satisfies the holographic principle and can naturally realizes the equation of state crossing 1 by discussing the evolution of the models in the w w plane we find that if cgeq1 w_hegeq1 and dotv0 keep for all time which are quintessencelike however if c1 whic... | [['we', 'discuss', 'the', 'evolution', 'of', 'holographic', 'hessence', 'model', 'which', 'satisfies', 'the', 'holographic', 'principle', 'and', 'can', 'naturally', 'realizes', 'the', 'equation', 'of', 'state', 'crossing', '1', 'by', 'discussing', 'the', 'evolution', 'of', 'the', 'models', 'in', 'the', 'w', 'w', 'plane... | [-0.11201803020267474, 0.155728318427473, -0.10991496684951614, 0.028490013380316228, -0.07603061272094798, -0.1566937457948848, 0.022534359857966802, 0.3116038168281919, -0.28914953781423547, -0.30269438569255247, 0.10523922016815931, -0.2654539689967277, -0.08000297767270093, 0.139445037910282, 0.02256628042181032, 0... |
706.2212 | Predicting the progress of diffusively limited chemical reactions in the
presence of chaotic advection | The effects of chaotic advection and diffusion on fast chemical reactions in
two-dimensional fluid flows are investigated using experimentally measured
stretching fields and fluorescent monitoring of the local concentration. Flow
symmetry, Reynolds number, and mean path length affect the spatial distribution
and time... | physics.flu-dyn physics.chem-ph | the effects of chaotic advection and diffusion on fast chemical reactions in twodimensional fluid flows are investigated using experimentally measured stretching fields and fluorescent monitoring of the local concentration flow symmetry reynolds number and mean path length affect the spatial distribution and time depen... | [['the', 'effects', 'of', 'chaotic', 'advection', 'and', 'diffusion', 'on', 'fast', 'chemical', 'reactions', 'in', 'twodimensional', 'fluid', 'flows', 'are', 'investigated', 'using', 'experimentally', 'measured', 'stretching', 'fields', 'and', 'fluorescent', 'monitoring', 'of', 'the', 'local', 'concentration', 'flow', ... | [-0.17822039160854752, 0.24017348751516604, -0.07853322605092772, 0.02793608266269652, 0.0004041919437884467, -0.1171491931479356, -0.01726005709639228, 0.3279583369177289, -0.33525722477267067, -0.29265421529005214, 0.0495783261395423, -0.26958438608704544, -0.08519751544780575, 0.16810170611048617, 0.0352106168695793... |
706.2213 | Non-abelian Reidemeister torsion for twist knots | This paper gives an explicit formula for the SL_2(C)-non-abelian Reidemeister
torsion as defined in [Dub06] in the case of twist knots. For hyperbolic twist
knots, we also prove that the non-abelian Reidemeister torsion at the holonomy
representation can be expressed as a rational function evaluated at the cusp
shape... | math.GT | this paper gives an explicit formula for the sl_2cnonabelian reidemeister torsion as defined in dub06 in the case of twist knots for hyperbolic twist knots we also prove that the nonabelian reidemeister torsion at the holonomy representation can be expressed as a rational function evaluated at the cusp shape of the kno... | [['this', 'paper', 'gives', 'an', 'explicit', 'formula', 'for', 'the', 'sl_2cnonabelian', 'reidemeister', 'torsion', 'as', 'defined', 'in', 'dub06', 'in', 'the', 'case', 'of', 'twist', 'knots', 'for', 'hyperbolic', 'twist', 'knots', 'we', 'also', 'prove', 'that', 'the', 'nonabelian', 'reidemeister', 'torsion', 'at', 't... | [-0.2563493933901191, 0.10956619429663988, -0.131734717823565, 0.12456556564895437, -0.12467639718204737, -0.12110739856027067, -0.04824676971649751, 0.3330560614168644, -0.27946857623755933, -0.2668593302369118, 0.00243269604165107, -0.18975540003739297, -0.18388803478330373, 0.20697032548487188, -0.12507352391898166,... |
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