id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
710.1153 | Verification of Ptime Reducibility for system F Terms: Type Inference
in<br> Dual Light Affine Logic | In a previous work Baillot and Terui introduced Dual light affine logic
(DLAL) as a variant of Light linear logic suitable for guaranteeing complexity
properties on lambda calculus terms: all typable terms can be evaluated in
polynomial time by beta reduction and all Ptime functions can be represented.
In the present... | cs.LO cs.CC | in a previous work baillot and terui introduced dual light affine logic dlal as a variant of light linear logic suitable for guaranteeing complexity properties on lambda calculus terms all typable terms can be evaluated in polynomial time by beta reduction and all ptime functions can be represented in the present work ... | [['in', 'a', 'previous', 'work', 'baillot', 'and', 'terui', 'introduced', 'dual', 'light', 'affine', 'logic', 'dlal', 'as', 'a', 'variant', 'of', 'light', 'linear', 'logic', 'suitable', 'for', 'guaranteeing', 'complexity', 'properties', 'on', 'lambda', 'calculus', 'terms', 'all', 'typable', 'terms', 'can', 'be', 'evalu... | [-0.1371875512949397, 0.05281462333684342, -0.08191393061944868, 0.06867878840910682, -0.10340661220087678, -0.18250919353892714, 0.05598097429116281, 0.3457932591570162, -0.33857188968037344, -0.2669532232695317, 0.08017675337521771, -0.1949332319035203, -0.14761163952010395, 0.19802641838920854, -0.1323242429108153, ... |
710.1154 | Dynamically induced scalar quark confinement: A link between chiral
symmetry breaking and confinement | Employing functional approaches the infrared behaviour of Landau gauge QCD
vertex functions is investigated. Results for the ghost-gluon, three-gluon and
quark-gluon vertex functions are presented. As can be analytically shown a
linear rising potential between heavy quarks is generated by infrared
singularities in th... | hep-ph hep-lat | employing functional approaches the infrared behaviour of landau gauge qcd vertex functions is investigated results for the ghostgluon threegluon and quarkgluon vertex functions are presented as can be analytically shown a linear rising potential between heavy quarks is generated by infrared singularities in the dresse... | [['employing', 'functional', 'approaches', 'the', 'infrared', 'behaviour', 'of', 'landau', 'gauge', 'qcd', 'vertex', 'functions', 'is', 'investigated', 'results', 'for', 'the', 'ghostgluon', 'threegluon', 'and', 'quarkgluon', 'vertex', 'functions', 'are', 'presented', 'as', 'can', 'be', 'analytically', 'shown', 'a', 'l... | [-0.14553848859737628, 0.2828857906849589, -0.13386836111079903, 0.11484129378921352, -0.13083933699410408, -0.13724611725658178, 0.015128897430840879, 0.37855659471824765, -0.21557614847784862, -0.1869633708242327, -0.010537266671890392, -0.29698369972757066, -0.157911258044187, 0.04230937893735245, 0.0630453669582493... |
710.1155 | A note on local trigonal fibrations | We show that some of centeral fibers of degenerations of hyperelliptic curves
are realized as those trigonal curves. In particular, any hyperelliptic curve
can be the central fiber of a degeneration of trigonal curves.
| math.AG math.GT | we show that some of centeral fibers of degenerations of hyperelliptic curves are realized as those trigonal curves in particular any hyperelliptic curve can be the central fiber of a degeneration of trigonal curves | [['we', 'show', 'that', 'some', 'of', 'centeral', 'fibers', 'of', 'degenerations', 'of', 'hyperelliptic', 'curves', 'are', 'realized', 'as', 'those', 'trigonal', 'curves', 'in', 'particular', 'any', 'hyperelliptic', 'curve', 'can', 'be', 'the', 'central', 'fiber', 'of', 'a', 'degeneration', 'of', 'trigonal', 'curves']] | [-0.31662830532613123, 0.07391123287379742, -0.18048981859376936, 0.0578480094219699, -0.07740935993691285, -0.18596644579630459, -0.005930875787850131, 0.44781321563729737, -0.29714885325820156, -0.14811144899012466, 0.1069377113775717, -0.25477133138161717, -0.22946120177706084, 0.3938876273618503, -0.248574766669083... |
710.1156 | Eigenmode of Decision-By-Majority Process on Complex Networks | The nature of dynamics of opinion formation modeled as a decision-by-majority
process in complex networks is investigated using eigenmode analysis.
Hamiltonian of the system is defined, and estimated by eigenvectors of the
adjacency matrix constructed from several network models. The eigenmodes of
initial and final s... | cond-mat.dis-nn | the nature of dynamics of opinion formation modeled as a decisionbymajority process in complex networks is investigated using eigenmode analysis hamiltonian of the system is defined and estimated by eigenvectors of the adjacency matrix constructed from several network models the eigenmodes of initial and final state of... | [['the', 'nature', 'of', 'dynamics', 'of', 'opinion', 'formation', 'modeled', 'as', 'a', 'decisionbymajority', 'process', 'in', 'complex', 'networks', 'is', 'investigated', 'using', 'eigenmode', 'analysis', 'hamiltonian', 'of', 'the', 'system', 'is', 'defined', 'and', 'estimated', 'by', 'eigenvectors', 'of', 'the', 'ad... | [-0.1499615387149053, 0.08642255657748, -0.046734220699139246, 0.05498808217390894, 0.047914698388274404, -0.047068676037382184, -0.0212265459425135, 0.35354954060422233, -0.27256470827436813, -0.2822670036231563, 0.14431720067370582, -0.2699135239299846, -0.18825429626931883, 0.1341442719408094, 0.06896184967856293, 0... |
710.1157 | Multipartite circulant states with positive partial transposes | We construct a large class of multipartite qudit states which are positive
under the family of partial transpositions. The construction is based on
certain direct sum decomposition of the total Hilbert space displaying
characteristic circular structure and hence generalizes a class of bipartite
circulant states propo... | quant-ph | we construct a large class of multipartite qudit states which are positive under the family of partial transpositions the construction is based on certain direct sum decomposition of the total hilbert space displaying characteristic circular structure and hence generalizes a class of bipartite circulant states proposed... | [['we', 'construct', 'a', 'large', 'class', 'of', 'multipartite', 'qudit', 'states', 'which', 'are', 'positive', 'under', 'the', 'family', 'of', 'partial', 'transpositions', 'the', 'construction', 'is', 'based', 'on', 'certain', 'direct', 'sum', 'decomposition', 'of', 'the', 'total', 'hilbert', 'space', 'displaying', '... | [-0.14253923788666725, 0.15263117597981665, -0.024189343353112538, 0.020562866777181624, -0.08253788839404781, -0.13493382768705486, 0.008913023443892599, 0.28247442916035653, -0.26599910591418546, -0.2807131391763687, 0.08111428578384221, -0.2591139644756913, -0.17521083577225605, 0.20220438895126183, -0.0740373285363... |
710.1158 | Why the $a_1$ meson might be a difficult messenger for the restoration
of chiral symmetry | We perform a theoretical analysis of the $a_1$ resonance mass spectrum in
ultra-relativistic heavy ion collisions within a hadron/string transport
approach. Predictions for the $a_1$ yield and its mass distribution are given
for the GSI-FAIR and the critRHIC energy regime. The potential of the $a_1$
meson as a signal... | hep-ph | we perform a theoretical analysis of the a_1 resonance mass spectrum in ultrarelativistic heavy ion collisions within a hadronstring transport approach predictions for the a_1 yield and its mass distribution are given for the gsifair and the critrhic energy regime the potential of the a_1 meson as a signal for chiral s... | [['we', 'perform', 'a', 'theoretical', 'analysis', 'of', 'the', 'a_1', 'resonance', 'mass', 'spectrum', 'in', 'ultrarelativistic', 'heavy', 'ion', 'collisions', 'within', 'a', 'hadronstring', 'transport', 'approach', 'predictions', 'for', 'the', 'a_1', 'yield', 'and', 'its', 'mass', 'distribution', 'are', 'given', 'for... | [-0.12014116114424961, 0.19133295038681444, -0.1014277473603887, 0.1145162695561544, -0.03684093647317642, -0.1568411098507879, 0.026269327387683564, 0.3707933636667492, -0.24727344452948855, -0.2492053516477615, 0.05810503553397752, -0.2875531020465198, -0.01516599123794082, 0.09697251108196839, 0.022765010661444377, ... |
710.1159 | SmB$_6$: Topological insulator or semiconductor with valence-fluctuation
induced hopping transport? | We advert to the fact that presence of valence fluctuations (VFs) in
semiconductors with in-gap impurity bands unconditionally leads to dynamical
changes (fluctuations) of energies of localized impurity states. We provide
arguments that in the impurity subnetwork consisting of centers having energy
levels fluctuating... | cond-mat.str-el | we advert to the fact that presence of valence fluctuations vfs in semiconductors with ingap impurity bands unconditionally leads to dynamical changes fluctuations of energies of localized impurity states we provide arguments that in the impurity subnetwork consisting of centers having energy levels fluctuating around ... | [['we', 'advert', 'to', 'the', 'fact', 'that', 'presence', 'of', 'valence', 'fluctuations', 'vfs', 'in', 'semiconductors', 'with', 'ingap', 'impurity', 'bands', 'unconditionally', 'leads', 'to', 'dynamical', 'changes', 'fluctuations', 'of', 'energies', 'of', 'localized', 'impurity', 'states', 'we', 'provide', 'argument... | [-0.19152602065506197, 0.24301021204008758, -0.06563752078335704, 0.10564647595192371, -0.01126269736081766, -0.21426197085547616, 0.14198091659287004, 0.36459994740069435, -0.24670049905235059, -0.30442806832896646, -0.060944424487303854, -0.3528821803521105, -0.12340566772938699, 0.10399385979904453, -0.0171079574253... |
710.116 | Self-consistent simulation of quantum wires defined by local oxidation
of Ga[Al]As heterostructures | We calculate the electronic width of quantum wires as a function of their
lithographic width in analogy to experiments performed on nanostructures
defined by local oxidation of Ga[Al]As heterostructures. Two--dimensional
simulations of two parallel oxide lines on top of a Ga[Al]As heterostructure
defining a quantum w... | cond-mat.mes-hall | we calculate the electronic width of quantum wires as a function of their lithographic width in analogy to experiments performed on nanostructures defined by local oxidation of gaalas heterostructures twodimensional simulations of two parallel oxide lines on top of a gaalas heterostructure defining a quantum wire are c... | [['we', 'calculate', 'the', 'electronic', 'width', 'of', 'quantum', 'wires', 'as', 'a', 'function', 'of', 'their', 'lithographic', 'width', 'in', 'analogy', 'to', 'experiments', 'performed', 'on', 'nanostructures', 'defined', 'by', 'local', 'oxidation', 'of', 'gaalas', 'heterostructures', 'twodimensional', 'simulations... | [-0.13574336047902286, 0.1095361797417575, -0.06075161040072965, 0.010997177194151157, 0.01570903920681677, -0.1259269340781965, 0.07826774871895072, 0.4118765975722921, -0.2161765848471409, -0.3165723893129937, 0.02559376924372687, -0.3041574063441046, -0.11121565179255243, 0.20210798794978133, 0.050028533696536426, 0... |
710.1161 | Finite Size Scaling for the O(N) universality class from Renormalization
Group Methods | The QCD phase diagram at finite temperature and density is a topic of
considerable interest. Although much progress has been made in recent years,
some open questions remain. Even at zero density, the order of the transition
for two light flavors of fermions has not yet been conclusively established.
While considerab... | hep-lat | the qcd phase diagram at finite temperature and density is a topic of considerable interest although much progress has been made in recent years some open questions remain even at zero density the order of the transition for two light flavors of fermions has not yet been conclusively established while considerable evid... | [['the', 'qcd', 'phase', 'diagram', 'at', 'finite', 'temperature', 'and', 'density', 'is', 'a', 'topic', 'of', 'considerable', 'interest', 'although', 'much', 'progress', 'has', 'been', 'made', 'in', 'recent', 'years', 'some', 'open', 'questions', 'remain', 'even', 'at', 'zero', 'density', 'the', 'order', 'of', 'the', ... | [-0.10860704611547131, 0.20082251561179343, -0.11777466194224918, 0.057309614994518976, -0.04536472348645873, -0.1066371104323108, 0.08562045913940826, 0.3652616489625937, -0.18729299766242669, -0.2731689915101785, 0.12341149284777972, -0.3038781030684791, -0.10366075543387637, 0.1886976351477138, 0.05354507718520769, ... |
710.1162 | On the Effective Action of Noncommutative Yang-Mills Theory | We compute here the Yang-Mills effective action on Moyal space by integrating
over the scalar fields in a noncommutative scalar field theory with harmonic
term, minimally coupled to an external gauge potential. We also explain the
special regularisation scheme chosen here and give some links to the Schwinger
parametr... | hep-th math-ph math.MP | we compute here the yangmills effective action on moyal space by integrating over the scalar fields in a noncommutative scalar field theory with harmonic term minimally coupled to an external gauge potential we also explain the special regularisation scheme chosen here and give some links to the schwinger parametric re... | [['we', 'compute', 'here', 'the', 'yangmills', 'effective', 'action', 'on', 'moyal', 'space', 'by', 'integrating', 'over', 'the', 'scalar', 'fields', 'in', 'a', 'noncommutative', 'scalar', 'field', 'theory', 'with', 'harmonic', 'term', 'minimally', 'coupled', 'to', 'an', 'external', 'gauge', 'potential', 'we', 'also', ... | [-0.14649373199790716, 0.18958416456688051, -0.08110604191859884, 0.10944613108351346, -0.12851988674411852, -0.1456709922772021, -0.010104055039494509, 0.36043662573361107, -0.21130520339694717, -0.22477282400453283, 0.052339291836570705, -0.21793032068413712, -0.25155071448534727, 0.1442109578769774, -0.0763146480462... |
710.1163 | Bimonads and Hopf monads on categories | The purpose of this paper is to develop a theory of bimonads and Hopf monads
on arbitrary categories thus providing the possibility to transfer the
essentials of the theory of Hopf algebras in vector spaces to more general
settings. There are several extensions of this theory to {\em monoidal}
categories which in a c... | math.QA math.CT | the purpose of this paper is to develop a theory of bimonads and hopf monads on arbitrary categories thus providing the possibility to transfer the essentials of the theory of hopf algebras in vector spaces to more general settings there are several extensions of this theory to em monoidal categories which in a certain... | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'develop', 'a', 'theory', 'of', 'bimonads', 'and', 'hopf', 'monads', 'on', 'arbitrary', 'categories', 'thus', 'providing', 'the', 'possibility', 'to', 'transfer', 'the', 'essentials', 'of', 'the', 'theory', 'of', 'hopf', 'algebras', 'in', 'vector', 'spaces', 'to', ... | [-0.13382261884337945, 0.05791610321281964, -0.07315060339517085, 0.1027055106880734, -0.14701660382370255, -0.14791428334941503, 0.02118082814884664, 0.3610782644419528, -0.3918696054806516, -0.20373047880329706, 0.07829315984689408, -0.19080898135469587, -0.152937581403869, 0.15462861632069907, -0.1566129082275981, -... |
710.1164 | Recent progress on color confinement | The status is reviewed of the dual superconductivity of QCD vacuum as a
mechanism of color confinement.
| hep-lat | the status is reviewed of the dual superconductivity of qcd vacuum as a mechanism of color confinement | [['the', 'status', 'is', 'reviewed', 'of', 'the', 'dual', 'superconductivity', 'of', 'qcd', 'vacuum', 'as', 'a', 'mechanism', 'of', 'color', 'confinement']] | [-0.13362732025630333, 0.2786896401906715, -0.11358563645797617, 0.09398658883840065, -0.07268959974103115, -0.09545264236957711, 0.06158969682805678, 0.34719320079859567, -0.18114662937381687, -0.17274185116676724, 0.0815636949504123, -0.22653273942277713, -0.07493026970940478, 0.01736282053239205, -0.0628194756915464... |
710.1165 | Unbiased estimates of galaxy scaling relations from photometric redshift
surveys | Many physical properties of galaxies correlate with one another, and these
correlations are often used to constrain galaxy formation models. Such
correlations include the color-magnitude relation, the luminosity-size
relation, the Fundamental Plane, etc. However, the transformation from
observable (e.g. angular size,... | astro-ph | many physical properties of galaxies correlate with one another and these correlations are often used to constrain galaxy formation models such correlations include the colormagnitude relation the luminositysize relation the fundamental plane etc however the transformation from observable eg angular size apparent brigh... | [['many', 'physical', 'properties', 'of', 'galaxies', 'correlate', 'with', 'one', 'another', 'and', 'these', 'correlations', 'are', 'often', 'used', 'to', 'constrain', 'galaxy', 'formation', 'models', 'such', 'correlations', 'include', 'the', 'colormagnitude', 'relation', 'the', 'luminositysize', 'relation', 'the', 'fu... | [-0.03966205527859868, 0.055257119268811994, -0.13529348300976884, 0.17850190452284795, -0.15202196167623686, -0.11309464630713455, 0.035398041022929295, 0.4125010097776753, -0.24942401882407128, -0.3621142411884529, 0.06695782513132477, -0.29795179167896313, -0.10541913607743648, 0.23101587921648828, -0.06919138435749... |
710.1166 | Track Based Alignment of the ATLAS Silicon Detectors with the Robust
Alignment Algorithm | The Robust Alignment algorithm for the ATLAS silicon detectors is presented.
It is an iterative method based on centering residual and overlap residual
distributions. Tests on simulated and real data are discussed.
| physics.ins-det | the robust alignment algorithm for the atlas silicon detectors is presented it is an iterative method based on centering residual and overlap residual distributions tests on simulated and real data are discussed | [['the', 'robust', 'alignment', 'algorithm', 'for', 'the', 'atlas', 'silicon', 'detectors', 'is', 'presented', 'it', 'is', 'an', 'iterative', 'method', 'based', 'on', 'centering', 'residual', 'and', 'overlap', 'residual', 'distributions', 'tests', 'on', 'simulated', 'and', 'real', 'data', 'are', 'discussed']] | [-0.0523742282675812, 0.025828929054569016, -0.12009093107189983, 0.09191917573480168, 0.00860497506801039, -0.15853548480663449, -0.04093375359661877, 0.5084397702012211, -0.20155875658383593, -0.31847703544190153, 0.1501411244389601, -0.3242580845981138, -0.15923920911882306, 0.23528609867207706, -0.0604439465678297,... |
710.1167 | Planetary Stability Zones in Hierarchical Triple Star Systems | A symplectic integrator algorithm suitable for hierarchical triple systems is
formulated and tested. The positions of the stars are followed in hierarchical
Jacobi coordinates, whilst the planets are referenced purely to their primary.
The algorithm is fast, accurate and easily generalised to incorporate
collisions. ... | astro-ph | a symplectic integrator algorithm suitable for hierarchical triple systems is formulated and tested the positions of the stars are followed in hierarchical jacobi coordinates whilst the planets are referenced purely to their primary the algorithm is fast accurate and easily generalised to incorporate collisions there a... | [['a', 'symplectic', 'integrator', 'algorithm', 'suitable', 'for', 'hierarchical', 'triple', 'systems', 'is', 'formulated', 'and', 'tested', 'the', 'positions', 'of', 'the', 'stars', 'are', 'followed', 'in', 'hierarchical', 'jacobi', 'coordinates', 'whilst', 'the', 'planets', 'are', 'referenced', 'purely', 'to', 'their... | [-0.16512227905033205, 0.07477170841562297, -0.05236981888175816, 0.0861176021705457, -0.09324896038082, -0.09245267719835848, 0.04061373501411966, 0.367433397794092, -0.20360896818062946, -0.3280443348393247, 0.08060662634419026, -0.26071989175838395, -0.0946160861882507, 0.20144519524875323, -0.08453192826410806, 0.0... |
710.1168 | Density functional theory of inhomogeneous liquids. I. The liquid-vapor
interface in Lennard-Jones fluids | A simple model is proposed for the direct correlation function (DCF) for
simple fluids consisting of a hard-core contribution, a simple parametrized
core correction, and a mean-field tail. The model requires as input only the
free energy of the homogeneous fluid, obtained, e.g., from thermodynamic
perturbation theory... | cond-mat.stat-mech | a simple model is proposed for the direct correlation function dcf for simple fluids consisting of a hardcore contribution a simple parametrized core correction and a meanfield tail the model requires as input only the free energy of the homogeneous fluid obtained eg from thermodynamic perturbation theory comparison to... | [['a', 'simple', 'model', 'is', 'proposed', 'for', 'the', 'direct', 'correlation', 'function', 'dcf', 'for', 'simple', 'fluids', 'consisting', 'of', 'a', 'hardcore', 'contribution', 'a', 'simple', 'parametrized', 'core', 'correction', 'and', 'a', 'meanfield', 'tail', 'the', 'model', 'requires', 'as', 'input', 'only', '... | [-0.09742619491774927, 0.055417239395054906, -0.14384482030079446, 0.07074335705361921, -0.015091795491223985, -0.14204917429861696, 0.023120068335397675, 0.32603235766291616, -0.2462617655454034, -0.31332347862083804, 0.015658581598704174, -0.2607181541367688, -0.11510427798229185, 0.1907396155451848, 0.02517845706844... |
710.1169 | SU(2) Yang-Mills thermodynamics and photon physics | Based on quantitative predictions enabled by a nonperturbative approach to
Yang-Mills thermodynamics it is explained why the physics of photon {\sl
propagation} is not unlikely rooted in pure SU(2) gauge dynamics.
| hep-ph | based on quantitative predictions enabled by a nonperturbative approach to yangmills thermodynamics it is explained why the physics of photon sl propagation is not unlikely rooted in pure su2 gauge dynamics | [['based', 'on', 'quantitative', 'predictions', 'enabled', 'by', 'a', 'nonperturbative', 'approach', 'to', 'yangmills', 'thermodynamics', 'it', 'is', 'explained', 'why', 'the', 'physics', 'of', 'photon', 'sl', 'propagation', 'is', 'not', 'unlikely', 'rooted', 'in', 'pure', 'su2', 'gauge', 'dynamics']] | [-0.07539853525738563, 0.23644351863091992, -0.1781115696555184, 0.17468096227985958, -0.12561598792672157, -0.16033339595061638, 0.05591417296278861, 0.3560061824898566, -0.17616952306801273, -0.272930032964195, 0.009897513266262268, -0.2243100712376256, -0.19137240992859006, 0.13474775694551006, -0.025891240355708906... |
710.117 | Numerical study of metastable states in the T=0 RFIM | We study numerically the number of single-spin-flip stable states in the T=0
Random Field Ising Model (RFIM) on random regular graphs of connectivity $z=2$
and $z=4$ and on the cubic lattice. The annealed and quenched complexities
(i.e. the entropy densities) of the metastable states with given magnetization
are calc... | cond-mat.dis-nn cond-mat.stat-mech | we study numerically the number of singlespinflip stable states in the t0 random field ising model rfim on random regular graphs of connectivity z2 and z4 and on the cubic lattice the annealed and quenched complexities ie the entropy densities of the metastable states with given magnetization are calculated as a functi... | [['we', 'study', 'numerically', 'the', 'number', 'of', 'singlespinflip', 'stable', 'states', 'in', 'the', 't0', 'random', 'field', 'ising', 'model', 'rfim', 'on', 'random', 'regular', 'graphs', 'of', 'connectivity', 'z2', 'and', 'z4', 'and', 'on', 'the', 'cubic', 'lattice', 'the', 'annealed', 'and', 'quenched', 'comple... | [-0.17864457274133222, 0.2675159553293773, -0.06919203519155513, 0.06846668451350738, 0.04409783439304521, -0.10575364681178744, 0.08365138955017988, 0.37337086171387357, -0.2230510580888454, -0.24887356339418826, 0.06616484622986234, -0.280943345516286, -0.11591536239621804, 0.10539897749983171, 0.039540219230904304, ... |
710.1171 | Improved estimation of the MSEs and the MSE matrices for shrinkage
estimators of multivariate normal means and their applications | In this article we provide some nonnegative and positive estimators of the
mean squared errors(MSEs) for shrinkage estimators of multivariate normal
means. Proposed estimators are shown to improve on the uniformly minimum
variance unbiased estimator(UMVUE) under a quadratic loss criterion. A similar
improvement is al... | math.ST stat.TH | in this article we provide some nonnegative and positive estimators of the mean squared errorsmses for shrinkage estimators of multivariate normal means proposed estimators are shown to improve on the uniformly minimum variance unbiased estimatorumvue under a quadratic loss criterion a similar improvement is also obtai... | [['in', 'this', 'article', 'we', 'provide', 'some', 'nonnegative', 'and', 'positive', 'estimators', 'of', 'the', 'mean', 'squared', 'errorsmses', 'for', 'shrinkage', 'estimators', 'of', 'multivariate', 'normal', 'means', 'proposed', 'estimators', 'are', 'shown', 'to', 'improve', 'on', 'the', 'uniformly', 'minimum', 'va... | [-0.020805149853798336, -0.019054458641647537, -0.12302584551522343, 0.13090040607825865, -0.02984167473104081, -0.13178375617400567, 0.07041932961202073, 0.43341861868902004, -0.22172321138691298, -0.2209680615688521, 0.17557536982017558, -0.31755344353946324, -0.2165722789219286, 0.2208320758647368, -0.13836374397896... |
710.1172 | Combinatorial Alexander Duality -- a Short and Elementary Proof | Let X be a simplicial complex with the ground set V. Define its Alexander
dual as a simplicial complex X* = {A \subset V: V \setminus A \notin X}. The
combinatorial Alexander duality states that the i-th reduced homology group of
X is isomorphic to the (|V|-i-3)-th reduced cohomology group of X* (over a
given commuta... | math.CO | let x be a simplicial complex with the ground set v define its alexander dual as a simplicial complex x a subset v v setminus a notin x the combinatorial alexander duality states that the ith reduced homology group of x is isomorphic to the vi3th reduced cohomology group of x over a given commutative ring r we give a s... | [['let', 'x', 'be', 'a', 'simplicial', 'complex', 'with', 'the', 'ground', 'set', 'v', 'define', 'its', 'alexander', 'dual', 'as', 'a', 'simplicial', 'complex', 'x', 'a', 'subset', 'v', 'v', 'setminus', 'a', 'notin', 'x', 'the', 'combinatorial', 'alexander', 'duality', 'states', 'that', 'the', 'ith', 'reduced', 'homolo... | [-0.2764817982087614, 0.0268306967756543, -0.10811637299226932, -0.00014844001747942606, -0.12045891254712812, -0.21675297395768958, 0.030178853112166046, 0.3194245208421203, -0.43380497689129877, -0.13017687442727754, 0.04092310473979374, -0.2616546428838714, -0.10558436410959626, 0.08033522227626355, -0.1892984940777... |
710.1173 | Baryon masses with dynamical twisted mass fermions | We present results on the mass of the nucleon and the $\Delta$ using two
dynamical degenerate twisted mass quarks. The evaluation is performed at four
quark masses corresponding to a pion mass in the range of 690-300 MeV on
lattices of size 2.1 fm and 2.7 fm. We check for cutoff effects by evaluating
these baryon mas... | hep-lat hep-ph nucl-th | we present results on the mass of the nucleon and the delta using two dynamical degenerate twisted mass quarks the evaluation is performed at four quark masses corresponding to a pion mass in the range of 690300 mev on lattices of size 21 fm and 27 fm we check for cutoff effects by evaluating these baryon masses on lat... | [['we', 'present', 'results', 'on', 'the', 'mass', 'of', 'the', 'nucleon', 'and', 'the', 'delta', 'using', 'two', 'dynamical', 'degenerate', 'twisted', 'mass', 'quarks', 'the', 'evaluation', 'is', 'performed', 'at', 'four', 'quark', 'masses', 'corresponding', 'to', 'a', 'pion', 'mass', 'in', 'the', 'range', 'of', '6903... | [-0.09774911589152947, 0.22649943741271272, -0.051536905576710354, 0.10230917547340761, -0.009104220961139968, -0.07162410795629783, 0.12674689604542577, 0.36657619146773446, -0.16917572471384817, -0.2871883249109877, 0.06997470527562405, -0.30913521112505715, 0.02022146042129332, 0.1053315251426014, 0.0537716384099509... |
710.1174 | Confinement and dual superconductivity of QCD vacuum | The mechanism of dual superconductivity for confinement is reviewed.
| hep-lat | the mechanism of dual superconductivity for confinement is reviewed | [['the', 'mechanism', 'of', 'dual', 'superconductivity', 'for', 'confinement', 'is', 'reviewed']] | [-0.18991285231378344, 0.2678840292824639, -0.038705062948995166, 0.1604747309271867, -0.10554670915007591, -0.21993658070762953, 0.045378733426332474, 0.35523347225454116, -0.26148930771483314, -0.11831142091088825, 0.035429030656814575, -0.24097060515648788, -0.14067087529434097, 0.10386867572863896, -0.0420915474080... |
710.1175 | An alternative hypothesis for the outburst mechanism in Supergiant Fast
X-ray Transients: the case of IGR J11215-5952 | (ABRIDGED)- The physical mechanism responsible for the short outbursts in a
recently recognized class of High Mass X-ray Binaries, the Supergiant Fast
X-ray Transients (SFXTs), is still unknown. Two main hypotheses have been
proposed to date: the sudden accretion by the compact object of small ejections
originating i... | astro-ph | abridged the physical mechanism responsible for the short outbursts in a recently recognized class of high mass xray binaries the supergiant fast xray transients sfxts is still unknown two main hypotheses have been proposed to date the sudden accretion by the compact object of small ejections originating in a clumpy wi... | [['abridged', 'the', 'physical', 'mechanism', 'responsible', 'for', 'the', 'short', 'outbursts', 'in', 'a', 'recently', 'recognized', 'class', 'of', 'high', 'mass', 'xray', 'binaries', 'the', 'supergiant', 'fast', 'xray', 'transients', 'sfxts', 'is', 'still', 'unknown', 'two', 'main', 'hypotheses', 'have', 'been', 'pro... | [-0.08250579398582417, 0.12554586117017796, -0.1039911023311691, 0.1223604995112513, -0.1512084438863252, -0.11288202056301183, 0.08586286150912674, 0.42621879569050547, -0.16704385060582008, -0.3688773950388773, 0.1369798760352653, -0.2918945604114755, -0.0942810107590319, 0.22805235399622262, -0.10570745956141642, 0.... |
710.1176 | Autoresonant control of the many-electron dynamics in nonparabolic
quantum wells | The optical response of nonparabolic quantum wells is dominated by a strong
peak at the plasmon frequency. When the electrons reach the anharmonic regions,
resonant absorption becomes inefficient. This limitation is overcome by using a
chirped laser pulse in the autoresonant regime. By direct simulations using the
Wi... | cond-mat.mes-hall | the optical response of nonparabolic quantum wells is dominated by a strong peak at the plasmon frequency when the electrons reach the anharmonic regions resonant absorption becomes inefficient this limitation is overcome by using a chirped laser pulse in the autoresonant regime by direct simulations using the wigner p... | [['the', 'optical', 'response', 'of', 'nonparabolic', 'quantum', 'wells', 'is', 'dominated', 'by', 'a', 'strong', 'peak', 'at', 'the', 'plasmon', 'frequency', 'when', 'the', 'electrons', 'reach', 'the', 'anharmonic', 'regions', 'resonant', 'absorption', 'becomes', 'inefficient', 'this', 'limitation', 'is', 'overcome', ... | [-0.12741420852020383, 0.24033891962011694, -0.06207339562941343, 0.045397763667860996, -0.011888827591901645, -0.15827516154386104, 0.051567149522015826, 0.4423564958572388, -0.3004955336265266, -0.2808630554517731, 0.018362075382610782, -0.2616343951318413, -0.0802420134562999, 0.2671347118541598, -0.0121788049163296... |
710.1177 | Stochastic Cutoff Method for Long-Range Interacting Systems | A new Monte-Carlo method for long-range interacting systems is presented.
This method consists of eliminating interactions stochastically with the
detailed balance condition satisfied. When a pairwise interaction $V_{ij}$ of a
$N$-particle system decreases with the distance as $r_{ij}^{-\alpha}$,
computational time p... | cond-mat.dis-nn cond-mat.stat-mech | a new montecarlo method for longrange interacting systems is presented this method consists of eliminating interactions stochastically with the detailed balance condition satisfied when a pairwise interaction v_ij of a nparticle system decreases with the distance as r_ijalpha computational time per one monte carlo step... | [['a', 'new', 'montecarlo', 'method', 'for', 'longrange', 'interacting', 'systems', 'is', 'presented', 'this', 'method', 'consists', 'of', 'eliminating', 'interactions', 'stochastically', 'with', 'the', 'detailed', 'balance', 'condition', 'satisfied', 'when', 'a', 'pairwise', 'interaction', 'v_ij', 'of', 'a', 'nparticl... | [-0.17310502509483033, 0.14279169639139766, -0.03769932921171527, 0.044979472016689906, -0.011173582447673937, -0.1964203506012005, 0.019236412379100468, 0.3467160202562809, -0.24804628506829643, -0.3196462047982472, -0.01725790858964878, -0.32582516073616163, -0.08757155863427077, 0.16760918935478636, 0.05094088723111... |
710.1178 | The structure of Sally modules of rank one | A complete structure theorem of Sally modules of $\fkm$-primary ideals $I$ in
a Cohen-Macaulay local ring $(A, \m)$ satisfying the equality
$\e_1(I)=\e_0(I)-\ell_A(A/I)+1$ is given, where $\e_0(I)$ and $\e_1(I)$ denote
the first two Hilbert coefficients of $I$.
| math.AC math.AG | a complete structure theorem of sally modules of fkmprimary ideals i in a cohenmacaulay local ring a m satisfying the equality e_1ie_0iell_aai1 is given where e_0i and e_1i denote the first two hilbert coefficients of i | [['a', 'complete', 'structure', 'theorem', 'of', 'sally', 'modules', 'of', 'fkmprimary', 'ideals', 'i', 'in', 'a', 'cohenmacaulay', 'local', 'ring', 'a', 'm', 'satisfying', 'the', 'equality', 'e_1ie_0iell_aai1', 'is', 'given', 'where', 'e_0i', 'and', 'e_1i', 'denote', 'the', 'first', 'two', 'hilbert', 'coefficients', '... | [-0.2443633214570582, 0.016371214324060607, -0.06860041929244556, -0.003536757722031325, -0.0666349628693698, -0.19963259547127082, -0.07979903841281638, 0.24399449709145463, -0.35551705808543105, -0.10742602031677961, 0.08732850549345397, -0.264452850446105, -0.058169081067556846, 0.11454010680180919, -0.0931172787540... |
710.1179 | Dark matter-wave solitons in the dimensionality crossover | We consider the statics and dynamics of dark matter-wave solitons in the
dimensionality crossover regime from 3D to 1D. There, using the nonpolynomial
Schr\"{o}dinger mean-field model, we find that the anomalous mode of the
Bogoliubov spectrum has an eigenfrequency which coincides with the soliton
oscillation frequen... | cond-mat.other | we consider the statics and dynamics of dark matterwave solitons in the dimensionality crossover regime from 3d to 1d there using the nonpolynomial schrodinger meanfield model we find that the anomalous mode of the bogoliubov spectrum has an eigenfrequency which coincides with the soliton oscillation frequency obtained... | [['we', 'consider', 'the', 'statics', 'and', 'dynamics', 'of', 'dark', 'matterwave', 'solitons', 'in', 'the', 'dimensionality', 'crossover', 'regime', 'from', '3d', 'to', '1d', 'there', 'using', 'the', 'nonpolynomial', 'schrodinger', 'meanfield', 'model', 'we', 'find', 'that', 'the', 'anomalous', 'mode', 'of', 'the', '... | [-0.1418196635398393, 0.15338365062313114, -0.06864968852864371, 0.05275267680509039, -0.0362244370152001, -0.15696290061797624, 0.005380876856729572, 0.34711619461944077, -0.25205989880487323, -0.22259410445428926, 0.03751457934727731, -0.2836161053934951, -0.1390522925303904, 0.20332551081262437, 0.06441680639177377,... |
710.118 | Comparison of bar strengths in optical and near-infrared for the OSUBSGS
sample | We use a gravitational bar torque method to compare bar strengths (the
maximum tangential force normalized by radial force) in B and H-band images of
152 galaxies from the Ohio State University Bright Spiral Galaxy Survey. Our
main motivation is to check how much the difference in the rest-frame
wavelength could affe... | astro-ph | we use a gravitational bar torque method to compare bar strengths the maximum tangential force normalized by radial force in b and hband images of 152 galaxies from the ohio state university bright spiral galaxy survey our main motivation is to check how much the difference in the restframe wavelength could affect comp... | [['we', 'use', 'a', 'gravitational', 'bar', 'torque', 'method', 'to', 'compare', 'bar', 'strengths', 'the', 'maximum', 'tangential', 'force', 'normalized', 'by', 'radial', 'force', 'in', 'b', 'and', 'hband', 'images', 'of', '152', 'galaxies', 'from', 'the', 'ohio', 'state', 'university', 'bright', 'spiral', 'galaxy', '... | [-0.06981715852660793, 0.08899209584538652, -0.06985449703550706, 0.07973322202220544, -0.06442684023770401, -0.08671277623516434, 0.033824572655638416, 0.4212775114361966, -0.22610673603152723, -0.3413421108298713, 0.04054728983337843, -0.249392630826194, -0.052089652885721684, 0.19774140039318433, -0.0199183568160700... |
710.1181 | On the evolution and fate of supermassive stars | We study the evolution and fate of solar composition supermassive stars in
the mass range 60 - 1000 Msun. Our study is relevant both for very massive
objects observed in young stellar complexes as well as supermassive stars that
may potentially form through runaway stellar collisions. We predict the
outcomes of stell... | astro-ph | we study the evolution and fate of solar composition supermassive stars in the mass range 60 1000 msun our study is relevant both for very massive objects observed in young stellar complexes as well as supermassive stars that may potentially form through runaway stellar collisions we predict the outcomes of stellar evo... | [['we', 'study', 'the', 'evolution', 'and', 'fate', 'of', 'solar', 'composition', 'supermassive', 'stars', 'in', 'the', 'mass', 'range', '60', '1000', 'msun', 'our', 'study', 'is', 'relevant', 'both', 'for', 'very', 'massive', 'objects', 'observed', 'in', 'young', 'stellar', 'complexes', 'as', 'well', 'as', 'supermassi... | [-0.058657348463431194, 0.1815463315542729, -0.030565923336558998, 0.19037078177251926, -0.11394384131283285, -0.02818014556601739, 0.060865594969632536, 0.40131795037991536, -0.087872579512455, -0.3968210574000692, 0.05229004806591174, -0.30828230790435696, -0.016787967293893393, 0.206713802076709, -0.0604043541467641... |
710.1182 | Low-Density Parity-Check Codes for Nonergodic Block-Fading Channels | We solve the problem of designing powerful low-density parity-check (LDPC)
codes with iterative decoding for the block-fading channel. We first study the
case of maximum-likelihood decoding, and show that the design criterion is
rather straightforward. Unfortunately, optimal constructions for
maximum-likelihood decod... | cs.IT math.IT | we solve the problem of designing powerful lowdensity paritycheck ldpc codes with iterative decoding for the blockfading channel we first study the case of maximumlikelihood decoding and show that the design criterion is rather straightforward unfortunately optimal constructions for maximumlikelihood decoding do not pe... | [['we', 'solve', 'the', 'problem', 'of', 'designing', 'powerful', 'lowdensity', 'paritycheck', 'ldpc', 'codes', 'with', 'iterative', 'decoding', 'for', 'the', 'blockfading', 'channel', 'we', 'first', 'study', 'the', 'case', 'of', 'maximumlikelihood', 'decoding', 'and', 'show', 'that', 'the', 'design', 'criterion', 'is'... | [-0.2133655073644405, 0.010114733359954331, -0.07298680965192197, 0.11097376246732565, -0.03925846227224958, -0.36773236487793287, 0.07789700898195334, 0.4544571846556128, -0.28818216072290803, -0.22877801976721274, 0.12116037666917977, -0.15858244278541442, -0.22247685645863916, 0.1910901646550975, -0.1498864059849234... |
710.1183 | Connectivity of Addition Cayley Graphs | For any finite abelian group $G$ and any subset $S\seq G$, we determine the
connectivity of the addition Cayley graph induced by $S$ on $G$. Moreover, we
show that if this graph is not complete, then it possesses a minimum vertex cut
of a special, explicitly described form.
| math.CO math.NT | for any finite abelian group g and any subset sseq g we determine the connectivity of the addition cayley graph induced by s on g moreover we show that if this graph is not complete then it possesses a minimum vertex cut of a special explicitly described form | [['for', 'any', 'finite', 'abelian', 'group', 'g', 'and', 'any', 'subset', 'sseq', 'g', 'we', 'determine', 'the', 'connectivity', 'of', 'the', 'addition', 'cayley', 'graph', 'induced', 'by', 's', 'on', 'g', 'moreover', 'we', 'show', 'that', 'if', 'this', 'graph', 'is', 'not', 'complete', 'then', 'it', 'possesses', 'a',... | [-0.17112435925593403, 0.13760111637492764, -0.0740704891529489, 0.019685624345661477, -0.17476303447434244, -0.12231015947033116, 0.08005373815986071, 0.4191068462542001, -0.2755847147447949, -0.24863799037213655, 0.07718544209653393, -0.264168914333184, -0.1814394162650755, 0.1015628008964531, -0.07917517522706631, -... |
710.1184 | Geometric entanglement witnesses and bound entanglement | We study entanglement witnesses that can be constructed with regard to the
geometrical structure of the Hilbert-Schmidt space, i.e. we present how to use
these witnesses in the context of quantifying entanglement and the detection of
bound entangled states. We give examples for a particular three-parameter
family of ... | quant-ph | we study entanglement witnesses that can be constructed with regard to the geometrical structure of the hilbertschmidt space ie we present how to use these witnesses in the context of quantifying entanglement and the detection of bound entangled states we give examples for a particular threeparameter family of states t... | [['we', 'study', 'entanglement', 'witnesses', 'that', 'can', 'be', 'constructed', 'with', 'regard', 'to', 'the', 'geometrical', 'structure', 'of', 'the', 'hilbertschmidt', 'space', 'ie', 'we', 'present', 'how', 'to', 'use', 'these', 'witnesses', 'in', 'the', 'context', 'of', 'quantifying', 'entanglement', 'and', 'the',... | [-0.11247727516407179, 0.1563433994523297, -0.08394559878477101, 0.076332758291293, 0.01270549905375909, -0.13485128240722974, 0.023374237226701136, 0.34331456521304987, -0.22592966600273878, -0.2593741041876502, 0.101488895238756, -0.28411467851660516, -0.1653470653661732, 0.16317675173108986, -0.06550815099084718, 0.... |
710.1185 | Higher entropic uncertainty relations for anti-commuting observables | Uncertainty relations lie at the very core of quantum mechanics, and form the
cornerstone of essentially all quantum cryptographic applications. In
particular, they play an important role in cryptographic protocols in the
bounded-quantum-storage model, where proving the security of all existing
protocols ultimately r... | quant-ph | uncertainty relations lie at the very core of quantum mechanics and form the cornerstone of essentially all quantum cryptographic applications in particular they play an important role in cryptographic protocols in the boundedquantumstorage model where proving the security of all existing protocols ultimately reduces t... | [['uncertainty', 'relations', 'lie', 'at', 'the', 'very', 'core', 'of', 'quantum', 'mechanics', 'and', 'form', 'the', 'cornerstone', 'of', 'essentially', 'all', 'quantum', 'cryptographic', 'applications', 'in', 'particular', 'they', 'play', 'an', 'important', 'role', 'in', 'cryptographic', 'protocols', 'in', 'the', 'bo... | [-0.13189986654712507, 0.10092812472461818, -0.09739853310028232, 0.15565913218268823, -0.03714453317325122, -0.18747754715869994, 0.0647718996755899, 0.3164581136016916, -0.281472752396498, -0.29851417965506033, 0.09881237826825831, -0.2987230114678862, -0.13330532308487641, 0.2945446466941947, -0.10410668637343151, 0... |
710.1186 | Heavy quark symmetry constraints on semileptonic form factors and decay
widths of doubly heavy baryons | We show how heavy quark symmetry constraints on doubly heavy baryon
semileptonic decay widths can be used to test the validity of different quark
model calculations. The large discrepancies in the results observed between
different quark model approaches can be understood in terms of a severe
violation of heavy quark... | hep-ph nucl-th | we show how heavy quark symmetry constraints on doubly heavy baryon semileptonic decay widths can be used to test the validity of different quark model calculations the large discrepancies in the results observed between different quark model approaches can be understood in terms of a severe violation of heavy quark sp... | [['we', 'show', 'how', 'heavy', 'quark', 'symmetry', 'constraints', 'on', 'doubly', 'heavy', 'baryon', 'semileptonic', 'decay', 'widths', 'can', 'be', 'used', 'to', 'test', 'the', 'validity', 'of', 'different', 'quark', 'model', 'calculations', 'the', 'large', 'discrepancies', 'in', 'the', 'results', 'observed', 'betwe... | [-0.054735791943726485, 0.2818790108270558, -0.06799828097352693, 0.19381036354100395, -0.06728863571609917, -0.1507830121313575, 0.08641231990547786, 0.2958404284195396, -0.21580857616560212, -0.30156907111663245, -0.017956238344375944, -0.281409768034415, 0.02191766152351067, 0.10908372017277951, 0.027008472636727423... |
710.1187 | Stochastic thermodynamics: Principles and perspectives | Stochastic thermodynamics provides a framework for describing small systems
like colloids or biomolecules driven out of equilibrium but still in contact
with a heat bath. Both, a first-law like energy balance involving exchanged
heat and entropy production entering refinements of the second law can
consistently be de... | cond-mat.stat-mech cond-mat.soft | stochastic thermodynamics provides a framework for describing small systems like colloids or biomolecules driven out of equilibrium but still in contact with a heat bath both a firstlaw like energy balance involving exchanged heat and entropy production entering refinements of the second law can consistently be defined... | [['stochastic', 'thermodynamics', 'provides', 'a', 'framework', 'for', 'describing', 'small', 'systems', 'like', 'colloids', 'or', 'biomolecules', 'driven', 'out', 'of', 'equilibrium', 'but', 'still', 'in', 'contact', 'with', 'a', 'heat', 'bath', 'both', 'a', 'firstlaw', 'like', 'energy', 'balance', 'involving', 'excha... | [-0.10940483499225229, 0.13700993366271724, -0.11654307679110207, 0.12268312149588019, -0.05247390968352556, -0.17499457012861966, 0.03342629538103938, 0.2530731230452657, -0.3191180000305176, -0.2983487013578415, 0.07261395790427923, -0.33931404051184655, -0.12597982634417712, 0.2571597478296608, -0.000543264705687761... |
710.1188 | Towards a non-perturbative matching of HQET and QCD with dynamical light
quarks | We explain how the strategy of solving renormalization problems in HQET
non-perturbatively by a matching to QCD in finite volume can be implemented to
include dynamical fermions. As a primary application, some elements of an HQET
computation of the mass of the b-quark beyond the leading order with N_f=2 are
outlined.... | hep-lat | we explain how the strategy of solving renormalization problems in hqet nonperturbatively by a matching to qcd in finite volume can be implemented to include dynamical fermions as a primary application some elements of an hqet computation of the mass of the bquark beyond the leading order with n_f2 are outlined in part... | [['we', 'explain', 'how', 'the', 'strategy', 'of', 'solving', 'renormalization', 'problems', 'in', 'hqet', 'nonperturbatively', 'by', 'a', 'matching', 'to', 'qcd', 'in', 'finite', 'volume', 'can', 'be', 'implemented', 'to', 'include', 'dynamical', 'fermions', 'as', 'a', 'primary', 'application', 'some', 'elements', 'of... | [-0.10278019618166834, 0.2124826420171211, -0.09199380602558735, 0.063708922656622, -0.04390785874031578, -0.0791437555428114, 0.08892829663013313, 0.31493883868737976, -0.17993570047096824, -0.2631555097045834, 0.057345669070088874, -0.2756862975173753, -0.015527553267706678, 0.11617461881899047, 0.03522415317846872, ... |
710.1189 | IC5063: AGN driven outflow of warm and cold gas | We present new ATCA 17- and 24-GHz radio images and ESO-NTT optical spectra
of the radio-loud Seyfert galaxy IC5063, the first galaxy in which a fast (~
600 km/s) outflow of neutral hydrogen was discovered. The new radio data
confirm the triple radio structure with a central core and two resolved radio
lobes. This im... | astro-ph | we present new atca 17 and 24ghz radio images and esontt optical spectra of the radioloud seyfert galaxy ic5063 the first galaxy in which a fast 600 kms outflow of neutral hydrogen was discovered the new radio data confirm the triple radio structure with a central core and two resolved radio lobes this implies that the... | [['we', 'present', 'new', 'atca', '17', 'and', '24ghz', 'radio', 'images', 'and', 'esontt', 'optical', 'spectra', 'of', 'the', 'radioloud', 'seyfert', 'galaxy', 'ic5063', 'the', 'first', 'galaxy', 'in', 'which', 'a', 'fast', '600', 'kms', 'outflow', 'of', 'neutral', 'hydrogen', 'was', 'discovered', 'the', 'new', 'radio... | [-0.08335286592294884, 0.07017342620286544, 0.002409846620506786, 0.08592522843757565, -0.08765815378997949, -0.057315390773954825, 0.0034479637257148078, 0.4752827765668836, -0.17156399965304456, -0.28505066982455285, 0.05033365527360551, -0.26682317510386777, 0.02814201744886097, 0.178513870203863, 0.0332701935460153... |
710.119 | Power Efficient Scheduling under Delay Constraints over Multi-user
Wireless Channels | In this paper, we consider the problem of power efficient uplink scheduling
in a Time Division Multiple Access (TDMA) system over a fading wireless
channel. The objective is to minimize the power expenditure of each user
subject to satisfying individual user delay. We make the practical assumption
that the system sta... | cs.NI cs.MA | in this paper we consider the problem of power efficient uplink scheduling in a time division multiple access tdma system over a fading wireless channel the objective is to minimize the power expenditure of each user subject to satisfying individual user delay we make the practical assumption that the system statistics... | [['in', 'this', 'paper', 'we', 'consider', 'the', 'problem', 'of', 'power', 'efficient', 'uplink', 'scheduling', 'in', 'a', 'time', 'division', 'multiple', 'access', 'tdma', 'system', 'over', 'a', 'fading', 'wireless', 'channel', 'the', 'objective', 'is', 'to', 'minimize', 'the', 'power', 'expenditure', 'of', 'each', '... | [-0.1912558254689075, 0.005882297212271084, -0.054288247862258256, 0.03311422381356552, -0.08314443201338671, -0.20944858667565694, 0.14633259511083058, 0.4155635970656748, -0.29924579279989133, -0.3016855487100038, 0.10156988193133838, -0.23560277597567478, -0.14942906199635947, 0.16016949493905683, -0.114525762683453... |
710.1191 | Compacton-like solutions of the hydrodynamic system describing relaxing
media | We show the existence of a compacton-like solutions within the relaxing
hydrodynamic-type model and perform numerical study of attracting features of
these solutions.
| nlin.PS | we show the existence of a compactonlike solutions within the relaxing hydrodynamictype model and perform numerical study of attracting features of these solutions | [['we', 'show', 'the', 'existence', 'of', 'a', 'compactonlike', 'solutions', 'within', 'the', 'relaxing', 'hydrodynamictype', 'model', 'and', 'perform', 'numerical', 'study', 'of', 'attracting', 'features', 'of', 'these', 'solutions']] | [-0.18902246038550916, 0.001425775517102169, -0.1078625995989727, 0.038457929116228355, 0.012112352430172588, -0.10720536414452869, 0.041646445493983185, 0.28674152291015437, -0.24337471989185913, -0.24548393896902385, 0.1529017233127809, -0.31596163522614085, -0.17244425885703252, 0.1516348330769688, 0.043365792118255... |
710.1192 | The symmetries of five-dimensional minimal supergravity reduced to three
dimensions | The 14 Killing vectors of the target space for five-dimensional minimal
supergravity reduced to three dimensions are explicitly constructed in terms of
the original field variables. These vectors generate the Lie algebra of $G_2$.
We also construct a symmetrical $7\times7$ matrix representative of the coset
$G_{2(+2)... | gr-qc hep-th math-ph math.MP | the 14 killing vectors of the target space for fivedimensional minimal supergravity reduced to three dimensions are explicitly constructed in terms of the original field variables these vectors generate the lie algebra of g_2 we also construct a symmetrical 7times7 matrix representative of the coset g_22sl2rtimes sl2r ... | [['the', '14', 'killing', 'vectors', 'of', 'the', 'target', 'space', 'for', 'fivedimensional', 'minimal', 'supergravity', 'reduced', 'to', 'three', 'dimensions', 'are', 'explicitly', 'constructed', 'in', 'terms', 'of', 'the', 'original', 'field', 'variables', 'these', 'vectors', 'generate', 'the', 'lie', 'algebra', 'of... | [-0.14806660471691024, 0.1346356647985953, 0.014770869614073524, 0.0809684823681083, -0.09756560770242854, -0.08099764028641705, -0.05146763277136617, 0.32683115311104943, -0.22867545377704557, -0.23551621877898773, 0.13074882556328601, -0.2233491575655838, -0.15856129654545198, 0.10730795622630804, -0.0591870515469323... |
710.1193 | Effect of angular momentum distribution on gravitational loss-cone
instability in stellar clusters around massive BH | Small perturbations in spherical and thin disk stellar clusters surrounding
massive a black hole are studied. Due to the black hole, stars with
sufficiently low angular momentum escape from the system through the loss cone.
We show that stability properties of spherical clusters crucially depend on
whether the distri... | astro-ph | small perturbations in spherical and thin disk stellar clusters surrounding massive a black hole are studied due to the black hole stars with sufficiently low angular momentum escape from the system through the loss cone we show that stability properties of spherical clusters crucially depend on whether the distributio... | [['small', 'perturbations', 'in', 'spherical', 'and', 'thin', 'disk', 'stellar', 'clusters', 'surrounding', 'massive', 'a', 'black', 'hole', 'are', 'studied', 'due', 'to', 'the', 'black', 'hole', 'stars', 'with', 'sufficiently', 'low', 'angular', 'momentum', 'escape', 'from', 'the', 'system', 'through', 'the', 'loss', ... | [-0.12765446032530495, 0.16605258731925415, -0.11435248156721216, 0.12108834913011551, -0.08523724563530691, -0.0753278130765206, 0.02046127197709644, 0.37883393674911486, -0.22616922185711918, -0.29844602804985787, 0.0479398851263492, -0.28507218168427545, -0.03325883135299331, 0.18792911696281017, -0.0254037222018398... |
710.1194 | A systematic search for novae in M31 on a large set of digitized
archival Schmidt plates | This paper reports on the detection of optical novae in our neighbour galaxy
M31 based on digitized historical Tautenburg Schmidt plates. The accurate
positions of the detected novae lead to a much larger database when searching
for recurrent novae in M31. We conducted a systematic search for novae on 306
digitized T... | astro-ph | this paper reports on the detection of optical novae in our neighbour galaxy m31 based on digitized historical tautenburg schmidt plates the accurate positions of the detected novae lead to a much larger database when searching for recurrent novae in m31 we conducted a systematic search for novae on 306 digitized taute... | [['this', 'paper', 'reports', 'on', 'the', 'detection', 'of', 'optical', 'novae', 'in', 'our', 'neighbour', 'galaxy', 'm31', 'based', 'on', 'digitized', 'historical', 'tautenburg', 'schmidt', 'plates', 'the', 'accurate', 'positions', 'of', 'the', 'detected', 'novae', 'lead', 'to', 'a', 'much', 'larger', 'database', 'wh... | [-0.056309355370509406, 0.05481521516797349, -0.0767976122032248, 0.06551356079654011, -0.0997102801753342, -0.1602958099072357, 0.14443499785337074, 0.40365533753827537, -0.1432245483709057, -0.3994312264517673, 0.16360736377629378, -0.3818467273631279, -0.06771311983667153, 0.25766190220920115, -0.08154617299211861, ... |
710.1195 | Maximizing phonon thermal conductance for ballistic membranes | At low temperatures, phonon scattering can become so weak that phonon
transport becomes ballistic. We calculate the ballistic phonon conductance G
for membranes using elasticity theory, considering the transition from three to
two dimensions. We discuss the temperature and thickness dependence and
especially concentr... | cond-mat.mes-hall cond-mat.mtrl-sci | at low temperatures phonon scattering can become so weak that phonon transport becomes ballistic we calculate the ballistic phonon conductance g for membranes using elasticity theory considering the transition from three to two dimensions we discuss the temperature and thickness dependence and especially concentrate on... | [['at', 'low', 'temperatures', 'phonon', 'scattering', 'can', 'become', 'so', 'weak', 'that', 'phonon', 'transport', 'becomes', 'ballistic', 'we', 'calculate', 'the', 'ballistic', 'phonon', 'conductance', 'g', 'for', 'membranes', 'using', 'elasticity', 'theory', 'considering', 'the', 'transition', 'from', 'three', 'to'... | [-0.14202188752096845, 0.23940804923768155, -0.04067148120520869, -0.002926736000517849, -0.03975117734808009, -0.16425104594964068, 0.047070874459677725, 0.4137383943016175, -0.27863730854005553, -0.22649928989994805, 0.033866172132547945, -0.3392010298994137, -0.10881033292389475, 0.2152972125186352, 0.04650170184322... |
710.1196 | The volume densities of GMCs in M81 | HI features near young star clusters in M81 are identified as the
photodissociated surfaces of Giant Molecular Clouds (GMCs) from which the young
stars have recently formed. The HI column densities of these features show a
weak trend, from undetectable values inside R = 3.7 kpc and increasing rapidly
to values around... | astro-ph | hi features near young star clusters in m81 are identified as the photodissociated surfaces of giant molecular clouds gmcs from which the young stars have recently formed the hi column densities of these features show a weak trend from undetectable values inside r 37 kpc and increasing rapidly to values around 3 x 1021... | [['hi', 'features', 'near', 'young', 'star', 'clusters', 'in', 'm81', 'are', 'identified', 'as', 'the', 'photodissociated', 'surfaces', 'of', 'giant', 'molecular', 'clouds', 'gmcs', 'from', 'which', 'the', 'young', 'stars', 'have', 'recently', 'formed', 'the', 'hi', 'column', 'densities', 'of', 'these', 'features', 'sh... | [-0.06520025946726558, 0.11797651525325799, -0.041584121228061516, 0.05817824998604014, 0.016253101586579756, -0.02656497514967331, 0.046590008276746524, 0.4357766384689959, -0.14066567492577772, -0.34912350796636876, 0.010324678687260823, -0.2844600198977509, -0.002093994093491537, 0.13577746055048268, -0.009758570992... |
710.1197 | The interplay between radio jets and ISM in sub-kpc radio sources | This paper reviews the evidence for interaction between radio jets and their
environment in small and intermediate (sub-kpc) scale radio sources.
Observations of gas (both neutral hydrogen and ionised gas) have shown the
presence of fast (> 1000 km/s) outflows likely originating from this
interaction. The characteris... | astro-ph | this paper reviews the evidence for interaction between radio jets and their environment in small and intermediate subkpc scale radio sources observations of gas both neutral hydrogen and ionised gas have shown the presence of fast 1000 kms outflows likely originating from this interaction the characteristics of these ... | [['this', 'paper', 'reviews', 'the', 'evidence', 'for', 'interaction', 'between', 'radio', 'jets', 'and', 'their', 'environment', 'in', 'small', 'and', 'intermediate', 'subkpc', 'scale', 'radio', 'sources', 'observations', 'of', 'gas', 'both', 'neutral', 'hydrogen', 'and', 'ionised', 'gas', 'have', 'shown', 'the', 'pre... | [-0.12884835784828638, 0.12176664944706579, 0.002596444687095739, 0.10741264494017587, -0.09297625799426588, -0.03883285108377557, 0.025358985814510578, 0.4683296392529698, -0.16314651376678277, -0.3326811814775406, 0.0857553127038261, -0.2871061994189049, -0.062356443823141566, 0.18824737126765362, 0.05513285255943567... |
710.1198 | Signature of the interaction between dark energy and dark matter in
galaxy clusters | We investigate the influence of an interaction between dark energy and dark
matter upon the dynamics of galaxy clusters. We obtain the general
Layser-Irvine equation in the presence of interactions, and find how, in that
case, the virial theorem stands corrected. Using optical, X-ray and weak
lensing data from 33 rel... | astro-ph | we investigate the influence of an interaction between dark energy and dark matter upon the dynamics of galaxy clusters we obtain the general layserirvine equation in the presence of interactions and find how in that case the virial theorem stands corrected using optical xray and weak lensing data from 33 relaxed galax... | [['we', 'investigate', 'the', 'influence', 'of', 'an', 'interaction', 'between', 'dark', 'energy', 'and', 'dark', 'matter', 'upon', 'the', 'dynamics', 'of', 'galaxy', 'clusters', 'we', 'obtain', 'the', 'general', 'layserirvine', 'equation', 'in', 'the', 'presence', 'of', 'interactions', 'and', 'find', 'how', 'in', 'tha... | [-0.13408099378492416, 0.1151719210585205, -0.13576056828536648, 0.15539551774660745, -0.08837911408461098, -0.08197481133088115, 0.00590776160381557, 0.3261505030649936, -0.23718975065276027, -0.3687802258368936, -0.007666701948480858, -0.2902347367212531, -0.04581349283745069, 0.1460035138408698, 0.08772916118392632,... |
710.1199 | Commensurate anisotropic oscillator, SU(2) coherent states and the
classical limit | We demonstrate a formally exact quantum-classical correspondence between the
stationary coherent states associated with the commensurate anisotropic
two-dimensional harmonic oscillator and the classical Lissajous orbits. Our
derivation draws upon earlier work of Louck et al [1973 \textit {J. Math.
Phys.} \textbf {14}... | quant-ph | we demonstrate a formally exact quantumclassical correspondence between the stationary coherent states associated with the commensurate anisotropic twodimensional harmonic oscillator and the classical lissajous orbits our derivation draws upon earlier work of louck et al 1973 textit j math phys textbf 14 692 wherein th... | [['we', 'demonstrate', 'a', 'formally', 'exact', 'quantumclassical', 'correspondence', 'between', 'the', 'stationary', 'coherent', 'states', 'associated', 'with', 'the', 'commensurate', 'anisotropic', 'twodimensional', 'harmonic', 'oscillator', 'and', 'the', 'classical', 'lissajous', 'orbits', 'our', 'derivation', 'dra... | [-0.11471915304751829, 0.1491376569327641, -0.08426077615931854, 0.016981647912713987, -0.057632947632958904, -0.08936790990314089, 0.06120407686278196, 0.326365596992909, -0.23668189060478645, -0.2217682046584673, 0.0062585599226807065, -0.2685242708268246, -0.16704116622861334, 0.18427663875561684, -0.049072379052036... |
710.12 | Quantum Causal Networks | Intervention theories of causality define a relationship as causal if
appropriately specified interventions to manipulate a putative cause tend to
produce changes in the putative effect. Interventionist causal theories are
commonly formalized by using directed graphs to represent causal relationships,
local probabili... | quant-ph | intervention theories of causality define a relationship as causal if appropriately specified interventions to manipulate a putative cause tend to produce changes in the putative effect interventionist causal theories are commonly formalized by using directed graphs to represent causal relationships local probability m... | [['intervention', 'theories', 'of', 'causality', 'define', 'a', 'relationship', 'as', 'causal', 'if', 'appropriately', 'specified', 'interventions', 'to', 'manipulate', 'a', 'putative', 'cause', 'tend', 'to', 'produce', 'changes', 'in', 'the', 'putative', 'effect', 'interventionist', 'causal', 'theories', 'are', 'commo... | [-0.09700674254447222, 0.08260766521759796, -0.10755938260257245, 0.1464271120755002, -0.15945012857019902, -0.1792658124230802, 0.06669068865198642, 0.3208198013585061, -0.2839950421154499, -0.29590797787159684, 0.028248461283743382, -0.26882558258064093, -0.2120033395253122, 0.11569024096988141, -0.1575526749379933, ... |
710.1201 | On the X-Ray Light Curve, Pulsed-Radio Emission, and Spin Frequency
Evolution of the Transient Anomalous X-Ray Pulsar Xte J1810--197 During its
X-Ray Outburst | We show that: (i) the long-term X-ray outburst light curve of the transient
AXP XTE J1810-197 can be accounted for by a fallback disk that is evolving
towards quiescence through a disk instability after having been heated by a
soft gamma-ray burst, (ii) the spin-frequency evolution of this source in the
same period c... | astro-ph | we show that i the longterm xray outburst light curve of the transient axp xte j1810197 can be accounted for by a fallback disk that is evolving towards quiescence through a disk instability after having been heated by a soft gammaray burst ii the spinfrequency evolution of this source in the same period can also be ex... | [['we', 'show', 'that', 'i', 'the', 'longterm', 'xray', 'outburst', 'light', 'curve', 'of', 'the', 'transient', 'axp', 'xte', 'j1810197', 'can', 'be', 'accounted', 'for', 'by', 'a', 'fallback', 'disk', 'that', 'is', 'evolving', 'towards', 'quiescence', 'through', 'a', 'disk', 'instability', 'after', 'having', 'been', '... | [-0.07161150040487066, 0.1598643863764711, -0.08345435763128166, 0.11727031064020772, -0.1593025567698587, -0.10713536771109854, 0.03317555476728286, 0.43757359700030685, -0.2374684422637105, -0.2978483644835492, 0.13807578752828267, -0.2870310718814532, -0.05427332708421044, 0.26465315515629184, -0.07007738023655379, ... |
710.1202 | N to Delta electromagnetic and axial form factors in full QCD | Lattice results on the N to Delta electromagnetic, axial-vector and
pseudoscalar form factors are evaluated using dynamical staggered sea quarks
and domain wall valence quarks for pion masses in the range of 580-350 MeV, as
well as, dynamical and quenched Wilson fermions for similar pion masses.
| hep-lat hep-ph nucl-ex nucl-th | lattice results on the n to delta electromagnetic axialvector and pseudoscalar form factors are evaluated using dynamical staggered sea quarks and domain wall valence quarks for pion masses in the range of 580350 mev as well as dynamical and quenched wilson fermions for similar pion masses | [['lattice', 'results', 'on', 'the', 'n', 'to', 'delta', 'electromagnetic', 'axialvector', 'and', 'pseudoscalar', 'form', 'factors', 'are', 'evaluated', 'using', 'dynamical', 'staggered', 'sea', 'quarks', 'and', 'domain', 'wall', 'valence', 'quarks', 'for', 'pion', 'masses', 'in', 'the', 'range', 'of', '580350', 'mev',... | [-0.058317251337899105, 0.4280394967955848, -0.00993340709246695, 0.17178726150757737, -0.02533206128217797, -0.07497127135284246, 0.14501920694278347, 0.4255228633681933, -0.07524235032291876, -0.23893515500757428, -0.03669255151568602, -0.32461150874280265, 0.028828036997260317, 0.09245264472232925, 0.135137201804253... |
710.1203 | Semantic distillation: a method for clustering objects by their
contextual specificity | Techniques for data-mining, latent semantic analysis, contextual search of
databases, etc. have long ago been developed by computer scientists working on
information retrieval (IR). Experimental scientists, from all disciplines,
having to analyse large collections of raw experimental data (astronomical,
physical, bio... | math.PR cs.DB math.ST q-bio.QM stat.ML stat.TH | techniques for datamining latent semantic analysis contextual search of databases etc have long ago been developed by computer scientists working on information retrieval ir experimental scientists from all disciplines having to analyse large collections of raw experimental data astronomical physical biological etc hav... | [['techniques', 'for', 'datamining', 'latent', 'semantic', 'analysis', 'contextual', 'search', 'of', 'databases', 'etc', 'have', 'long', 'ago', 'been', 'developed', 'by', 'computer', 'scientists', 'working', 'on', 'information', 'retrieval', 'ir', 'experimental', 'scientists', 'from', 'all', 'disciplines', 'having', 't... | [-0.010928344619433487, 0.06305398352013838, -0.11505161108169167, 0.09016492913848576, -0.09121668191876994, -0.14993535093909313, 0.06446539854423568, 0.3718175276618645, -0.2818878972430167, -0.3605208819613636, 0.09438209071408182, -0.27653835927986814, -0.16864639877024068, 0.20974969219569806, -0.0761408865508338... |
710.1204 | Ion trap quantum gates with amplitude-modulated laser beams | In ion traps, entangling gate operations can be realized by a bichromatic
pair of laser beams that collectively interact with the ions. In this paper, a
new method of modelling the laser-ion interaction is introduced that turns out
to be superior to standard techniques for the description of gate operations on
optica... | quant-ph | in ion traps entangling gate operations can be realized by a bichromatic pair of laser beams that collectively interact with the ions in this paper a new method of modelling the laserion interaction is introduced that turns out to be superior to standard techniques for the description of gate operations on optical qubi... | [['in', 'ion', 'traps', 'entangling', 'gate', 'operations', 'can', 'be', 'realized', 'by', 'a', 'bichromatic', 'pair', 'of', 'laser', 'beams', 'that', 'collectively', 'interact', 'with', 'the', 'ions', 'in', 'this', 'paper', 'a', 'new', 'method', 'of', 'modelling', 'the', 'laserion', 'interaction', 'is', 'introduced', ... | [-0.14159312726152257, 0.2208977386393048, -0.052491383437481665, -0.01937942488712831, 0.03953868613168256, -0.23512970171270703, 0.07277033569979045, 0.47677389474226795, -0.21510754877257102, -0.27502095965730505, 0.004866741950102492, -0.23793920555481488, -0.08985324858457124, 0.2892226102428699, -0.04216592929778... |
710.1205 | Full Scale Dynamic Response of a RC Building under Weak Seismic Motions
Using Earthquake Recordings, Ambient Vibrations and Modelling | In countries with a moderate seismic hazard, the classical methods developed
for strong motion prone countries to estimate the seismic behaviour and
subsequent vulnerability of existing buildings are often inadequate and not
financially realistic. The main goals of this paper are to show how the modal
analysis can co... | physics.geo-ph physics.class-ph | in countries with a moderate seismic hazard the classical methods developed for strong motion prone countries to estimate the seismic behaviour and subsequent vulnerability of existing buildings are often inadequate and not financially realistic the main goals of this paper are to show how the modal analysis can contri... | [['in', 'countries', 'with', 'a', 'moderate', 'seismic', 'hazard', 'the', 'classical', 'methods', 'developed', 'for', 'strong', 'motion', 'prone', 'countries', 'to', 'estimate', 'the', 'seismic', 'behaviour', 'and', 'subsequent', 'vulnerability', 'of', 'existing', 'buildings', 'are', 'often', 'inadequate', 'and', 'not'... | [-0.07896245661483205, 0.12199269776786562, -0.06237595621286682, 0.06813629069196608, -0.07410822067774732, -0.08033359645832297, 0.02561390126042219, 0.3802440824461178, -0.23431984241632325, -0.2891856225769598, 0.14193088079169225, -0.2694117158403838, -0.14210178391019596, 0.23139716216535014, -0.08649005654880458... |
710.1206 | Study of DiMuon Rare Beauty Decays with ATLAS and CMS | The LHC experiments will perform sensitive tests of physics beyond the
Standard Model (BSM). The investigation of decays of beauty hadrons represents
an alternative approach in addition to direct BSM searches. The ATLAS and CMS
efforts concentrate on those B-decays that can be efficiently selected already
at the firs... | hep-ex | the lhc experiments will perform sensitive tests of physics beyond the standard model bsm the investigation of decays of beauty hadrons represents an alternative approach in addition to direct bsm searches the atlas and cms efforts concentrate on those bdecays that can be efficiently selected already at the first and s... | [['the', 'lhc', 'experiments', 'will', 'perform', 'sensitive', 'tests', 'of', 'physics', 'beyond', 'the', 'standard', 'model', 'bsm', 'the', 'investigation', 'of', 'decays', 'of', 'beauty', 'hadrons', 'represents', 'an', 'alternative', 'approach', 'in', 'addition', 'to', 'direct', 'bsm', 'searches', 'the', 'atlas', 'an... | [-0.016451858851637337, 0.19017574574796267, -0.10206060036684253, 0.13236807822527008, -0.0711826864266879, -0.14733512635021248, 0.016268031948129646, 0.3420204169482791, -0.19489674482818892, -0.33069736866413485, 0.08455946098893903, -0.3726638489059128, 0.07243101706817037, 0.18828246575209223, 0.03839103849826469... |
710.1207 | Binaries and the dynamical mass of star clusters | The total mass of a distant star cluster is often derived from the virial
theorem, using line-of-sight velocity dispersion measurements and half-light
radii, under the implicit assumption that all stars are single (although it is
known that most stars form part of binary systems). The components of binary
stars exhib... | astro-ph | the total mass of a distant star cluster is often derived from the virial theorem using lineofsight velocity dispersion measurements and halflight radii under the implicit assumption that all stars are single although it is known that most stars form part of binary systems the components of binary stars exhibit orbital... | [['the', 'total', 'mass', 'of', 'a', 'distant', 'star', 'cluster', 'is', 'often', 'derived', 'from', 'the', 'virial', 'theorem', 'using', 'lineofsight', 'velocity', 'dispersion', 'measurements', 'and', 'halflight', 'radii', 'under', 'the', 'implicit', 'assumption', 'that', 'all', 'stars', 'are', 'single', 'although', '... | [-0.13573122261585854, 0.1471704385289649, -0.06529161371384441, 0.08565097187501972, -0.06940913734795064, -0.02264043874101051, 0.043844179405780795, 0.35066037641325654, -0.15506293800668852, -0.3781661340629294, 0.040760569885410616, -0.26834591356849913, -0.055776170084577976, 0.2211642799861479, -0.03219707910871... |
710.1208 | Diagrammatic Inference | Diagrammatic logics were introduced in 2002, with emphasis on the notions of
specifications and models. In this paper we improve the description of the
inference process, which is seen as a Yoneda functor on a bicategory of
fractions. A diagrammatic logic is defined from a morphism of limit sketches
(called a propaga... | cs.LO math.CT | diagrammatic logics were introduced in 2002 with emphasis on the notions of specifications and models in this paper we improve the description of the inference process which is seen as a yoneda functor on a bicategory of fractions a diagrammatic logic is defined from a morphism of limit sketches called a propagator whi... | [['diagrammatic', 'logics', 'were', 'introduced', 'in', '2002', 'with', 'emphasis', 'on', 'the', 'notions', 'of', 'specifications', 'and', 'models', 'in', 'this', 'paper', 'we', 'improve', 'the', 'description', 'of', 'the', 'inference', 'process', 'which', 'is', 'seen', 'as', 'a', 'yoneda', 'functor', 'on', 'a', 'bicat... | [-0.0991433195733619, 0.04343687740815193, -0.1408776239790384, 0.13229602221100736, -0.1252728111282425, -0.1029814585989106, 0.058713588819531634, 0.3703152241131056, -0.34140226540372715, -0.23785367181289543, 0.031886147529573985, -0.2136240506943686, -0.09853064542799031, 0.16158909113734093, -0.17848490433116415,... |
710.1209 | Crustal structure below Popocat\'epetl Volcano (Mexico) from analysis of
Rayleigh waves | An array of ten broadband stations was installed on the Popocat\'epetl
volcano (Mexico) for five months between October 2002 and February 2003. 26
regional and teleseismic earthquakes were selected and filtered in the
frequency time domain to extract the fundamental mode of the Rayleigh wave. The
average dispersion c... | physics.geo-ph | an array of ten broadband stations was installed on the popocatepetl volcano mexico for five months between october 2002 and february 2003 26 regional and teleseismic earthquakes were selected and filtered in the frequency time domain to extract the fundamental mode of the rayleigh wave the average dispersion curve was... | [['an', 'array', 'of', 'ten', 'broadband', 'stations', 'was', 'installed', 'on', 'the', 'popocatepetl', 'volcano', 'mexico', 'for', 'five', 'months', 'between', 'october', '2002', 'and', 'february', '2003', '26', 'regional', 'and', 'teleseismic', 'earthquakes', 'were', 'selected', 'and', 'filtered', 'in', 'the', 'frequ... | [-0.10943254567023587, 0.16350023280761417, -0.08791686480303537, 0.0561180027833285, -0.055996669744477354, -0.07550150971247317, 0.05686731706054447, 0.3888592290156202, -0.22363181112304364, -0.37528240289454046, 0.12386657151374456, -0.30766103702948694, -0.09682970431465315, 0.2122809277692189, -0.0466464822485295... |
710.121 | Dynamic parameters of structures extracted from ambient vibration
measurements: an aid for the seismic vulnerability assessment of existing
buildings in moderate seismic hazard regions | During the past two decades, the use of ambient vibrations for modal analysis
of structures has increased as compared to the traditional techniques (forced
vibrations). The Frequency Domain Decomposition method is nowadays widely used
in modal analysis because of its accuracy and simplicity. In this paper, we
first p... | physics.geo-ph physics.class-ph | during the past two decades the use of ambient vibrations for modal analysis of structures has increased as compared to the traditional techniques forced vibrations the frequency domain decomposition method is nowadays widely used in modal analysis because of its accuracy and simplicity in this paper we first present t... | [['during', 'the', 'past', 'two', 'decades', 'the', 'use', 'of', 'ambient', 'vibrations', 'for', 'modal', 'analysis', 'of', 'structures', 'has', 'increased', 'as', 'compared', 'to', 'the', 'traditional', 'techniques', 'forced', 'vibrations', 'the', 'frequency', 'domain', 'decomposition', 'method', 'is', 'nowadays', 'wi... | [-0.04929677922810827, 0.07723227241284414, -0.09326595121196338, 0.03226950080077846, -0.0829398435447365, -0.0861883125906544, 0.020921900851785073, 0.37705953674657006, -0.28862256490758487, -0.2676737551337906, 0.13960622260746147, -0.23342732265059438, -0.13081062248907982, 0.21057868930644222, -0.0539762333501130... |
710.1211 | D0-D0 Mixing at BaBar | The BaBar and Belle collaborations have recently found evidence for mixing
within the D meson system. We present some of the mixing search techniques used
by BaBar and their status as of the beginning of the summer 2007. These have
culminated in a measurement in the K decay final state of the D that is
inconsistent w... | hep-ex | the babar and belle collaborations have recently found evidence for mixing within the d meson system we present some of the mixing search techniques used by babar and their status as of the beginning of the summer 2007 these have culminated in a measurement in the k decay final state of the d that is inconsistent with ... | [['the', 'babar', 'and', 'belle', 'collaborations', 'have', 'recently', 'found', 'evidence', 'for', 'mixing', 'within', 'the', 'd', 'meson', 'system', 'we', 'present', 'some', 'of', 'the', 'mixing', 'search', 'techniques', 'used', 'by', 'babar', 'and', 'their', 'status', 'as', 'of', 'the', 'beginning', 'of', 'the', 'su... | [-0.07449023065560345, 0.178937250595373, -0.12492581301215869, 0.050811290068538, -0.02193771701639713, -0.1224300101496724, 0.10212817756500818, 0.27834201657557306, -0.14740606411290702, -0.3154508193482214, 0.08193993498049955, -0.33139689408465106, -0.05790760516842355, 0.14712871790085155, 0.03181002290099303, 0.... |
710.1212 | The nature of the light scalar mesons from their radiative decays | The nature of the light scalar mesons is one of the most intriguing open
challenges in hadronic spectroscopy. It is argued that radiative decays
involving these scalars can serve as an important decisive tool in establishing
their nature. In particular, special emphasis is made on the radiative decays
of the scalars ... | hep-ph | the nature of the light scalar mesons is one of the most intriguing open challenges in hadronic spectroscopy it is argued that radiative decays involving these scalars can serve as an important decisive tool in establishing their nature in particular special emphasis is made on the radiative decays of the scalars thems... | [['the', 'nature', 'of', 'the', 'light', 'scalar', 'mesons', 'is', 'one', 'of', 'the', 'most', 'intriguing', 'open', 'challenges', 'in', 'hadronic', 'spectroscopy', 'it', 'is', 'argued', 'that', 'radiative', 'decays', 'involving', 'these', 'scalars', 'can', 'serve', 'as', 'an', 'important', 'decisive', 'tool', 'in', 'e... | [-0.08072897244985781, 0.21196135395999788, -0.03728199609228083, 0.14524791409683138, -0.06543153678039498, -0.16479681521918424, 0.008882084103911562, 0.3524724466197595, -0.18755899674677592, -0.23217901859331774, 0.032335912909459426, -0.3224824131812548, -0.05335954939506042, 0.16179124906350784, 0.076743763567867... |
710.1213 | Exploiting soliton decay and phase fluctuations in atom chip
interferometry of Bose-Einstein condensates | We show that the decay of a soliton into vortices provides a mechanism for
measuring the initial phase difference between two merging Bose-Einstein
condensates. At very low temperatures, the mechanism is resonant, operating
only when the clouds start in anti-phase. But at higher temperatures, phase
fluctuations trigg... | cond-mat.other | we show that the decay of a soliton into vortices provides a mechanism for measuring the initial phase difference between two merging boseeinstein condensates at very low temperatures the mechanism is resonant operating only when the clouds start in antiphase but at higher temperatures phase fluctuations trigger vortex... | [['we', 'show', 'that', 'the', 'decay', 'of', 'a', 'soliton', 'into', 'vortices', 'provides', 'a', 'mechanism', 'for', 'measuring', 'the', 'initial', 'phase', 'difference', 'between', 'two', 'merging', 'boseeinstein', 'condensates', 'at', 'very', 'low', 'temperatures', 'the', 'mechanism', 'is', 'resonant', 'operating',... | [-0.18806171611349068, 0.27997576098972826, -0.08978440156834347, 0.05540842485085674, -0.011978873870534342, -0.12974220942810513, 0.075190933695942, 0.38502393081114533, -0.24821533370773527, -0.3129734351310167, 0.04769937859931856, -0.25172991662422256, -0.031221295099998457, 0.17830314529599267, 0.0411904558455676... |
710.1214 | Shot-noise of quantum chaotic systems in the classical limit | Semiclassical methods can now explain many mesoscopic effects (shot-noise,
conductance fluctuations, etc) in clean chaotic systems, such as chaotic
quantum dots. In the deep classical limit (wavelength much less than system
size) the Ehrenfest time (the time for a wavepacket to spread to a classical
size) plays a cru... | cond-mat.mes-hall nlin.CD | semiclassical methods can now explain many mesoscopic effects shotnoise conductance fluctuations etc in clean chaotic systems such as chaotic quantum dots in the deep classical limit wavelength much less than system size the ehrenfest time the time for a wavepacket to spread to a classical size plays a crucial role and... | [['semiclassical', 'methods', 'can', 'now', 'explain', 'many', 'mesoscopic', 'effects', 'shotnoise', 'conductance', 'fluctuations', 'etc', 'in', 'clean', 'chaotic', 'systems', 'such', 'as', 'chaotic', 'quantum', 'dots', 'in', 'the', 'deep', 'classical', 'limit', 'wavelength', 'much', 'less', 'than', 'system', 'size', '... | [-0.11499096896304879, 0.11802441716382775, -0.06488628617393537, 0.00660510657390556, -0.017510860899015317, -0.14013838048588154, 0.08107291877452473, 0.3129630306488068, -0.22298866362219583, -0.2678538996260613, 0.009342083711872656, -0.27493083052914824, -0.18512335724839823, 0.24454346841534222, -0.13111466158010... |
710.1215 | Measuring the spin up of the Accreting Millisecond Pulsar XTE J1751-305 | We perform a timing analysis on RXTE data of the accreting millisecond pulsar
XTE J1751-305 observed during the April 2002 outburst. After having corrected
for Doppler effects on the pulse phases due to the orbital motion of the
source, we performed a timing analysis on the phase delays, which gives, for
the first ti... | astro-ph | we perform a timing analysis on rxte data of the accreting millisecond pulsar xte j1751305 observed during the april 2002 outburst after having corrected for doppler effects on the pulse phases due to the orbital motion of the source we performed a timing analysis on the phase delays which gives for the first time for ... | [['we', 'perform', 'a', 'timing', 'analysis', 'on', 'rxte', 'data', 'of', 'the', 'accreting', 'millisecond', 'pulsar', 'xte', 'j1751305', 'observed', 'during', 'the', 'april', '2002', 'outburst', 'after', 'having', 'corrected', 'for', 'doppler', 'effects', 'on', 'the', 'pulse', 'phases', 'due', 'to', 'the', 'orbital', ... | [-0.12662729572788892, 0.11274190209680178, -0.08129057032746752, 0.07952549859735389, -0.0896841631018383, -0.04737666878805859, 0.1133148263472969, 0.3633820956288758, -0.1976067995774891, -0.35832305058394953, 0.1568894777525911, -0.30992852605413646, 0.0015475394952079375, 0.2873526722571607, -0.029910630574134196,... |
710.1216 | Spin resonance of 2D electrons in a large-area silicon MOSFET | We report electron spin resonance (ESR) measurements on a large-area silicon
MOSFET. An ESR signal at g-factor 1.9999(1), and with a linewidth of 0.6 G, is
observed and found to arise from two-dimensional (2D) electrons at the Si/SiO2
interface. The signal and its intensity show a pronounced dependence on applied
gat... | cond-mat.mtrl-sci cond-mat.other | we report electron spin resonance esr measurements on a largearea silicon mosfet an esr signal at gfactor 199991 and with a linewidth of 06 g is observed and found to arise from twodimensional 2d electrons at the sisio2 interface the signal and its intensity show a pronounced dependence on applied gate voltage at gate ... | [['we', 'report', 'electron', 'spin', 'resonance', 'esr', 'measurements', 'on', 'a', 'largearea', 'silicon', 'mosfet', 'an', 'esr', 'signal', 'at', 'gfactor', '199991', 'and', 'with', 'a', 'linewidth', 'of', '06', 'g', 'is', 'observed', 'and', 'found', 'to', 'arise', 'from', 'twodimensional', '2d', 'electrons', 'at', '... | [-0.11247204620239995, 0.18050730774669782, 0.00705815225496496, -0.017841053144238367, 0.00751486393672071, -0.23092898262844405, 0.09591731283683003, 0.434834087300196, -0.2454004751644996, -0.3479924793110082, -0.0068315110177520596, -0.33044213025520247, -0.049818320412254126, 0.27318119055085016, 0.047414980452965... |
710.1217 | Exploring the QCD phase diagram | Lattice simulations employing reweighting and Taylor expansion techniques
have predicted a (\mu,T)-phase diagram according to general expectations, with
an analytic quark-hadron crossover at \mu=0 turning into a first order
transition at some critical chemical potential \mu_E. By contrast, recent
simulations using im... | hep-ph | lattice simulations employing reweighting and taylor expansion techniques have predicted a mutphase diagram according to general expectations with an analytic quarkhadron crossover at mu0 turning into a first order transition at some critical chemical potential mu_e by contrast recent simulations using imgainary mu fol... | [['lattice', 'simulations', 'employing', 'reweighting', 'and', 'taylor', 'expansion', 'techniques', 'have', 'predicted', 'a', 'mutphase', 'diagram', 'according', 'to', 'general', 'expectations', 'with', 'an', 'analytic', 'quarkhadron', 'crossover', 'at', 'mu0', 'turning', 'into', 'a', 'first', 'order', 'transition', 'a... | [-0.07184922395848066, 0.14337536575847068, -0.11899861782414359, 0.09560513221468402, -0.05488347873654006, -0.13727186479365583, 0.1287120099197019, 0.3888903218409363, -0.19921931416768604, -0.26999854984101634, 0.13685834929918134, -0.2807803527223614, -0.10973619598298225, 0.17014693066993225, 0.02579602774279485,... |
710.1218 | Luminescence evidence for bulk and surface excitons in free xenon
clusters | Cathodoluminescence spectra of free xenon clusters produced by condensation
of xenon-argon gas mixtures in supersonic jets expanding into vacuum were
studied. By varying initial experimental parameters, including xenon
concentration, we could obtain clusters with a xenon core (300-3500 atoms)
covered by an argon oute... | physics.atm-clus physics.optics | cathodoluminescence spectra of free xenon clusters produced by condensation of xenonargon gas mixtures in supersonic jets expanding into vacuum were studied by varying initial experimental parameters including xenon concentration we could obtain clusters with a xenon core 3003500 atoms covered by an argon outer shell a... | [['cathodoluminescence', 'spectra', 'of', 'free', 'xenon', 'clusters', 'produced', 'by', 'condensation', 'of', 'xenonargon', 'gas', 'mixtures', 'in', 'supersonic', 'jets', 'expanding', 'into', 'vacuum', 'were', 'studied', 'by', 'varying', 'initial', 'experimental', 'parameters', 'including', 'xenon', 'concentration', '... | [-0.014017595761986234, 0.23781317088490372, -0.031335814137647085, 0.03906486252983382, 0.03942420800909573, -0.09090754581893282, 0.045312742042073674, 0.4272613835109528, -0.21273543559332458, -0.3533540699313315, 0.030974892279414763, -0.3483070505046567, 0.028815820562299484, 0.1520719318650663, 0.0550210741384662... |
710.1219 | First results of the Noether theorem for Hopf-algebra spacetime
symmetries | We summarize here the first results obtained using a technique we recently
developed for the Noether analysis of Hopf-algebra spacetime symmetries,
including the derivation of conserved charges for field theories in
noncommutative spacetimes of canonical or kappa-Minkowski type.
| gr-qc | we summarize here the first results obtained using a technique we recently developed for the noether analysis of hopfalgebra spacetime symmetries including the derivation of conserved charges for field theories in noncommutative spacetimes of canonical or kappaminkowski type | [['we', 'summarize', 'here', 'the', 'first', 'results', 'obtained', 'using', 'a', 'technique', 'we', 'recently', 'developed', 'for', 'the', 'noether', 'analysis', 'of', 'hopfalgebra', 'spacetime', 'symmetries', 'including', 'the', 'derivation', 'of', 'conserved', 'charges', 'for', 'field', 'theories', 'in', 'noncommuta... | [-0.12677565417987735, 0.09074226625900912, -0.09756966190118539, 0.08410416636615992, -0.1206245556424715, -0.11132642522601313, -0.058645734750347116, 0.2902559106189169, -0.16598056266574482, -0.2452535738580321, 0.06939628082756444, -0.23739444052702502, -0.17935024690201604, 0.17891999862867555, -0.077574902373415... |
710.122 | From Bruhat intervals to intersection lattices and a conjecture of
Postnikov | We prove the conjecture of A. Postnikov that (A) the number of regions in the
inversion hyperplane arrangement associated with a permutation $w\in \Sn$ is at
most the number of elements below $w$ in the Bruhat order, and (B) that
equality holds if and only if $w$ avoids the patterns 4231, 35142, 42513 and
351624. Fur... | math.CO | we prove the conjecture of a postnikov that a the number of regions in the inversion hyperplane arrangement associated with a permutation win sn is at most the number of elements below w in the bruhat order and b that equality holds if and only if w avoids the patterns 4231 35142 42513 and 351624 furthermore assertion ... | [['we', 'prove', 'the', 'conjecture', 'of', 'a', 'postnikov', 'that', 'a', 'the', 'number', 'of', 'regions', 'in', 'the', 'inversion', 'hyperplane', 'arrangement', 'associated', 'with', 'a', 'permutation', 'win', 'sn', 'is', 'at', 'most', 'the', 'number', 'of', 'elements', 'below', 'w', 'in', 'the', 'bruhat', 'order', ... | [-0.1868559803863588, 0.1303705965651066, -0.06910751486845713, 0.056147746489192026, -0.10854874331354429, -0.12960667529426115, 0.1084780977227118, 0.288718730452404, -0.3206857951892224, -0.2593777987991156, 0.08710986710450795, -0.2345696158653092, -0.15133905576242665, 0.16965211294674581, -0.12647240203971574, -0... |
710.1221 | Sensitivity of the magnetic state of a spin lattice on itinerant
electron orbital phase | Spatially extended localized spins can interact via indirect exchange
interaction through Friedel oscillations in the Fermi sea. In arrays of
localized spins such interaction can lead to a magnetically ordered phase.
Without external magnetic field such a phase is well understood via a
"two-impurity" Kondo model. Her... | cond-mat.mes-hall | spatially extended localized spins can interact via indirect exchange interaction through friedel oscillations in the fermi sea in arrays of localized spins such interaction can lead to a magnetically ordered phase without external magnetic field such a phase is well understood via a twoimpurity kondo model here we emp... | [['spatially', 'extended', 'localized', 'spins', 'can', 'interact', 'via', 'indirect', 'exchange', 'interaction', 'through', 'friedel', 'oscillations', 'in', 'the', 'fermi', 'sea', 'in', 'arrays', 'of', 'localized', 'spins', 'such', 'interaction', 'can', 'lead', 'to', 'a', 'magnetically', 'ordered', 'phase', 'without',... | [-0.2551066383321801, 0.3258533382558086, -0.021325768819183445, 0.11091684133175425, -0.042592503549007885, -0.10840216219383345, 0.07770162068956186, 0.41414957457180185, -0.3125037821428327, -0.2996602228141568, -0.015426098947214443, -0.2763984345757727, -0.11161054199917263, 0.15024060160745709, 0.1224789385176316... |
710.1222 | Euler Characteristic of real nondegenerate tropical complete
intersections | We define nondegenerate tropical complete intersections imitating the
corresponding definition in complex algebraic geometry. As in the complex
situation, all nonzero intersection multiplicity numbers between tropical
hypersurfaces defining a nondegenerate tropical complete intersection are equal
to 1. The intersecti... | math.AG math.CO | we define nondegenerate tropical complete intersections imitating the corresponding definition in complex algebraic geometry as in the complex situation all nonzero intersection multiplicity numbers between tropical hypersurfaces defining a nondegenerate tropical complete intersection are equal to 1 the intersection mu... | [['we', 'define', 'nondegenerate', 'tropical', 'complete', 'intersections', 'imitating', 'the', 'corresponding', 'definition', 'in', 'complex', 'algebraic', 'geometry', 'as', 'in', 'the', 'complex', 'situation', 'all', 'nonzero', 'intersection', 'multiplicity', 'numbers', 'between', 'tropical', 'hypersurfaces', 'defini... | [-0.22186418870836497, 0.05839029005449265, -0.094145866304636, 0.11839582947734743, -0.09073878812044858, -0.11655742291733623, -0.03686394418776035, 0.23067239028960465, -0.33184112475812433, -0.18354743108898403, 0.10283702219836414, -0.25821249674074354, -0.1898453245171695, 0.1590488106608391, -0.2030049081146717,... |
710.1223 | Jet broadening in unstable non-Abelian plasmas | We perform numerical simulations of the QCD Boltzmann-Vlasov equation
including both hard elastic particle collisions and soft interactions mediated
by classical Yang-Mills fields. We provide an estimate of the coupling of jets
to a hot plasma which is independent of infrared cutoffs. For weakly-coupled
anisotropic p... | hep-ph nucl-th | we perform numerical simulations of the qcd boltzmannvlasov equation including both hard elastic particle collisions and soft interactions mediated by classical yangmills fields we provide an estimate of the coupling of jets to a hot plasma which is independent of infrared cutoffs for weaklycoupled anisotropic plasmas ... | [['we', 'perform', 'numerical', 'simulations', 'of', 'the', 'qcd', 'boltzmannvlasov', 'equation', 'including', 'both', 'hard', 'elastic', 'particle', 'collisions', 'and', 'soft', 'interactions', 'mediated', 'by', 'classical', 'yangmills', 'fields', 'we', 'provide', 'an', 'estimate', 'of', 'the', 'coupling', 'of', 'jets... | [-0.1590335625474171, 0.2738486062499046, -0.12563445935368797, 0.11450772183341405, -0.07649079673192515, -0.09447480033412176, -0.040511776803321735, 0.4072474623799965, -0.19908368564461187, -0.28039865825645705, -0.008928182902896115, -0.2637630697610157, 0.0005074421748749271, 0.13128139126059468, 0.07196949905044... |
710.1224 | Quantum cohomology of minuscule homogeneous spaces III : semi-simplicity
and consequences | We prove that the quantum cohomology ring of any minuscule or cominuscule
homogeneous space, specialized at q=1, is semisimple. This implies that complex
conjugation defines an algebra automorphism of the quantum cohomology ring
localized at the quantum parameter. We check that this involution coincides
with the stra... | math.AG | we prove that the quantum cohomology ring of any minuscule or cominuscule homogeneous space specialized at q1 is semisimple this implies that complex conjugation defines an algebra automorphism of the quantum cohomology ring localized at the quantum parameter we check that this involution coincides with the strange dua... | [['we', 'prove', 'that', 'the', 'quantum', 'cohomology', 'ring', 'of', 'any', 'minuscule', 'or', 'cominuscule', 'homogeneous', 'space', 'specialized', 'at', 'q1', 'is', 'semisimple', 'this', 'implies', 'that', 'complex', 'conjugation', 'defines', 'an', 'algebra', 'automorphism', 'of', 'the', 'quantum', 'cohomology', 'r... | [-0.2741399336239842, 0.1001134888046196, -0.10885073378926417, 0.05887330264486678, -0.11001735602001675, -0.1796745138746671, -0.035921520013438506, 0.2820766353827031, -0.3704991073454501, -0.14699308192510097, 0.04934480137642107, -0.2061052218110102, -0.15926044900351982, 0.16599516131243378, -0.16859024400382921,... |
710.1225 | Evidence of the virtual Anderson transition in a narrow impurity band of
p-GaAs/AlGaAs quantum wells: $\epsilon_4$ conductivity and electric breakdown
at low temperatures | In highly doped uncompensated p-type layers within the central part of
GaAs/AlGaAs quantum wells at low temperatures we observed an activated behavior
of the conductivity with low activation energies (1-3) meV which can not be
ascribed to standard mechanisms. We attribute this behavior to the
delocalization of hole s... | cond-mat.dis-nn cond-mat.mtrl-sci | in highly doped uncompensated ptype layers within the central part of gaasalgaas quantum wells at low temperatures we observed an activated behavior of the conductivity with low activation energies 13 mev which can not be ascribed to standard mechanisms we attribute this behavior to the delocalization of hole states ne... | [['in', 'highly', 'doped', 'uncompensated', 'ptype', 'layers', 'within', 'the', 'central', 'part', 'of', 'gaasalgaas', 'quantum', 'wells', 'at', 'low', 'temperatures', 'we', 'observed', 'an', 'activated', 'behavior', 'of', 'the', 'conductivity', 'with', 'low', 'activation', 'energies', '13', 'mev', 'which', 'can', 'not... | [-0.12977773775009954, 0.23209177983350734, -0.016500246165466147, 0.06352493377943826, 0.027444099265968438, -0.17375821948993997, 0.11679902781328433, 0.35767929060721254, -0.27491032129366805, -0.3121610289854727, -0.0017442996136799276, -0.3163274105930005, -0.09149812034566898, 0.14429142833995937, -0.020452729786... |
710.1226 | NIR Femtosecond Control of Resonance-Mediated Generation of Coherent
Broadband UV Emission | We use shaped near-infrared (NIR) pulses to control the generation of
coherent broadband ultraviolet (UV) radiation in an atomic resonance-mediated
(2+1) three-photon excitation. Experimental and theoretical results are
presented for phase controlling the total emitted UV yield in atomic sodium
(Na). Based on our con... | physics.atom-ph physics.chem-ph | we use shaped nearinfrared nir pulses to control the generation of coherent broadband ultraviolet uv radiation in an atomic resonancemediated 21 threephoton excitation experimental and theoretical results are presented for phase controlling the total emitted uv yield in atomic sodium na based on our confirmed understan... | [['we', 'use', 'shaped', 'nearinfrared', 'nir', 'pulses', 'to', 'control', 'the', 'generation', 'of', 'coherent', 'broadband', 'ultraviolet', 'uv', 'radiation', 'in', 'an', 'atomic', 'resonancemediated', '21', 'threephoton', 'excitation', 'experimental', 'and', 'theoretical', 'results', 'are', 'presented', 'for', 'phas... | [-0.051949486167480546, 0.17373521357949356, -0.01925038422147433, 0.005201168461935595, 0.007929445281624793, -0.1142085552153488, 0.04872586576578518, 0.535496431911985, -0.184852620412906, -0.27866755139703553, -0.002856597448699176, -0.24292890492205818, -0.06290458655295272, 0.27210653175599875, -0.023911579207827... |
710.1227 | A DC magnetic metamaterial | Electromagnetic metamaterials are a class of materials which have been
artificially structured on a subwavelength scale. They are currently the focus
of a great deal of interest because they allow access to previously
unrealisable properties like a negative refractive index. Most metamaterial
designs have so far been... | cond-mat.mtrl-sci | electromagnetic metamaterials are a class of materials which have been artificially structured on a subwavelength scale they are currently the focus of a great deal of interest because they allow access to previously unrealisable properties like a negative refractive index most metamaterial designs have so far been bas... | [['electromagnetic', 'metamaterials', 'are', 'a', 'class', 'of', 'materials', 'which', 'have', 'been', 'artificially', 'structured', 'on', 'a', 'subwavelength', 'scale', 'they', 'are', 'currently', 'the', 'focus', 'of', 'a', 'great', 'deal', 'of', 'interest', 'because', 'they', 'allow', 'access', 'to', 'previously', 'u... | [-0.14365699482792668, 0.15190783161930901, -0.034888438061522, -0.011115783309274964, -0.14089508800092956, -0.14995632544962753, -0.015482835852187769, 0.4716087726683452, -0.17986018718140007, -0.2943413617667453, 0.08114726050788987, -0.28201034929731794, -0.14808629045648308, 0.26852838942331486, -0.00775789748556... |
710.1228 | Axion-Dilaton Quantum String Cosmology for Flux Compactification and its
Symmetry Breaking | The Wheeler-De Witt equation of type IIB quantum string cosmology
compactified with constant internal H-fluxes on a 6-torus, whose volume modulus
is frozen, is solved under the WKB approximation. The spontaneous symmetry
breaking of the S-duality group by H-fluxes is also examined.
| hep-th gr-qc | the wheelerde witt equation of type iib quantum string cosmology compactified with constant internal hfluxes on a 6torus whose volume modulus is frozen is solved under the wkb approximation the spontaneous symmetry breaking of the sduality group by hfluxes is also examined | [['the', 'wheelerde', 'witt', 'equation', 'of', 'type', 'iib', 'quantum', 'string', 'cosmology', 'compactified', 'with', 'constant', 'internal', 'hfluxes', 'on', 'a', '6torus', 'whose', 'volume', 'modulus', 'is', 'frozen', 'is', 'solved', 'under', 'the', 'wkb', 'approximation', 'the', 'spontaneous', 'symmetry', 'breaki... | [-0.2179785632040529, 0.17415142385289073, -0.11265812240335868, 0.1088001337761636, -0.15550212537692415, -0.17577800432974028, -0.007451837630166362, 0.2700610346149742, -0.2624022119368116, -0.18535609588780927, 0.13216057331079528, -0.19506752039749353, -0.11535218505776443, 0.09252472110979613, -0.0492111131094307... |
710.1229 | Photon pressure induced test mass deformation in gravitational-wave
detectors | A widely used assumption within the gravitational-wave community has so far
been that a test mass acts like a rigid body for frequencies in the detection
band, i.e. for frequencies far below the first internal resonance. In this
article we demonstrate that localized forces, applied for example by a photon
pressure ac... | gr-qc | a widely used assumption within the gravitationalwave community has so far been that a test mass acts like a rigid body for frequencies in the detection band ie for frequencies far below the first internal resonance in this article we demonstrate that localized forces applied for example by a photon pressure actuator c... | [['a', 'widely', 'used', 'assumption', 'within', 'the', 'gravitationalwave', 'community', 'has', 'so', 'far', 'been', 'that', 'a', 'test', 'mass', 'acts', 'like', 'a', 'rigid', 'body', 'for', 'frequencies', 'in', 'the', 'detection', 'band', 'ie', 'for', 'frequencies', 'far', 'below', 'the', 'first', 'internal', 'resona... | [-0.09415270379245204, 0.17852522146206387, -0.03453175777559812, 0.059212375209023504, -0.04923942608317149, -0.09447210898488453, 0.04189190252194392, 0.36886772590199696, -0.216209393949968, -0.33881849229105354, 0.06879937798072844, -0.2613210230297649, -0.11145620211267594, 0.23414014128382443, -0.0058856467613182... |
710.123 | Density functional study of the electronic and vibrational properties of
TiOCl | We present the phonon spectrum of TiOCl computed using hybrid density
functional theory (DFT). A complete analysis of the spectrum is performed for
the space group Pmmn (high symmetry phase) and the space group P2_1/m (low
symmetry phase), which is the symmetry of the spin-Peierls phase. We show that
the nonlocal cor... | cond-mat.str-el | we present the phonon spectrum of tiocl computed using hybrid density functional theory dft a complete analysis of the spectrum is performed for the space group pmmn high symmetry phase and the space group p2_1m low symmetry phase which is the symmetry of the spinpeierls phase we show that the nonlocal correlations pre... | [['we', 'present', 'the', 'phonon', 'spectrum', 'of', 'tiocl', 'computed', 'using', 'hybrid', 'density', 'functional', 'theory', 'dft', 'a', 'complete', 'analysis', 'of', 'the', 'spectrum', 'is', 'performed', 'for', 'the', 'space', 'group', 'pmmn', 'high', 'symmetry', 'phase', 'and', 'the', 'space', 'group', 'p2_1m', '... | [-0.1556474767544026, 0.1640971283723336, -0.1159042485066623, 0.06396049158767768, -0.052557154161308614, -0.06861086680169498, 0.09536518468355228, 0.4148430445689767, -0.2673433270778448, -0.2597410648780328, 0.04305328835829324, -0.31724855488181, -0.16890451113974292, 0.12358440767552349, 0.06920901082071756, 0.02... |
710.1231 | Dynamics of vortex penetration, jumpwise instabilities and nonlinear
surface resistance of type-II superconductors in strong rf fields | We consider nonlinear dynamics of a single vortex in a superconductor in a
strong rf magnetic field $B_0\sin\omega t$. Using the London theory, we
calculate the dissipated power $Q(B_0,\omega)$, and the transient time scales
of vortex motion for the linear Bardeen-Stephen viscous drag force, which
results in unphysic... | cond-mat.supr-con | we consider nonlinear dynamics of a single vortex in a superconductor in a strong rf magnetic field b_0sinomega t using the london theory we calculate the dissipated power qb_0omega and the transient time scales of vortex motion for the linear bardeenstephen viscous drag force which results in unphysically high vortex ... | [['we', 'consider', 'nonlinear', 'dynamics', 'of', 'a', 'single', 'vortex', 'in', 'a', 'superconductor', 'in', 'a', 'strong', 'rf', 'magnetic', 'field', 'b_0sinomega', 't', 'using', 'the', 'london', 'theory', 'we', 'calculate', 'the', 'dissipated', 'power', 'qb_0omega', 'and', 'the', 'transient', 'time', 'scales', 'of'... | [-0.19184807040969193, 0.2218225281346762, -0.0736188838495512, 0.022955324411017622, -0.0528113590273104, -0.11475177951212079, 0.03897911891456336, 0.32556710401429656, -0.26719525652100773, -0.2614868343421138, 0.02833155933913613, -0.26219043924689733, -0.07600217155349266, 0.22878803060702788, 0.024287402639302985... |
710.1232 | A Canonical Quadratic Form on the Determinant Line of a Flat Vector
Bundle | We introduce and study a canonical quadratic form, called the torsion
quadratic form, of the determinant line of a flat vector bundle over a closed
oriented odd-dimensional manifold. This quadratic form caries less information
than the refined analytic torsion, introduced in our previous work, but is
easier to constr... | math.DG math.GT | we introduce and study a canonical quadratic form called the torsion quadratic form of the determinant line of a flat vector bundle over a closed oriented odddimensional manifold this quadratic form caries less information than the refined analytic torsion introduced in our previous work but is easier to construct and ... | [['we', 'introduce', 'and', 'study', 'a', 'canonical', 'quadratic', 'form', 'called', 'the', 'torsion', 'quadratic', 'form', 'of', 'the', 'determinant', 'line', 'of', 'a', 'flat', 'vector', 'bundle', 'over', 'a', 'closed', 'oriented', 'odddimensional', 'manifold', 'this', 'quadratic', 'form', 'caries', 'less', 'informa... | [-0.18796723426838843, 0.06204517965495048, -0.08828295247377387, 0.10874223478550583, -0.1619093045966978, -0.13060886561388857, -0.01629082256949496, 0.30611489066618613, -0.2928930905048104, -0.26444788295012933, 0.054829321296527, -0.21266617999417473, -0.2343183669245577, 0.20871208985229076, -0.09078880804644406,... |
710.1233 | Dynamics of Domain Walls for Split and Runaway Potentials | We demonstrate that the evolution of wall-like inhomogeneities in run-away
potentials, characteristic of dynamical supersymmetry breaking and moduli
stabilisation, is very similar to the evolution of domain wall networks
associated with double well potentials. Instabilities that would lead to a
rapid decay of domain ... | hep-ph | we demonstrate that the evolution of walllike inhomogeneities in runaway potentials characteristic of dynamical supersymmetry breaking and moduli stabilisation is very similar to the evolution of domain wall networks associated with double well potentials instabilities that would lead to a rapid decay of domain walls c... | [['we', 'demonstrate', 'that', 'the', 'evolution', 'of', 'walllike', 'inhomogeneities', 'in', 'runaway', 'potentials', 'characteristic', 'of', 'dynamical', 'supersymmetry', 'breaking', 'and', 'moduli', 'stabilisation', 'is', 'very', 'similar', 'to', 'the', 'evolution', 'of', 'domain', 'wall', 'networks', 'associated', ... | [-0.11415472243013036, 0.20475311341703448, -0.12346166447919403, 0.1129935232606024, -0.0963310502274519, -0.11224730795699084, -0.00807463857703484, 0.3665604749395966, -0.2888947171119288, -0.30900390423898005, 0.09801394959840064, -0.2125590036933621, -0.09232852818309051, 0.16302167575181517, -0.02078679399405662,... |
710.1234 | Hamming Distance for Conjugates | Let x, y be strings of equal length. The Hamming distance h(x,y) between x
and y is the number of positions in which x and y differ. If x is a cyclic
shift of y, we say x and y are conjugates. We consider f(x,y), the Hamming
distance between the conjugates xy and yx. Over a binary alphabet f(x,y) is
always even, and ... | math.CO | let x y be strings of equal length the hamming distance hxy between x and y is the number of positions in which x and y differ if x is a cyclic shift of y we say x and y are conjugates we consider fxy the hamming distance between the conjugates xy and yx over a binary alphabet fxy is always even and must satisfy a furt... | [['let', 'x', 'y', 'be', 'strings', 'of', 'equal', 'length', 'the', 'hamming', 'distance', 'hxy', 'between', 'x', 'and', 'y', 'is', 'the', 'number', 'of', 'positions', 'in', 'which', 'x', 'and', 'y', 'differ', 'if', 'x', 'is', 'a', 'cyclic', 'shift', 'of', 'y', 'we', 'say', 'x', 'and', 'y', 'are', 'conjugates', 'we', '... | [-0.2251413423479313, 0.1599751653206546, -0.05204755518408049, 0.03526115164027682, -0.016315706562073456, -0.23945806522720625, 0.0706086233302596, 0.42405350719179424, -0.3453173593839719, -0.19756640805280767, 0.03307980529830924, -0.3309291881708694, -0.05379089009948075, 0.13566173338553025, -0.09702536275699025,... |
710.1235 | Large diamagnetic persistent currents | In multichannel rings, evanescent modes will always co-exist with propagating
modes. The evanescent modes can carry a very large diamagnetic persistent
current that can oscillate with energy and are very sensitive to impurity
scattering. This provides a natural explanation for the large diamagnetic
persistent current... | cond-mat.mes-hall | in multichannel rings evanescent modes will always coexist with propagating modes the evanescent modes can carry a very large diamagnetic persistent current that can oscillate with energy and are very sensitive to impurity scattering this provides a natural explanation for the large diamagnetic persistent currents obse... | [['in', 'multichannel', 'rings', 'evanescent', 'modes', 'will', 'always', 'coexist', 'with', 'propagating', 'modes', 'the', 'evanescent', 'modes', 'can', 'carry', 'a', 'very', 'large', 'diamagnetic', 'persistent', 'current', 'that', 'can', 'oscillate', 'with', 'energy', 'and', 'are', 'very', 'sensitive', 'to', 'impurit... | [-0.2525458900684801, 0.3131143214025845, -0.053522401676673326, 0.0967183861915449, -0.11273935988234977, -0.1905400449759327, -0.01632142546198641, 0.3653929339100917, -0.24107303435448557, -0.24959945872736475, 0.017384513140617248, -0.3348722365141536, -0.09776718555561577, 0.1921752040119221, 0.019784434446288895,... |
710.1236 | Detection of Spin Correlations in Optical Lattices by Light Scattering | We show that spin correlations of atoms in an optical lattice can be
reconstructed by coupling the system to the light, and by measuring
correlations between the emitted photons. This principle is the basis for a
method to characterize states in quantum computation and simulation with
optical lattices. As examples, w... | quant-ph | we show that spin correlations of atoms in an optical lattice can be reconstructed by coupling the system to the light and by measuring correlations between the emitted photons this principle is the basis for a method to characterize states in quantum computation and simulation with optical lattices as examples we stud... | [['we', 'show', 'that', 'spin', 'correlations', 'of', 'atoms', 'in', 'an', 'optical', 'lattice', 'can', 'be', 'reconstructed', 'by', 'coupling', 'the', 'system', 'to', 'the', 'light', 'and', 'by', 'measuring', 'correlations', 'between', 'the', 'emitted', 'photons', 'this', 'principle', 'is', 'the', 'basis', 'for', 'a',... | [-0.14183796119109235, 0.21962582678315812, -0.0883358614930116, 0.03457942853385569, 0.05941245658323169, -0.09261245232568506, 0.0469001714099089, 0.4070303674568148, -0.2836724152610473, -0.3067126056891592, 0.04633299724424861, -0.3162822451661615, -0.11396427671698962, 0.21030417314785368, 0.04775002494716318, 0.0... |
710.1237 | On the computation of Galois representations associated to level one
modular forms | In this paper we explicitly compute mod-l Galois representations associated
to modular forms. To be precise, we look at cases with l<=23 and the modular
forms considered will be cusp forms of level 1 and weight up to 22. We present
the result in terms of polynomials associated to the projectivised
representations. As... | math.NT | in this paper we explicitly compute modl galois representations associated to modular forms to be precise we look at cases with l23 and the modular forms considered will be cusp forms of level 1 and weight up to 22 we present the result in terms of polynomials associated to the projectivised representations as an appli... | [['in', 'this', 'paper', 'we', 'explicitly', 'compute', 'modl', 'galois', 'representations', 'associated', 'to', 'modular', 'forms', 'to', 'be', 'precise', 'we', 'look', 'at', 'cases', 'with', 'l23', 'and', 'the', 'modular', 'forms', 'considered', 'will', 'be', 'cusp', 'forms', 'of', 'level', '1', 'and', 'weight', 'up'... | [-0.15567218116822018, 0.05441875190434444, -0.09369815416985015, 0.08313738580192506, -0.10300120063450026, -0.080697992566865, 0.0049135788340472445, 0.3221031965255953, -0.3192588589761568, -0.2705043964020476, 0.09134329994128126, -0.2680003743962911, -0.214755979012293, 0.21972190033968375, -0.08276845753678809, 0... |
710.1238 | Field-tunable magnetic phases in a semiconductor-based two-dimensional
Kondo lattice | We show the existence of intrinsic localized spins in mesoscopic
high-mobility GaAs/AlGaAs heterostructures. Non-equilibrium transport
spectroscopy reveals a quasi-regular distribution of the spins, and indicates
that the spins interact indirectly via the conduction electrons. The
interaction between spins manifests ... | cond-mat.mes-hall | we show the existence of intrinsic localized spins in mesoscopic highmobility gaasalgaas heterostructures nonequilibrium transport spectroscopy reveals a quasiregular distribution of the spins and indicates that the spins interact indirectly via the conduction electrons the interaction between spins manifests in charac... | [['we', 'show', 'the', 'existence', 'of', 'intrinsic', 'localized', 'spins', 'in', 'mesoscopic', 'highmobility', 'gaasalgaas', 'heterostructures', 'nonequilibrium', 'transport', 'spectroscopy', 'reveals', 'a', 'quasiregular', 'distribution', 'of', 'the', 'spins', 'and', 'indicates', 'that', 'the', 'spins', 'interact', ... | [-0.22665801121308127, 0.2344075016115652, -0.0452558584582265, 0.025685279825096573, -0.0032283082695269004, -0.18944237673488573, 0.04019636239447608, 0.37387273445483143, -0.2901825005779179, -0.31268347333359525, -0.03471733547171684, -0.3173555572539931, -0.12543230083755907, 0.22025710581120375, 0.027827930627002... |
710.1239 | On Connections between the Quantum and Hydrodynamical Pictures of Matter | We present a general, model-independent, quantum statistical treatment of the
connection between the quantum and hydrodynamical pictures of reservoir driven
macroscopic systems. This treatment is centred on the large scale properties of
locally conserved hydrodynamical observables and is designed to form a bridge
bet... | math-ph cond-mat.stat-mech math.MP quant-ph | we present a general modelindependent quantum statistical treatment of the connection between the quantum and hydrodynamical pictures of reservoir driven macroscopic systems this treatment is centred on the large scale properties of locally conserved hydrodynamical observables and is designed to form a bridge between q... | [['we', 'present', 'a', 'general', 'modelindependent', 'quantum', 'statistical', 'treatment', 'of', 'the', 'connection', 'between', 'the', 'quantum', 'and', 'hydrodynamical', 'pictures', 'of', 'reservoir', 'driven', 'macroscopic', 'systems', 'this', 'treatment', 'is', 'centred', 'on', 'the', 'large', 'scale', 'properti... | [-0.12010195671395837, 0.14928425927503078, -0.17142057605087757, 0.10701457442637012, -0.009421644780291793, -0.09841356460546034, 0.021066429550581446, 0.28395191037013906, -0.2638175967423355, -0.2622455490309221, 0.041669817134628404, -0.26718286820002557, -0.10776864390765481, 0.16348402404144188, 0.00556380862733... |
710.124 | Electroformation in a flow chamber with solution exchange as a means of
preparation of flaccid giant vesicles | A recently described technique (Estes and Mayer, Biochim. Biophys. Acta 1712
(2005) 152--160) for the preparation of giant unilamellar vesicles (GUVs) in
solutions with high ionic strength is examined. By observing a series of
osmotic swellings followed by vesicle bursts upon a micropipette transfer of a
single POPC ... | cond-mat.soft | a recently described technique estes and mayer biochim biophys acta 1712 2005 152160 for the preparation of giant unilamellar vesicles guvs in solutions with high ionic strength is examined by observing a series of osmotic swellings followed by vesicle bursts upon a micropipette transfer of a single popc guv from a suc... | [['a', 'recently', 'described', 'technique', 'estes', 'and', 'mayer', 'biochim', 'biophys', 'acta', '1712', '2005', '152160', 'for', 'the', 'preparation', 'of', 'giant', 'unilamellar', 'vesicles', 'guvs', 'in', 'solutions', 'with', 'high', 'ionic', 'strength', 'is', 'examined', 'by', 'observing', 'a', 'series', 'of', '... | [-0.08781994741114502, 0.11294620830029509, -0.11318352519391248, -0.06390847903542006, 0.009861794121276874, -0.1358419087751267, 0.06535390575523846, 0.32928966035923135, -0.18984520055640203, -0.2815416373240833, 0.06186958972270636, -0.2488268362895514, -0.14306270861281797, 0.19109182220507556, -0.0589158016507728... |
710.1241 | The Debye-Waller factor of stabilized delta-Pu | The Debye-Waller factor has been calculated for stabilized delta-phase
plutonium with 5% aluminum. A quasi-harmonic Born-von Karman force model with
temperature dependent phonon frequencies was used to calculate the mean-square
thermal atomic displacement from absolute zero to 800 K. Implementation of the
observed an... | cond-mat.mtrl-sci | the debyewaller factor has been calculated for stabilized deltaphase plutonium with 5 aluminum a quasiharmonic bornvon karman force model with temperature dependent phonon frequencies was used to calculate the meansquare thermal atomic displacement from absolute zero to 800 k implementation of the observed anomalous so... | [['the', 'debyewaller', 'factor', 'has', 'been', 'calculated', 'for', 'stabilized', 'deltaphase', 'plutonium', 'with', '5', 'aluminum', 'a', 'quasiharmonic', 'bornvon', 'karman', 'force', 'model', 'with', 'temperature', 'dependent', 'phonon', 'frequencies', 'was', 'used', 'to', 'calculate', 'the', 'meansquare', 'therma... | [-0.07963885299184105, 0.28727978075304156, -0.06559510331135243, 0.004969702610238032, -0.027534788985080508, -0.1496112575934438, 0.07117184821981937, 0.40930362113497476, -0.24563698571133005, -0.29140456480143423, 0.0605771191873249, -0.3238445905524052, 0.028021880134474486, 0.20072387330054137, 0.0678505730254321... |
710.1242 | What Have Spacetime, Shape and Symmetry to Do with Thermodynamics? | Some highly speculative and serendipitous ideas that might relate
thermodynamics, spacetime, shape and symmetry are brought together. A
hypothetical spacetime comprising a pointwise lattice with a fixed metric is
considered. If there were absolute symmetry between displacement and time it is
suggested that the veloci... | physics.gen-ph | some highly speculative and serendipitous ideas that might relate thermodynamics spacetime shape and symmetry are brought together a hypothetical spacetime comprising a pointwise lattice with a fixed metric is considered if there were absolute symmetry between displacement and time it is suggested that the velocity of ... | [['some', 'highly', 'speculative', 'and', 'serendipitous', 'ideas', 'that', 'might', 'relate', 'thermodynamics', 'spacetime', 'shape', 'and', 'symmetry', 'are', 'brought', 'together', 'a', 'hypothetical', 'spacetime', 'comprising', 'a', 'pointwise', 'lattice', 'with', 'a', 'fixed', 'metric', 'is', 'considered', 'if', '... | [-0.13447327283211052, 0.1885125575938366, -0.10439780870502866, 0.06332340054654491, -0.1280968538139368, -0.1602339803971149, 0.033571994762767, 0.37081536412006244, -0.30077819913827086, -0.3152930296051341, 0.10707844050921267, -0.2950037741102278, -0.1339198944089632, 0.1779331254168741, -0.08656276258438625, 0.00... |
710.1243 | A Detailed Study of 2S 0114+650 with the RXTE | We present the results of a detailed study of the high mass X-ray binary 2S
0114+650 made with the pointed instruments onboard the Rossi X-ray Timing
Explorer. The spectral and temporal behaviour of this source was examined over
the pulse, orbital, and super-orbital timescales, covering $\sim$2 cycles of
the 30.7 d s... | astro-ph | we present the results of a detailed study of the high mass xray binary 2s 0114650 made with the pointed instruments onboard the rossi xray timing explorer the spectral and temporal behaviour of this source was examined over the pulse orbital and superorbital timescales covering sim2 cycles of the 307 d superorbital mo... | [['we', 'present', 'the', 'results', 'of', 'a', 'detailed', 'study', 'of', 'the', 'high', 'mass', 'xray', 'binary', '2s', '0114650', 'made', 'with', 'the', 'pointed', 'instruments', 'onboard', 'the', 'rossi', 'xray', 'timing', 'explorer', 'the', 'spectral', 'and', 'temporal', 'behaviour', 'of', 'this', 'source', 'was',... | [-0.1483356033459427, 0.14748634648282408, -0.08301317442574811, 0.08976816455880937, -0.1075765354070449, -0.0688254128255677, 0.0944916028463153, 0.4363650168070751, -0.22710909244010027, -0.3400742931109739, 0.09129117323110274, -0.2645832555220894, -0.06184826365660694, 0.20704063093592603, -0.08632315786738078, 0.... |
710.1244 | The Three-Dimensional Behavior of Spiral Shocks in Protoplanetary Disks | In this dissertation, I describe theoretical and numerical studies that
address the three-dimensional behavior of spiral shocks in protoplanetary disks
and the controversial topic of gas giant formation by disk instability. For
this work, I discuss characteristics of gravitational instabilities (GIs) in
bursting and ... | astro-ph | in this dissertation i describe theoretical and numerical studies that address the threedimensional behavior of spiral shocks in protoplanetary disks and the controversial topic of gas giant formation by disk instability for this work i discuss characteristics of gravitational instabilities gis in bursting and asymptot... | [['in', 'this', 'dissertation', 'i', 'describe', 'theoretical', 'and', 'numerical', 'studies', 'that', 'address', 'the', 'threedimensional', 'behavior', 'of', 'spiral', 'shocks', 'in', 'protoplanetary', 'disks', 'and', 'the', 'controversial', 'topic', 'of', 'gas', 'giant', 'formation', 'by', 'disk', 'instability', 'for... | [-0.10735922540673831, 0.12919352293635408, -0.04669753573576196, 0.10565793887427491, -0.050510485159854096, -0.07795019687101659, -0.005589513908166231, 0.3665575965928535, -0.2338506676386007, -0.25052680532810173, 0.10535577813473841, -0.22741726646199822, -0.10005909557609509, 0.16703683207290143, 0.00194638379099... |
710.1245 | Spectroscopy of strontium Rydberg states using electromagnetically
induced transparency | We report on the all-optical detection of Rydberg states in a effusive atomic
beam of strontium atoms using electromagnetically induced transparency (EIT).
Using narrow-linewidth CW lasers we obtain an EIT linewidth of 5 MHz. To
illustrate the high spectroscopic resolution offered by this method, we have
measured iso... | quant-ph | we report on the alloptical detection of rydberg states in a effusive atomic beam of strontium atoms using electromagnetically induced transparency eit using narrowlinewidth cw lasers we obtain an eit linewidth of 5 mhz to illustrate the high spectroscopic resolution offered by this method we have measured isotope shif... | [['we', 'report', 'on', 'the', 'alloptical', 'detection', 'of', 'rydberg', 'states', 'in', 'a', 'effusive', 'atomic', 'beam', 'of', 'strontium', 'atoms', 'using', 'electromagnetically', 'induced', 'transparency', 'eit', 'using', 'narrowlinewidth', 'cw', 'lasers', 'we', 'obtain', 'an', 'eit', 'linewidth', 'of', '5', 'mh... | [-0.09711591112361827, 0.2829983156835611, -0.0245420469076071, -0.023726763528391297, 0.05971637945359861, -0.15796807213542116, 0.12078097276881494, 0.5182523279332779, -0.189651572870248, -0.25263572043188337, -0.05369891566191603, -0.2572377372769193, 0.009459266789965856, 0.25536421143358023, 0.023828720509953483,... |
710.1246 | Growth rates of the Weibel and tearing mode instabilities in a
relativistic pair plasma | We present an algorithm for solving the linear dispersion relation in an
inhomogeneous, magnetised, relativistic plasma. The method is a generalisation
of a previously reported algorithm that was limited to the homogeneous case.
The extension involves projecting the spatial dependence of the perturbations
onto a set ... | astro-ph | we present an algorithm for solving the linear dispersion relation in an inhomogeneous magnetised relativistic plasma the method is a generalisation of a previously reported algorithm that was limited to the homogeneous case the extension involves projecting the spatial dependence of the perturbations onto a set of bas... | [['we', 'present', 'an', 'algorithm', 'for', 'solving', 'the', 'linear', 'dispersion', 'relation', 'in', 'an', 'inhomogeneous', 'magnetised', 'relativistic', 'plasma', 'the', 'method', 'is', 'a', 'generalisation', 'of', 'a', 'previously', 'reported', 'algorithm', 'that', 'was', 'limited', 'to', 'the', 'homogeneous', 'c... | [-0.12132334207184613, 0.0357819392712554, -0.11572293576598168, 0.06784975422546267, -0.0661207475643605, -0.08581891248375177, -0.003256264217197895, 0.34053980322554706, -0.22842123541049658, -0.2576893211379647, 0.0809959817836061, -0.2299635986983776, -0.11805498088896274, 0.23296444322355092, 0.026085536243394016... |
710.1247 | Quasiparticle evolution and pseudogap formation in V2O3: An infrared
spectroscopy study | The infrared conductivity of V2O3 is measured in the whole phase diagram.
Quasiparticles appear above the Neel temperature TN and eventually disappear
further enhancing the temperature, leading to a pseudogap in the optical
spectrum above 425 K. Our calculations demonstrate that this loss of coherence
can be explaine... | cond-mat.str-el cond-mat.mtrl-sci | the infrared conductivity of v2o3 is measured in the whole phase diagram quasiparticles appear above the neel temperature tn and eventually disappear further enhancing the temperature leading to a pseudogap in the optical spectrum above 425 k our calculations demonstrate that this loss of coherence can be explained onl... | [['the', 'infrared', 'conductivity', 'of', 'v2o3', 'is', 'measured', 'in', 'the', 'whole', 'phase', 'diagram', 'quasiparticles', 'appear', 'above', 'the', 'neel', 'temperature', 'tn', 'and', 'eventually', 'disappear', 'further', 'enhancing', 'the', 'temperature', 'leading', 'to', 'a', 'pseudogap', 'in', 'the', 'optical... | [-0.1413440224066188, 0.27143081301186656, -0.085063538531761, 0.016475636039011747, -0.027141467464757683, -0.12393692333274815, 0.13189948996222473, 0.39262864528860475, -0.2857917894290972, -0.24901071134984162, 0.06556036542287638, -0.3367405389022978, -0.09467730117089386, 0.14288646847457637, 0.016927058949972255... |
710.1248 | Realization of abstract convex geometries by point configurations, Part
1 | The Edelman-Jamison problem is to characterize those abstract convex
geometries that are representable by a set of points in the plane. We show that
some natural modification of the Edelman-Jamison problem is equivalent to the
well known NP-hard order type problem.
| math.CO | the edelmanjamison problem is to characterize those abstract convex geometries that are representable by a set of points in the plane we show that some natural modification of the edelmanjamison problem is equivalent to the well known nphard order type problem | [['the', 'edelmanjamison', 'problem', 'is', 'to', 'characterize', 'those', 'abstract', 'convex', 'geometries', 'that', 'are', 'representable', 'by', 'a', 'set', 'of', 'points', 'in', 'the', 'plane', 'we', 'show', 'that', 'some', 'natural', 'modification', 'of', 'the', 'edelmanjamison', 'problem', 'is', 'equivalent', 't... | [-0.11079668927078064, 0.02184552811563779, -0.008078547719961558, 0.150371902437212, -0.12575402316183615, -0.08335259565128347, 0.00499340003499618, 0.3840593248605728, -0.3868229719690787, -0.2707857618657633, 0.13345106011435676, -0.28064191601095867, -0.2088805981553518, 0.19888544307114223, -0.13797799060837582, ... |
710.1249 | Dynamically correlated regions and configurational entropy in
supercooled liquids | When a liquid is cooled below its melting temperature, if crystallization is
avoided, it forms a glass. This phenomenon, called glass transition, is
characterized by a marked increase of viscosity, about 14 orders of magnitude,
in a narrow temperature interval. The microscopic mechanism behind the glass
transition is... | cond-mat.dis-nn cond-mat.soft cond-mat.stat-mech | when a liquid is cooled below its melting temperature if crystallization is avoided it forms a glass this phenomenon called glass transition is characterized by a marked increase of viscosity about 14 orders of magnitude in a narrow temperature interval the microscopic mechanism behind the glass transition is still poo... | [['when', 'a', 'liquid', 'is', 'cooled', 'below', 'its', 'melting', 'temperature', 'if', 'crystallization', 'is', 'avoided', 'it', 'forms', 'a', 'glass', 'this', 'phenomenon', 'called', 'glass', 'transition', 'is', 'characterized', 'by', 'a', 'marked', 'increase', 'of', 'viscosity', 'about', '14', 'orders', 'of', 'magn... | [-0.10090828945852306, 0.2056833038934403, -0.10867540803180736, 0.04249244247429853, -0.023486400759404797, -0.09093784594074544, 0.056160474334381774, 0.3377672802446943, -0.296347473644548, -0.27677134082366067, 0.11208418505883211, -0.2905794870840688, -0.14031973409836587, 0.14533485049201755, -0.02130832855562823... |
710.125 | Quantum-dot thermometry | We present a method for the measurement of a temperature differential across
a single quantum dot that has transmission resonances that are separated in
energy by much more than the thermal energy. We determine numerically that the
method is accurate to within a few percent across a wide range of parameters.
The prop... | cond-mat.mtrl-sci cond-mat.stat-mech | we present a method for the measurement of a temperature differential across a single quantum dot that has transmission resonances that are separated in energy by much more than the thermal energy we determine numerically that the method is accurate to within a few percent across a wide range of parameters the proposed... | [['we', 'present', 'a', 'method', 'for', 'the', 'measurement', 'of', 'a', 'temperature', 'differential', 'across', 'a', 'single', 'quantum', 'dot', 'that', 'has', 'transmission', 'resonances', 'that', 'are', 'separated', 'in', 'energy', 'by', 'much', 'more', 'than', 'the', 'thermal', 'energy', 'we', 'determine', 'numer... | [-0.08835982180520309, 0.157977595566267, -0.09154926595020008, 0.04445708229582398, 0.014833269696907106, -0.16986132971381387, 0.04586418807725366, 0.3898711183209376, -0.23570094147629767, -0.3258848924369338, 0.034726336965875994, -0.2849737355171377, -0.10149647171766195, 0.3041995795645628, -0.008998962649402309,... |
710.1251 | Biconical structures in two-dimensional anisotropic Heisenberg
antiferromagnets | Square lattice Heisenberg and XY antiferromagnets with uniaxial anisotropy in
a field along the easy axis are studied. Based on ground state considerations
and Monte Carlo simulations, the role of biconical structures in the transition
region between the antiferromagnetic and spin--flop phases is analyzed. In
particu... | cond-mat.stat-mech | square lattice heisenberg and xy antiferromagnets with uniaxial anisotropy in a field along the easy axis are studied based on ground state considerations and monte carlo simulations the role of biconical structures in the transition region between the antiferromagnetic and spinflop phases is analyzed in particular add... | [['square', 'lattice', 'heisenberg', 'and', 'xy', 'antiferromagnets', 'with', 'uniaxial', 'anisotropy', 'in', 'a', 'field', 'along', 'the', 'easy', 'axis', 'are', 'studied', 'based', 'on', 'ground', 'state', 'considerations', 'and', 'monte', 'carlo', 'simulations', 'the', 'role', 'of', 'biconical', 'structures', 'in', ... | [-0.24113366997335106, 0.231741922812148, -0.006989322191657266, 0.01921948212566349, -0.06388421951851342, -0.14159535517501354, 0.031511651424807496, 0.44252088759094477, -0.2656883366726106, -0.24717187424539588, 0.06362211336727341, -0.3182064960419666, -0.07675178619865619, 0.13039112883598136, 0.15471177063386676... |
710.1252 | Estimates on trapped modes in deformed quantum layers | We use a logarithmic Lieb-Thirring inequality for two-dimensional
Schroedinger operators and establish estimates on trapped modes in
geometrically deformed quantum layers.
| math-ph math.MP | we use a logarithmic liebthirring inequality for twodimensional schroedinger operators and establish estimates on trapped modes in geometrically deformed quantum layers | [['we', 'use', 'a', 'logarithmic', 'liebthirring', 'inequality', 'for', 'twodimensional', 'schroedinger', 'operators', 'and', 'establish', 'estimates', 'on', 'trapped', 'modes', 'in', 'geometrically', 'deformed', 'quantum', 'layers']] | [-0.10228017810732126, 0.14509330840692633, -0.020012178059135164, 0.12003896349952334, -0.010009295983417403, -0.25140419307475287, 0.02462240472197577, 0.3332721592769736, -0.24697489859092803, -0.16433928231708705, 0.0751724091436093, -0.3915013685112908, -0.11120687602531343, 0.22613058296874874, -0.063221466999190... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.