id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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706.1914 | Approche variationnelle pour le calcul bay\'esien dans les probl\`emes
inverses en imagerie | In a non supervised Bayesian estimation approach for inverse problems in
imaging systems, one tries to estimate jointly the unknown image pixels $\fb$
and the hyperparameters $\thetab$. This is, in general, done through the joint
posterior law $p(\fb,\thetab|\gb)$. The expression of this joint law is often
very compl... | physics.data-an physics.comp-ph | in a non supervised bayesian estimation approach for inverse problems in imaging systems one tries to estimate jointly the unknown image pixels fb and the hyperparameters thetab this is in general done through the joint posterior law pfbthetabgb the expression of this joint law is often very complex and its exploration... | [['in', 'a', 'non', 'supervised', 'bayesian', 'estimation', 'approach', 'for', 'inverse', 'problems', 'in', 'imaging', 'systems', 'one', 'tries', 'to', 'estimate', 'jointly', 'the', 'unknown', 'image', 'pixels', 'fb', 'and', 'the', 'hyperparameters', 'thetab', 'this', 'is', 'in', 'general', 'done', 'through', 'the', 'j... | [-0.05836969513424988, 0.04246244381715636, -0.10844084066583921, 0.08466569084554301, -0.07496507264325145, -0.15297751574557852, 0.0897640546127522, 0.4077932545751856, -0.2869821365634034, -0.32342176473214784, 0.10388848185743484, -0.2189237223121158, -0.15401750704449227, 0.173775960156852, -0.11441358497991956, 0... |
706.1915 | How to disentangle two braided Hopf algebras | We show how to define the tensor product of two braided Hopf algebras.
| math.QA | we show how to define the tensor product of two braided hopf algebras | [['we', 'show', 'how', 'to', 'define', 'the', 'tensor', 'product', 'of', 'two', 'braided', 'hopf', 'algebras']] | [-0.2103145460669811, 0.13509394292934582, -0.02040394080372957, 0.08605936628121597, -0.16950181527779654, -0.1299691481085924, -0.14157992515426415, 0.423042563864818, -0.5198641935220132, -0.12248075237640968, 0.1000514212064445, -0.15656326625209588, -0.2789524762103191, 0.08249184045080955, -0.12682929778328308, -... |
706.1916 | GRMHD/RMHD Simulations and Stability of Magnetized Spine-Sheath
Relativistic Jets | A new general relativistic magnetohydrodynamics (GRMHD) code ``RAISHIN'' used
to simulate jet generation by rotating and non-rotating black holes with a
geometrically thin Keplarian accretion disk finds that the jet develops a
spine-sheath structure in the rotating black hole case. Spine-sheath structure
and strong m... | astro-ph | a new general relativistic magnetohydrodynamics grmhd code raishin used to simulate jet generation by rotating and nonrotating black holes with a geometrically thin keplarian accretion disk finds that the jet develops a spinesheath structure in the rotating black hole case spinesheath structure and strong magnetic fiel... | [['a', 'new', 'general', 'relativistic', 'magnetohydrodynamics', 'grmhd', 'code', 'raishin', 'used', 'to', 'simulate', 'jet', 'generation', 'by', 'rotating', 'and', 'nonrotating', 'black', 'holes', 'with', 'a', 'geometrically', 'thin', 'keplarian', 'accretion', 'disk', 'finds', 'that', 'the', 'jet', 'develops', 'a', 's... | [-0.17937217621115048, 0.1678050468304442, -0.029800579535385854, 0.08135394248418816, -0.099756330083702, -0.11525552386500507, -0.07938672444942302, 0.3500690442315432, -0.23408005739963036, -0.2696668513508254, 0.043154137629773937, -0.21054607336232556, 0.013654784065128977, 0.25036724129856763, 0.03232464537944032... |
706.1917 | Propagation of travelling waves in sub-excitable systems driven by noise
and periodic forcing | It has been reported that traveling waves propagate periodically and stably
in sub-excitable systems driven by noise [Phys. Rev. Lett. \textbf{88}, 138301
(2002)]. As a further investigation, here we observe different types of
traveling waves under different noises and periodic forces, using a simplified
Oregonator m... | nlin.CD nlin.PS physics.flu-dyn physics.med-ph | it has been reported that traveling waves propagate periodically and stably in subexcitable systems driven by noise phys rev lett textbf88 138301 2002 as a further investigation here we observe different types of traveling waves under different noises and periodic forces using a simplified oregonator model depending on... | [['it', 'has', 'been', 'reported', 'that', 'traveling', 'waves', 'propagate', 'periodically', 'and', 'stably', 'in', 'subexcitable', 'systems', 'driven', 'by', 'noise', 'phys', 'rev', 'lett', 'textbf88', '138301', '2002', 'as', 'a', 'further', 'investigation', 'here', 'we', 'observe', 'different', 'types', 'of', 'trave... | [-0.1814226254724284, 0.19256370430097067, -0.06499090102478498, 0.02658626152608521, -0.05354538981990162, -0.10891982918980009, 0.02864188218500647, 0.3857904146581593, -0.264707668467209, -0.28659615345390105, 0.0755956405504016, -0.26779308287631265, -0.2163504569424975, 0.21975659838843545, -0.022090445434470182, ... |
706.1918 | Affine Buildings and Tropical Convexity | The notion of convexity in tropical geometry is closely related to notions of
convexity in the theory of affine buildings. We explore this relationship from
a combinatorial and computational perspective. Our results include a convex
hull algorithm for the Bruhat--Tits building of SL$_d(K)$ and techniques for
computin... | math.MG math.CO | the notion of convexity in tropical geometry is closely related to notions of convexity in the theory of affine buildings we explore this relationship from a combinatorial and computational perspective our results include a convex hull algorithm for the bruhattits building of sl_dk and techniques for computing with apa... | [['the', 'notion', 'of', 'convexity', 'in', 'tropical', 'geometry', 'is', 'closely', 'related', 'to', 'notions', 'of', 'convexity', 'in', 'the', 'theory', 'of', 'affine', 'buildings', 'we', 'explore', 'this', 'relationship', 'from', 'a', 'combinatorial', 'and', 'computational', 'perspective', 'our', 'results', 'include... | [-0.049429191138357094, 0.020610688820069785, -0.14591044004648507, 0.10518943691669508, -0.10265548620643744, -0.11665240192222734, 0.029087673828038278, 0.29255568363898715, -0.3596522333262878, -0.26265420928207595, 0.1387058750111718, -0.24491605260084534, -0.24675721939393255, 0.24528420621226, -0.2571099349405876... |
706.1919 | Simple dynamic exchange-correlation kernel of the uniform electron gas | We propose a simple dynamic exchange-correlation kernel of the uniform
electron gas. We model the reduction of the electron-electron interaction due
to short-range exchange-correlation effects by introducing a
frequency-dependent error-function effective interaction. By imposing the
fulfillment of the compresibility ... | cond-mat.mtrl-sci | we propose a simple dynamic exchangecorrelation kernel of the uniform electron gas we model the reduction of the electronelectron interaction due to shortrange exchangecorrelation effects by introducing a frequencydependent errorfunction effective interaction by imposing the fulfillment of the compresibility and the th... | [['we', 'propose', 'a', 'simple', 'dynamic', 'exchangecorrelation', 'kernel', 'of', 'the', 'uniform', 'electron', 'gas', 'we', 'model', 'the', 'reduction', 'of', 'the', 'electronelectron', 'interaction', 'due', 'to', 'shortrange', 'exchangecorrelation', 'effects', 'by', 'introducing', 'a', 'frequencydependent', 'errorf... | [-0.11984920931870785, 0.08188163282591879, -0.10026267482784151, 0.14689878586760183, -0.04458683586598915, -0.08591848265244569, 0.07296493797229579, 0.3431997398535411, -0.225046268629807, -0.2878984366313635, -0.002782849991625106, -0.2968050645733321, -0.13635176843331184, 0.09227087085112286, 0.06832763106550699,... |
706.192 | On a problem of Duke-Erdos-Rodl on cycle-connected subgraphs | In this short note, we prove that for \beta < 1/5 every graph G with n
vertices and n^{2-\beta} edges contains a subgraph G' with at least
cn^{2-2\beta} edges such that every pair of edges in G' lie together on a cycle
of length at most 8. Moreover edges in G' which share a vertex lie together on
a cycle of length at... | math.CO math.NT | in this short note we prove that for beta 15 every graph g with n vertices and n2beta edges contains a subgraph g with at least cn22beta edges such that every pair of edges in g lie together on a cycle of length at most 8 moreover edges in g which share a vertex lie together on a cycle of length at most 6 this result i... | [['in', 'this', 'short', 'note', 'we', 'prove', 'that', 'for', 'beta', '15', 'every', 'graph', 'g', 'with', 'n', 'vertices', 'and', 'n2beta', 'edges', 'contains', 'a', 'subgraph', 'g', 'with', 'at', 'least', 'cn22beta', 'edges', 'such', 'that', 'every', 'pair', 'of', 'edges', 'in', 'g', 'lie', 'together', 'on', 'a', 'c... | [-0.1898574874345443, 0.13966334666582514, -0.02562609884634982, -0.04391047185614567, -0.07732147336247619, -0.15722140550245473, 0.08928727740306913, 0.392714672020556, -0.24809158905294298, -0.3434770027934401, 0.06239056752356528, -0.3639719143573103, -0.12004903784700106, 0.11056203307744897, -0.08707595472281546,... |
706.1921 | Test of hadronic interaction models with data from the Pierre Auger
Observatory | The Pierre Auger Observatory allows the measurement of both longitudinal
profiles and lateral particle distributions of high-energy showers. The former
trace the overall shower development, mainly of the electromagnetic component
close to the core where the latter reflect the particle densities in the tail
of the sho... | astro-ph | the pierre auger observatory allows the measurement of both longitudinal profiles and lateral particle distributions of highenergy showers the former trace the overall shower development mainly of the electromagnetic component close to the core where the latter reflect the particle densities in the tail of the shower f... | [['the', 'pierre', 'auger', 'observatory', 'allows', 'the', 'measurement', 'of', 'both', 'longitudinal', 'profiles', 'and', 'lateral', 'particle', 'distributions', 'of', 'highenergy', 'showers', 'the', 'former', 'trace', 'the', 'overall', 'shower', 'development', 'mainly', 'of', 'the', 'electromagnetic', 'component', '... | [-0.0673786740326746, 0.23874881170605394, -0.06752236913995478, 0.11217095681931824, -0.027457529911771417, -0.02620564039203931, -0.08024475085549057, 0.37781813581558793, -0.21368670796298167, -0.3498949222097343, 0.05732318376910619, -0.35982333300860114, 0.007491370557214726, 0.16332726616793397, 0.103667342612011... |
706.1922 | Spontaneous Symmetry Breaking and Decoherence in Superconductors | We show that superconductors have a thin spectrum associated with spontaneous
symmetry breaking similar to that of antiferromagnets, while still being in
full agreement with Elitzur's theorem, which forbids the spontaneous breaking
of local (gauge) symmetries. This thin spectrum in the superconductors consists
of in-... | cond-mat.supr-con | we show that superconductors have a thin spectrum associated with spontaneous symmetry breaking similar to that of antiferromagnets while still being in full agreement with elitzurs theorem which forbids the spontaneous breaking of local gauge symmetries this thin spectrum in the superconductors consists of ingap state... | [['we', 'show', 'that', 'superconductors', 'have', 'a', 'thin', 'spectrum', 'associated', 'with', 'spontaneous', 'symmetry', 'breaking', 'similar', 'to', 'that', 'of', 'antiferromagnets', 'while', 'still', 'being', 'in', 'full', 'agreement', 'with', 'elitzurs', 'theorem', 'which', 'forbids', 'the', 'spontaneous', 'brea... | [-0.21574710341519676, 0.21143661213379042, -0.046691468929768436, 0.05646973401922474, -0.08539574370822972, -0.1154468042918274, 0.08151540262850984, 0.3448713666617146, -0.21047383162658662, -0.277384832145698, 0.05026278020199647, -0.2961975064115702, -0.10840512870992017, 0.1318337963392777, 0.018860263106439054, ... |
706.1923 | A Novel phase in the phase structure of the $(g\phi^4 + h\phi^6)_{1+1}$
field theoretic model | In view of the newly discovered and physically acceptable $PT$ symmetric and
non-Hermitian models, we reinvestigated the phase structure of the
($g\phi^{4}+h\phi^{6}$)$_{1+1}$ Hermitian model. The reinvestigation concerns
the possibility of a phase transition from the original Hermitian and $PT$
symmetric phase to a ... | hep-th | in view of the newly discovered and physically acceptable pt symmetric and nonhermitian models we reinvestigated the phase structure of the gphi4hphi6_11 hermitian model the reinvestigation concerns the possibility of a phase transition from the original hermitian and pt symmetric phase to a nonhermitian and pt symmetr... | [['in', 'view', 'of', 'the', 'newly', 'discovered', 'and', 'physically', 'acceptable', 'pt', 'symmetric', 'and', 'nonhermitian', 'models', 'we', 'reinvestigated', 'the', 'phase', 'structure', 'of', 'the', 'gphi4hphi6_11', 'hermitian', 'model', 'the', 'reinvestigation', 'concerns', 'the', 'possibility', 'of', 'a', 'phas... | [-0.11326714523157944, 0.16066017905108004, -0.08998305731380131, 0.049332624574134995, -0.05974007125602651, -0.1656246930227494, 0.05663806216245631, 0.343352084350239, -0.2343270356592701, -0.2952486731908249, 0.06270134375334667, -0.25575976676968787, -0.17567820549553317, 0.09416752912233875, -0.02305569951618019,... |
706.1924 | Long-Distance Entanglement Distribution with Single-Photon Sources | We present an efficient architecture for quantum repeaters based on
single-photon sources in combination with quantum memories for photons. Errors
inherent to previous repeater protocols using photon-pair sources are
eliminated, leading to a significant gain in efficiency. We establish the
requirements on the single-... | quant-ph | we present an efficient architecture for quantum repeaters based on singlephoton sources in combination with quantum memories for photons errors inherent to previous repeater protocols using photonpair sources are eliminated leading to a significant gain in efficiency we establish the requirements on the singlephoton s... | [['we', 'present', 'an', 'efficient', 'architecture', 'for', 'quantum', 'repeaters', 'based', 'on', 'singlephoton', 'sources', 'in', 'combination', 'with', 'quantum', 'memories', 'for', 'photons', 'errors', 'inherent', 'to', 'previous', 'repeater', 'protocols', 'using', 'photonpair', 'sources', 'are', 'eliminated', 'le... | [-0.15933821235899814, 0.1313983099468169, -0.04026012916117907, 0.04086225874722004, 0.017736554555594922, -0.1936665468569845, 0.1484213877702132, 0.5184943603351713, -0.15751036124303938, -0.3103664684668183, 0.026937741017900408, -0.3259733194485307, -0.015706747025251388, 0.3258270360529423, -0.1128999854810536, 0... |
706.1925 | Hamiltonian Theory of Adiabatic Motion of Relativistic Charged Particles | A general Hamiltonian theory for the adiabatic motion of relativistic charged
particles confined by slowly-varying background electromagnetic fields is
presented based on a unified Lie-transform perturbation analysis in extended
phase space (which includes energy and time as independent coordinates) for all
three adi... | physics.plasm-ph physics.space-ph | a general hamiltonian theory for the adiabatic motion of relativistic charged particles confined by slowlyvarying background electromagnetic fields is presented based on a unified lietransform perturbation analysis in extended phase space which includes energy and time as independent coordinates for all three adiabatic... | [['a', 'general', 'hamiltonian', 'theory', 'for', 'the', 'adiabatic', 'motion', 'of', 'relativistic', 'charged', 'particles', 'confined', 'by', 'slowlyvarying', 'background', 'electromagnetic', 'fields', 'is', 'presented', 'based', 'on', 'a', 'unified', 'lietransform', 'perturbation', 'analysis', 'in', 'extended', 'pha... | [-0.1379375366875362, 0.20085638980516166, -0.09421100576435203, 0.0640101050831499, -0.05886430746835211, -0.102365439138932, -0.06485492705816295, 0.2843292538697521, -0.23707109056008252, -0.2934573496273462, 0.045439165412023176, -0.23355185868137557, -0.07002163597423097, 0.18566775022233176, -0.00954777024605352,... |
706.1926 | Towards understanding and modelling office daily life | Measuring and modeling human behavior is a very complex task. In this paper
we present our initial thoughts on modeling and automatic recognition of some
human activities in an office. We argue that to successfully model human
activities, we need to consider both individual behavior and group dynamics. To
demonstrate... | cs.CV cs.CY | measuring and modeling human behavior is a very complex task in this paper we present our initial thoughts on modeling and automatic recognition of some human activities in an office we argue that to successfully model human activities we need to consider both individual behavior and group dynamics to demonstrate these... | [['measuring', 'and', 'modeling', 'human', 'behavior', 'is', 'a', 'very', 'complex', 'task', 'in', 'this', 'paper', 'we', 'present', 'our', 'initial', 'thoughts', 'on', 'modeling', 'and', 'automatic', 'recognition', 'of', 'some', 'human', 'activities', 'in', 'an', 'office', 'we', 'argue', 'that', 'to', 'successfully', ... | [-0.0877154959580646, 0.045598272424495705, -0.11124131887291487, 0.051276560643544564, -0.10230963333294942, -0.1031046426998308, 0.0313697369536385, 0.47159349551567664, -0.19556063637137414, -0.35307822812062045, 0.08077655623917683, -0.28550966665721855, -0.2676899424395882, 0.21645938727216651, -0.1774182913538355... |
706.1927 | The Heegaard structure of Dehn filled manifolds | We expect manifolds obtained by Dehn filling to inherit properties from the
knot manifold. To what extent does that hold true for the Heegaard structure?
We study four changes to the Heegaard structure that may occur after filling:
(1) Heegaard genus decreases, (2) a new Heegaard surface is created, (3) a
non-stabili... | math.GT | we expect manifolds obtained by dehn filling to inherit properties from the knot manifold to what extent does that hold true for the heegaard structure we study four changes to the heegaard structure that may occur after filling 1 heegaard genus decreases 2 a new heegaard surface is created 3 a nonstabilized heegaard s... | [['we', 'expect', 'manifolds', 'obtained', 'by', 'dehn', 'filling', 'to', 'inherit', 'properties', 'from', 'the', 'knot', 'manifold', 'to', 'what', 'extent', 'does', 'that', 'hold', 'true', 'for', 'the', 'heegaard', 'structure', 'we', 'study', 'four', 'changes', 'to', 'the', 'heegaard', 'structure', 'that', 'may', 'occ... | [-0.2123844501011185, 0.15014377411088756, -0.105088128358062, 0.17286413710596216, -0.10231253263763447, -0.2505459073994659, 0.019862828254858907, 0.36574845565244174, -0.2352621083269214, -0.3536487255866329, 0.10402574585491998, -0.22702568650452626, -0.16088192328675371, 0.2013661098292368, -0.13262713678642854, -... |
706.1928 | Generalized Continuous-Time Random Walks (CTRW), Subordination by
Hitting Times and Fractional Dynamics | Functional limit theorem for continuous-time random walks (CTRW) are found in
general case of dependent waiting times and jump sizes that are also position
dependent. The limiting anomalous diffusion is described in terms of fractional
dynamics. Probabilistic interpretation of generalized fractional evolution is
give... | math.PR math.AP | functional limit theorem for continuoustime random walks ctrw are found in general case of dependent waiting times and jump sizes that are also position dependent the limiting anomalous diffusion is described in terms of fractional dynamics probabilistic interpretation of generalized fractional evolution is given in te... | [['functional', 'limit', 'theorem', 'for', 'continuoustime', 'random', 'walks', 'ctrw', 'are', 'found', 'in', 'general', 'case', 'of', 'dependent', 'waiting', 'times', 'and', 'jump', 'sizes', 'that', 'are', 'also', 'position', 'dependent', 'the', 'limiting', 'anomalous', 'diffusion', 'is', 'described', 'in', 'terms', '... | [-0.09987234155464805, 0.22515958062662134, -0.08082531273750396, 0.10244928303592164, -0.027460451237857342, -0.1032500359197629, 0.03324329140114373, 0.36607805986342756, -0.28272911838801773, -0.2429076656056889, 0.10761678599599941, -0.23801811837494888, -0.14269663419189124, 0.18321758343292208, -0.081653904820117... |
706.1929 | Study on Hilbert's Eighth Problems | In this paper, we used the principle of sieve function transformation to improve sieve method and the prime number theorem in the arithmetic sequence.For this, we proved General Riemann Hypothesis and Riemann Hypothesis to be true. further, we improved Selberg's line sieve method and proved Goldbach Conjecture and Twin... | math.GM | in this paper we used the principle of sieve function transformation to improve sieve method and the prime number theorem in the arithmetic sequencefor this we proved general riemann hypothesis and riemann hypothesis to be true further we improved selbergs line sieve method and proved goldbach conjecture and twin prime... | [['in', 'this', 'paper', 'we', 'used', 'the', 'principle', 'of', 'sieve', 'function', 'transformation', 'to', 'improve', 'sieve', 'method', 'and', 'the', 'prime', 'number', 'theorem', 'in', 'the', 'arithmetic', 'sequencefor', 'this', 'we', 'proved', 'general', 'riemann', 'hypothesis', 'and', 'riemann', 'hypothesis', 't... | [-0.13131789329927415, 0.004711282400724788, -0.18868535918494064, 0.18040341447340325, -0.10164407584816218, -0.1752179560251534, 0.06292793837880405, 0.2601157861451308, -0.3291483666126927, -0.3360522391895453, 0.0875669071256804, -0.17425116220644365, -0.16082500359225377, 0.26540012741461394, -0.1564224504244824, ... |
706.193 | LARES/WEBER-SAT and the equivalence principle | It has often been claimed that the proposed Earth artificial satellite
LARES/WEBER-SAT-whose primary goal is, in fact, the measurement of the general
relativistic Lense-Thirring effect at a some percent level-would allow to
greatly improve, among (many) other things, the present-day (10^-13) level of
accuracy in test... | gr-qc astro-ph hep-ph physics.space-ph | it has often been claimed that the proposed earth artificial satellite lareswebersatwhose primary goal is in fact the measurement of the general relativistic lensethirring effect at a some percent levelwould allow to greatly improve among many other things the presentday 1013 level of accuracy in testing the equivalenc... | [['it', 'has', 'often', 'been', 'claimed', 'that', 'the', 'proposed', 'earth', 'artificial', 'satellite', 'lareswebersatwhose', 'primary', 'goal', 'is', 'in', 'fact', 'the', 'measurement', 'of', 'the', 'general', 'relativistic', 'lensethirring', 'effect', 'at', 'a', 'some', 'percent', 'levelwould', 'allow', 'to', 'grea... | [-0.11909806535819943, 0.10868143740246135, -0.01567718663430783, 0.07957424857167088, -0.03962285465069031, -0.03344372267510449, 0.04296821084794369, 0.33238985327208476, -0.22054044762103076, -0.41041172258137315, 0.09736277880617993, -0.28919201928159494, -0.12151738498987777, 0.24614970233772746, -0.09197736356016... |
706.1931 | Systematic corrections to the measured cosmological constant as a result
of local inhomogeneity | We calculate the systematic inhomogeneity-induced correction to the
cosmological constant that one would infer from an analysis of the luminosities
and redshifts of Type Ia supernovae, assuming a homogeneous universe. The
calculation entails a post-Newtonian expansion within the framework of second
order perturbation... | astro-ph gr-qc | we calculate the systematic inhomogeneityinduced correction to the cosmological constant that one would infer from an analysis of the luminosities and redshifts of type ia supernovae assuming a homogeneous universe the calculation entails a postnewtonian expansion within the framework of second order perturbation theor... | [['we', 'calculate', 'the', 'systematic', 'inhomogeneityinduced', 'correction', 'to', 'the', 'cosmological', 'constant', 'that', 'one', 'would', 'infer', 'from', 'an', 'analysis', 'of', 'the', 'luminosities', 'and', 'redshifts', 'of', 'type', 'ia', 'supernovae', 'assuming', 'a', 'homogeneous', 'universe', 'the', 'calcu... | [-0.07418153515602109, 0.10845246997443243, -0.10913336773582992, 0.10728180164763775, -0.12037405034355006, -0.06916824627389834, 0.03492570187242999, 0.35167865882854626, -0.209322953477361, -0.3286861608351753, 0.05472757398863049, -0.2906880051992294, -0.02777447841548901, 0.18851953410512196, -0.00855428433764047,... |
706.1932 | Probabilistic purification of noisy coherent states | A basic feasible probabilistic purification of unknown noisy coherent states,
outgoing from different state preparations with unknown mean number of thermal
photons, is proposed. The scheme is based only on a linear-optical network with
an avalanche photo-diode or heterodyne (homodyne) detection used to post-select
a... | quant-ph | a basic feasible probabilistic purification of unknown noisy coherent states outgoing from different state preparations with unknown mean number of thermal photons is proposed the scheme is based only on a linearoptical network with an avalanche photodiode or heterodyne homodyne detection used to postselect a successfu... | [['a', 'basic', 'feasible', 'probabilistic', 'purification', 'of', 'unknown', 'noisy', 'coherent', 'states', 'outgoing', 'from', 'different', 'state', 'preparations', 'with', 'unknown', 'mean', 'number', 'of', 'thermal', 'photons', 'is', 'proposed', 'the', 'scheme', 'is', 'based', 'only', 'on', 'a', 'linearoptical', 'n... | [-0.09222014623281377, 0.16610712433843713, -0.09925974819766865, 0.021419527890181846, -0.013124642449177125, -0.2663690443997356, 0.08660439853238958, 0.35562081952494656, -0.25556071286237886, -0.2897776270348748, 0.06925493247664152, -0.21280811485749754, -0.08836251542776484, 0.2390001954230353, -0.124211143734018... |
706.1933 | Nonlocal explanation of stationary and nonstationary regimes in cascaded
soliton pulse compression | We study soliton pulse compression in materials with cascaded quadratic
nonlinearities, and show that the group-velocity mismatch creates two different
temporally nonlocal regimes. They correspond to what is known as the stationary
and nonstationary regimes. The theory accurately predicts the transition to the
statio... | physics.optics | we study soliton pulse compression in materials with cascaded quadratic nonlinearities and show that the groupvelocity mismatch creates two different temporally nonlocal regimes they correspond to what is known as the stationary and nonstationary regimes the theory accurately predicts the transition to the stationary r... | [['we', 'study', 'soliton', 'pulse', 'compression', 'in', 'materials', 'with', 'cascaded', 'quadratic', 'nonlinearities', 'and', 'show', 'that', 'the', 'groupvelocity', 'mismatch', 'creates', 'two', 'different', 'temporally', 'nonlocal', 'regimes', 'they', 'correspond', 'to', 'what', 'is', 'known', 'as', 'the', 'statio... | [-0.13586832993762352, 0.19142667864574692, -0.06468108357288517, 0.09747473411530685, -0.05072627702835374, -0.21892041426438552, -0.01992636105233732, 0.43526292481244755, -0.30972904024215847, -0.21860499121248722, 0.06637209064389865, -0.24766492343042046, -0.20100974613943925, 0.1908019263870441, -0.02729810249337... |
706.1934 | Low Mass Dimuons Produced in Relativistic Nuclear Collisions | The NA60 experiment has measured low-mass muon pair production in In-In
collisions at 158 A GeV with unprecedented precision. We show that this data is
reproduced very well by a dynamical model with parameters scaled from fits to
measurements of hadronic transverse mass spectra and Hanbury-Brown and Twiss
correlation... | hep-ph | the na60 experiment has measured lowmass muon pair production in inin collisions at 158 a gev with unprecedented precision we show that this data is reproduced very well by a dynamical model with parameters scaled from fits to measurements of hadronic transverse mass spectra and hanburybrown and twiss correlations in p... | [['the', 'na60', 'experiment', 'has', 'measured', 'lowmass', 'muon', 'pair', 'production', 'in', 'inin', 'collisions', 'at', '158', 'a', 'gev', 'with', 'unprecedented', 'precision', 'we', 'show', 'that', 'this', 'data', 'is', 'reproduced', 'very', 'well', 'by', 'a', 'dynamical', 'model', 'with', 'parameters', 'scaled',... | [-0.049317685851234604, 0.26226480830241183, -0.16396863643418658, 0.12702316268643535, 0.036418093006465244, -0.08742693458281627, -0.03933935912368311, 0.3547610642557794, -0.160301927248524, -0.3525048928441141, -0.05919375662183897, -0.36019195057028397, 0.11184543110006913, 0.15507203234698286, 0.06173301492394371... |
706.1935 | Toward Forecasting Volcanic Eruptions using Seismic Noise | During inter-eruption periods, magma pressurization yields subtle changes of
the elastic properties of volcanic edifices. We use the reproducibility
properties of the ambient seismic noise recorded on the Piton de la Fournaise
volcano to measure relative seismic velocity variations of less than 0.1 % with
a temporal ... | physics.geo-ph | during intereruption periods magma pressurization yields subtle changes of the elastic properties of volcanic edifices we use the reproducibility properties of the ambient seismic noise recorded on the piton de la fournaise volcano to measure relative seismic velocity variations of less than 01 with a temporal resoluti... | [['during', 'intereruption', 'periods', 'magma', 'pressurization', 'yields', 'subtle', 'changes', 'of', 'the', 'elastic', 'properties', 'of', 'volcanic', 'edifices', 'we', 'use', 'the', 'reproducibility', 'properties', 'of', 'the', 'ambient', 'seismic', 'noise', 'recorded', 'on', 'the', 'piton', 'de', 'la', 'fournaise'... | [-0.09912153411879325, 0.2321703118783341, -0.06744747669638498, 0.08695495768409708, -0.050104592947046396, 0.006502552995579722, 0.011602258848775502, 0.34749982759619696, -0.24933232206841122, -0.3282270356202903, 0.15740194181284017, -0.2754502695312587, -0.14648064195036725, 0.2421610743192065, -0.1218268953532021... |
706.1936 | The characterization of the Carleson measures for analytic Besov spaces:
a simple proof | We give a simple proof of the characterization of the Carleson measures for
the weighted analytic Besov spaces. Such characterization provides some
information on the radial variation of an analytic Besov function.
| math.CV | we give a simple proof of the characterization of the carleson measures for the weighted analytic besov spaces such characterization provides some information on the radial variation of an analytic besov function | [['we', 'give', 'a', 'simple', 'proof', 'of', 'the', 'characterization', 'of', 'the', 'carleson', 'measures', 'for', 'the', 'weighted', 'analytic', 'besov', 'spaces', 'such', 'characterization', 'provides', 'some', 'information', 'on', 'the', 'radial', 'variation', 'of', 'an', 'analytic', 'besov', 'function']] | [-0.14194238831987604, 0.00784765697289913, -0.14981143787736073, 0.20032539498060942, -0.12846843601437286, 0.006989389439695515, 0.007138122484320775, 0.34948383923619986, -0.28098726412281394, -0.1561106294975616, 0.12893476161116268, -0.23573000502074137, -0.11440990393748507, 0.3224477751646191, -0.162151895943679... |
706.1937 | Secondary invariants for Frechet algebras, quasihomomorphisms, and the
residue Chern character | This paper has been replaced by arXiv:0804.1042 and arXiv:0804.1048
| math.KT math-ph math.MP | this paper has been replaced by arxiv08041042 and arxiv08041048 | [['this', 'paper', 'has', 'been', 'replaced', 'by', 'arxiv08041042', 'and', 'arxiv08041048']] | [-0.012681672615664346, 0.13217275416744606, -0.11085785685905389, -0.13780519747108752, -0.02617491302745683, -0.11203001200088433, -0.05543049579552774, 0.4127047721828733, -0.17328119384390966, -0.3069134759051459, 0.22665754918541228, -0.2513264183487211, -0.21133850222187384, 0.136775798031262, -0.1947385706007480... |
706.1938 | Comments on the Quantum Afterburner | A process has been proposed to increase the efficiency of an ideal Otto cycle
via a quantum heat engine that has no cooler reservoir. We show that such a
process is not feasible.
| quant-ph | a process has been proposed to increase the efficiency of an ideal otto cycle via a quantum heat engine that has no cooler reservoir we show that such a process is not feasible | [['a', 'process', 'has', 'been', 'proposed', 'to', 'increase', 'the', 'efficiency', 'of', 'an', 'ideal', 'otto', 'cycle', 'via', 'a', 'quantum', 'heat', 'engine', 'that', 'has', 'no', 'cooler', 'reservoir', 'we', 'show', 'that', 'such', 'a', 'process', 'is', 'not', 'feasible']] | [-0.10857719211190035, 0.10269961888931875, -0.10270279171791943, -0.011720937048239372, -0.08823119882832874, -0.1072380768671406, 0.10013853822778346, 0.4199331547274734, -0.23359790354064017, -0.2257543205086029, 0.1303968199698085, -0.2910843334640517, -0.11495673419399695, 0.31463269161229784, -0.08624588174632553... |
706.1939 | 3-He in the Milky Way Interstellar Medium: Ionization Structure | The cosmic abundance of the 3-He isotope has important implications for many
fields of astrophysics. We are using the 8.665 GHz hyperfine transition of
3-He+ to determine the 3-He/H abundance in Milky Way HII regions and planetary
nebulae. This is one in a series of papers in which we discuss issues involved
in deriv... | astro-ph | the cosmic abundance of the 3he isotope has important implications for many fields of astrophysics we are using the 8665 ghz hyperfine transition of 3he to determine the 3heh abundance in milky way hii regions and planetary nebulae this is one in a series of papers in which we discuss issues involved in deriving accura... | [['the', 'cosmic', 'abundance', 'of', 'the', '3he', 'isotope', 'has', 'important', 'implications', 'for', 'many', 'fields', 'of', 'astrophysics', 'we', 'are', 'using', 'the', '8665', 'ghz', 'hyperfine', 'transition', 'of', '3he', 'to', 'determine', 'the', '3heh', 'abundance', 'in', 'milky', 'way', 'hii', 'regions', 'an... | [-0.023446848799999392, 0.08190618096002361, -0.06566338854549864, 0.10571432081337276, -0.0561436109833806, -0.09202350794448186, 0.05129813525225904, 0.40960731758278307, -0.2003490573167209, -0.3463948016544267, 0.025828675051728832, -0.27774120967487914, -0.03513593532113453, 0.20065050228041106, -0.030332523056747... |
706.194 | Efficient method for detection of periodic orbits in chaotic maps and
flows | An algorithm for detecting unstable periodic orbits in chaotic systems [Phys.
Rev. E, 60 (1999), pp. 6172-6175] which combines the set of stabilising
transformations proposed by Schmelcher and Diakonos [Phys. Rev. Lett., 78
(1997), pp. 4733-4736] with a modified semi-implicit Euler iterative scheme and
seeding with p... | nlin.CD | an algorithm for detecting unstable periodic orbits in chaotic systems phys rev e 60 1999 pp 61726175 which combines the set of stabilising transformations proposed by schmelcher and diakonos phys rev lett 78 1997 pp 47334736 with a modified semiimplicit euler iterative scheme and seeding with periodic orbits of neighb... | [['an', 'algorithm', 'for', 'detecting', 'unstable', 'periodic', 'orbits', 'in', 'chaotic', 'systems', 'phys', 'rev', 'e', '60', '1999', 'pp', '61726175', 'which', 'combines', 'the', 'set', 'of', 'stabilising', 'transformations', 'proposed', 'by', 'schmelcher', 'and', 'diakonos', 'phys', 'rev', 'lett', '78', '1997', 'p... | [-0.1609613576028548, 0.08083784920574809, -0.05693580616817045, -0.027324783892823414, -0.031454894063453184, -0.1257174842257323, 0.030180305051331163, 0.29727845346846477, -0.2231759462120563, -0.31552401822133186, 0.057387516555485615, -0.23820604243417864, -0.1944242747085606, 0.24283555201020654, -0.1005161425265... |
706.1941 | Twistor Actions for Self-Dual Supergravities | We give holomorphic Chern-Simons-like action functionals on supertwistor
space for self-dual supergravity theories in four dimensions, dealing with
N=0,...,8 supersymmetries, the cases where different parts of the R-symmetry
are gauged, and with or without a cosmological constant. The gauge group is
formally the grou... | hep-th gr-qc math-ph math.DG math.MP | we give holomorphic chernsimonslike action functionals on supertwistor space for selfdual supergravity theories in four dimensions dealing with n08 supersymmetries the cases where different parts of the rsymmetry are gauged and with or without a cosmological constant the gauge group is formally the group of holomorphic... | [['we', 'give', 'holomorphic', 'chernsimonslike', 'action', 'functionals', 'on', 'supertwistor', 'space', 'for', 'selfdual', 'supergravity', 'theories', 'in', 'four', 'dimensions', 'dealing', 'with', 'n08', 'supersymmetries', 'the', 'cases', 'where', 'different', 'parts', 'of', 'the', 'rsymmetry', 'are', 'gauged', 'and... | [-0.1720848004718166, 0.12279192475004468, -0.03824230759413144, 0.048457813975742996, -0.11419430678419837, -0.11160068977795062, -0.022587337548237874, 0.3155822646206057, -0.1843253854072627, -0.24835644134345952, 0.09546886385875591, -0.24411687509524166, -0.16570762380180076, 0.11253551836125553, -0.09370461184800... |
706.1942 | On Jordan Derivations of Triangular Algebras | In this short note we prove that every Jordan derivation of triangular
algebras is a derivation.
| math.RA | in this short note we prove that every jordan derivation of triangular algebras is a derivation | [['in', 'this', 'short', 'note', 'we', 'prove', 'that', 'every', 'jordan', 'derivation', 'of', 'triangular', 'algebras', 'is', 'a', 'derivation']] | [-0.24092502484563738, 0.0437816396006383, -0.14446098083863035, 0.02151324925944209, -0.11273200449068099, -0.15398317456129007, -0.08763109050050844, 0.3567997806239873, -0.30920561170205474, -0.05809474771376699, 0.08720325899048476, -0.2475595639552921, -0.2394795542350039, 0.16959110263269395, -0.1799623957485892,... |
706.1943 | The wreath product of Z with Z has Hilbert compression exponent 2/3 | Let G be a finitely generated group, equipped with the word metric d
associated with some finite set of generators. The Hilbert compression exponent
of G is the supremum over all $\alpha\ge 0$ such that there exists a Lipschitz
mapping $f:G\to L_2$ and a constant $c>0$ such that for all $x,y\in G$ we have
$\|f(x)-f(y... | math.MG math.FA math.GR | let g be a finitely generated group equipped with the word metric d associated with some finite set of generators the hilbert compression exponent of g is the supremum over all alphage 0 such that there exists a lipschitz mapping fgto l_2 and a constant c0 such that for all xyin g we have fxfy_2ge cdxyalpha in citeags0... | [['let', 'g', 'be', 'a', 'finitely', 'generated', 'group', 'equipped', 'with', 'the', 'word', 'metric', 'd', 'associated', 'with', 'some', 'finite', 'set', 'of', 'generators', 'the', 'hilbert', 'compression', 'exponent', 'of', 'g', 'is', 'the', 'supremum', 'over', 'all', 'alphage', '0', 'such', 'that', 'there', 'exists... | [-0.176510163311951, 0.15331643353617275, -0.08545177825073773, -0.0014406774915476268, -0.06074903981061652, -0.16412025434617825, 0.005635151021600326, 0.4051018709090547, -0.3116163497357673, -0.15922613534205984, 0.10857855454391896, -0.32790195844440817, -0.11348941258511672, 0.21694494030986713, -0.07779647986552... |
706.1944 | On the nature of optical nuclei in FR I radio-galaxies from ACS/HST
imaging polarimetry | We obtained optical imaging polarimetry with the ACS/HRC aboard the HST of
the 9 closest radio-galaxies in the 3C catalogue with an FR I morphology. The
nuclear sources seen in direct HST images in these galaxies are found to be
highly polarized with levels in the range ~2-11 % with a median value of 7 %.
We discuss ... | astro-ph | we obtained optical imaging polarimetry with the acshrc aboard the hst of the 9 closest radiogalaxies in the 3c catalogue with an fr i morphology the nuclear sources seen in direct hst images in these galaxies are found to be highly polarized with levels in the range 211 with a median value of 7 we discuss the differen... | [['we', 'obtained', 'optical', 'imaging', 'polarimetry', 'with', 'the', 'acshrc', 'aboard', 'the', 'hst', 'of', 'the', '9', 'closest', 'radiogalaxies', 'in', 'the', '3c', 'catalogue', 'with', 'an', 'fr', 'i', 'morphology', 'the', 'nuclear', 'sources', 'seen', 'in', 'direct', 'hst', 'images', 'in', 'these', 'galaxies', ... | [-0.07492830726295167, 0.11040879605455123, -0.04869929333504827, 0.09978919969793705, -0.11435475115757825, -0.0989795318041406, -0.009552983283630289, 0.473725644232526, -0.2053786350753174, -0.31614800323985487, 0.037963147384745835, -0.25223278336686755, -0.04041918534707574, 0.1804397613770683, -0.0430541954073415... |
706.1945 | Non-circular motion evidences in the circumnuclear region of M100 (NGC
4321) | We analyse new integral field spectroscopy of the inner region (central 2.5
kpc) of the spiral galaxy NGC 4321 to study the peculiar kinematics of this
region. Fourier analysis of the velocity residuals obtained by subtracting an
axisymmetric rotation model from the $\rm H\alpha$ velocity field, indicates
that the di... | astro-ph | we analyse new integral field spectroscopy of the inner region central 25 kpc of the spiral galaxy ngc 4321 to study the peculiar kinematics of this region fourier analysis of the velocity residuals obtained by subtracting an axisymmetric rotation model from the rm halpha velocity field indicates that the distortions a... | [['we', 'analyse', 'new', 'integral', 'field', 'spectroscopy', 'of', 'the', 'inner', 'region', 'central', '25', 'kpc', 'of', 'the', 'spiral', 'galaxy', 'ngc', '4321', 'to', 'study', 'the', 'peculiar', 'kinematics', 'of', 'this', 'region', 'fourier', 'analysis', 'of', 'the', 'velocity', 'residuals', 'obtained', 'by', 's... | [-0.08206488772719406, 0.05094111434449256, -0.10447315195712938, 0.07183482904590412, -0.07129916159266775, -0.04777310947644186, -0.00416783551934879, 0.3812743896639652, -0.2559501573506912, -0.29624969701928255, 0.07121073984837328, -0.22696715149967614, -0.04365360273302279, 0.18727948784627105, -0.031343414344023... |
706.1946 | Origin of matter in the universe | We extend the standard model with two iso-singlet color triplet scalars, one
singlet real scalar and one singlet fermion. The new fields are odd under an
unbroken Z_2 discrete symmetry while the standard model particles are even. The
decays of the singlet real scalar into three standard model quarks (antiquarks)
with... | hep-ph | we extend the standard model with two isosinglet color triplet scalars one singlet real scalar and one singlet fermion the new fields are odd under an unbroken z_2 discrete symmetry while the standard model particles are even the decays of the singlet real scalar into three standard model quarks antiquarks with three s... | [['we', 'extend', 'the', 'standard', 'model', 'with', 'two', 'isosinglet', 'color', 'triplet', 'scalars', 'one', 'singlet', 'real', 'scalar', 'and', 'one', 'singlet', 'fermion', 'the', 'new', 'fields', 'are', 'odd', 'under', 'an', 'unbroken', 'z_2', 'discrete', 'symmetry', 'while', 'the', 'standard', 'model', 'particle... | [-0.09573745107605257, 0.3684622788747803, -0.0351353038692463, 0.1734532273395826, -0.07877785714257879, -0.20827539728862013, -0.009483297016891075, 0.30103035569759723, -0.1866349831564736, -0.31803863664079485, 0.004412318030656635, -0.30742530278747776, 0.004806878228266617, 0.09163957602301798, 0.1405576145745643... |
706.1947 | Macroscopic effects in attosecond pulse generation | We examine how the generation and propagation of high-order harmonics in a
partly ionized gas medium affect their strength and synchronization. The
temporal properties of the resulting attosecond pulses generated in long gas
targets can be significantly influenced by macroscopic effects, in particular
by the intensit... | physics.optics physics.atom-ph | we examine how the generation and propagation of highorder harmonics in a partly ionized gas medium affect their strength and synchronization the temporal properties of the resulting attosecond pulses generated in long gas targets can be significantly influenced by macroscopic effects in particular by the intensity in ... | [['we', 'examine', 'how', 'the', 'generation', 'and', 'propagation', 'of', 'highorder', 'harmonics', 'in', 'a', 'partly', 'ionized', 'gas', 'medium', 'affect', 'their', 'strength', 'and', 'synchronization', 'the', 'temporal', 'properties', 'of', 'the', 'resulting', 'attosecond', 'pulses', 'generated', 'in', 'long', 'ga... | [-0.10057942110134728, 0.2181053390579947, -0.04883264559791999, 0.07022408872523628, 0.01916466548965637, -0.03694819378028257, 0.004134777488626456, 0.4680886183227046, -0.27712208999509225, -0.28237940980058707, 0.03418084446424514, -0.22736785979418273, -0.0894523327385358, 0.19694211413518767, 0.002539928649353345... |
706.1948 | Electronic spin transport and spin precession in single graphene layers
at room temperature | The specific band structure of graphene, with its unique valley structure and
Dirac neutrality point separating hole states from electron states has led to
the observation of new electronic transport phenomena such as anomalously
quantized Hall effects, absence of weak localization and the existence of a
minimum cond... | cond-mat.mes-hall | the specific band structure of graphene with its unique valley structure and dirac neutrality point separating hole states from electron states has led to the observation of new electronic transport phenomena such as anomalously quantized hall effects absence of weak localization and the existence of a minimum conducti... | [['the', 'specific', 'band', 'structure', 'of', 'graphene', 'with', 'its', 'unique', 'valley', 'structure', 'and', 'dirac', 'neutrality', 'point', 'separating', 'hole', 'states', 'from', 'electron', 'states', 'has', 'led', 'to', 'the', 'observation', 'of', 'new', 'electronic', 'transport', 'phenomena', 'such', 'as', 'a... | [-0.16533729702624603, 0.19165968251250246, -0.016403251018132056, -0.009637442775462713, -0.0430440426862333, -0.19272934609120163, 0.05507198582670432, 0.398682635745739, -0.2735411693173613, -0.31067589574034654, 0.025835098639029584, -0.32095104122452217, -0.0985206671158427, 0.19383904768962085, 0.0593093545552726... |
706.1949 | Ising spin glass models versus Ising models: an effective mapping at
high temperature III. Rigorous formulation and detailed proof for general
graphs | Recently, it has been shown that, when the dimension of a graph turns out to
be infinite dimensional in a broad sense, the upper critical surface and the
corresponding critical behavior of an arbitrary Ising spin glass model defined
over such a graph, can be exactly mapped on the critical surface and behavior
of a no... | cond-mat.dis-nn cond-mat.stat-mech | recently it has been shown that when the dimension of a graph turns out to be infinite dimensional in a broad sense the upper critical surface and the corresponding critical behavior of an arbitrary ising spin glass model defined over such a graph can be exactly mapped on the critical surface and behavior of a non rand... | [['recently', 'it', 'has', 'been', 'shown', 'that', 'when', 'the', 'dimension', 'of', 'a', 'graph', 'turns', 'out', 'to', 'be', 'infinite', 'dimensional', 'in', 'a', 'broad', 'sense', 'the', 'upper', 'critical', 'surface', 'and', 'the', 'corresponding', 'critical', 'behavior', 'of', 'an', 'arbitrary', 'ising', 'spin', ... | [-0.09287133016855026, 0.12269405714157569, -0.10554208129110654, 0.07334314509395684, -0.0926312645842806, -0.16986413770055736, 0.05080178138535818, 0.3410829118567339, -0.2585192918709387, -0.2635956008384843, 0.1284639841586907, -0.24082327317392008, -0.17388834357697364, 0.17676750150249115, -0.06104261199371856, ... |
706.195 | Electron-phonon and electron-electron interactions in organic field
effect transistors | Recent experiments have demonstrated that the performances of organic FETs
strongly depend on the dielectric properties of the gate insulator. In
particular, it has been shown that the temperature dependence of the mobility
evolves from a metallic-like to an insulating behavior upon increasing the
dielectric constant... | cond-mat.str-el | recent experiments have demonstrated that the performances of organic fets strongly depend on the dielectric properties of the gate insulator in particular it has been shown that the temperature dependence of the mobility evolves from a metalliclike to an insulating behavior upon increasing the dielectric constant of t... | [['recent', 'experiments', 'have', 'demonstrated', 'that', 'the', 'performances', 'of', 'organic', 'fets', 'strongly', 'depend', 'on', 'the', 'dielectric', 'properties', 'of', 'the', 'gate', 'insulator', 'in', 'particular', 'it', 'has', 'been', 'shown', 'that', 'the', 'temperature', 'dependence', 'of', 'the', 'mobility... | [-0.15182496645588658, 0.19128397927687327, -0.05021187150850892, -0.02227485231027852, 0.017653092185092957, -0.1209604937688822, 0.06225790254790912, 0.38626876327487614, -0.2509275314148477, -0.29163211380544396, 0.009764569079426607, -0.3158521311184795, -0.15270475219435914, 0.18568928741139465, -0.009024444794685... |
706.1951 | Wigner crystals of ions as quantum hard drives | Atomic systems in regular lattices are intriguing systems for implementing
ideas in quantum simulation and information processing. Focusing on laser
cooled ions forming Wigner crystals in Penning traps, we find a robust and
simple approach to engineering non-trivial 2-body interactions sufficient for
universal quantu... | quant-ph | atomic systems in regular lattices are intriguing systems for implementing ideas in quantum simulation and information processing focusing on laser cooled ions forming wigner crystals in penning traps we find a robust and simple approach to engineering nontrivial 2body interactions sufficient for universal quantum comp... | [['atomic', 'systems', 'in', 'regular', 'lattices', 'are', 'intriguing', 'systems', 'for', 'implementing', 'ideas', 'in', 'quantum', 'simulation', 'and', 'information', 'processing', 'focusing', 'on', 'laser', 'cooled', 'ions', 'forming', 'wigner', 'crystals', 'in', 'penning', 'traps', 'we', 'find', 'a', 'robust', 'and... | [-0.1112820849707925, 0.17460975916298066, -0.0351660185196023, 0.0496178193040836, 0.014604183909897175, -0.27176399076541446, 0.031042530370968175, 0.41091436041909973, -0.2439787922496045, -0.25241249294974555, 0.04459532539584433, -0.24960668762156993, -0.11931139498627112, 0.24658558377421197, -0.00220104646085715... |
706.1952 | Canonical representatives for residue classes of a polynomial ideal and
orthogonality | The aim of this paper is to unveil an unexpected relationship between the
normal form of a polynomial with respect to a polynomial ideal and the more
geometric concept of orthogonality. We present a new way to calculate the
normal form of a polynomial with respect to a polynomial ideal I in the ring of
multivariate p... | math.AC math.AG | the aim of this paper is to unveil an unexpected relationship between the normal form of a polynomial with respect to a polynomial ideal and the more geometric concept of orthogonality we present a new way to calculate the normal form of a polynomial with respect to a polynomial ideal i in the ring of multivariate poly... | [['the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'unveil', 'an', 'unexpected', 'relationship', 'between', 'the', 'normal', 'form', 'of', 'a', 'polynomial', 'with', 'respect', 'to', 'a', 'polynomial', 'ideal', 'and', 'the', 'more', 'geometric', 'concept', 'of', 'orthogonality', 'we', 'present', 'a', 'new', 'way', 'to'... | [-0.1848595475948406, 0.07065121050262176, -0.11965872721804172, 0.015462673305216985, -0.12525283559657557, -0.08563761882599175, 0.012601677653590966, 0.324832934626983, -0.33097687632459954, -0.17393187206531346, 0.07444848906316016, -0.21680595286997015, -0.1597569206940759, 0.16027100244056933, -0.0385186922995700... |
706.1953 | Generators of II_1 Factors | In 2005, Shen introduced a new invariant, $\mathcal G(N)$, of a diffuse von
Neumann algebra $N$ with a fixed faithful trace, and he used this invariant to
give a unified approach to showing that large classes of ${\mathrm{II}}_1$
factors $M$ are singly generated. This paper focuses on properties of this
invariant. We... | math.OA | in 2005 shen introduced a new invariant mathcal gn of a diffuse von neumann algebra n with a fixed faithful trace and he used this invariant to give a unified approach to showing that large classes of mathrmii_1 factors m are singly generated this paper focuses on properties of this invariant we relate mathcal gm to th... | [['in', '2005', 'shen', 'introduced', 'a', 'new', 'invariant', 'mathcal', 'gn', 'of', 'a', 'diffuse', 'von', 'neumann', 'algebra', 'n', 'with', 'a', 'fixed', 'faithful', 'trace', 'and', 'he', 'used', 'this', 'invariant', 'to', 'give', 'a', 'unified', 'approach', 'to', 'showing', 'that', 'large', 'classes', 'of', 'mathr... | [-0.14977621048903808, 0.18465384480853875, -0.01514832831155031, 0.027528565164464405, -0.05184248351038266, -0.18210447473594776, -0.03390330033442483, 0.32580746893579954, -0.26556411975851424, -0.20964279907922714, 0.07765947611023409, -0.2844955381865685, -0.10302165808896414, 0.1593019634186744, -0.12098206988153... |
706.1954 | SPM Bulletin 21 | Contents: 1. Editor's note; 2. Personal impressions from the SPM07 meeting;
3. Research announcements; 3.1. Coloring ordinals by reals; 3.2. Long Borel
Hierarchies; 3.3. Rothberger's property in finite powers; 3.4. Special subsets
of the reals and tree forcing notions; 3.5. All automorphisms of the Calkin
algebra are... | math.GN math.CO math.LO | contents 1 editors note 2 personal impressions from the spm07 meeting 3 research announcements 31 coloring ordinals by reals 32 long borel hierarchies 33 rothbergers property in finite powers 34 special subsets of the reals and tree forcing notions 35 all automorphisms of the calkin algebra are inner 36 continuous sele... | [['contents', '1', 'editors', 'note', '2', 'personal', 'impressions', 'from', 'the', 'spm07', 'meeting', '3', 'research', 'announcements', '31', 'coloring', 'ordinals', 'by', 'reals', '32', 'long', 'borel', 'hierarchies', '33', 'rothbergers', 'property', 'in', 'finite', 'powers', '34', 'special', 'subsets', 'of', 'the'... | [-0.1803338107119705, 0.1409107647505739, 0.0031873053340341455, 0.1303541336248639, -0.12098149343904469, -0.12266532507955387, 0.07735608516746671, 0.3264717808317503, -0.3052629242020269, -0.2799853268730384, 0.1423793644932229, -0.32158990747355404, -0.03818036890864092, 0.13185444764883048, -0.11617043937846858, -... |
706.1955 | Effect of disorder on a Pomeranchuk instability | We study the effect of disorder on the order parameter equation and
transition temperature of a Pomeranchuk-type Fermi-surface instability using
replica mean field theory. We consider the example of a phase transition to a
$d_{x^2 +y^2}$ type Fermi surface distortion, and show that, in the regime
where such a transit... | cond-mat.str-el cond-mat.dis-nn | we study the effect of disorder on the order parameter equation and transition temperature of a pomeranchuktype fermisurface instability using replica mean field theory we consider the example of a phase transition to a d_x2 y2 type fermi surface distortion and show that in the regime where such a transition is second ... | [['we', 'study', 'the', 'effect', 'of', 'disorder', 'on', 'the', 'order', 'parameter', 'equation', 'and', 'transition', 'temperature', 'of', 'a', 'pomeranchuktype', 'fermisurface', 'instability', 'using', 'replica', 'mean', 'field', 'theory', 'we', 'consider', 'the', 'example', 'of', 'a', 'phase', 'transition', 'to', '... | [-0.19751949377972236, 0.2160468636417484, -0.10956155743073434, 0.0815894254693821, -0.043541909824620854, -0.12008047801878383, 0.10852317833415966, 0.3287288969273659, -0.24627531372862768, -0.2563346279983191, 0.05076265156001566, -0.3115275331792679, -0.1670742992341439, 0.11534368993833344, 0.029597775153617594, ... |
706.1956 | Spherical Continuous Wavelet Transforms arising from sections of the
Lorentz group | We consider the conformal group of the unit sphere $S^{n-1},$ the so-called
proper Lorentz group Spin$^+(1,n),$ for the study of spherical continuous
wavelet transforms (CWT). Our approach is based on the method for construction
of general coherent states associated to square integrable group
representations over hom... | math.RT math.GR | we consider the conformal group of the unit sphere sn1 the socalled proper lorentz group spin1n for the study of spherical continuous wavelet transforms cwt our approach is based on the method for construction of general coherent states associated to square integrable group representations over homogeneous spaces the u... | [['we', 'consider', 'the', 'conformal', 'group', 'of', 'the', 'unit', 'sphere', 'sn1', 'the', 'socalled', 'proper', 'lorentz', 'group', 'spin1n', 'for', 'the', 'study', 'of', 'spherical', 'continuous', 'wavelet', 'transforms', 'cwt', 'our', 'approach', 'is', 'based', 'on', 'the', 'method', 'for', 'construction', 'of', ... | [-0.12132928155354972, 0.10340066999030018, -0.08288348128935169, 0.020719432915163944, -0.0999906431830137, -0.022205553143514228, -0.0018052084745503352, 0.37653073555499805, -0.29517533356461245, -0.15509773261814577, 0.13743642929723854, -0.23339188249293166, -0.12990565655646144, 0.1890804754230423, -0.07411695254... |
706.1957 | Level-rank duality of untwisted and twisted D-branes of the so(N)_K WZW
model | We analyze the level-rank duality of untwisted and epsilon-twisted D-branes
of the so(N)_K WZW model. Untwisted D-branes of so(N)_K are characterized by
integrable tensor and spinor representations of so(N)_K. Level-rank duality
maps untwisted so(N)_K D-branes corresponding to (equivalence classes of)
tensor represen... | hep-th | we analyze the levelrank duality of untwisted and epsilontwisted dbranes of the son_k wzw model untwisted dbranes of son_k are characterized by integrable tensor and spinor representations of son_k levelrank duality maps untwisted son_k dbranes corresponding to equivalence classes of tensor representations onto those o... | [['we', 'analyze', 'the', 'levelrank', 'duality', 'of', 'untwisted', 'and', 'epsilontwisted', 'dbranes', 'of', 'the', 'son_k', 'wzw', 'model', 'untwisted', 'dbranes', 'of', 'son_k', 'are', 'characterized', 'by', 'integrable', 'tensor', 'and', 'spinor', 'representations', 'of', 'son_k', 'levelrank', 'duality', 'maps', '... | [-0.19486276925924947, 0.20007030082114416, -0.036796112179610076, 0.14366551541994946, -0.05803560506205494, -0.17958648334366872, -0.05175281038927827, 0.31821707051758674, -0.22188710359235606, -0.1684851350591463, 0.11036299808891308, -0.2214987698723288, -0.1397071974899839, 0.10396660203068499, -0.120910442881651... |
706.1958 | Fano threefolds with noncyclic torsion in the divisor class group | In this note we study Fano threefolds with noncyclic torsion in the divisor
class group. Since they can all be obtained as quotients of Fano threefolds, we
get also all examples that can be obtained as quotients of low codimension
Fanos in the weighted projective space.
| math.AG | in this note we study fano threefolds with noncyclic torsion in the divisor class group since they can all be obtained as quotients of fano threefolds we get also all examples that can be obtained as quotients of low codimension fanos in the weighted projective space | [['in', 'this', 'note', 'we', 'study', 'fano', 'threefolds', 'with', 'noncyclic', 'torsion', 'in', 'the', 'divisor', 'class', 'group', 'since', 'they', 'can', 'all', 'be', 'obtained', 'as', 'quotients', 'of', 'fano', 'threefolds', 'we', 'get', 'also', 'all', 'examples', 'that', 'can', 'be', 'obtained', 'as', 'quotients... | [-0.19401275783615268, 0.06369121376748967, -0.09445679908537347, 0.12255671068408486, -0.08234519844004155, -0.1707268856951724, -0.03485817177241425, 0.3826608618154474, -0.28611381351947784, -0.22072972430159216, 0.12217513064641262, -0.24912538970618145, -0.20153587981653603, 0.2577810306304499, -0.2455557732154493... |
706.1959 | The Black Hole Mass of Abell 1836-BCG and Abell 3565-BCG | Two brightest cluster galaxies (BCGs), namely Abell 1836-BCG and Abell
3565-BCG, were observed with the Advanced Camera for Surveys (ACS) and the
Space Telescope Imaging Spectrograph (STIS) on board the Hubble Space
Telescope. By modeling the available photometric and kinematic data, it
resulted that the mass of Abel... | astro-ph | two brightest cluster galaxies bcgs namely abell 1836bcg and abell 3565bcg were observed with the advanced camera for surveys acs and the space telescope imaging spectrograph stis on board the hubble space telescope by modeling the available photometric and kinematic data it resulted that the mass of abell 1836bcg and ... | [['two', 'brightest', 'cluster', 'galaxies', 'bcgs', 'namely', 'abell', '1836bcg', 'and', 'abell', '3565bcg', 'were', 'observed', 'with', 'the', 'advanced', 'camera', 'for', 'surveys', 'acs', 'and', 'the', 'space', 'telescope', 'imaging', 'spectrograph', 'stis', 'on', 'board', 'the', 'hubble', 'space', 'telescope', 'by... | [-0.03061348502524197, 0.08250549782514421, -0.10069318315494925, 0.06950941492593096, -0.20167780493295961, -0.08200044512388206, -0.03639081830248957, 0.48041998474828657, -0.019832221130209583, -0.4086913720013634, 0.10297611073004984, -0.3214851045500367, -0.0346887377992032, 0.2652783241243132, 0.02079293370667484... |
706.196 | Compressibility and equation of state of finite nuclei | We present a new approach for calculating the nuclear equation of state and
compressibility for finite nuclei using the density-constrained Hartree-Fock
method.
| nucl-th | we present a new approach for calculating the nuclear equation of state and compressibility for finite nuclei using the densityconstrained hartreefock method | [['we', 'present', 'a', 'new', 'approach', 'for', 'calculating', 'the', 'nuclear', 'equation', 'of', 'state', 'and', 'compressibility', 'for', 'finite', 'nuclei', 'using', 'the', 'densityconstrained', 'hartreefock', 'method']] | [-0.008591263639655981, 0.09630104321563109, -0.1784655675292015, 0.09589169129983267, 0.01623903578993949, -0.09789282894185321, 0.09950430511327629, 0.3283849307759242, -0.2115501866210252, -0.22185689278624274, -0.018890403232283214, -0.2829617624255744, -0.04409186880696903, 0.1858275908214802, 0.13244180935858327,... |
706.1961 | Kleinian groups with ubiquitous surface subgroups | We show that every finitely-generated free subgroup of a right-angled,
co-compact Kleinian reflection group is contained in a surface subgroup.
| math.GT | we show that every finitelygenerated free subgroup of a rightangled cocompact kleinian reflection group is contained in a surface subgroup | [['we', 'show', 'that', 'every', 'finitelygenerated', 'free', 'subgroup', 'of', 'a', 'rightangled', 'cocompact', 'kleinian', 'reflection', 'group', 'is', 'contained', 'in', 'a', 'surface', 'subgroup']] | [-0.26969544449821115, 0.131119899766054, -0.15127248961944134, 0.028087125375168397, -0.17104249484837056, -0.14082380975596606, 0.03268678453750908, 0.5133619850501419, -0.40493319034576414, -0.09270922653377056, 0.09377224416821264, -0.340522550791502, -0.09104174969252199, 0.26685661196243016, -0.316667659394443, -... |
706.1962 | Dynamical and Observational Constraints on Additional Planets in Highly
Eccentric Planetary Systems | Long time coverage and high radial velocity precision have allowed for the
discovery of additional objects in known planetary systems. Many of the
extrasolar planets detected have highly eccentric orbits, which raises the
question of how likely those systems are to host additional planets. We
investigate six systems ... | astro-ph | long time coverage and high radial velocity precision have allowed for the discovery of additional objects in known planetary systems many of the extrasolar planets detected have highly eccentric orbits which raises the question of how likely those systems are to host additional planets we investigate six systems which... | [['long', 'time', 'coverage', 'and', 'high', 'radial', 'velocity', 'precision', 'have', 'allowed', 'for', 'the', 'discovery', 'of', 'additional', 'objects', 'in', 'known', 'planetary', 'systems', 'many', 'of', 'the', 'extrasolar', 'planets', 'detected', 'have', 'highly', 'eccentric', 'orbits', 'which', 'raises', 'the',... | [-0.19326565168391335, 0.10463398696631718, -0.03868007828468378, 0.036866105894531896, -0.11654133138141896, -0.1848038100903119, 0.12957104718030601, 0.3299702934028817, -0.13800008865860355, -0.35489148462952025, 0.10346359598801248, -0.2857181044741416, -0.09712167395751031, 0.19481438218245387, -0.0828961878195142... |
706.1963 | Galaxy Cluster Gas Mass Fraction and Hubble Parameter versus Redshift
Constraints on Dark Energy | Galaxy cluster gas mass fraction versus redshift data and Hubble parameter
versus redshift data are used to jointly constrain dark energy models. These
constraints favor the Einstein cosmological constant limit of dark energy but
do not strongly rule out slowly-evolving dark energy.
| astro-ph | galaxy cluster gas mass fraction versus redshift data and hubble parameter versus redshift data are used to jointly constrain dark energy models these constraints favor the einstein cosmological constant limit of dark energy but do not strongly rule out slowlyevolving dark energy | [['galaxy', 'cluster', 'gas', 'mass', 'fraction', 'versus', 'redshift', 'data', 'and', 'hubble', 'parameter', 'versus', 'redshift', 'data', 'are', 'used', 'to', 'jointly', 'constrain', 'dark', 'energy', 'models', 'these', 'constraints', 'favor', 'the', 'einstein', 'cosmological', 'constant', 'limit', 'of', 'dark', 'ene... | [-0.10117965242187936, 0.12389874438356076, -0.11231896384353084, 0.20846675837501175, -0.21984654217071475, -0.14832616799200574, 0.06663451490125485, 0.37583631702831816, -0.15205151144237744, -0.4217909870757943, 0.0041265249352103895, -0.23718447362383208, 0.1515425918180318, 0.16053427784936503, 0.0591322937869422... |
706.1964 | Testing Radiative Neutrino Mass Generation at the LHC | We have investigated in detail a model that contains an additional SU(2)
singlet and triplet scalar fields than the Standard Model (SM). This allows the
radiative generation of Majorana neutrino masses at two-loop order with the
help of doubly charged Higgs bosons that arise from the extended Higgs sector.
We studied... | hep-ph hep-ex | we have investigated in detail a model that contains an additional su2 singlet and triplet scalar fields than the standard model sm this allows the radiative generation of majorana neutrino masses at twoloop order with the help of doubly charged higgs bosons that arise from the extended higgs sector we studied in detai... | [['we', 'have', 'investigated', 'in', 'detail', 'a', 'model', 'that', 'contains', 'an', 'additional', 'su2', 'singlet', 'and', 'triplet', 'scalar', 'fields', 'than', 'the', 'standard', 'model', 'sm', 'this', 'allows', 'the', 'radiative', 'generation', 'of', 'majorana', 'neutrino', 'masses', 'at', 'twoloop', 'order', 'w... | [-0.08191938802118001, 0.31728047720161007, 0.005967241503449894, 0.20249026152711405, -0.051309557182194536, -0.20773751792757836, 0.0038386276479117397, 0.3068112044075374, -0.2123010638792631, -0.2610371673891191, 0.024826160016155608, -0.3199151620109935, -0.05659262816046722, 0.11645533356187475, 0.119199254912822... |
706.1965 | SDSS J080531.84+481233.0: An Unresolved L Dwarf/T Dwarf Binary | SDSS J080531.84+481233.0 is a peculiar L-type dwarf that exhibits unusually
blue near-infrared and mid-infrared colors and divergent optical (L4) and
near-infrared (L9.5) spectral classifications. These peculiar spectral traits
have been variously attributed to condensate cloud effects or subsolar
metallicity. Here I... | astro-ph | sdss j080531844812330 is a peculiar ltype dwarf that exhibits unusually blue nearinfrared and midinfrared colors and divergent optical l4 and nearinfrared l95 spectral classifications these peculiar spectral traits have been variously attributed to condensate cloud effects or subsolar metallicity here i present an impr... | [['sdss', 'j080531844812330', 'is', 'a', 'peculiar', 'ltype', 'dwarf', 'that', 'exhibits', 'unusually', 'blue', 'nearinfrared', 'and', 'midinfrared', 'colors', 'and', 'divergent', 'optical', 'l4', 'and', 'nearinfrared', 'l95', 'spectral', 'classifications', 'these', 'peculiar', 'spectral', 'traits', 'have', 'been', 'va... | [-0.05853196023088594, 0.1228266385193131, -0.10074888886291684, 0.07826498189653039, -0.13183562806269122, -0.15050651915667504, 0.07609210143032662, 0.43839464657482385, -0.2028607852835036, -0.3507305334505189, 0.07375322787005002, -0.2768020866212645, -0.08123136670032592, 0.17542158560309226, -0.09734345962578765,... |
706.1966 | On the lack of relation between physics and "Quantum discord and
Maxwell's demons" | The information-theoretic arguments presented in a recent publication on
"Quantum discord and Maxwell's demons" are discussed, and found not to address
the problem specified by Maxwell. Two interrelated and definitive exorcisms of
the demon, one purely thermodynamic, and the other quantum-thermodynamic are
briefly di... | quant-ph | the informationtheoretic arguments presented in a recent publication on quantum discord and maxwells demons are discussed and found not to address the problem specified by maxwell two interrelated and definitive exorcisms of the demon one purely thermodynamic and the other quantumthermodynamic are briefly discussed for... | [['the', 'informationtheoretic', 'arguments', 'presented', 'in', 'a', 'recent', 'publication', 'on', 'quantum', 'discord', 'and', 'maxwells', 'demons', 'are', 'discussed', 'and', 'found', 'not', 'to', 'address', 'the', 'problem', 'specified', 'by', 'maxwell', 'two', 'interrelated', 'and', 'definitive', 'exorcisms', 'of... | [-0.08938037280560679, 0.08229198441976338, -0.08361700824145409, 0.06885352139406413, -0.11446261838150834, -0.20261181120136842, 0.06355899142652967, 0.28794620780147684, -0.2510322171073515, -0.2981157033044158, 0.12257350349993201, -0.29003541017837314, -0.12088381480968115, 0.1991759638880714, -0.13897434072297754... |
706.1967 | Chemical evolution of the Small Magellanic Cloud based on planetary
nebulae | We investigate the chemical evolution of the Small Magellanic Cloud (SMC)
based on abundance data of planetary nebulae (PNe). The main goal is to
investigate the time evolution of the oxygen abundance in this galaxy by
deriving an age-metallicity relation. Such a relation is of fundamental
importance as an observatio... | astro-ph | we investigate the chemical evolution of the small magellanic cloud smc based on abundance data of planetary nebulae pne the main goal is to investigate the time evolution of the oxygen abundance in this galaxy by deriving an agemetallicity relation such a relation is of fundamental importance as an observational const... | [['we', 'investigate', 'the', 'chemical', 'evolution', 'of', 'the', 'small', 'magellanic', 'cloud', 'smc', 'based', 'on', 'abundance', 'data', 'of', 'planetary', 'nebulae', 'pne', 'the', 'main', 'goal', 'is', 'to', 'investigate', 'the', 'time', 'evolution', 'of', 'the', 'oxygen', 'abundance', 'in', 'this', 'galaxy', 'b... | [-0.05066832462658307, 0.0397243753760839, -0.09052021505859946, 0.11532555085848019, -0.07595374336753073, -0.006789042030244933, 0.0791716006632279, 0.41602649378390716, -0.1940486173854359, -0.3819912524943772, 0.03775425279465188, -0.22554130431879976, -0.032042477812085836, 0.20280826156314496, -0.0699436841262338... |
706.1968 | The Riemann hypothesis - an elementary analytic approach based on
complex Laplace transform | An elementary analytic proof of the famous Riemann hypothesis is given. The
main "accent" of the proof is a both using of the 2-dimensional double real and
complex Laplace integral representations of the Green function $\mid z
\mid^{-2}$.
| math.GM | an elementary analytic proof of the famous riemann hypothesis is given the main accent of the proof is a both using of the 2dimensional double real and complex laplace integral representations of the green function mid z mid2 | [['an', 'elementary', 'analytic', 'proof', 'of', 'the', 'famous', 'riemann', 'hypothesis', 'is', 'given', 'the', 'main', 'accent', 'of', 'the', 'proof', 'is', 'a', 'both', 'using', 'of', 'the', '2dimensional', 'double', 'real', 'and', 'complex', 'laplace', 'integral', 'representations', 'of', 'the', 'green', 'function'... | [-0.13006310623038458, 0.02267639350651046, -0.1633751332206098, 0.12996004761599406, -0.119922323397839, -0.057294487135132424, -0.015171769301633577, 0.2777152870957916, -0.25136017396643356, -0.19231997291884712, 0.1290130961208126, -0.23723108266052362, -0.2053467738583709, 0.24772569053881877, -0.04355785263249197... |
706.1969 | Formation of singularities for a transport equation with nonlocal
velocity | We study a 1D transport equation with nonlocal velocity and show the
formation of singularities in finite time for a generic family of initial data.
By adding a diffusion term the finite time singularity is prevented and the
solutions exist globally in time.
| math.AP | we study a 1d transport equation with nonlocal velocity and show the formation of singularities in finite time for a generic family of initial data by adding a diffusion term the finite time singularity is prevented and the solutions exist globally in time | [['we', 'study', 'a', '1d', 'transport', 'equation', 'with', 'nonlocal', 'velocity', 'and', 'show', 'the', 'formation', 'of', 'singularities', 'in', 'finite', 'time', 'for', 'a', 'generic', 'family', 'of', 'initial', 'data', 'by', 'adding', 'a', 'diffusion', 'term', 'the', 'finite', 'time', 'singularity', 'is', 'preven... | [-0.1985610721654497, 0.10755964725949736, -0.1047597321313481, 0.035817529407849664, -0.035334178484803025, -0.14376467857293265, -0.013912984624851582, 0.3071103147339336, -0.30945366902580096, -0.2082350656476825, 0.142616844633161, -0.28350753345808316, -0.09508034942108531, 0.13869188145496125, 0.01725874353893274... |
706.197 | Energy Density-Flux Correlations in an Unusual Quantum State and in the
Vacuum | In this paper we consider the question of the degree to which negative and
positive energy are intertwined. We examine in more detail a previously studied
quantum state of the massless minimally coupled scalar field, which we call a
``Helfer state''. This is a state in which the energy density can be made
arbitrarily... | quant-ph gr-qc hep-th | in this paper we consider the question of the degree to which negative and positive energy are intertwined we examine in more detail a previously studied quantum state of the massless minimally coupled scalar field which we call a helfer state this is a state in which the energy density can be made arbitrarily negative... | [['in', 'this', 'paper', 'we', 'consider', 'the', 'question', 'of', 'the', 'degree', 'to', 'which', 'negative', 'and', 'positive', 'energy', 'are', 'intertwined', 'we', 'examine', 'in', 'more', 'detail', 'a', 'previously', 'studied', 'quantum', 'state', 'of', 'the', 'massless', 'minimally', 'coupled', 'scalar', 'field'... | [-0.13413124245506797, 0.2043443103944777, -0.07118189736523411, 0.10239837626037611, -0.0025059431613507596, -0.11648324816572395, 0.02411229199602861, 0.3423532314801758, -0.22311165787702936, -0.3137842047045177, 0.06341601458505135, -0.2794392583612882, -0.09275472589514472, 0.15156700223345648, -0.0085639328053432... |
706.1971 | Low-lying Wilson Dirac operator eigenvector mixing in dynamical overlap
Hybrid Monte-Carlo | Current dynamical overlap fermion hybrid Monte Carlo simulations encounter
large fermionic forces when there is mixing between near zero-eigenvectors of
the kernel operator. This leads to low acceptance rates when there is a large
density of near zero eigenvectors. I present a method where these large forces
are elim... | hep-lat | current dynamical overlap fermion hybrid monte carlo simulations encounter large fermionic forces when there is mixing between near zeroeigenvectors of the kernel operator this leads to low acceptance rates when there is a large density of near zero eigenvectors i present a method where these large forces are eliminate... | [['current', 'dynamical', 'overlap', 'fermion', 'hybrid', 'monte', 'carlo', 'simulations', 'encounter', 'large', 'fermionic', 'forces', 'when', 'there', 'is', 'mixing', 'between', 'near', 'zeroeigenvectors', 'of', 'the', 'kernel', 'operator', 'this', 'leads', 'to', 'low', 'acceptance', 'rates', 'when', 'there', 'is', '... | [-0.14243500105612264, 0.22732133922886244, -0.05657672899763418, 0.07009342464779009, -0.010359195246703074, -0.14133639599025674, 0.05848486579606852, 0.34624628137938585, -0.2732077782172002, -0.30174463857672634, 0.08740026978893747, -0.27478073142734916, -0.11556599641224675, 0.14172703480418725, 0.000740147319539... |
706.1972 | Excitonic Mott transition in type-II quantum dots | Photoluminescence spectra measured on a type-II GaSb/GaAs quantum dot
ensemble at high excitation power indicate a Mott transition from the low
density state comprising of spatially-indirect excitons to a high density
electron-plasma state. Under the influence of a very high magnetic field, the
electron-plasma that i... | cond-mat.other | photoluminescence spectra measured on a typeii gasbgaas quantum dot ensemble at high excitation power indicate a mott transition from the low density state comprising of spatiallyindirect excitons to a high density electronplasma state under the influence of a very high magnetic field the electronplasma that is formed ... | [['photoluminescence', 'spectra', 'measured', 'on', 'a', 'typeii', 'gasbgaas', 'quantum', 'dot', 'ensemble', 'at', 'high', 'excitation', 'power', 'indicate', 'a', 'mott', 'transition', 'from', 'the', 'low', 'density', 'state', 'comprising', 'of', 'spatiallyindirect', 'excitons', 'to', 'a', 'high', 'density', 'electronp... | [-0.13971485744498796, 0.24454626430741558, -0.06851798589972748, 0.020351556386261925, 0.06090415516568316, -0.15657290239360624, 0.08141032069274304, 0.39924590807344956, -0.19681303597734137, -0.29872892740166795, 0.013349228282064453, -0.31364219654667175, 0.009081630588714348, 0.1368772651274073, 0.074009512993112... |
706.1973 | Skew-Hadamard matrices of orders 436, 580 and 988 exist | We construct two difference families on each of the cyclic groups of order
109, 145 and 247, and use them to construct skew-Hadamard matrices of orders
436, 580 and 988. Such difference families and matrices are constructed here
for the first time. The matrices are constructed by using the Goethals-Seidel
array.
| math.CO | we construct two difference families on each of the cyclic groups of order 109 145 and 247 and use them to construct skewhadamard matrices of orders 436 580 and 988 such difference families and matrices are constructed here for the first time the matrices are constructed by using the goethalsseidel array | [['we', 'construct', 'two', 'difference', 'families', 'on', 'each', 'of', 'the', 'cyclic', 'groups', 'of', 'order', '109', '145', 'and', '247', 'and', 'use', 'them', 'to', 'construct', 'skewhadamard', 'matrices', 'of', 'orders', '436', '580', 'and', '988', 'such', 'difference', 'families', 'and', 'matrices', 'are', 'co... | [-0.13422780177172491, 0.15223880121301786, 0.02446969076260632, 0.04080048230860163, 0.0046684967682642095, -0.05205251330363692, 0.04667589331374449, 0.37772733572066997, -0.2300142310194525, -0.40141291586755246, 0.20435833126562192, -0.33266517103594895, -0.1113188101124822, 0.19565637471775213, 0.02383502747169604... |
706.1974 | Towards a microscopic theory of toroidal moments in bulk periodic
crystals | We present a theoretical analysis of magnetic toroidal moments in periodic
systems, in the limit in which the toroidal moments are caused by a time and
space reversal symmetry breaking arrangement of localized magnetic dipole
moments. We summarize the basic definitions for finite systems and address the
question of h... | cond-mat.str-el cond-mat.mtrl-sci | we present a theoretical analysis of magnetic toroidal moments in periodic systems in the limit in which the toroidal moments are caused by a time and space reversal symmetry breaking arrangement of localized magnetic dipole moments we summarize the basic definitions for finite systems and address the question of how t... | [['we', 'present', 'a', 'theoretical', 'analysis', 'of', 'magnetic', 'toroidal', 'moments', 'in', 'periodic', 'systems', 'in', 'the', 'limit', 'in', 'which', 'the', 'toroidal', 'moments', 'are', 'caused', 'by', 'a', 'time', 'and', 'space', 'reversal', 'symmetry', 'breaking', 'arrangement', 'of', 'localized', 'magnetic'... | [-0.1740538016798213, 0.14369359199461246, -0.040590988753666714, 0.10593476437971668, -0.04380890670053791, -0.057620048961537176, 0.041530592281433625, 0.382300075024453, -0.25846618323229514, -0.2729241457756955, 0.08682626628907138, -0.26006326329255436, -0.17893919519955553, 0.17879662870769228, -0.015216780485325... |
706.1975 | Proper Motions in the Galactic Bulge: Plaut's Window | A proper motion study of a field of 20' x 20' inside Plaut's low extinction
window (l,b)=(0 deg,-8 deg), has been completed. Relative proper motions and
photographic BV photometry have been derived for ~21,000 stars reaching to
V~20.5 mag, based on the astrometric reduction of 43 photographic plates,
spanning over 21... | astro-ph | a proper motion study of a field of 20 x 20 inside plauts low extinction window lb0 deg8 deg has been completed relative proper motions and photographic bv photometry have been derived for 21000 stars reaching to v205 mag based on the astrometric reduction of 43 photographic plates spanning over 21 years of epoch diffe... | [['a', 'proper', 'motion', 'study', 'of', 'a', 'field', 'of', '20', 'x', '20', 'inside', 'plauts', 'low', 'extinction', 'window', 'lb0', 'deg8', 'deg', 'has', 'been', 'completed', 'relative', 'proper', 'motions', 'and', 'photographic', 'bv', 'photometry', 'have', 'been', 'derived', 'for', '21000', 'stars', 'reaching', ... | [-0.03324508450627894, 0.10602895119003934, -0.11871343646145394, 0.026989377687849026, -0.13161964181229868, -0.039945997357963385, 0.11400323588677289, 0.4744144139152743, -0.14455341430758958, -0.40371898249032495, 0.033263511609147964, -0.32680403269799035, 0.05153027518135372, 0.22815519489393085, -0.1076929211916... |
706.1976 | Tidal dwarf galaxies as a test of fundamental physics | Within the cold dark matter (CDM) framework tidal dwarf galaxies (TDGs)
cannot contain dark matter, so the recent results by Bournaud et al. (2007)
that 3 rotating TDGs do show significant evidence for being dark matter
dominated is inconsistent with the current concordance cosmological theory
unless yet another dark... | astro-ph | within the cold dark matter cdm framework tidal dwarf galaxies tdgs cannot contain dark matter so the recent results by bournaud et al 2007 that 3 rotating tdgs do show significant evidence for being dark matter dominated is inconsistent with the current concordance cosmological theory unless yet another dark matter co... | [['within', 'the', 'cold', 'dark', 'matter', 'cdm', 'framework', 'tidal', 'dwarf', 'galaxies', 'tdgs', 'can', 'not', 'contain', 'dark', 'matter', 'so', 'the', 'recent', 'results', 'by', 'bournaud', 'et', 'al', '2007', 'that', '3', 'rotating', 'tdgs', 'do', 'show', 'significant', 'evidence', 'for', 'being', 'dark', 'mat... | [-0.11747809714870527, 0.13916644247631968, -0.14482661741527003, 0.15419049151565156, -0.13533551246768588, -0.11477617130925258, -0.04593251141422014, 0.3538173058083177, -0.19764677589862711, -0.39190331991348004, 0.019557401635554722, -0.2027100751331697, -0.12898346999686006, 0.17627456202689146, -0.09072147754227... |
706.1977 | Challenging the Cosmological Constant | We outline a dynamical dark energy scenario whose signatures may be
simultaneously tested by astronomical observations and laboratory experiments.
The dark energy is a field with slightly sub-gravitational couplings to matter,
a logarithmic self-interaction potential with a scale tuned to $\sim 10^{-3}
{\rm eV}$, as ... | astro-ph gr-qc hep-ph hep-th | we outline a dynamical dark energy scenario whose signatures may be simultaneously tested by astronomical observations and laboratory experiments the dark energy is a field with slightly subgravitational couplings to matter a logarithmic selfinteraction potential with a scale tuned to sim 103 rm ev as is usual in quint... | [['we', 'outline', 'a', 'dynamical', 'dark', 'energy', 'scenario', 'whose', 'signatures', 'may', 'be', 'simultaneously', 'tested', 'by', 'astronomical', 'observations', 'and', 'laboratory', 'experiments', 'the', 'dark', 'energy', 'is', 'a', 'field', 'with', 'slightly', 'subgravitational', 'couplings', 'to', 'matter', '... | [-0.13813042311562537, 0.2614670056457014, -0.11302653327926665, 0.12651460154647876, -0.08030713340309681, -0.13600999986114426, 0.019038500178029036, 0.30591001721811206, -0.24879633083284255, -0.3924216350800741, 0.0461332088824134, -0.27113473628188284, -0.0010631261435569141, 0.15496667903717354, 0.002784764314095... |
706.1978 | On the Stopping Time of a Bouncing Ball | We study a simple model of a bouncing ball that takes explicitely into
account the elastic deformability of the body and the energy dissipation due to
internal friction. We show that this model is not subject to the problem of
inelastic collapse, that is, it does not allow an infinite number of impacts in
a finite ti... | math-ph math.MP | we study a simple model of a bouncing ball that takes explicitely into account the elastic deformability of the body and the energy dissipation due to internal friction we show that this model is not subject to the problem of inelastic collapse that is it does not allow an infinite number of impacts in a finite time we... | [['we', 'study', 'a', 'simple', 'model', 'of', 'a', 'bouncing', 'ball', 'that', 'takes', 'explicitely', 'into', 'account', 'the', 'elastic', 'deformability', 'of', 'the', 'body', 'and', 'the', 'energy', 'dissipation', 'due', 'to', 'internal', 'friction', 'we', 'show', 'that', 'this', 'model', 'is', 'not', 'subject', 't... | [-0.12572576689976497, 0.15176591991419824, -0.1467147240147806, 0.03954188937510336, -0.08653064626315148, -0.10106850147136662, 0.05157750384826766, 0.36408618411584065, -0.2390361371274927, -0.2561997683847895, 0.07330959518831962, -0.26657307668045016, -0.15849454103424998, 0.20598771167218244, -0.04146034375875081... |
706.1979 | Black hole radiation spectrum in LQG: Isolated Horizon framework | Recent detailed analysis within the Loop Quantum Gravity calculation of black
hole entropy shows a stair-like structure in the behavior of entropy as a
function of horizon area. The non-trivial distribution of the degeneracy of the
black hole horizon area eigenstates is at the origin of this behavior. This
degeneracy... | gr-qc | recent detailed analysis within the loop quantum gravity calculation of black hole entropy shows a stairlike structure in the behavior of entropy as a function of horizon area the nontrivial distribution of the degeneracy of the black hole horizon area eigenstates is at the origin of this behavior this degeneracy distr... | [['recent', 'detailed', 'analysis', 'within', 'the', 'loop', 'quantum', 'gravity', 'calculation', 'of', 'black', 'hole', 'entropy', 'shows', 'a', 'stairlike', 'structure', 'in', 'the', 'behavior', 'of', 'entropy', 'as', 'a', 'function', 'of', 'horizon', 'area', 'the', 'nontrivial', 'distribution', 'of', 'the', 'degener... | [-0.16313298397231846, 0.059146298160776496, -0.15603311243932694, 0.14678879510844126, -0.04861874045804143, -0.11645483447238802, 0.05178150113439187, 0.2719168123602867, -0.18921249866485595, -0.31066506208851935, 0.07107312389882281, -0.33765533242374657, -0.08353668415918947, 0.18391135210637002, -0.03904596472624... |
706.198 | Bubbles in the Self-Accelerating Universe | We revisit the issue of the stability in the Dvali-Gabadadze-Porrati model,
by considering the nucleation of bubbles of the conventional branch within the
self-accelerating branch. We construct an instanton describing this process in
the thin wall approximation. On one side of the bubble wall, the bulk consists
of th... | hep-th astro-ph gr-qc | we revisit the issue of the stability in the dvaligabadadzeporrati model by considering the nucleation of bubbles of the conventional branch within the selfaccelerating branch we construct an instanton describing this process in the thin wall approximation on one side of the bubble wall the bulk consists of the exterio... | [['we', 'revisit', 'the', 'issue', 'of', 'the', 'stability', 'in', 'the', 'dvaligabadadzeporrati', 'model', 'by', 'considering', 'the', 'nucleation', 'of', 'bubbles', 'of', 'the', 'conventional', 'branch', 'within', 'the', 'selfaccelerating', 'branch', 'we', 'construct', 'an', 'instanton', 'describing', 'this', 'proces... | [-0.14389702019340903, 0.14008003198267485, -0.13540826702081313, 0.042946913168277145, -0.10920057163676085, -0.0927914386276005, 0.03333318084505295, 0.3349794923150212, -0.23590571650659203, -0.2369750874235451, 0.12543908442098733, -0.27263746969401836, -0.10557170876980129, 0.12773134367576816, -0.0305314699518951... |
706.1981 | Equilibrium configurations of two charged masses in General Relativity | An asymptotically flat static solution of Einstein-Maxwell equations which
describes the field of two non-extreme Reissner - Nordstr\"om sources in
equilibrium is presented. It is expressed in terms of physical parameters of
the sources (their masses, charges and separating distance). Very simple
analytical forms wer... | gr-qc hep-th | an asymptotically flat static solution of einsteinmaxwell equations which describes the field of two nonextreme reissner nordstrom sources in equilibrium is presented it is expressed in terms of physical parameters of the sources their masses charges and separating distance very simple analytical forms were found for t... | [['an', 'asymptotically', 'flat', 'static', 'solution', 'of', 'einsteinmaxwell', 'equations', 'which', 'describes', 'the', 'field', 'of', 'two', 'nonextreme', 'reissner', 'nordstrom', 'sources', 'in', 'equilibrium', 'is', 'presented', 'it', 'is', 'expressed', 'in', 'terms', 'of', 'physical', 'parameters', 'of', 'the', ... | [-0.1805186518074446, 0.08154019027135521, -0.1093835555849938, 0.11758161484900022, -0.05834942182499758, -0.18848901162166673, -0.005207079656186028, 0.3208907890645131, -0.1936043749668334, -0.27049639690126304, 0.13029970172267985, -0.33124675840454204, -0.06988815378814175, 0.1945146353715296, -0.04484324758006653... |
706.1982 | Limits on primordial power spectrum resolution: An inflationary flow
analysis | We investigate the ability of current CMB data to reliably constrain the form
of the primordial power spectrum generated during inflation. We attempt to
identify more exotic power spectra that yield equally good fits to the data as
simple power-law spectra. In order to test a wide variety of spectral shapes,
we combi... | astro-ph | we investigate the ability of current cmb data to reliably constrain the form of the primordial power spectrum generated during inflation we attempt to identify more exotic power spectra that yield equally good fits to the data as simple powerlaw spectra in order to test a wide variety of spectral shapes we combine the... | [['we', 'investigate', 'the', 'ability', 'of', 'current', 'cmb', 'data', 'to', 'reliably', 'constrain', 'the', 'form', 'of', 'the', 'primordial', 'power', 'spectrum', 'generated', 'during', 'inflation', 'we', 'attempt', 'to', 'identify', 'more', 'exotic', 'power', 'spectra', 'that', 'yield', 'equally', 'good', 'fits', ... | [-0.08074714514471623, 0.11692057266286432, -0.08673446133781598, 0.10876054146813074, -0.07671769752520986, -0.14520011751762057, -0.010738728160758434, 0.3635487378570841, -0.24701393339132247, -0.37482663472569405, 0.06411199738611122, -0.2799881698745308, -0.043228165766094125, 0.2386507458199938, -0.00290637363259... |
706.1983 | The Heavy Ion Physics Program with ATLAS at the LHC | The first Pb+Pb collisions at the Large Hadron Collider (LHC) at sqrts_NN =
5.52 TeV are imminent. Heavy ion collisions at the LHC provide an extended
energy lever arm to the existing measurements made at RHIC and SPS, especially
in hard (large-Q^2) processes. In this contribution an overview of the ATLAS
detector is... | nucl-ex | the first pbpb collisions at the large hadron collider lhc at sqrts_nn 552 tev are imminent heavy ion collisions at the lhc provide an extended energy lever arm to the existing measurements made at rhic and sps especially in hard largeq2 processes in this contribution an overview of the atlas detector is given and the ... | [['the', 'first', 'pbpb', 'collisions', 'at', 'the', 'large', 'hadron', 'collider', 'lhc', 'at', 'sqrts_nn', '552', 'tev', 'are', 'imminent', 'heavy', 'ion', 'collisions', 'at', 'the', 'lhc', 'provide', 'an', 'extended', 'energy', 'lever', 'arm', 'to', 'the', 'existing', 'measurements', 'made', 'at', 'rhic', 'and', 'sp... | [-0.05315783446511397, 0.23911696808958927, -0.1469469278262785, 0.13223901907734287, -0.00949064175455043, -0.15583104408131196, -0.13150572271014635, 0.3278193795623688, -0.21218899302184582, -0.292635306966706, 0.007980150253010484, -0.4007301787451769, 0.1793138427230028, 0.1658617958605576, 0.07739723070452993, 0.... |
706.1984 | Measurements of Top Properties at the Tevatron | The large data samples of thousands of top events collected at the Tevatron
experiments CDF and D0 allow for a variety of measurements to analyze the
properties of the top quark. Guided by the question "Is the top quark observed
at the Tevatron really the top quark of the standard model,'' we present
Tevatron analyse... | hep-ex | the large data samples of thousands of top events collected at the tevatron experiments cdf and d0 allow for a variety of measurements to analyze the properties of the top quark guided by the question is the top quark observed at the tevatron really the top quark of the standard model we present tevatron analyses study... | [['the', 'large', 'data', 'samples', 'of', 'thousands', 'of', 'top', 'events', 'collected', 'at', 'the', 'tevatron', 'experiments', 'cdf', 'and', 'd0', 'allow', 'for', 'a', 'variety', 'of', 'measurements', 'to', 'analyze', 'the', 'properties', 'of', 'the', 'top', 'quark', 'guided', 'by', 'the', 'question', 'is', 'the',... | [-0.02662614771695591, 0.22944491862341068, -0.045258529819981304, 0.11956055147903646, -0.06954128439213302, -0.11939242020314343, 0.12941449815623982, 0.2391210774089708, -0.23145053458811585, -0.25758247738054324, -0.019164812613040382, -0.39950699924469685, 0.0784503291036154, 0.13754945975825797, 0.151786719838720... |
706.1985 | Examining the Location of the Magnetopause in an Undergraduate Lab | Integrating areas of current research into undergraduate physics labs can be
a difficult task. The location of the magnetopause is one problem that can be
examined with no prior exposure to space physics. The magnetopause location can
be viewed as a pressure balance between the dynamic pressure of the solar wind
and ... | physics.space-ph physics.ed-ph | integrating areas of current research into undergraduate physics labs can be a difficult task the location of the magnetopause is one problem that can be examined with no prior exposure to space physics the magnetopause location can be viewed as a pressure balance between the dynamic pressure of the solar wind and the ... | [['integrating', 'areas', 'of', 'current', 'research', 'into', 'undergraduate', 'physics', 'labs', 'can', 'be', 'a', 'difficult', 'task', 'the', 'location', 'of', 'the', 'magnetopause', 'is', 'one', 'problem', 'that', 'can', 'be', 'examined', 'with', 'no', 'prior', 'exposure', 'to', 'space', 'physics', 'the', 'magnetop... | [-0.03461622483720464, 0.10781805293850047, -0.10969732106424683, 0.1071179024105476, -0.12065660623710386, -0.117779509549237, 0.05032798276121212, 0.3747431478840261, -0.2894294507308932, -0.4353173979180903, 0.07759035203879129, -0.24904117077465884, -0.08546541710884488, 0.23921756819467838, -0.041249494922678334, ... |
706.1986 | Electronic band structure and carrier effective mass in calcium
aluminates | First-principles electronic band structure investigations of five compounds
of the CaO-Al2O3 family, 3CaO.Al2O3, 12CaO.7Al2O3, CaO.Al2O3, CaO.2Al2O3 and
CaO.6Al2O3, as well as CaO and alpha-, theta- and kappa-Al2O3 are performed. We
find that the conduction band in the complex oxides is formed from the oxygen
antibon... | cond-mat.mtrl-sci | firstprinciples electronic band structure investigations of five compounds of the caoal2o3 family 3caoal2o3 12cao7al2o3 caoal2o3 cao2al2o3 and cao6al2o3 as well as cao and alpha theta and kappaal2o3 are performed we find that the conduction band in the complex oxides is formed from the oxygen antibonding pstates and al... | [['firstprinciples', 'electronic', 'band', 'structure', 'investigations', 'of', 'five', 'compounds', 'of', 'the', 'caoal2o3', 'family', '3caoal2o3', '12cao7al2o3', 'caoal2o3', 'cao2al2o3', 'and', 'cao6al2o3', 'as', 'well', 'as', 'cao', 'and', 'alpha', 'theta', 'and', 'kappaal2o3', 'are', 'performed', 'we', 'find', 'tha... | [-0.14153445463856323, 0.19186330827161377, 0.005489165649602288, 0.04349049441991251, 0.004463643950753306, -0.11394091189038336, 0.10113281702005975, 0.4248298237982549, -0.2513730884447955, -0.3281900211841914, 0.01770450363523866, -0.3294782318632331, -0.13066972239890642, 0.13903629506954499, 0.048337479730610526,... |
706.1987 | Dynamics of the solar chromosphere. V. High-frequency modulation in
ultraviolet image sequences from TRACE | We search for signatures of high-frequency oscillations in the upper solar
photosphere and low chromosphere in the context of acoustic heating of outer
stellar atmospheres. We use ultraviolet image sequences of a quiet center-disk
area from the Transition Region and Coronal Explorer (TRACE) mission which were
taken w... | astro-ph | we search for signatures of highfrequency oscillations in the upper solar photosphere and low chromosphere in the context of acoustic heating of outer stellar atmospheres we use ultraviolet image sequences of a quiet centerdisk area from the transition region and coronal explorer trace mission which were taken with str... | [['we', 'search', 'for', 'signatures', 'of', 'highfrequency', 'oscillations', 'in', 'the', 'upper', 'solar', 'photosphere', 'and', 'low', 'chromosphere', 'in', 'the', 'context', 'of', 'acoustic', 'heating', 'of', 'outer', 'stellar', 'atmospheres', 'we', 'use', 'ultraviolet', 'image', 'sequences', 'of', 'a', 'quiet', 'c... | [-0.0983997890689352, 0.15047802953449718, -0.02754408751934534, 0.11351888426725054, -0.09606172533494828, -0.0765765669857501, 0.03840402831519896, 0.41749974716367433, -0.2095382613779293, -0.34533613210442127, 0.10313395551565918, -0.27839770402829345, -0.08156914623668854, 0.23374840479118575, -0.07166030994017092... |
706.1988 | Lectures on Astronomy, Astrophysics, and Cosmology | This is a written version of a series of lectures aimed at undergraduate
students in astrophysics/particle theory/particle experiment. We summarize the
important progress made in recent years towards understanding high energy
astrophysical processes and we survey the state of the art regarding the
concordance model o... | physics.ed-ph astro-ph | this is a written version of a series of lectures aimed at undergraduate students in astrophysicsparticle theoryparticle experiment we summarize the important progress made in recent years towards understanding high energy astrophysical processes and we survey the state of the art regarding the concordance model of cos... | [['this', 'is', 'a', 'written', 'version', 'of', 'a', 'series', 'of', 'lectures', 'aimed', 'at', 'undergraduate', 'students', 'in', 'astrophysicsparticle', 'theoryparticle', 'experiment', 'we', 'summarize', 'the', 'important', 'progress', 'made', 'in', 'recent', 'years', 'towards', 'understanding', 'high', 'energy', 'a... | [-0.08439016549686051, 0.08415431849172582, -0.12721465793235795, 0.0758498121133965, -0.09530397998573988, -0.0677164208913303, 0.006108350444423116, 0.3070803405109631, -0.17473703309002778, -0.3782481892925242, 0.1089204708063651, -0.2822428277147043, -0.08943753924382769, 0.21761568329479222, -0.06629985483710776, ... |
706.1989 | Interplay and optimization of decoherence mechanisms in the optical
control of spin quantum bits implemented on a semiconductor quantum dot | We study the influence of the environment on an optically induced rotation of
a single electron spin in a charged semiconductor quantum dot. We analyze the
decoherence mechanisms resulting from the dynamical lattice response to the
charge evolution induced in a trion-based optical spin control scheme.
Moreover, we st... | cond-mat.mes-hall quant-ph | we study the influence of the environment on an optically induced rotation of a single electron spin in a charged semiconductor quantum dot we analyze the decoherence mechanisms resulting from the dynamical lattice response to the charge evolution induced in a trionbased optical spin control scheme moreover we study th... | [['we', 'study', 'the', 'influence', 'of', 'the', 'environment', 'on', 'an', 'optically', 'induced', 'rotation', 'of', 'a', 'single', 'electron', 'spin', 'in', 'a', 'charged', 'semiconductor', 'quantum', 'dot', 'we', 'analyze', 'the', 'decoherence', 'mechanisms', 'resulting', 'from', 'the', 'dynamical', 'lattice', 'res... | [-0.16956495863293136, 0.1966116835100072, -0.0262718301512732, 0.03058759139923856, 0.054285261000714395, -0.13376591387801334, 0.07759343065352232, 0.3826128185595855, -0.26925435930121044, -0.2775475483941884, 0.046465275513801016, -0.2572576491208362, -0.10555142360115963, 0.2343415512649481, -0.006103068231297118,... |
706.199 | Applying Extensive Air Shower Universality to Ground Detector Data | Air shower universality states that the electromagnetic part of
hadron-induced extensive air showers (EAS) can be completely described in terms
of the primary energy and shower age. In addition, simulations show that the
muon part is well characterized by an overall normalization which depends on
the primary particle... | astro-ph hep-ex | air shower universality states that the electromagnetic part of hadroninduced extensive air showers eas can be completely described in terms of the primary energy and shower age in addition simulations show that the muon part is well characterized by an overall normalization which depends on the primary particle and ha... | [['air', 'shower', 'universality', 'states', 'that', 'the', 'electromagnetic', 'part', 'of', 'hadroninduced', 'extensive', 'air', 'showers', 'eas', 'can', 'be', 'completely', 'described', 'in', 'terms', 'of', 'the', 'primary', 'energy', 'and', 'shower', 'age', 'in', 'addition', 'simulations', 'show', 'that', 'the', 'mu... | [-0.04952868362216605, 0.27342156767884157, -0.07682681674036898, 0.13721350004018007, 0.01203722937858289, 0.015419226336609764, -0.06279177797871843, 0.39219448561828163, -0.2366841128768073, -0.3990336886040636, 0.035166514448139854, -0.28391415677657444, -0.059930955770319885, 0.14698866473333239, 0.041961968684396... |
706.1991 | Antiproliferative MCR peptides block physical interaction of insulin
with retinoblastoma protein (RB) in human lung cancer cells | Fifteen years ago, a structural analysis of the hormone insulin and the
retinoblastoma tumor suppressor protein (RB) revealed that they may physically
interact with one another. Subsequently, an RB peptide corresponding to the
proposed RB binding site for insulin was found to recognize full-length insulin
in vitro. A... | q-bio.SC q-bio.BM | fifteen years ago a structural analysis of the hormone insulin and the retinoblastoma tumor suppressor protein rb revealed that they may physically interact with one another subsequently an rb peptide corresponding to the proposed rb binding site for insulin was found to recognize fulllength insulin in vitro as part of... | [['fifteen', 'years', 'ago', 'a', 'structural', 'analysis', 'of', 'the', 'hormone', 'insulin', 'and', 'the', 'retinoblastoma', 'tumor', 'suppressor', 'protein', 'rb', 'revealed', 'that', 'they', 'may', 'physically', 'interact', 'with', 'one', 'another', 'subsequently', 'an', 'rb', 'peptide', 'corresponding', 'to', 'the... | [-0.04008285863632669, 0.12642820877874877, 0.005144499142521194, 0.030444624523158742, -0.01432784114565168, -0.17604864158221528, 0.08500272866647628, 0.392096966401353, -0.2063777447725106, -0.2550592199946214, 0.03864884714741737, -0.25338679722103313, -0.22912101992386386, 0.1721810615893469, -0.08058315796975463,... |
706.1992 | Masses and decay modes of charmonia using a confinement model | The masses of charmonium s and p-states, pseudoscalar and vector decay
constants, leptonic, hadronic as well as radiative decay widths for charmonia
have been computed in the framework of extended harmonic confinement model
without any additional parameters. The outcome in comparison with other
contemporary theoretic... | hep-ph | the masses of charmonium s and pstates pseudoscalar and vector decay constants leptonic hadronic as well as radiative decay widths for charmonia have been computed in the framework of extended harmonic confinement model without any additional parameters the outcome in comparison with other contemporary theoretical and ... | [['the', 'masses', 'of', 'charmonium', 's', 'and', 'pstates', 'pseudoscalar', 'and', 'vector', 'decay', 'constants', 'leptonic', 'hadronic', 'as', 'well', 'as', 'radiative', 'decay', 'widths', 'for', 'charmonia', 'have', 'been', 'computed', 'in', 'the', 'framework', 'of', 'extended', 'harmonic', 'confinement', 'model',... | [0.011092034922912717, 0.2341401176992804, -0.01375959082506597, 0.14318482340546324, -0.052863377630710605, -0.17653251606971027, 0.03476054927334189, 0.4274657168984413, -0.16616785377264023, -0.26895745016634465, -0.005759504153393209, -0.2755573481321335, 0.022507262360304595, 0.15575226612854748, 0.141235677171498... |
706.1993 | On pathwise uniqueness for reflecting Brownian motion in $C^{1+\gamma}$
domains | Pathwise uniqueness holds for the Skorokhod stochastic differential equation
in $C^{1+\gamma}$ domains in $\mathbb{R}^d$ for $\gamma >1/2$ and $d\geq3$.
| math.PR | pathwise uniqueness holds for the skorokhod stochastic differential equation in c1gamma domains in mathbbrd for gamma 12 and dgeq3 | [['pathwise', 'uniqueness', 'holds', 'for', 'the', 'skorokhod', 'stochastic', 'differential', 'equation', 'in', 'c1gamma', 'domains', 'in', 'mathbbrd', 'for', 'gamma', '12', 'and', 'dgeq3']] | [-0.1338442036587941, 0.022049825442464727, -0.025308775960614805, 0.13916062798939252, -0.07519816254314624, -0.15875705978588053, 0.009020434447417134, 0.33177970153720754, -0.36730108267970774, -0.09315597599274233, 0.1264398514023541, -0.3276836909353733, -0.02347193726975667, 0.20384030151916177, -0.15969347110704... |
706.1994 | On the Quantum Jarzynski Identity | In this note, we will discuss how to compactly express and prove the
Jarzynski identity for an open quantum system with dissipative dynamics. We
will avoid explicitly measuring the work directly, which is tantamount to
continuously monitoring the system, and instead measure the heat flow from the
environment. We repr... | cond-mat.stat-mech quant-ph | in this note we will discuss how to compactly express and prove the jarzynski identity for an open quantum system with dissipative dynamics we will avoid explicitly measuring the work directly which is tantamount to continuously monitoring the system and instead measure the heat flow from the environment we represent t... | [['in', 'this', 'note', 'we', 'will', 'discuss', 'how', 'to', 'compactly', 'express', 'and', 'prove', 'the', 'jarzynski', 'identity', 'for', 'an', 'open', 'quantum', 'system', 'with', 'dissipative', 'dynamics', 'we', 'will', 'avoid', 'explicitly', 'measuring', 'the', 'work', 'directly', 'which', 'is', 'tantamount', 'to... | [-0.11939875832758844, 0.10279336297699046, -0.10952130789810326, 0.0513279207443702, -0.045961625466588885, -0.13914591308566743, 0.01980632855265867, 0.3692181838210672, -0.3380189758550841, -0.2407922588987276, 0.11770829217130085, -0.2865253735682927, -0.16010411891620607, 0.20406202514423058, -0.06034075479255989,... |
706.1995 | The Leo Elliptical NGC 3379: A Metal-Poor Halo Emerges | We have used the ACS camera on HST to obtain (V,I) photometry for 5300
red-giant stars in the halo of the dominant Leo-group member NGC 3379, a galaxy
usually regarded as a classic normal giant elliptical. We use this sample of
stars to derive the metallicity distribution function (MDF) for its outer-halo
field stars... | astro-ph | we have used the acs camera on hst to obtain vi photometry for 5300 redgiant stars in the halo of the dominant leogroup member ngc 3379 a galaxy usually regarded as a classic normal giant elliptical we use this sample of stars to derive the metallicity distribution function mdf for its outerhalo field stars 33 kpc from... | [['we', 'have', 'used', 'the', 'acs', 'camera', 'on', 'hst', 'to', 'obtain', 'vi', 'photometry', 'for', '5300', 'redgiant', 'stars', 'in', 'the', 'halo', 'of', 'the', 'dominant', 'leogroup', 'member', 'ngc', '3379', 'a', 'galaxy', 'usually', 'regarded', 'as', 'a', 'classic', 'normal', 'giant', 'elliptical', 'we', 'use'... | [-0.03412185678924073, 0.0582058077218802, -0.12035790809800159, 0.09554171855997329, -0.13192761621827878, -0.056664299062499986, 0.03623440621535562, 0.4662881494546522, -0.11412371923300739, -0.33742106754543283, 0.0035956237820236516, -0.3022624006384312, -0.017644991324236404, 0.20632963320431746, -0.0833965958446... |
706.1996 | Planet RB: a personal contribution to a proteomic map of human
retinoblastoma protein | As I compress on the canvas of a few pages here major results of my research
on the retinoblastoma tumor suppressor protein (RB) spreading over the past 15
years, an exciting picture emerges on this unique host molecule which surpasses
in its complexity even that of the most capable viral proteins known to date.
Acco... | q-bio.BM q-bio.SC | as i compress on the canvas of a few pages here major results of my research on the retinoblastoma tumor suppressor protein rb spreading over the past 15 years an exciting picture emerges on this unique host molecule which surpasses in its complexity even that of the most capable viral proteins known to date accordingl... | [['as', 'i', 'compress', 'on', 'the', 'canvas', 'of', 'a', 'few', 'pages', 'here', 'major', 'results', 'of', 'my', 'research', 'on', 'the', 'retinoblastoma', 'tumor', 'suppressor', 'protein', 'rb', 'spreading', 'over', 'the', 'past', '15', 'years', 'an', 'exciting', 'picture', 'emerges', 'on', 'this', 'unique', 'host',... | [-0.043049758560985765, 0.14784391507192277, -0.0063848000128644625, 0.015583924057155654, -0.052492830518318656, -0.15357485502450305, 0.10071669440329462, 0.3766704390139936, -0.25813413694782134, -0.2829672603613951, 0.06840144443687039, -0.2782516755623283, -0.1821873717632919, 0.20053784997964447, -0.0691770226044... |
706.1997 | HST Photometry for the Halo Stars in the Leo Elliptical NGC 3377 | We have used the ACS camera on HST to obtain (V,I) photometry for 57,000
red-giant stars in the halo of the Leo elliptical NGC 3377. We use this sample
of stars to derive the metallicity distribution function (MDF) for its halo
field stars, and comment on its chemical evolution history compared with both
larger and s... | astro-ph | we have used the acs camera on hst to obtain vi photometry for 57000 redgiant stars in the halo of the leo elliptical ngc 3377 we use this sample of stars to derive the metallicity distribution function mdf for its halo field stars and comment on its chemical evolution history compared with both larger and smaller e ga... | [['we', 'have', 'used', 'the', 'acs', 'camera', 'on', 'hst', 'to', 'obtain', 'vi', 'photometry', 'for', '57000', 'redgiant', 'stars', 'in', 'the', 'halo', 'of', 'the', 'leo', 'elliptical', 'ngc', '3377', 'we', 'use', 'this', 'sample', 'of', 'stars', 'to', 'derive', 'the', 'metallicity', 'distribution', 'function', 'mdf... | [-0.02518327271536691, 0.07929080593635263, -0.1204007769653496, 0.094444638377657, -0.14683339711943214, -0.04290384074071577, 0.08038036441818501, 0.451611758035142, -0.08735795509270854, -0.38260677975874086, -0.021057505063557375, -0.3009455836581765, 0.0037981934074196033, 0.23507486233817568, -0.08484809411068757... |
706.1998 | Proposal for a two-channel quantum dot setup: Prediction for the
capacitance lineshape | We have made a detailed proposal for a two-channel quantum dot setup. The
energy scales in the problem are such that we are able to make connection with
the two-channel Anderson model, which, in spite of being well-known in the
context of heavy-Fermion systems remained theoretically elusive until recently
and lacked ... | cond-mat.mes-hall cond-mat.str-el | we have made a detailed proposal for a twochannel quantum dot setup the energy scales in the problem are such that we are able to make connection with the twochannel anderson model which in spite of being wellknown in the context of heavyfermion systems remained theoretically elusive until recently and lacked a mesosco... | [['we', 'have', 'made', 'a', 'detailed', 'proposal', 'for', 'a', 'twochannel', 'quantum', 'dot', 'setup', 'the', 'energy', 'scales', 'in', 'the', 'problem', 'are', 'such', 'that', 'we', 'are', 'able', 'to', 'make', 'connection', 'with', 'the', 'twochannel', 'anderson', 'model', 'which', 'in', 'spite', 'of', 'being', 'w... | [-0.13637597162801868, 0.0666040646896223, -0.10180119651321991, 0.05394986240814129, -0.05633564670689595, -0.20472376718400762, 0.033772789320956245, 0.3762247710942458, -0.22300556900863272, -0.28999248839532715, 0.05714580284294266, -0.28658424196048427, -0.1607051049478543, 0.2402965861151759, -0.04878422735521617... |
706.1999 | Spacetime Indeterminacy and Holographic Noise | A new kind of quantum indeterminacy of transverse position is shown to arise
from quantum degrees of freedom of spacetime, based on the assumption that
classical trajectories can be defined no better than the diffraction limit of
Planck scale waves. Indeterminacy of the angular orientation of particle
trajectories du... | gr-qc astro-ph hep-th | a new kind of quantum indeterminacy of transverse position is shown to arise from quantum degrees of freedom of spacetime based on the assumption that classical trajectories can be defined no better than the diffraction limit of planck scale waves indeterminacy of the angular orientation of particle trajectories due to... | [['a', 'new', 'kind', 'of', 'quantum', 'indeterminacy', 'of', 'transverse', 'position', 'is', 'shown', 'to', 'arise', 'from', 'quantum', 'degrees', 'of', 'freedom', 'of', 'spacetime', 'based', 'on', 'the', 'assumption', 'that', 'classical', 'trajectories', 'can', 'be', 'defined', 'no', 'better', 'than', 'the', 'diffrac... | [-0.17824472062135543, 0.2025293621252884, -0.11916877131758107, 0.10508710413076286, -0.09434209872395857, -0.12326047042812649, -0.009820739903827072, 0.2731378089913444, -0.25341058401957256, -0.2879152737394277, 0.033630452457047696, -0.28647456844526065, -0.08539857483481535, 0.20746230553895412, -0.06521482168810... |
706.2 | General Depolarized Pure States: Identification and Properties | The Schmidt decomposition is an important tool in the study of quantum
systems especially for the quantification of the entanglement of pure states.
However, the Schmidt decomposition is only unique for bipartite pure states,
and some multipartite pure states. Here a generalized Schmidt decomposition is
given for sta... | quant-ph | the schmidt decomposition is an important tool in the study of quantum systems especially for the quantification of the entanglement of pure states however the schmidt decomposition is only unique for bipartite pure states and some multipartite pure states here a generalized schmidt decomposition is given for states wh... | [['the', 'schmidt', 'decomposition', 'is', 'an', 'important', 'tool', 'in', 'the', 'study', 'of', 'quantum', 'systems', 'especially', 'for', 'the', 'quantification', 'of', 'the', 'entanglement', 'of', 'pure', 'states', 'however', 'the', 'schmidt', 'decomposition', 'is', 'only', 'unique', 'for', 'bipartite', 'pure', 'st... | [-0.10713687913012829, 0.15707609174792692, -0.10927975552138125, 0.06300615490354265, 0.009132466193675847, -0.13869784457037354, 0.003666659464395725, 0.28511005828138625, -0.24356356865754075, -0.2579906338337108, 0.14049458799314327, -0.24946520799346786, -0.13791668357899284, 0.18836775405498424, -0.02904960601175... |
706.2001 | Polymers in a vacuum | In a variety of situations, isolated polymer molecules are found in a vacuum
and here we examine their properties. Angular momentum conservation is shown to
significantly alter the average size of a chain and its conservation is only
broken slowly by thermal radiation. The time autocorrelation for monomer
position os... | cond-mat.soft cond-mat.stat-mech | in a variety of situations isolated polymer molecules are found in a vacuum and here we examine their properties angular momentum conservation is shown to significantly alter the average size of a chain and its conservation is only broken slowly by thermal radiation the time autocorrelation for monomer position oscilla... | [['in', 'a', 'variety', 'of', 'situations', 'isolated', 'polymer', 'molecules', 'are', 'found', 'in', 'a', 'vacuum', 'and', 'here', 'we', 'examine', 'their', 'properties', 'angular', 'momentum', 'conservation', 'is', 'shown', 'to', 'significantly', 'alter', 'the', 'average', 'size', 'of', 'a', 'chain', 'and', 'its', 'c... | [-0.21989788695868542, 0.26679968850358443, -0.05909961013684926, 0.09806896051775445, -0.016630174855099007, -0.16767610061146757, -0.01957658630083589, 0.3889984587536139, -0.31116935847436683, -0.27529500863131356, 0.06072062427547815, -0.2786942020387334, -0.04670390658737982, 0.15930802596404273, 0.035868874668855... |
706.2002 | Neutron Transfer Reactions for Deformed Nuclei Using Sturmian Basis | We study the spin-parity distribution P(J$^{\pi}$,E) of $^{156}$Gd excited
states above the neutron separation energy that are expected to be populated
via the neutron pickup reaction $^{157}$Gd($^{3}$He,$^{4}$He)$^{156}$Gd. In
general, modeling of the spin-parity distribution is important for the
applicability of th... | nucl-th | we study the spinparity distribution pjpie of 156gd excited states above the neutron separation energy that are expected to be populated via the neutron pickup reaction 157gd3he4he156gd in general modeling of the spinparity distribution is important for the applicability of the surrogate reaction technique as a method ... | [['we', 'study', 'the', 'spinparity', 'distribution', 'pjpie', 'of', '156gd', 'excited', 'states', 'above', 'the', 'neutron', 'separation', 'energy', 'that', 'are', 'expected', 'to', 'be', 'populated', 'via', 'the', 'neutron', 'pickup', 'reaction', '157gd3he4he156gd', 'in', 'general', 'modeling', 'of', 'the', 'spinpari... | [-0.06744467042780553, 0.17125753892872195, -0.06168232127786793, 0.0741639082096159, -0.011556482684010496, -0.08758310590010997, 0.04581536071804854, 0.30528469982628637, -0.21441700444198572, -0.24600447986203317, -0.04656001483090222, -0.31529538829166154, -0.011848112095433933, 0.14544434279400426, 0.0906594773848... |
706.2003 | Numerical Measurements of the Spectrum in Magnetohydrodynamic Turbulence | We report the results of an extensive set of direct numerical simulations of
forced, incompressible, magnetohydrodynamic turbulence with a strong guide
field. The aim is to resolve the controversy regarding the power law exponent
(\alpha, say) of the field perpendicular energy spectrum E(k_\perp) \propto
k_\perp ^ {\... | astro-ph nlin.CD physics.flu-dyn physics.plasm-ph | we report the results of an extensive set of direct numerical simulations of forced incompressible magnetohydrodynamic turbulence with a strong guide field the aim is to resolve the controversy regarding the power law exponent alpha say of the field perpendicular energy spectrum ek_perp propto k_perp alpha the two main... | [['we', 'report', 'the', 'results', 'of', 'an', 'extensive', 'set', 'of', 'direct', 'numerical', 'simulations', 'of', 'forced', 'incompressible', 'magnetohydrodynamic', 'turbulence', 'with', 'a', 'strong', 'guide', 'field', 'the', 'aim', 'is', 'to', 'resolve', 'the', 'controversy', 'regarding', 'the', 'power', 'law', '... | [-0.17026403502871593, 0.07511877917980504, -0.07775918705156074, 0.03647389222751372, -0.08654168572053701, -0.10029012919791663, -0.01760057914070785, 0.36690689182529845, -0.238998823830237, -0.3147033543876508, 0.06439223846246023, -0.24033369516400854, -0.08497717259839797, 0.23785242564044892, 0.04176883057225496... |
706.2004 | Bifurcations and chaos in semiconductor superlattices with a tilted
magnetic field | We study the effects of dissipation on electron transport in a semiconductor
superlattice with an applied bias voltage and a magnetic field that is tilted
relative to the superlattice axis.In previous work, we showed that although the
applied fields are stationary,they act like a THz plane wave, which strongly
couple... | cond-mat.other | we study the effects of dissipation on electron transport in a semiconductor superlattice with an applied bias voltage and a magnetic field that is tilted relative to the superlattice axisin previous work we showed that although the applied fields are stationarythey act like a thz plane wave which strongly couples the ... | [['we', 'study', 'the', 'effects', 'of', 'dissipation', 'on', 'electron', 'transport', 'in', 'a', 'semiconductor', 'superlattice', 'with', 'an', 'applied', 'bias', 'voltage', 'and', 'a', 'magnetic', 'field', 'that', 'is', 'tilted', 'relative', 'to', 'the', 'superlattice', 'axisin', 'previous', 'work', 'we', 'showed', '... | [-0.2079023691018977, 0.17936227835389218, -0.05410292697082956, 0.05341063421582248, -0.028242802833639353, -0.11459391636058822, 0.02892643702658201, 0.34481719593584004, -0.29472297698508293, -0.2654230759445844, 0.031689195538222394, -0.24950815776017926, -0.165011450444581, 0.23029721057641186, -0.0078633052856145... |
706.2005 | QCD String as Vortex String in Seiberg-Dual Theory | We construct a classical vortex string solution in a Seiberg-dual theory of
N=1 supersymmetric SO(N_c) QCD which flows to a confining phase. We claim that
this vortex string is a QCD string, as previouly argued by M.Strassler. In
SO(N_c) QCD, it is known that stable QCD strings exist even in the presence of
dynamical... | hep-th | we construct a classical vortex string solution in a seibergdual theory of n1 supersymmetric son_c qcd which flows to a confining phase we claim that this vortex string is a qcd string as previouly argued by mstrassler in son_c qcd it is known that stable qcd strings exist even in the presence of dynamical quarks we sh... | [['we', 'construct', 'a', 'classical', 'vortex', 'string', 'solution', 'in', 'a', 'seibergdual', 'theory', 'of', 'n1', 'supersymmetric', 'son_c', 'qcd', 'which', 'flows', 'to', 'a', 'confining', 'phase', 'we', 'claim', 'that', 'this', 'vortex', 'string', 'is', 'a', 'qcd', 'string', 'as', 'previouly', 'argued', 'by', 'm... | [-0.17620934404884325, 0.2736332025520052, -0.15422441178199017, 0.1513375497765303, -0.02338581701571291, -0.11457774090531254, 0.03692786390963716, 0.3221859460075696, -0.17470431752559362, -0.1631374955741745, 0.07324848769790013, -0.25857991026714444, -0.15284932048455108, 0.058807561096424855, -0.02626031078398227... |
706.2006 | The Nature of the Far-UV Break in the Energy Distribution of Quasars | A prominent continuum steepening is observed in quasar energy distributions
near 1100A. We review possible interpretations for the physical origin of this
so-called far-UV break.
| astro-ph | a prominent continuum steepening is observed in quasar energy distributions near 1100a we review possible interpretations for the physical origin of this socalled faruv break | [['a', 'prominent', 'continuum', 'steepening', 'is', 'observed', 'in', 'quasar', 'energy', 'distributions', 'near', '1100a', 'we', 'review', 'possible', 'interpretations', 'for', 'the', 'physical', 'origin', 'of', 'this', 'socalled', 'faruv', 'break']] | [-0.06874361284077167, 0.07361926421523095, -0.1136529221199453, 0.22670083358883858, -0.13291950043290854, -0.09693058321252465, 0.024033785872161387, 0.4486970674991608, -0.17213215712457897, -0.27439628932625054, 0.0002648518746718764, -0.2636207652837038, -0.07623769037425518, 0.09851150296628475, -0.04262757092714... |
706.2007 | Reconstruction of metabolic networks from high-throughput metabolite
profiling data: in silico analysis of red blood cell metabolism | We investigate the ability of algorithms developed for reverse engineering of
transcriptional regulatory networks to reconstruct metabolic networks from
high-throughput metabolite profiling data. For this, we generate synthetic
metabolic profiles for benchmarking purposes based on a well-established model
for red blo... | q-bio.MN | we investigate the ability of algorithms developed for reverse engineering of transcriptional regulatory networks to reconstruct metabolic networks from highthroughput metabolite profiling data for this we generate synthetic metabolic profiles for benchmarking purposes based on a wellestablished model for red blood cel... | [['we', 'investigate', 'the', 'ability', 'of', 'algorithms', 'developed', 'for', 'reverse', 'engineering', 'of', 'transcriptional', 'regulatory', 'networks', 'to', 'reconstruct', 'metabolic', 'networks', 'from', 'highthroughput', 'metabolite', 'profiling', 'data', 'for', 'this', 'we', 'generate', 'synthetic', 'metaboli... | [-0.038227716484985685, 0.02248846017316265, -0.007504261582035501, 0.14062812508804337, -0.05994018276643781, -0.1536915458361003, 0.051851481544117464, 0.4339200226976624, -0.2641264768317342, -0.2957085166346141, 0.06455919817243791, -0.24873417940096193, -0.24628342744753748, 0.2763791254321816, -0.0575809235254056... |
706.2008 | DOT tomography of the solar atmosphere. IV. Magnetic patches in
internetwork areas | We use G-band and Ca II H image sequences from the Dutch Open Telescope (DOT)
to study magnetic elements that appear as bright points in internetwork parts
of the quiet solar photosphere and chromosphere. We find that many of these
bright points appear recurrently with varying intensity and horizontal motion
within l... | astro-ph | we use gband and ca ii h image sequences from the dutch open telescope dot to study magnetic elements that appear as bright points in internetwork parts of the quiet solar photosphere and chromosphere we find that many of these bright points appear recurrently with varying intensity and horizontal motion within longerl... | [['we', 'use', 'gband', 'and', 'ca', 'ii', 'h', 'image', 'sequences', 'from', 'the', 'dutch', 'open', 'telescope', 'dot', 'to', 'study', 'magnetic', 'elements', 'that', 'appear', 'as', 'bright', 'points', 'in', 'internetwork', 'parts', 'of', 'the', 'quiet', 'solar', 'photosphere', 'and', 'chromosphere', 'we', 'find', '... | [-0.12730719085211736, 0.19581610325024545, 0.017663724232723353, 0.09680194277180372, -0.02424840291581341, -0.05390208586710539, 0.0236477458927726, 0.43192743787705135, -0.2390528966495971, -0.3591125309603275, 0.07819211292233536, -0.2568385436260787, -0.12510900008475176, 0.18109258291495106, -0.02907539814214365,... |
706.2009 | Satellite Galaxies and Fossil Groups in the Millennium Simulation | We use a semianalytic galaxy catalogue constructed from the Millennium
Simulation to study the satellites of isolated galaxies in the LCDM cosmogony.
This sample (~80,000$ bright primaries, surrounded by ~178,000 satellites)
allows the characterization, with minimal statistical uncertainty, of the
dynamical propertie... | astro-ph | we use a semianalytic galaxy catalogue constructed from the millennium simulation to study the satellites of isolated galaxies in the lcdm cosmogony this sample 80000 bright primaries surrounded by 178000 satellites allows the characterization with minimal statistical uncertainty of the dynamical properties of satellit... | [['we', 'use', 'a', 'semianalytic', 'galaxy', 'catalogue', 'constructed', 'from', 'the', 'millennium', 'simulation', 'to', 'study', 'the', 'satellites', 'of', 'isolated', 'galaxies', 'in', 'the', 'lcdm', 'cosmogony', 'this', 'sample', '80000', 'bright', 'primaries', 'surrounded', 'by', '178000', 'satellites', 'allows',... | [-0.1030375235017809, 0.06456150456313695, -0.1299471692844093, 0.12432230285177116, -0.10794394307909076, -0.042349210341675575, 0.011446331875334842, 0.3908193297615713, -0.1744318016183873, -0.39309818479323794, 0.035765169578713965, -0.28595545873915895, -0.03990955875818983, 0.18595754638697734, -0.043825759039963... |
706.201 | Information-theoretic security without an honest majority | We present six multiparty protocols with information-theoretic security that
tolerate an arbitrary number of corrupt participants. All protocols assume
pairwise authentic private channels and a broadcast channel (in a single case,
we require a simultaneous broadcast channel). We give protocols for veto, vote,
anonymo... | cs.CR | we present six multiparty protocols with informationtheoretic security that tolerate an arbitrary number of corrupt participants all protocols assume pairwise authentic private channels and a broadcast channel in a single case we require a simultaneous broadcast channel we give protocols for veto vote anonymous bit tra... | [['we', 'present', 'six', 'multiparty', 'protocols', 'with', 'informationtheoretic', 'security', 'that', 'tolerate', 'an', 'arbitrary', 'number', 'of', 'corrupt', 'participants', 'all', 'protocols', 'assume', 'pairwise', 'authentic', 'private', 'channels', 'and', 'a', 'broadcast', 'channel', 'in', 'a', 'single', 'case'... | [-0.26999918412249746, 0.02714151615885824, -0.04425987353276336, 0.018783812392816953, -0.03134566560136468, -0.3788618856643358, 0.19666115133522805, 0.41110966586915965, -0.23485498098536195, -0.30046238944855297, 0.06629073612779128, -0.26658412650374047, -0.04791054147128225, 0.13101802118321398, -0.16929196982299... |
706.2011 | Dynamic fibrils in H-alpha and C IV | Aim: To study the interaction of the solar chromosphere with the transition
region, in particular active-region jets in the transition region and their
relation to chromospheric fibrils. Methods: We carefully align image sequences
taken simultaneously in C IV with the Transition Region and Coronal Explorer
and in H-a... | astro-ph | aim to study the interaction of the solar chromosphere with the transition region in particular activeregion jets in the transition region and their relation to chromospheric fibrils methods we carefully align image sequences taken simultaneously in c iv with the transition region and coronal explorer and in halpha wit... | [['aim', 'to', 'study', 'the', 'interaction', 'of', 'the', 'solar', 'chromosphere', 'with', 'the', 'transition', 'region', 'in', 'particular', 'activeregion', 'jets', 'in', 'the', 'transition', 'region', 'and', 'their', 'relation', 'to', 'chromospheric', 'fibrils', 'methods', 'we', 'carefully', 'align', 'image', 'seque... | [-0.02948054226991885, 0.16128352084334063, 0.020648052642012343, 0.14067998668452836, -0.10020644200746627, -0.12143421604243272, 0.0004760648069136283, 0.5298467431765269, -0.2076310880619156, -0.3153218641767607, 0.06646588668432635, -0.29115188531577585, -0.13270393742919517, 0.1366745822254897, -0.0306157878255950... |
706.2012 | Spinons and triplons in spatially anisotropic frustrated
antiferromagnets | The search for elementary excitations with fractional quantum numbers is a
central challenge in modern condensed matter physics. We explore the
possibility in a realistic model for several materials, the spin-1/2 spatially
anisotropic frustrated Heisenberg antiferromagnet in two dimensions. By
restricting the Hilbert... | cond-mat.str-el cond-mat.stat-mech | the search for elementary excitations with fractional quantum numbers is a central challenge in modern condensed matter physics we explore the possibility in a realistic model for several materials the spin12 spatially anisotropic frustrated heisenberg antiferromagnet in two dimensions by restricting the hilbert space ... | [['the', 'search', 'for', 'elementary', 'excitations', 'with', 'fractional', 'quantum', 'numbers', 'is', 'a', 'central', 'challenge', 'in', 'modern', 'condensed', 'matter', 'physics', 'we', 'explore', 'the', 'possibility', 'in', 'a', 'realistic', 'model', 'for', 'several', 'materials', 'the', 'spin12', 'spatially', 'an... | [-0.17972152043865727, 0.28654450659534114, -0.03249430686035859, 0.13048670446899321, -0.058344092873656855, -0.16847156560397708, 0.017249738080759667, 0.34739716899847345, -0.25926917493177043, -0.2619169825205712, 0.0032744179637770035, -0.3524968738335052, -0.08248838223558518, 0.16592510252459242, 0.1039617675389... |
706.2013 | A transient Markov chain with finitely many cutpoints | We give an example of a transient reversible Markov chain that almost surely
has only a finite number of cutpoints. We explain how this is relevant to a
conjecture of Diaconis and Freedman and a question of Kaimanovich. We also
answer Kaimanovich's question when the Markov chain is a nearest-neighbor
random walk on a... | math.PR | we give an example of a transient reversible markov chain that almost surely has only a finite number of cutpoints we explain how this is relevant to a conjecture of diaconis and freedman and a question of kaimanovich we also answer kaimanovichs question when the markov chain is a nearestneighbor random walk on a tree | [['we', 'give', 'an', 'example', 'of', 'a', 'transient', 'reversible', 'markov', 'chain', 'that', 'almost', 'surely', 'has', 'only', 'a', 'finite', 'number', 'of', 'cutpoints', 'we', 'explain', 'how', 'this', 'is', 'relevant', 'to', 'a', 'conjecture', 'of', 'diaconis', 'and', 'freedman', 'and', 'a', 'question', 'of', '... | [-0.13776159272952512, 0.20097678369096353, -0.07948700694197958, 0.11312060411384499, -0.09199636795304038, -0.1656778314404867, 0.13127302347936415, 0.40932672382755714, -0.2916772803122347, -0.2068542465271259, 0.13510366657071493, -0.26210850950923154, -0.1674919533458623, 0.1669441188092936, -0.09730739862742749, ... |
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