id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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710.1853 | Engineering many-body quantum dynamics by disorder | Going beyond the currently investigated regimes in experiments on quantum
transport of ultracold atoms in disordered potentials, we predict a crossover
between regular and quantum-chaotic dynamics when varying the strength of
disorder. Our spectral approach is based on the Bose-Hubbard model describing
interacting at... | cond-mat.dis-nn cond-mat.stat-mech | going beyond the currently investigated regimes in experiments on quantum transport of ultracold atoms in disordered potentials we predict a crossover between regular and quantumchaotic dynamics when varying the strength of disorder our spectral approach is based on the bosehubbard model describing interacting atoms in... | [['going', 'beyond', 'the', 'currently', 'investigated', 'regimes', 'in', 'experiments', 'on', 'quantum', 'transport', 'of', 'ultracold', 'atoms', 'in', 'disordered', 'potentials', 'we', 'predict', 'a', 'crossover', 'between', 'regular', 'and', 'quantumchaotic', 'dynamics', 'when', 'varying', 'the', 'strength', 'of', '... | [-0.11356917156458453, 0.2336665140234946, -0.061147490807343274, 0.05001976833259112, 0.06769725449245285, -0.19184981697572417, 0.05351679327460811, 0.35552285416166723, -0.24478035859395691, -0.24200446789877283, 0.006794046742818606, -0.31342908710149336, -0.14198151340616155, 0.17237007585469127, 0.071151176708991... |
710.1854 | Area distances of Convex Plane Curves and Improper Affine Spheres | The area distance to a convex plane curve is an important concept in computer
vision. In this paper we describe a strong link between area distances and
improper affine spheres. This link makes possible a better understanding of
both theories. The concepts of the theory of affine spheres lead to a new
definition of a... | math.DG | the area distance to a convex plane curve is an important concept in computer vision in this paper we describe a strong link between area distances and improper affine spheres this link makes possible a better understanding of both theories the concepts of the theory of affine spheres lead to a new definition of an are... | [['the', 'area', 'distance', 'to', 'a', 'convex', 'plane', 'curve', 'is', 'an', 'important', 'concept', 'in', 'computer', 'vision', 'in', 'this', 'paper', 'we', 'describe', 'a', 'strong', 'link', 'between', 'area', 'distances', 'and', 'improper', 'affine', 'spheres', 'this', 'link', 'makes', 'possible', 'a', 'better', ... | [-0.1743188619312614, 0.01869316710743611, -0.12366357420317152, 0.06983454681043937, -0.1201867653113423, -0.11798734676017604, 0.06349543303679299, 0.39588912647932467, -0.30050550695659234, -0.2571353018283844, 0.08336547873867205, -0.24333517096297005, -0.2086868200056029, 0.22812107401062745, -0.16732672523387304,... |
710.1855 | Divergent estimation error in portfolio optimization and in linear
regression | The problem of estimation error in portfolio optimization is discussed, in
the limit where the portfolio size N and the sample size T go to infinity such
that their ratio is fixed. The estimation error strongly depends on the ratio
N/T and diverges for a critical value of this parameter. This divergence is the
manife... | q-fin.PM physics.soc-ph | the problem of estimation error in portfolio optimization is discussed in the limit where the portfolio size n and the sample size t go to infinity such that their ratio is fixed the estimation error strongly depends on the ratio nt and diverges for a critical value of this parameter this divergence is the manifestatio... | [['the', 'problem', 'of', 'estimation', 'error', 'in', 'portfolio', 'optimization', 'is', 'discussed', 'in', 'the', 'limit', 'where', 'the', 'portfolio', 'size', 'n', 'and', 'the', 'sample', 'size', 't', 'go', 'to', 'infinity', 'such', 'that', 'their', 'ratio', 'is', 'fixed', 'the', 'estimation', 'error', 'strongly', '... | [-0.10514356544976976, 0.09247037335878586, -0.036819380184659, 0.07294586080639083, -0.0678926687511545, -0.12208075167126015, 0.08152234339851792, 0.30722194008466575, -0.2990937255510763, -0.32604889569318846, 0.15811588645016603, -0.2925946915193516, -0.1389014615282072, 0.20410535285765885, -0.10844935468953698, 0... |
710.1856 | Impact of Dark Matter Annihilation on the High-Redshift Intergalactic
Medium | We reexamine the impact of dark matter (DM) annihilation on the intergalactic
medium, taking into account the clumping of DM particles. We find that energy
injection from the annihilation of the thermal relic DM particles may
significantly raise the gas temperature at high redshifts and leave a strong
imprint on the ... | astro-ph | we reexamine the impact of dark matter dm annihilation on the intergalactic medium taking into account the clumping of dm particles we find that energy injection from the annihilation of the thermal relic dm particles may significantly raise the gas temperature at high redshifts and leave a strong imprint on the cosmol... | [['we', 'reexamine', 'the', 'impact', 'of', 'dark', 'matter', 'dm', 'annihilation', 'on', 'the', 'intergalactic', 'medium', 'taking', 'into', 'account', 'the', 'clumping', 'of', 'dm', 'particles', 'we', 'find', 'that', 'energy', 'injection', 'from', 'the', 'annihilation', 'of', 'the', 'thermal', 'relic', 'dm', 'particl... | [-0.09879057698004369, 0.20748914874369098, -0.11689086255907852, 0.15556685663183892, -0.10133486790882965, -0.04601143787725158, 0.012309992470608284, 0.34356269472709267, -0.22704012445624797, -0.35065574715695075, -0.008744150991000796, -0.29103243704484677, 0.06542726960634032, 0.1823443552561765, 0.10978680248222... |
710.1857 | Concentric Characterization and Classification of Complex Network Nodes:
Theory and Application to Institutional Collaboration | Differently from theoretical scale-free networks, most of real networks
present multi-scale behavior with nodes structured in different types of
functional groups and communities. While the majority of approaches for
classification of nodes in a complex network has relied on local measurements
of the topology/connect... | physics.soc-ph physics.data-an | differently from theoretical scalefree networks most of real networks present multiscale behavior with nodes structured in different types of functional groups and communities while the majority of approaches for classification of nodes in a complex network has relied on local measurements of the topologyconnectivity a... | [['differently', 'from', 'theoretical', 'scalefree', 'networks', 'most', 'of', 'real', 'networks', 'present', 'multiscale', 'behavior', 'with', 'nodes', 'structured', 'in', 'different', 'types', 'of', 'functional', 'groups', 'and', 'communities', 'while', 'the', 'majority', 'of', 'approaches', 'for', 'classification', ... | [-0.13563484165933914, 0.04949064068690253, -0.06466566054829552, 0.06580751794778432, -0.04672513433130613, -0.11773705103208461, 0.07286488246753227, 0.36127501736821915, -0.2480681148426811, -0.3477975418851808, 0.07948887160879774, -0.3040839444292942, -0.1848842648705613, 0.16023956985979262, -0.03627838789786134,... |
710.1858 | Traveling waves in a one-dimensional random medium | We consider solutions of a scalar reaction-diffusion equation of the ignition
type with a random, stationary and ergodic reaction rate. We show that
solutions of the Cauchy problem spread with a deterministic rate in the long
time limit. We also establish existence of generalized random traveling waves
and of transit... | math.AP math.PR | we consider solutions of a scalar reactiondiffusion equation of the ignition type with a random stationary and ergodic reaction rate we show that solutions of the cauchy problem spread with a deterministic rate in the long time limit we also establish existence of generalized random traveling waves and of transition fr... | [['we', 'consider', 'solutions', 'of', 'a', 'scalar', 'reactiondiffusion', 'equation', 'of', 'the', 'ignition', 'type', 'with', 'a', 'random', 'stationary', 'and', 'ergodic', 'reaction', 'rate', 'we', 'show', 'that', 'solutions', 'of', 'the', 'cauchy', 'problem', 'spread', 'with', 'a', 'deterministic', 'rate', 'in', 't... | [-0.19447396590628407, 0.1325942810032178, -0.04575365259026347, 0.06204451092264869, -0.03305279974910346, -0.13627034619619902, 0.07237985420718111, 0.30563368553465065, -0.3013681106946685, -0.1411857738921588, 0.1269606691996821, -0.2834795288233595, -0.18104236048053612, 0.1448652684688568, 0.014491401942954823, 0... |
710.1859 | Noether Charge and Black Hole Entropy in Modified Theories of Gravity | The entropy of black holes in modified theories of gravity is examined in the
Palatini formalism using the Noether Charge approach. It is shown that, if the
gravitational coupling constant is properly identified, the entropy of a black
hole is one-quarter of the horizon area in f(R) theories coupled to conformally
in... | gr-qc | the entropy of black holes in modified theories of gravity is examined in the palatini formalism using the noether charge approach it is shown that if the gravitational coupling constant is properly identified the entropy of a black hole is onequarter of the horizon area in fr theories coupled to conformally invariant ... | [['the', 'entropy', 'of', 'black', 'holes', 'in', 'modified', 'theories', 'of', 'gravity', 'is', 'examined', 'in', 'the', 'palatini', 'formalism', 'using', 'the', 'noether', 'charge', 'approach', 'it', 'is', 'shown', 'that', 'if', 'the', 'gravitational', 'coupling', 'constant', 'is', 'properly', 'identified', 'the', 'e... | [-0.16910575884415907, 0.16125074675410697, -0.09833699307852874, 0.1416739178950795, -0.0731362648377264, -0.1829297408004533, -0.09335784880763472, 0.27764712186978646, -0.16252580874909958, -0.26411372359359153, 0.0645694426698524, -0.33154090411995574, -0.13466554603763614, 0.1434730841709232, -0.09600812137230402,... |
710.186 | Spitzer Observations of NGC 1333: A Study of Structure and Evolution in
a Nearby Embedded Cluster | We present a comprehensive analysis of structure in the young, embedded
cluster, NGC 1333 using members identified with Spitzer and 2MASS photometry
based on their IR-excess emission. In total, 137 members are identified in this
way, composed of 39 protostars and 98 more evolved pre-main sequence stars with
disks. Of... | astro-ph | we present a comprehensive analysis of structure in the young embedded cluster ngc 1333 using members identified with spitzer and 2mass photometry based on their irexcess emission in total 137 members are identified in this way composed of 39 protostars and 98 more evolved premain sequence stars with disks of the latte... | [['we', 'present', 'a', 'comprehensive', 'analysis', 'of', 'structure', 'in', 'the', 'young', 'embedded', 'cluster', 'ngc', '1333', 'using', 'members', 'identified', 'with', 'spitzer', 'and', '2mass', 'photometry', 'based', 'on', 'their', 'irexcess', 'emission', 'in', 'total', '137', 'members', 'are', 'identified', 'in... | [-0.07866894460221374, 0.12246552160377178, -0.08777185745323852, 0.07227287992949034, -0.05081037399092262, -0.058611021105510495, 0.05351479898733184, 0.47815514155293687, -0.16942733708613864, -0.34826345852343366, 0.04578825846753413, -0.28276771747429547, -0.034947865594100826, 0.1508357341414618, -0.0550378160793... |
710.1861 | Dissociative electron attachment to the H2O molecule. II. Nuclear
dynamics on coupled electronic surfaces within the local complex potential
model | We report the results of a first-principles study of dissociative electron
attachment to H2O. The cross sections are obtained from nuclear dynamics
calculations carried out in full dimensionality within the local complex
potential model by using the multi-configuration time-dependent Hartree method.
The calculations ... | physics.chem-ph | we report the results of a firstprinciples study of dissociative electron attachment to h2o the cross sections are obtained from nuclear dynamics calculations carried out in full dimensionality within the local complex potential model by using the multiconfiguration timedependent hartree method the calculations employ ... | [['we', 'report', 'the', 'results', 'of', 'a', 'firstprinciples', 'study', 'of', 'dissociative', 'electron', 'attachment', 'to', 'h2o', 'the', 'cross', 'sections', 'are', 'obtained', 'from', 'nuclear', 'dynamics', 'calculations', 'carried', 'out', 'in', 'full', 'dimensionality', 'within', 'the', 'local', 'complex', 'po... | [-0.08852383804088997, 0.09017167701130205, -0.03168695162970982, 0.09295628642543453, 0.016137734335454214, -0.13499988303277533, 0.03911699871451869, 0.39979750195765773, -0.22235037260984927, -0.2833251816710468, 0.03268565192638299, -0.2625825588478346, -0.10884840807014796, 0.13168849368079033, 0.08464203861466679... |
710.1862 | Primes, Pi, and Irrationality Measure | A folklore proof of Euclid's theorem on the infinitude of primes uses the
Euler product and the irrationality of $\zeta(2) = \pi^2/6$. A quantified form
of Euclid's Theorem is Bertrand's postulate $p_{n+1} < 2p_n$. By quantifying
the folklore proof using an irrationality measure for $6/\pi^2$, we give a
proof (commun... | math.NT math.GM | a folklore proof of euclids theorem on the infinitude of primes uses the euler product and the irrationality of zeta2 pi26 a quantified form of euclids theorem is bertrands postulate p_n1 2p_n by quantifying the folklore proof using an irrationality measure for 6pi2 we give a proof communicated to paulo ribenboim in 20... | [['a', 'folklore', 'proof', 'of', 'euclids', 'theorem', 'on', 'the', 'infinitude', 'of', 'primes', 'uses', 'the', 'euler', 'product', 'and', 'the', 'irrationality', 'of', 'zeta2', 'pi26', 'a', 'quantified', 'form', 'of', 'euclids', 'theorem', 'is', 'bertrands', 'postulate', 'p_n1', '2p_n', 'by', 'quantifying', 'the', '... | [-0.1957991926309963, 0.03989650270499017, -0.2315960801128919, 0.17611651073869627, -0.1043926575453952, -0.1428683182069411, 0.11713622317959865, 0.1285149884565423, -0.2171375018854936, -0.28995954788600403, 0.06628881435026415, -0.27112161786838745, -0.10465416862086083, 0.24697398606998225, -0.17099732522231836, -... |
710.1863 | The Detection of Molecular Gas in the Outskirts of NGC 6946 | We present the results of a search for molecular gas emission via the CO line
in the far outer disk of the nearby spiral, NGC 6946. The positions targeted
were chosen to lie on or near previously-identified outer disk HII regions.
Molecular gas was clearly detected out to 1.3 R$_{25}$, with a further
tentative detect... | astro-ph | we present the results of a search for molecular gas emission via the co line in the far outer disk of the nearby spiral ngc 6946 the positions targeted were chosen to lie on or near previouslyidentified outer disk hii regions molecular gas was clearly detected out to 13 r_25 with a further tentative detection at 14 r_... | [['we', 'present', 'the', 'results', 'of', 'a', 'search', 'for', 'molecular', 'gas', 'emission', 'via', 'the', 'co', 'line', 'in', 'the', 'far', 'outer', 'disk', 'of', 'the', 'nearby', 'spiral', 'ngc', '6946', 'the', 'positions', 'targeted', 'were', 'chosen', 'to', 'lie', 'on', 'or', 'near', 'previouslyidentified', 'ou... | [-0.0840890115485853, 0.03837255487794273, 0.009270988105185283, 0.03925538092709271, -0.0074152038024833345, -0.021634714904087034, 0.08453082859554702, 0.4419753131616837, -0.1288448321673082, -0.3313299362921411, 0.06045848525508906, -0.27346381081185145, -0.016336011575760357, 0.15075162779925402, 0.044160261738357... |
710.1864 | Reparameterization invariance of NRQED self-energy corrections and
improved theory for excited D states in hydrogenlike systems | Canonically, the quantum electrodynamic radiative corrections in bound
systems have been evaluated in photon energy regularization, i. e. using a
noncovariant overlapping parameter that separates the high-energy relativistic
scales of the virtual quanta from the nonrelativistic domain. Here, we
calculate the higher-o... | hep-ph | canonically the quantum electrodynamic radiative corrections in bound systems have been evaluated in photon energy regularization i e using a noncovariant overlapping parameter that separates the highenergy relativistic scales of the virtual quanta from the nonrelativistic domain here we calculate the higherorder corre... | [['canonically', 'the', 'quantum', 'electrodynamic', 'radiative', 'corrections', 'in', 'bound', 'systems', 'have', 'been', 'evaluated', 'in', 'photon', 'energy', 'regularization', 'i', 'e', 'using', 'a', 'noncovariant', 'overlapping', 'parameter', 'that', 'separates', 'the', 'highenergy', 'relativistic', 'scales', 'of'... | [-0.08025075227161434, 0.1978981152707798, -0.09965153147301106, 0.10604319824275743, -0.02679578255792366, -0.13007743687969503, 0.01024713371793313, 0.34004818975368395, -0.2091056652210444, -0.308295789270479, -0.039930264637413844, -0.2943544705163374, -0.07170185520287568, 0.18848046085962625, 0.036179910222434, 0... |
710.1865 | Invariant Yang-Mills connections over Non-Reductive Pseudo-Riemannian
Homogeneous Spaces | We study invariant gauge fields over the 4-dimensional non-reductive
pseudo-Riemannian homogeneous spaces G/K recently classified by Fels & Renner
(2006). Given H compact semi-simple, classification results are obtained for
principal H-bundles over G/K admitting: (1) a G-action (by bundle
automorphisms) projecting to... | math-ph math.MP | we study invariant gauge fields over the 4dimensional nonreductive pseudoriemannian homogeneous spaces gk recently classified by fels renner 2006 given h compact semisimple classification results are obtained for principal hbundles over gk admitting 1 a gaction by bundle automorphisms projecting to left multiplication ... | [['we', 'study', 'invariant', 'gauge', 'fields', 'over', 'the', '4dimensional', 'nonreductive', 'pseudoriemannian', 'homogeneous', 'spaces', 'gk', 'recently', 'classified', 'by', 'fels', 'renner', '2006', 'given', 'h', 'compact', 'semisimple', 'classification', 'results', 'are', 'obtained', 'for', 'principal', 'hbundle... | [-0.21696959431907525, 0.06569151893297442, -0.04951147933089949, 0.06515224727570448, -0.1220186667168232, -0.16228640039435813, -0.024223086316211347, 0.36163707207055895, -0.2713523597421395, -0.2040478159418569, 0.11578666405751001, -0.2639564776794911, -0.179984604891041, 0.1713679665335397, -0.09563712178086914, ... |
710.1866 | Can we see naked singularities? | We study singularities which can form in a spherically symmetric
gravitational collapse of a general matter field obeying weak energy condition.
We show that no energy can reach an outside observer from a null naked
singularity. That means they will not be a serious threat to the Cosmic
Censorship Conjecture (CCC). F... | gr-qc astro-ph hep-th | we study singularities which can form in a spherically symmetric gravitational collapse of a general matter field obeying weak energy condition we show that no energy can reach an outside observer from a null naked singularity that means they will not be a serious threat to the cosmic censorship conjecture ccc for the ... | [['we', 'study', 'singularities', 'which', 'can', 'form', 'in', 'a', 'spherically', 'symmetric', 'gravitational', 'collapse', 'of', 'a', 'general', 'matter', 'field', 'obeying', 'weak', 'energy', 'condition', 'we', 'show', 'that', 'no', 'energy', 'can', 'reach', 'an', 'outside', 'observer', 'from', 'a', 'null', 'naked'... | [-0.18549067081585235, 0.11434804477812577, -0.1564203898971235, 0.16145161462502852, -0.11628097138184655, -0.16579197471063317, -0.017652887518384626, 0.3190243366906153, -0.19506843639205076, -0.23097736387613363, 0.10607666961108667, -0.2795262190359478, -0.0711726550923361, 0.1799983893870376, -0.0749698634525495,... |
710.1867 | Impact of non-standard neutrino interactions on future oscillation
experiments | We study the performance of reactor and superbeam neutrino experiments in the
presence of non-standard interactions (NSI). We find that for some non-standard
terms, reactor and superbeam experiments would yield conflicting result in the
theta-13 determination, while in other cases, they may agree well with each
other... | hep-ph | we study the performance of reactor and superbeam neutrino experiments in the presence of nonstandard interactions nsi we find that for some nonstandard terms reactor and superbeam experiments would yield conflicting result in the theta13 determination while in other cases they may agree well with each other but the re... | [['we', 'study', 'the', 'performance', 'of', 'reactor', 'and', 'superbeam', 'neutrino', 'experiments', 'in', 'the', 'presence', 'of', 'nonstandard', 'interactions', 'nsi', 'we', 'find', 'that', 'for', 'some', 'nonstandard', 'terms', 'reactor', 'and', 'superbeam', 'experiments', 'would', 'yield', 'conflicting', 'result'... | [-0.075161425746046, 0.16195353238605137, -0.011040005462682741, 0.0960790247461477, -0.08673092447827722, -0.13971639517694712, 0.08645013951544844, 0.34909084240017935, -0.22478973690615317, -0.32423524974390516, 0.12377741176033999, -0.33383748609150304, -0.09831759716968896, 0.24472809561560754, -0.0267413980869013... |
710.1868 | Non-perturbative microscopic theory of superconducting fluctuations near
a quantum critical point | We consider an inhomogeneous anisotropic gap superconductor in the vicinity
of the quantum critical point, where the transition temperature is suppressed
to zero by disorder. Starting with the BCS Hamiltonian, we derive the
Ginzburg-Landau action for the superconducting order parameter. It is shown
that the critical ... | cond-mat.supr-con cond-mat.dis-nn | we consider an inhomogeneous anisotropic gap superconductor in the vicinity of the quantum critical point where the transition temperature is suppressed to zero by disorder starting with the bcs hamiltonian we derive the ginzburglandau action for the superconducting order parameter it is shown that the critical theory ... | [['we', 'consider', 'an', 'inhomogeneous', 'anisotropic', 'gap', 'superconductor', 'in', 'the', 'vicinity', 'of', 'the', 'quantum', 'critical', 'point', 'where', 'the', 'transition', 'temperature', 'is', 'suppressed', 'to', 'zero', 'by', 'disorder', 'starting', 'with', 'the', 'bcs', 'hamiltonian', 'we', 'derive', 'the'... | [-0.1684156599633783, 0.20015003860701175, -0.08690169112484776, 0.061325165859078254, -0.038677235606474424, -0.1647789538654844, 0.10500387461438089, 0.2731366815317548, -0.21970224615678274, -0.22167954333074225, -0.0033742207412482397, -0.33594968170066575, -0.14503152098171831, 0.17097075265999673, 0.0400474951077... |
710.1869 | Flavor from Minimal Flavor Violation & a Viable Randall-Sundrum Model | We present a variant of the warped extra dimension, Randall-Sundrum (RS),
framework which is based on five dimensional (5D) minimal flavor violation
(MFV), in which the only sources of flavor breaking are two 5D anarchic Yukawa
matrices. The Yukawa matrices also control the bulk masses, which are
responsible for the ... | hep-ph | we present a variant of the warped extra dimension randallsundrum rs framework which is based on five dimensional 5d minimal flavor violation mfv in which the only sources of flavor breaking are two 5d anarchic yukawa matrices the yukawa matrices also control the bulk masses which are responsible for the resulting flav... | [['we', 'present', 'a', 'variant', 'of', 'the', 'warped', 'extra', 'dimension', 'randallsundrum', 'rs', 'framework', 'which', 'is', 'based', 'on', 'five', 'dimensional', '5d', 'minimal', 'flavor', 'violation', 'mfv', 'in', 'which', 'the', 'only', 'sources', 'of', 'flavor', 'breaking', 'are', 'two', '5d', 'anarchic', 'y... | [-0.1014139402177145, 0.2339271436499732, -0.0029432950043343604, 0.1557789270001598, -0.08384385204392754, -0.1879150075302584, 0.08212161098014224, 0.27655748784153616, -0.22246130055095503, -0.30452170334059125, 0.09786585983907416, -0.22775395119184239, -0.06885863647093987, 0.10370707500696102, 0.00520802296468998... |
710.187 | Lossless Representation of Graphs using Distributions | We consider complete graphs with edge weights and/or node weights taking
values in some set. In the first part of this paper, we show that a large
number of graphs are completely determined, up to isomorphism, by the
distribution of their sub-triangles. In the second part, we propose graph
representations in terms of... | math.CO cs.CV | we consider complete graphs with edge weights andor node weights taking values in some set in the first part of this paper we show that a large number of graphs are completely determined up to isomorphism by the distribution of their subtriangles in the second part we propose graph representations in terms of onedimens... | [['we', 'consider', 'complete', 'graphs', 'with', 'edge', 'weights', 'andor', 'node', 'weights', 'taking', 'values', 'in', 'some', 'set', 'in', 'the', 'first', 'part', 'of', 'this', 'paper', 'we', 'show', 'that', 'a', 'large', 'number', 'of', 'graphs', 'are', 'completely', 'determined', 'up', 'to', 'isomorphism', 'by',... | [-0.13667309247767148, 0.10765341999738112, -0.0055122675131196565, 0.00455226082779953, -0.06983555587332534, -0.07038638981757686, 0.06265752854271103, 0.4052829548311622, -0.3406556949991247, -0.29902063176926713, 0.10058474139431896, -0.30117987833269266, -0.1465187068461724, 0.12831142169787832, -0.070966990775955... |
710.1871 | Entanglement entropy and multifractality at localization transitions | The von Neumann entanglement entropy is a useful measure to characterize a
quantum phase transition. We investigate the non-analyticity of this entropy at
disorder-dominated quantum phase transitions in non-interacting electronic
systems. At these critical points, the von Neumann entropy is determined by the
single p... | cond-mat.mes-hall cond-mat.dis-nn | the von neumann entanglement entropy is a useful measure to characterize a quantum phase transition we investigate the nonanalyticity of this entropy at disorderdominated quantum phase transitions in noninteracting electronic systems at these critical points the von neumann entropy is determined by the single particle ... | [['the', 'von', 'neumann', 'entanglement', 'entropy', 'is', 'a', 'useful', 'measure', 'to', 'characterize', 'a', 'quantum', 'phase', 'transition', 'we', 'investigate', 'the', 'nonanalyticity', 'of', 'this', 'entropy', 'at', 'disorderdominated', 'quantum', 'phase', 'transitions', 'in', 'noninteracting', 'electronic', 's... | [-0.1525909855084207, 0.23284722031810537, -0.1153969500043716, 0.09299657138203307, 0.058231676319757335, -0.1866171562780017, 0.003863036419856004, 0.2682535574780419, -0.273408075937858, -0.1832011206424795, 0.068442196369198, -0.34536047666691816, -0.16096065168340618, 0.15493521251594827, 0.010747667652769731, 0.1... |
710.1872 | Constraining the Mass Profiles of Stellar Systems: Schwarzschild
Modeling of Discrete Velocity Datasets | (ABRIDGED) We present a new Schwarzschild orbit-superposition code designed
to model discrete datasets composed of velocities of individual kinematic
tracers in a dynamical system. This constitutes an extension of previous
implementations that can only address continuous data in the form of (the
moments of) velocity ... | astro-ph | abridged we present a new schwarzschild orbitsuperposition code designed to model discrete datasets composed of velocities of individual kinematic tracers in a dynamical system this constitutes an extension of previous implementations that can only address continuous data in the form of the moments of velocity distribu... | [['abridged', 'we', 'present', 'a', 'new', 'schwarzschild', 'orbitsuperposition', 'code', 'designed', 'to', 'model', 'discrete', 'datasets', 'composed', 'of', 'velocities', 'of', 'individual', 'kinematic', 'tracers', 'in', 'a', 'dynamical', 'system', 'this', 'constitutes', 'an', 'extension', 'of', 'previous', 'implemen... | [-0.1323972738685076, 0.044918046785195245, -0.11523770920059827, 0.0841995035618419, -0.09416421825848659, -0.0891927008410625, 0.03320461488675091, 0.3705834886266895, -0.22869684677363328, -0.3433531958776003, 0.054517744088694316, -0.24634097663424503, -0.06125511166199931, 0.22079512040601648, -0.04838255776454206... |
710.1873 | The scalar perturbation spectral index n_s: WMAP sensitivity to
unresolved point sources | Precision measurement of the scalar perturbation spectral index, n_s, from
the Wilkinson Microwave Anisotropy Probe temperature angular power spectrum
requires the subtraction of unresolved point source power. Here we reconsider
this issue. First, we note a peculiarity in the WMAP temperature likelihood's
response to... | astro-ph | precision measurement of the scalar perturbation spectral index n_s from the wilkinson microwave anisotropy probe temperature angular power spectrum requires the subtraction of unresolved point source power here we reconsider this issue first we note a peculiarity in the wmap temperature likelihoods response to the sou... | [['precision', 'measurement', 'of', 'the', 'scalar', 'perturbation', 'spectral', 'index', 'n_s', 'from', 'the', 'wilkinson', 'microwave', 'anisotropy', 'probe', 'temperature', 'angular', 'power', 'spectrum', 'requires', 'the', 'subtraction', 'of', 'unresolved', 'point', 'source', 'power', 'here', 'we', 'reconsider', 't... | [-0.0754110877653593, 0.09565122937703074, -0.06557718910214311, 0.09630023122934456, -0.11335173333542267, -0.15708977726873438, 0.0528524123963241, 0.3734288464591143, -0.2387759130666209, -0.3444980706526298, 0.06432024594773668, -0.3328684661353353, -0.004646355106786129, 0.1888883542228056, -0.05216649741122109, 0... |
710.1874 | Soft probes of high density QCD physics with CMS | The CMS heavy-ion program will probe QCD matter under extreme conditions. Its
capabilities for the study of global observables and soft probes are described.
| nucl-ex | the cms heavyion program will probe qcd matter under extreme conditions its capabilities for the study of global observables and soft probes are described | [['the', 'cms', 'heavyion', 'program', 'will', 'probe', 'qcd', 'matter', 'under', 'extreme', 'conditions', 'its', 'capabilities', 'for', 'the', 'study', 'of', 'global', 'observables', 'and', 'soft', 'probes', 'are', 'described']] | [-0.09819585511771341, 0.22603791688258448, -0.22033675534961125, 0.15836598739648858, -0.03191337554987209, -0.09403007219467933, -0.0907842389230306, 0.32935464459781844, -0.22504120118295154, -0.2936658753703038, 0.12887190266822776, -0.27491600896852714, 0.05048803969596823, 0.1670422504345576, 0.03725851816125214,... |
710.1875 | Dissipative Strong-Field Electrodynamics | A dissipative Lorentz-covariant Ohm's law which uses only the electromagnetic
degrees of freedom is proposed. For large conductivity, Maxwell equations
equipped with this Ohm's law reduce to the equations of Force-Free
Electrodynamics (FFE) with small dissipative corrections, but only in the
regions where the ideal F... | astro-ph | a dissipative lorentzcovariant ohms law which uses only the electromagnetic degrees of freedom is proposed for large conductivity maxwell equations equipped with this ohms law reduce to the equations of forcefree electrodynamics ffe with small dissipative corrections but only in the regions where the ideal ffe 4current... | [['a', 'dissipative', 'lorentzcovariant', 'ohms', 'law', 'which', 'uses', 'only', 'the', 'electromagnetic', 'degrees', 'of', 'freedom', 'is', 'proposed', 'for', 'large', 'conductivity', 'maxwell', 'equations', 'equipped', 'with', 'this', 'ohms', 'law', 'reduce', 'to', 'the', 'equations', 'of', 'forcefree', 'electrodyna... | [-0.18054450786916815, 0.14829845634884523, -0.03676503444792795, 0.013279138774168297, -0.15752875178166834, -0.16048589955679463, -0.038021965105979716, 0.22344675232641031, -0.2122192993973855, -0.2858125684843933, -0.016017648629981597, -0.2843871657110629, -0.08041418160571427, 0.18405952073822607, -0.042195480744... |
710.1876 | A Possible Periodicity in the Radio Lightcurves of 3C454.3 | During the period 1966.5 - 2006.2 the 15GHz and 8GHz lightcurves of 3C454.3
(z=0.859) show a qsasi-periodicity of ~12.8 yr (~6.9 yr in the rest frame of
the source) with a double-bump structure. This periodic behaviour is
interpreted in terms of a rotating double-jet model in which the two jets are
created from the b... | astro-ph | during the period 19665 20062 the 15ghz and 8ghz lightcurves of 3c4543 z0859 show a qsasiperiodicity of 128 yr 69 yr in the rest frame of the source with a doublebump structure this periodic behaviour is interpreted in terms of a rotating doublejet model in which the two jets are created from the black holes in a binar... | [['during', 'the', 'period', '19665', '20062', 'the', '15ghz', 'and', '8ghz', 'lightcurves', 'of', '3c4543', 'z0859', 'show', 'a', 'qsasiperiodicity', 'of', '128', 'yr', '69', 'yr', 'in', 'the', 'rest', 'frame', 'of', 'the', 'source', 'with', 'a', 'doublebump', 'structure', 'this', 'periodic', 'behaviour', 'is', 'inter... | [-0.16166945681746664, 0.17201115925402927, -0.05632774972362877, 0.0818886442816463, -0.048630009630116926, -0.038558059315807344, 0.021377637324019753, 0.3879155193873007, -0.22727250840900273, -0.33011730182273635, 0.13573615958287927, -0.259059512152754, -0.04581183188289789, 0.22825208674024405, -0.078909493452901... |
710.1877 | Number of Bound States of Schroedinger Operators with Matrix-Valued
Potentials | We give a CLR type bound on the number of bound states of Schroedinger
operators with matrix-valued potentials using the functional integral method of
Lieb. This significantly improves the constant in this inequality obtained
earlier by Hundertmark.
| math-ph math.MP | we give a clr type bound on the number of bound states of schroedinger operators with matrixvalued potentials using the functional integral method of lieb this significantly improves the constant in this inequality obtained earlier by hundertmark | [['we', 'give', 'a', 'clr', 'type', 'bound', 'on', 'the', 'number', 'of', 'bound', 'states', 'of', 'schroedinger', 'operators', 'with', 'matrixvalued', 'potentials', 'using', 'the', 'functional', 'integral', 'method', 'of', 'lieb', 'this', 'significantly', 'improves', 'the', 'constant', 'in', 'this', 'inequality', 'obt... | [-0.11478105043942058, 0.08083550531316448, -0.0829995033406728, 0.03937179169214859, -0.03871263664945759, -0.15881043510209467, 0.09105464116342969, 0.272859184625181, -0.19352620120185451, -0.3225953774778424, 0.04466245247592294, -0.2553073301709987, -0.16955852271938646, 0.20144887258474892, -0.04710414514851731, ... |
710.1878 | \rho D^*D^* vertex from QCD sum rules | We calculate the form factors and the coupling constant in the $\rho D^* D^*$
vertex in the framework of QCD sum rules. We evaluate the three point
correlation functions of the vertex considering both $\rho$ and $D^*$ mesons
off--shell. The form factors obtained are very different but give the same
coupling constant:... | hep-ph | we calculate the form factors and the coupling constant in the rho d d vertex in the framework of qcd sum rules we evaluate the three point correlation functions of the vertex considering both rho and d mesons offshell the form factors obtained are very different but give the same coupling constant g_rho d d 66 pm 031 ... | [['we', 'calculate', 'the', 'form', 'factors', 'and', 'the', 'coupling', 'constant', 'in', 'the', 'rho', 'd', 'd', 'vertex', 'in', 'the', 'framework', 'of', 'qcd', 'sum', 'rules', 'we', 'evaluate', 'the', 'three', 'point', 'correlation', 'functions', 'of', 'the', 'vertex', 'considering', 'both', 'rho', 'and', 'd', 'mes... | [-0.18121044197067304, 0.18293586204117032, -0.0671860251549474, 0.08616343109120786, -0.028676869905173357, -0.1841555604527534, 0.0904413466669724, 0.3357310761553301, -0.20549461200938257, -0.28024925627339053, -0.0030569816608732882, -0.3358559500373585, -0.08205622422482661, 0.06582468157817781, 0.0798581808175839... |
710.1879 | Cyclotomic FFTs with Reduced Additive Complexities Based on a Novel
Common Subexpression Elimination Algorithm | In this paper, we first propose a novel common subexpression elimination
(CSE) algorithm for matrix-vector multiplications over characteristic-2 fields.
As opposed to previously proposed CSE algorithms, which usually focus on
complexity savings due to recurrences of subexpressions, our CSE algorithm
achieves two type... | cs.IT cs.CC math.CO math.IT | in this paper we first propose a novel common subexpression elimination cse algorithm for matrixvector multiplications over characteristic2 fields as opposed to previously proposed cse algorithms which usually focus on complexity savings due to recurrences of subexpressions our cse algorithm achieves two types of compl... | [['in', 'this', 'paper', 'we', 'first', 'propose', 'a', 'novel', 'common', 'subexpression', 'elimination', 'cse', 'algorithm', 'for', 'matrixvector', 'multiplications', 'over', 'characteristic2', 'fields', 'as', 'opposed', 'to', 'previously', 'proposed', 'cse', 'algorithms', 'which', 'usually', 'focus', 'on', 'complexi... | [-0.1328251924926201, 0.00710679241868181, -0.04426198458068271, 0.03485976123823825, -0.10256901875434987, -0.1128389759739218, 0.1002394838796401, 0.3766403572089904, -0.28574877709925045, -0.3558376781329249, 0.11022171226074606, -0.1957793069459432, -0.21379253752859292, 0.2313616555266544, -0.13229791684059705, 0.... |
710.188 | Operator Theory and Complex Geometry | One approach to multivariate operator theory involves concepts and techniques
from algebraic and complex geometry and is formulated in terms of Hilbert
modules. In these notes we provide an introduction to this approach including
many proofs. We are particularly interested in examples related to hermitian
holomorphic... | math.FA math.SP | one approach to multivariate operator theory involves concepts and techniques from algebraic and complex geometry and is formulated in terms of hilbert modules in these notes we provide an introduction to this approach including many proofs we are particularly interested in examples related to hermitian holomorphic vec... | [['one', 'approach', 'to', 'multivariate', 'operator', 'theory', 'involves', 'concepts', 'and', 'techniques', 'from', 'algebraic', 'and', 'complex', 'geometry', 'and', 'is', 'formulated', 'in', 'terms', 'of', 'hilbert', 'modules', 'in', 'these', 'notes', 'we', 'provide', 'an', 'introduction', 'to', 'this', 'approach', ... | [-0.09356782087561441, 0.06644462460984263, -0.034113807852069536, 0.07240984176751226, -0.09153401053044945, -0.1054877581904293, -0.014725102900411003, 0.3714168146097412, -0.2872363330175479, -0.2267934785108082, 0.14292396823390544, -0.2700940799317323, -0.21385670896464337, 0.22466333538953526, -0.1528634924557991... |
710.1881 | Descartes' Rule of Signs by an Easy Induction | If c is a positive number, Descartes' rule of signs implies that multiplying
a polynomial f(x) by c - x introduces an odd number of changes of sign in the
coefficients. We turn this around, proving this fact about sign changes
inductively and deriving Descartes' rule from it.
| math.GM | if c is a positive number descartes rule of signs implies that multiplying a polynomial fx by c x introduces an odd number of changes of sign in the coefficients we turn this around proving this fact about sign changes inductively and deriving descartes rule from it | [['if', 'c', 'is', 'a', 'positive', 'number', 'descartes', 'rule', 'of', 'signs', 'implies', 'that', 'multiplying', 'a', 'polynomial', 'fx', 'by', 'c', 'x', 'introduces', 'an', 'odd', 'number', 'of', 'changes', 'of', 'sign', 'in', 'the', 'coefficients', 'we', 'turn', 'this', 'around', 'proving', 'this', 'fact', 'about'... | [-0.22517503615706524, 0.11405587058911902, -0.06685196489412734, -0.0089071431578672, -0.12244849628273477, -0.18155256181241983, 0.11731061165993835, 0.2928213039611248, -0.3378158875919403, -0.29674688749451267, 0.047107895556341935, -0.265413562851423, -0.17771114227659207, 0.15849956105205606, -0.05824015638295640... |
710.1882 | "Jet-Ridge" effect in heavy ion collisions as a back splash from stopped
parton | I propose a simple explanation of the ``ridge'' seen in the near-side jet
two-particle correlation function in heavy ion collisions at RHIC. This could
be a cumulative shock wave produced in liquid-like matter by an energetic
stopped parton. Splash of liquid in the direction opposite to the fast
penetrating object is... | hep-ph | i propose a simple explanation of the ridge seen in the nearside jet twoparticle correlation function in heavy ion collisions at rhic this could be a cumulative shock wave produced in liquidlike matter by an energetic stopped parton splash of liquid in the direction opposite to the fast penetrating object is a known ef... | [['i', 'propose', 'a', 'simple', 'explanation', 'of', 'the', 'ridge', 'seen', 'in', 'the', 'nearside', 'jet', 'twoparticle', 'correlation', 'function', 'in', 'heavy', 'ion', 'collisions', 'at', 'rhic', 'this', 'could', 'be', 'a', 'cumulative', 'shock', 'wave', 'produced', 'in', 'liquidlike', 'matter', 'by', 'an', 'ener... | [-0.14588555613798754, 0.2446162471509472, -0.18512342424264977, 0.14142795207843717, -0.08254824038062777, -0.07951956222632102, -0.061244762180639165, 0.4162353623977729, -0.2757544606285436, -0.2230978208673852, -0.017187644030366624, -0.2951375035090106, 0.02151056418461459, 0.1193995143686022, 0.046290574337222744... |
710.1883 | R-invariant New Inflation Model vs Supersymmetric Standard Model | We revisit the implications of the R-invariant New Inflation model to the
supersymmetric standard model in light of recent discussion of gravitino
production processes by the decay of the inflaton or the supersymmetry breaking
field. We show that the models with supergravity mediation do not go well with
the R-invari... | hep-ph | we revisit the implications of the rinvariant new inflation model to the supersymmetric standard model in light of recent discussion of gravitino production processes by the decay of the inflaton or the supersymmetry breaking field we show that the models with supergravity mediation do not go well with the rinvariant n... | [['we', 'revisit', 'the', 'implications', 'of', 'the', 'rinvariant', 'new', 'inflation', 'model', 'to', 'the', 'supersymmetric', 'standard', 'model', 'in', 'light', 'of', 'recent', 'discussion', 'of', 'gravitino', 'production', 'processes', 'by', 'the', 'decay', 'of', 'the', 'inflaton', 'or', 'the', 'supersymmetry', 'b... | [-0.09042268311562136, 0.2440048717923565, -0.057796436216716374, 0.15774554408949995, -0.1240208818963857, -0.18614795628439532, -0.004241611065189226, 0.2875849113782543, -0.22768403735832063, -0.34212117349951093, 0.09170207207479916, -0.23451620058387246, -0.09206364717795898, 0.09339408678699011, -0.02969896593430... |
710.1884 | Charmonium Spectroscopy Below Open Flavor Threshold | Latest experimental results in the charmonium spectroscopy below D-barD
breakup threshold are reviewed.
| hep-ex | latest experimental results in the charmonium spectroscopy below dbard breakup threshold are reviewed | [['latest', 'experimental', 'results', 'in', 'the', 'charmonium', 'spectroscopy', 'below', 'dbard', 'breakup', 'threshold', 'are', 'reviewed']] | [-0.05250446795700835, 0.3634833632251964, -0.04030357931668942, 0.19726054313091132, 0.0026306832352509866, -0.164160950252643, 0.12904403458994168, 0.3519937047161735, -0.13535894166964751, -0.17135853563936856, -0.09122847447780749, -0.44460174441337585, 0.019145843716194995, 0.20053632786640754, 0.12688400990849075... |
710.1885 | Initial state dependence in multi-electron threshold ionization of atoms | It is shown that the geometry of multi-electron threshold ionization in atoms
depends on the initial configuration of bound electrons. The reason for this
behavior is found in the stability properties of the classical fixed point of
the equations of motion for multiple threshold fragmentation. Specifically for
three-... | physics.atom-ph | it is shown that the geometry of multielectron threshold ionization in atoms depends on the initial configuration of bound electrons the reason for this behavior is found in the stability properties of the classical fixed point of the equations of motion for multiple threshold fragmentation specifically for threeelectr... | [['it', 'is', 'shown', 'that', 'the', 'geometry', 'of', 'multielectron', 'threshold', 'ionization', 'in', 'atoms', 'depends', 'on', 'the', 'initial', 'configuration', 'of', 'bound', 'electrons', 'the', 'reason', 'for', 'this', 'behavior', 'is', 'found', 'in', 'the', 'stability', 'properties', 'of', 'the', 'classical', ... | [-0.10861509589433789, 0.1778134731377693, -0.0832235510758263, 0.08820457911698465, 0.03868007160316994, -0.09168326204761545, 0.0400198066849856, 0.32881948763029056, -0.23173600710690656, -0.27744593750685453, 0.00626841365567785, -0.2576828631275195, -0.1002508769445914, 0.16925747833274146, 0.058055866390783736, 0... |
710.1886 | On the Spectrum of the Dirichlet Laplacian in a Narrow Strip, II | We consider the Dirichlet Laplacian in a family of narrow unbounded domains.
As the width of these domains goes to 0, we study the asymptotic behavior of
the eigenvalues that lie below the essential spectrum and the asymptotic
behavior of the corresponding eigenfunctions.
| math.SP | we consider the dirichlet laplacian in a family of narrow unbounded domains as the width of these domains goes to 0 we study the asymptotic behavior of the eigenvalues that lie below the essential spectrum and the asymptotic behavior of the corresponding eigenfunctions | [['we', 'consider', 'the', 'dirichlet', 'laplacian', 'in', 'a', 'family', 'of', 'narrow', 'unbounded', 'domains', 'as', 'the', 'width', 'of', 'these', 'domains', 'goes', 'to', '0', 'we', 'study', 'the', 'asymptotic', 'behavior', 'of', 'the', 'eigenvalues', 'that', 'lie', 'below', 'the', 'essential', 'spectrum', 'and', ... | [-0.16524398868340393, 0.07567303684854143, -0.0643764672324408, 0.07811837465783884, -0.08811494676656155, -0.05709390644373935, 0.02070186009933782, 0.33428378715071566, -0.2864759941260482, -0.22059405751006547, 0.152035930180424, -0.32702683137599814, -0.12372290915376398, 0.12396456446325363, -0.010046495232991007... |
710.1887 | The Hubble series: Convergence properties and redshift variables | In cosmography, cosmokinetics, and cosmology it is quite common to encounter
physical quantities expanded as a Taylor series in the cosmological redshift z.
Perhaps the most well-known exemplar of this phenomenon is the Hubble relation
between distance and redshift. However, we now have considerable high-z data
avail... | gr-qc | in cosmography cosmokinetics and cosmology it is quite common to encounter physical quantities expanded as a taylor series in the cosmological redshift z perhaps the most wellknown exemplar of this phenomenon is the hubble relation between distance and redshift however we now have considerable highz data available for ... | [['in', 'cosmography', 'cosmokinetics', 'and', 'cosmology', 'it', 'is', 'quite', 'common', 'to', 'encounter', 'physical', 'quantities', 'expanded', 'as', 'a', 'taylor', 'series', 'in', 'the', 'cosmological', 'redshift', 'z', 'perhaps', 'the', 'most', 'wellknown', 'exemplar', 'of', 'this', 'phenomenon', 'is', 'the', 'hu... | [-0.06013028753543856, 0.08650565875437662, -0.1227789134174481, 0.11070826747258863, -0.11486387625554245, -0.10015137360603157, 0.04962238260745027, 0.3766258774743041, -0.22331892129384137, -0.27131538649707615, 0.1245822227692175, -0.29773278802494024, -0.04763556940200364, 0.21821785538901237, -0.02968061660529575... |
710.1888 | Electric polarizability of the neutron in dynamical quark ensembles | The background field method for measuring the electric polarizability of the
neutron is adapted to the dynamical quark case, resulting in the calculation of
(certain space-time integrals over) three- and four-point functions. Particular
care is taken to disentangle polarizability effects from the effects of
subjectin... | hep-lat | the background field method for measuring the electric polarizability of the neutron is adapted to the dynamical quark case resulting in the calculation of certain spacetime integrals over three and fourpoint functions particular care is taken to disentangle polarizability effects from the effects of subjecting the neu... | [['the', 'background', 'field', 'method', 'for', 'measuring', 'the', 'electric', 'polarizability', 'of', 'the', 'neutron', 'is', 'adapted', 'to', 'the', 'dynamical', 'quark', 'case', 'resulting', 'in', 'the', 'calculation', 'of', 'certain', 'spacetime', 'integrals', 'over', 'three', 'and', 'fourpoint', 'functions', 'pa... | [-0.12168895916851319, 0.23338967110232814, -0.10029465834225487, 0.08734668085083325, -0.08108939024342639, -0.06536263085360153, 0.05439319843730039, 0.33348076843211183, -0.1733755976488085, -0.25616030565098574, 0.01330241279388049, -0.2927778268880818, -0.0376246512827018, 0.16293180304700913, 0.03860255712946958,... |
710.1889 | Understanding Transcriptional Regulation Using De-novo Sequence Motif
Discovery, Network Inference and Interactome Data | Gene regulation is a complex process involving the role of several genomic
elements which work in concert to drive spatio-temporal expression. The
experimental characterization of gene regulatory elements is a very complex and
resource-intensive process. One of the major goals in computational biology is
the \textit{... | q-bio.GN | gene regulation is a complex process involving the role of several genomic elements which work in concert to drive spatiotemporal expression the experimental characterization of gene regulatory elements is a very complex and resourceintensive process one of the major goals in computational biology is the textitinsilico... | [['gene', 'regulation', 'is', 'a', 'complex', 'process', 'involving', 'the', 'role', 'of', 'several', 'genomic', 'elements', 'which', 'work', 'in', 'concert', 'to', 'drive', 'spatiotemporal', 'expression', 'the', 'experimental', 'characterization', 'of', 'gene', 'regulatory', 'elements', 'is', 'a', 'very', 'complex', '... | [-0.07723986648342662, 0.04307819773244796, -0.021990233860816416, 0.06594863380790432, -0.07089010207567005, -0.09409323146091346, 0.060140018358682455, 0.3762270599198391, -0.2632862816795621, -0.30995068676325505, 0.08724725111760297, -0.28171869875886574, -0.23917266043028737, 0.2172726254840089, -0.090258504139360... |
710.189 | Majorana spinors and extended Lorentz symmetry in four-dimensional
theory | An extended local Lorentz symmetry in four-dimensional (4D) theory is
considered. A source of this symmetry is a group of general linear
transformations of four-component Majorana spinors GL(4,M) which is isomorphic
to GL(4,R) and is the covering of an extended Lorentz group in a 6D Minkowski
space M(3,3) including s... | gr-qc | an extended local lorentz symmetry in fourdimensional 4d theory is considered a source of this symmetry is a group of general linear transformations of fourcomponent majorana spinors gl4m which is isomorphic to gl4r and is the covering of an extended lorentz group in a 6d minkowski space m33 including superluminal and ... | [['an', 'extended', 'local', 'lorentz', 'symmetry', 'in', 'fourdimensional', '4d', 'theory', 'is', 'considered', 'a', 'source', 'of', 'this', 'symmetry', 'is', 'a', 'group', 'of', 'general', 'linear', 'transformations', 'of', 'fourcomponent', 'majorana', 'spinors', 'gl4m', 'which', 'is', 'isomorphic', 'to', 'gl4r', 'an... | [-0.17168748011522575, 0.19225418710658357, -0.06315118653844752, 0.06999874762559176, -0.13400218481599482, -0.15038295820199266, -0.10079404027047002, 0.35036097821628975, -0.19614334377142306, -0.26138027471770436, 0.04963924919469784, -0.24460891505959861, -0.15782812901934284, 0.08322082950125732, -0.0573025009626... |
710.1891 | What makes the Crab pulsar shine? | Our high time resolution observations of individual pulses from the Crab
pulsar show that the main pulse and interpulse differ in temporal behavior,
spectral behavior, polarization and dispersion. The main pulse properties are
consistent with one current model of pulsar radio emission, namely, soliton
collapse in str... | astro-ph | our high time resolution observations of individual pulses from the crab pulsar show that the main pulse and interpulse differ in temporal behavior spectral behavior polarization and dispersion the main pulse properties are consistent with one current model of pulsar radio emission namely soliton collapse in strong pla... | [['our', 'high', 'time', 'resolution', 'observations', 'of', 'individual', 'pulses', 'from', 'the', 'crab', 'pulsar', 'show', 'that', 'the', 'main', 'pulse', 'and', 'interpulse', 'differ', 'in', 'temporal', 'behavior', 'spectral', 'behavior', 'polarization', 'and', 'dispersion', 'the', 'main', 'pulse', 'properties', 'a... | [-0.11046019909818741, 0.1508453031719634, -0.10220042673454648, 0.13385584127867, -0.15459800916582797, -0.12376894366179565, 0.012570061015360283, 0.4604623836719177, -0.2622897295337735, -0.2992353461908572, 0.05394578178256228, -0.2556886635756007, -0.03966376711226379, 0.24625632861826682, -0.053623752197767535, -... |
710.1892 | Conjugacy classes of solutions to equations and inequations over
hyperbolic groups | We study conjugacy classes of solutions to systems of equations and
inequations over torsion-free hyperbolic groups, and describe an algorithm to
recognize whether or not there are finitely many conjugacy classes of solutions
to such a system. The class of immutable subgroups of hyperbolic groups is
introduced, which... | math.GR | we study conjugacy classes of solutions to systems of equations and inequations over torsionfree hyperbolic groups and describe an algorithm to recognize whether or not there are finitely many conjugacy classes of solutions to such a system the class of immutable subgroups of hyperbolic groups is introduced which is fu... | [['we', 'study', 'conjugacy', 'classes', 'of', 'solutions', 'to', 'systems', 'of', 'equations', 'and', 'inequations', 'over', 'torsionfree', 'hyperbolic', 'groups', 'and', 'describe', 'an', 'algorithm', 'to', 'recognize', 'whether', 'or', 'not', 'there', 'are', 'finitely', 'many', 'conjugacy', 'classes', 'of', 'solutio... | [-0.18022193010741225, 0.07126941834758327, -0.08571727615263727, 0.06371068771598705, -0.13438467482208377, -0.10707570207563953, -0.006056704927080621, 0.3567779393763178, -0.367077734010915, -0.26989872267909554, 0.1342724229277034, -0.282329464240724, -0.1429682327337408, 0.2544293299595463, -0.15865370384805524, 0... |
710.1893 | Quasistatically varying log-normal distribution in the middle scale
region of Japanese land prices | Employing data on the assessed value of land in 1974--2007 Japan, we exhibit
a quasistatically varying log-normal distribution in the middle scale region.
In the derivation, a Non-Gibrat's law under the detailed quasi-balance is
adopted together with two approximations. The resultant distribution is
power-law with th... | q-fin.ST physics.soc-ph | employing data on the assessed value of land in 19742007 japan we exhibit a quasistatically varying lognormal distribution in the middle scale region in the derivation a nongibrats law under the detailed quasibalance is adopted together with two approximations the resultant distribution is powerlaw with the varying exp... | [['employing', 'data', 'on', 'the', 'assessed', 'value', 'of', 'land', 'in', '19742007', 'japan', 'we', 'exhibit', 'a', 'quasistatically', 'varying', 'lognormal', 'distribution', 'in', 'the', 'middle', 'scale', 'region', 'in', 'the', 'derivation', 'a', 'nongibrats', 'law', 'under', 'the', 'detailed', 'quasibalance', 'i... | [-0.07954216735105556, 0.13180293323066417, -0.13631724613248417, 0.07857069030800594, -0.004287566218552834, -0.07819548329237, 0.0659080206550252, 0.33548990104089277, -0.2541214122464604, -0.33542789020898317, 0.10297516935348215, -0.2721895269385659, -0.06847037147214212, 0.19048913657702138, -0.044908752562051714,... |
710.1894 | Deriving confinement via RG decimations | We present the general framework and building blocks of a recent derivation
of the fact that the SU(2) LGT is in a confining phase for all values of the
coupling $0 < \beta < \infty$, for space-time dimension $d \leq 4$. The method
employs approximate but explicitly computable RG decimations that are shown to
constra... | hep-lat | we present the general framework and building blocks of a recent derivation of the fact that the su2 lgt is in a confining phase for all values of the coupling 0 beta infty for spacetime dimension d leq 4 the method employs approximate but explicitly computable rg decimations that are shown to constrain the exact parti... | [['we', 'present', 'the', 'general', 'framework', 'and', 'building', 'blocks', 'of', 'a', 'recent', 'derivation', 'of', 'the', 'fact', 'that', 'the', 'su2', 'lgt', 'is', 'in', 'a', 'confining', 'phase', 'for', 'all', 'values', 'of', 'the', 'coupling', '0', 'beta', 'infty', 'for', 'spacetime', 'dimension', 'd', 'leq', '... | [-0.1236345934743486, 0.1429256599048695, -0.0626422273808548, 0.05522078011756692, -0.03927287380682611, -0.16098489458495868, 0.06622867290773488, 0.3362782633144267, -0.2419136084757651, -0.26959137570207253, 0.0872782560675464, -0.2637463318820618, -0.1361780980590118, 0.14169873482594855, 0.03495729338566336, 0.03... |
710.1895 | Measurement of correlated b-bbar production in p-pbar collisions at
sqrt(s)=1960GeV | We present a measurement of the correlated $b\bar{b}$ production cross
section. The data used in this analysis were taken with the upgraded CDF
detector (CDF II) at the Fermilab Tevatron collider, and correspond to an
integrated luminosity of 742 pb$^{-1}$. We utilize muon pairs with invariant
mass $5 \leq m_{\mu\mu}... | hep-ex | we present a measurement of the correlated bbarb production cross section the data used in this analysis were taken with the upgraded cdf detector cdf ii at the fermilab tevatron collider and correspond to an integrated luminosity of 742 pb1 we utilize muon pairs with invariant mass 5 leq m_mumu leq 80 gevcc produced b... | [['we', 'present', 'a', 'measurement', 'of', 'the', 'correlated', 'bbarb', 'production', 'cross', 'section', 'the', 'data', 'used', 'in', 'this', 'analysis', 'were', 'taken', 'with', 'the', 'upgraded', 'cdf', 'detector', 'cdf', 'ii', 'at', 'the', 'fermilab', 'tevatron', 'collider', 'and', 'correspond', 'to', 'an', 'int... | [-0.016455050029211722, 0.23895378301378634, -0.04065654258488021, 0.07774723381315526, 0.020656326648275384, -0.1555875500083947, 0.03227476124579209, 0.35367592927984526, -0.13517851380203835, -0.3391374251118205, -0.0629232822197917, -0.449835494496539, 0.14426468330298048, 0.13756779421952967, 0.06283382363006716, ... |
710.1896 | The Long-term Radiative Evolution of Anomalous X-ray Pulsar 1E 2259+586
after its 2002 Outburst | We present an analysis of five X-ray Multi-Mirror Mission (XMM) observations
of the anomalous X-ray pulsar (AXP) 1E 2259+586 taken in 2004 and 2005 during
its relaxation following its 2002 outburst. We compare these data with those of
five previous XMM observations taken in 2002 and 2003, and find the observed
flux d... | astro-ph | we present an analysis of five xray multimirror mission xmm observations of the anomalous xray pulsar axp 1e 2259586 taken in 2004 and 2005 during its relaxation following its 2002 outburst we compare these data with those of five previous xmm observations taken in 2002 and 2003 and find the observed flux decay is well... | [['we', 'present', 'an', 'analysis', 'of', 'five', 'xray', 'multimirror', 'mission', 'xmm', 'observations', 'of', 'the', 'anomalous', 'xray', 'pulsar', 'axp', '1e', '2259586', 'taken', 'in', '2004', 'and', '2005', 'during', 'its', 'relaxation', 'following', 'its', '2002', 'outburst', 'we', 'compare', 'these', 'data', '... | [-0.06195508723951949, 0.09636473019273377, -0.10325376654170382, 0.13444155292445342, -0.10682623567358021, -0.10132979158565257, 0.044854858806537626, 0.4654739734906595, -0.15159626233219667, -0.405538806366255, 0.1335208754188571, -0.3473440275518495, -0.0774047669131779, 0.262339282561618, -0.06995164886912675, 0.... |
710.1897 | Gravitational-Wave Astronomy with Inspiral Signals of Spinning
Compact-Object Binaries | Inspiral signals from binary compact objects (black holes and neutron stars)
are primary targets of the ongoing searches by ground-based gravitational-wave
interferometers (LIGO, Virgo, GEO-600 and TAMA-300). We present
parameter-estimation simulations for inspirals of black-hole--neutron-star
binaries using Markov-c... | astro-ph gr-qc | inspiral signals from binary compact objects black holes and neutron stars are primary targets of the ongoing searches by groundbased gravitationalwave interferometers ligo virgo geo600 and tama300 we present parameterestimation simulations for inspirals of blackholeneutronstar binaries using markovchain montecarlo met... | [['inspiral', 'signals', 'from', 'binary', 'compact', 'objects', 'black', 'holes', 'and', 'neutron', 'stars', 'are', 'primary', 'targets', 'of', 'the', 'ongoing', 'searches', 'by', 'groundbased', 'gravitationalwave', 'interferometers', 'ligo', 'virgo', 'geo600', 'and', 'tama300', 'we', 'present', 'parameterestimation',... | [-0.13243125619080204, 0.11623376106178442, -0.033950205215324575, 0.06620845532743261, -0.0851730786765424, -0.028839299430211005, 0.010219728024318241, 0.4059850573969575, -0.1324997985878816, -0.370360352170582, 0.1070002058467183, -0.3268040465047726, -0.0736300648494552, 0.29020634316301974, 0.013243410686174264, ... |
710.1898 | On moduli spaces of quiver representations associated with dimer models | We give a sufficient condition for the moduli space of quiver representations
associated with a dimer model to be smooth for a general stability parameter.
We also show that the moduli space in this case is a crepant resolution of the
toric variety determined by the Newton polygon of the characteristic
polynomial.
| math.AG | we give a sufficient condition for the moduli space of quiver representations associated with a dimer model to be smooth for a general stability parameter we also show that the moduli space in this case is a crepant resolution of the toric variety determined by the newton polygon of the characteristic polynomial | [['we', 'give', 'a', 'sufficient', 'condition', 'for', 'the', 'moduli', 'space', 'of', 'quiver', 'representations', 'associated', 'with', 'a', 'dimer', 'model', 'to', 'be', 'smooth', 'for', 'a', 'general', 'stability', 'parameter', 'we', 'also', 'show', 'that', 'the', 'moduli', 'space', 'in', 'this', 'case', 'is', 'a',... | [-0.15653668374467927, 0.05861883875555717, -0.12145513392841586, 0.07627810811838852, -0.10451122043797603, -0.13787799351848662, -0.023184014743982025, 0.33947193941387993, -0.33930070289912134, -0.20662293661063394, 0.12399814536463684, -0.128063755396467, -0.17988537721192607, 0.1899210340477741, -0.143656098068906... |
710.1899 | Additional Constants of Motion for a Discretization of the
Calogero--Moser Model | The maximal super-integrability of a discretization of the Calogero--Moser
model introduced by Nijhoff and Pang is presented. An explicit formula for the
additional constants of motion is given.
| nlin.SI | the maximal superintegrability of a discretization of the calogeromoser model introduced by nijhoff and pang is presented an explicit formula for the additional constants of motion is given | [['the', 'maximal', 'superintegrability', 'of', 'a', 'discretization', 'of', 'the', 'calogeromoser', 'model', 'introduced', 'by', 'nijhoff', 'and', 'pang', 'is', 'presented', 'an', 'explicit', 'formula', 'for', 'the', 'additional', 'constants', 'of', 'motion', 'is', 'given']] | [-0.15830256590353592, 0.10699621154396612, -0.07388071220235101, 0.03434037128629695, -0.09078144514933228, -0.1481921548921881, -0.004302752345600831, 0.2547775711864233, -0.2594365637217249, -0.2506384262482503, 0.09486528647227845, -0.2557866493007168, -0.1407627958937415, 0.19412369450687297, -0.12965472751030965,... |
710.19 | Experimentally scalable protocol for identification of correctable codes | The task of finding a correctable encoding that protects against some
physical quantum process is in general hard. Two main obstacles are that an
exponential number of experiments are needed to gain complete information about
the quantum process, and known algorithmic methods for finding correctable
encodings involve... | quant-ph | the task of finding a correctable encoding that protects against some physical quantum process is in general hard two main obstacles are that an exponential number of experiments are needed to gain complete information about the quantum process and known algorithmic methods for finding correctable encodings involve ope... | [['the', 'task', 'of', 'finding', 'a', 'correctable', 'encoding', 'that', 'protects', 'against', 'some', 'physical', 'quantum', 'process', 'is', 'in', 'general', 'hard', 'two', 'main', 'obstacles', 'are', 'that', 'an', 'exponential', 'number', 'of', 'experiments', 'are', 'needed', 'to', 'gain', 'complete', 'information... | [-0.14628134790786304, 0.15037420229131132, -0.04861525614031179, 0.09354592796888367, -0.018609020218718797, -0.18471361288995763, 0.08406678340492532, 0.402683948578183, -0.31278678637571894, -0.26443920046805813, 0.13369747664343545, -0.2377948850057586, -0.16773838777775973, 0.2382595881909067, -0.10133084182649157... |
710.1901 | Robin functions for complex manifolds and applications | We prove a generalization of the second variation formula of the Robin
function associated to a smooth variation of domains in C^N to the case of the
c-Robin function associated to a smooth variation of domains in a complex
manifold M equipped with a Hermitian metric and a smooth, nonnegative function
c. Our purpose ... | math.CV | we prove a generalization of the second variation formula of the robin function associated to a smooth variation of domains in cn to the case of the crobin function associated to a smooth variation of domains in a complex manifold m equipped with a hermitian metric and a smooth nonnegative function c our purpose is tha... | [['we', 'prove', 'a', 'generalization', 'of', 'the', 'second', 'variation', 'formula', 'of', 'the', 'robin', 'function', 'associated', 'to', 'a', 'smooth', 'variation', 'of', 'domains', 'in', 'cn', 'to', 'the', 'case', 'of', 'the', 'crobin', 'function', 'associated', 'to', 'a', 'smooth', 'variation', 'of', 'domains', '... | [-0.16042161417170997, 0.023058755899688636, -0.08372789812160701, 0.055894284395546445, -0.13448776721545472, -0.1389169340169557, 0.00519320652706594, 0.3789061487697792, -0.2937424350529909, -0.20833155716110657, 0.09362182343838646, -0.2329850008870225, -0.1791651282720722, 0.17160101318107238, -0.14052017590757915... |
710.1902 | Decompositions of Laurent polynomials | In the 1920's, Ritt studied the operation of functional composition g o h(x)
= g(h(x)) on complex rational functions. In the case of polynomials, he
described all the ways in which a polynomial can have multiple `prime
factorizations' with respect to this operation. Despite significant effort by
Ritt and others, litt... | math.NT math.AG | in the 1920s ritt studied the operation of functional composition g o hx ghx on complex rational functions in the case of polynomials he described all the ways in which a polynomial can have multiple prime factorizations with respect to this operation despite significant effort by ritt and others little progress has be... | [['in', 'the', '1920s', 'ritt', 'studied', 'the', 'operation', 'of', 'functional', 'composition', 'g', 'o', 'hx', 'ghx', 'on', 'complex', 'rational', 'functions', 'in', 'the', 'case', 'of', 'polynomials', 'he', 'described', 'all', 'the', 'ways', 'in', 'which', 'a', 'polynomial', 'can', 'have', 'multiple', 'prime', 'fac... | [-0.14289298398653044, 0.0288223823118541, -0.09214127857445015, 0.02999465907147775, -0.060525642707943916, -0.10778446786312593, 0.01769139118001072, 0.35583658105590277, -0.31061323049167794, -0.24328554528571356, 0.08152785127361616, -0.26055974097301565, -0.17002387781523995, 0.20462529371596044, -0.11107452344984... |
710.1903 | Cosmic Strings and Weak Gravitational Lensing | We study the deflection of light in the background of a "wiggly" cosmic
string, and investigate whether it is possible to detect cosmic strings by
means of weak gravitational lensing. For straight strings without small-scale
structure there are no signals. In the case of strings with small-scale
structure leading to ... | astro-ph | we study the deflection of light in the background of a wiggly cosmic string and investigate whether it is possible to detect cosmic strings by means of weak gravitational lensing for straight strings without smallscale structure there are no signals in the case of strings with smallscale structure leading to a local g... | [['we', 'study', 'the', 'deflection', 'of', 'light', 'in', 'the', 'background', 'of', 'a', 'wiggly', 'cosmic', 'string', 'and', 'investigate', 'whether', 'it', 'is', 'possible', 'to', 'detect', 'cosmic', 'strings', 'by', 'means', 'of', 'weak', 'gravitational', 'lensing', 'for', 'straight', 'strings', 'without', 'smalls... | [-0.17232305509707396, 0.12525156107618418, -0.09373810043273208, 0.12732748819204667, -0.07889961519672929, -0.041635383950412136, -0.01402871992422251, 0.3628776354362836, -0.2752402220592574, -0.28825504868920593, 0.04525990083264103, -0.2929415767257278, -0.08371165778219432, 0.17931102229668214, 0.0075072253900568... |
710.1904 | Relativistic generalization of Brownian Motion | The relativistic generalization of the Brownian motion is discussed. We show
that the transformation property of the noise term is determined by requiring
for the equilibrium distribution function to be Lorentz invariant, such as the
J\"uttner distribution function. It is shown that this requirement generates an
enta... | hep-th cond-mat.stat-mech hep-ph | the relativistic generalization of the brownian motion is discussed we show that the transformation property of the noise term is determined by requiring for the equilibrium distribution function to be lorentz invariant such as the juttner distribution function it is shown that this requirement generates an entanglemen... | [['the', 'relativistic', 'generalization', 'of', 'the', 'brownian', 'motion', 'is', 'discussed', 'we', 'show', 'that', 'the', 'transformation', 'property', 'of', 'the', 'noise', 'term', 'is', 'determined', 'by', 'requiring', 'for', 'the', 'equilibrium', 'distribution', 'function', 'to', 'be', 'lorentz', 'invariant', 's... | [-0.11717289028366884, 0.16514713598903305, -0.16676853903784203, 0.09481712521340412, -0.05750116377782363, -0.09754836436790916, -0.035278828671345346, 0.35759165023381895, -0.3394672555848956, -0.26649740524590015, 0.042122705674801884, -0.2512104818955637, -0.18558252300493994, 0.14724290418223693, -0.0822545478729... |
710.1905 | Nonextensive hydrodynamics for relativistic heavy-ion collisions | The nonextensive one-dimensional version of a hydrodynamical model for
multiparticle production processes is proposed and discussed. It is based on
nonextensive statistics assumed in the form proposed by Tsallis and
characterized by a nonextensivity parameter $q$. In this formulation the
parameter $q$ characterizes s... | nucl-th hep-ph | the nonextensive onedimensional version of a hydrodynamical model for multiparticle production processes is proposed and discussed it is based on nonextensive statistics assumed in the form proposed by tsallis and characterized by a nonextensivity parameter q in this formulation the parameter q characterizes some speci... | [['the', 'nonextensive', 'onedimensional', 'version', 'of', 'a', 'hydrodynamical', 'model', 'for', 'multiparticle', 'production', 'processes', 'is', 'proposed', 'and', 'discussed', 'it', 'is', 'based', 'on', 'nonextensive', 'statistics', 'assumed', 'in', 'the', 'form', 'proposed', 'by', 'tsallis', 'and', 'characterized... | [-0.0960387836776449, 0.15304324513397596, -0.17563827681066146, 0.08470753809850631, -0.022840048531712644, -0.14788640565881184, -0.022020476216907968, 0.23337750612147923, -0.2569883337228334, -0.24305235759901075, -0.01479136103820377, -0.27938317412177827, -0.08233913483403238, 0.16519349171772021, -0.027270542634... |
710.1906 | The interrelation between the generation of large-scale electric fields
and that of large-scale magnetic fields during inflation | The interrelation between the generation of large-scale electric fields and
that of large-scale magnetic fields due to the breaking of the conformal
invariance of the electromagnetic field in inflationary cosmology is studied.
It is shown that if large-scale magnetic fields with a sufficiently large
amplitude are gen... | astro-ph hep-ph hep-th | the interrelation between the generation of largescale electric fields and that of largescale magnetic fields due to the breaking of the conformal invariance of the electromagnetic field in inflationary cosmology is studied it is shown that if largescale magnetic fields with a sufficiently large amplitude are generated... | [['the', 'interrelation', 'between', 'the', 'generation', 'of', 'largescale', 'electric', 'fields', 'and', 'that', 'of', 'largescale', 'magnetic', 'fields', 'due', 'to', 'the', 'breaking', 'of', 'the', 'conformal', 'invariance', 'of', 'the', 'electromagnetic', 'field', 'in', 'inflationary', 'cosmology', 'is', 'studied'... | [-0.2252530568225105, 0.24046349714267745, -0.022312709277061974, 0.09895039250123736, -0.09004577688158374, -0.05103889422185005, -0.06976255703054063, 0.3557333802319553, -0.2635578109487279, -0.32342800755717166, 0.10801136535624271, -0.177605934450658, -0.16537544169552523, 0.20044842598105028, 0.05079897317065768,... |
710.1907 | Cross sections for meson-meson nonresonant reactions | Meson-meson nonresonant reactions governed by the quark-interchange mechanism
are studied in a potential that is derived from QCD. S-wave elastic phase
shifts for I=2 \pi\pi and I=3/2 K \pi scattering are obtained with wave
functions determined by the central spin-independent term of the potential. The
reactions incl... | nucl-th | mesonmeson nonresonant reactions governed by the quarkinterchange mechanism are studied in a potential that is derived from qcd swave elastic phase shifts for i2 pipi and i32 k pi scattering are obtained with wave functions determined by the central spinindependent term of the potential the reactions include inelastic ... | [['mesonmeson', 'nonresonant', 'reactions', 'governed', 'by', 'the', 'quarkinterchange', 'mechanism', 'are', 'studied', 'in', 'a', 'potential', 'that', 'is', 'derived', 'from', 'qcd', 'swave', 'elastic', 'phase', 'shifts', 'for', 'i2', 'pipi', 'and', 'i32', 'k', 'pi', 'scattering', 'are', 'obtained', 'with', 'wave', 'f... | [-0.1536814209272658, 0.27045417767658364, -0.07741009344787624, 0.08094031645002057, 0.013578870579901073, -0.15990518793842057, 0.05022539280616911, 0.34038073759681237, -0.20580531704581517, -0.21572223069961183, -0.13552754102480927, -0.4053605121249954, -0.030637022094500328, 0.11095247657552439, 0.200645923192496... |
710.1908 | Pseudo-random number generator based on asymptotic deterministic
randomness | An approach to generate the pseudorandom-bit sequence from the asymptotic
deterministic randomness system is proposed in this Letter. We study the
characteristic of multi-value correspondence of the asymptotic deterministic
randomness constructed by the piecewise linear map and the noninvertible
nonlinearity transfor... | nlin.CD | an approach to generate the pseudorandombit sequence from the asymptotic deterministic randomness system is proposed in this letter we study the characteristic of multivalue correspondence of the asymptotic deterministic randomness constructed by the piecewise linear map and the noninvertible nonlinearity transform and... | [['an', 'approach', 'to', 'generate', 'the', 'pseudorandombit', 'sequence', 'from', 'the', 'asymptotic', 'deterministic', 'randomness', 'system', 'is', 'proposed', 'in', 'this', 'letter', 'we', 'study', 'the', 'characteristic', 'of', 'multivalue', 'correspondence', 'of', 'the', 'asymptotic', 'deterministic', 'randomnes... | [-0.14185241404726792, 0.05714332612806174, -0.1389756845019292, 0.09044344070134684, -0.0047454492188990114, -0.14588329988376547, 0.07392148591170553, 0.3190271327815329, -0.3294228035180519, -0.21196504064525168, 0.10774079299493072, -0.24957979331569125, -0.2040625791453446, 0.19078965504498532, -0.0892266371869482... |
710.1909 | In which Financial Markets do Mutual Fund Theorems hold true? | The Mutual Fund Theorem (MFT) is considered in a general semimartingale
financial market S with a finite time horizon T, where agents maximize expected
utility of terminal wealth. It is established that:
1) Let N be the wealth process of the num\'eraire portfolio (i.e. the optimal
portfolio for the log utility). If... | q-fin.TR math.OC | the mutual fund theorem mft is considered in a general semimartingale financial market s with a finite time horizon t where agents maximize expected utility of terminal wealth it is established that 1 let n be the wealth process of the numeraire portfolio ie the optimal portfolio for the log utility if any pathindepend... | [['the', 'mutual', 'fund', 'theorem', 'mft', 'is', 'considered', 'in', 'a', 'general', 'semimartingale', 'financial', 'market', 's', 'with', 'a', 'finite', 'time', 'horizon', 't', 'where', 'agents', 'maximize', 'expected', 'utility', 'of', 'terminal', 'wealth', 'it', 'is', 'established', 'that', '1', 'let', 'n', 'be', ... | [-0.08734195129186924, 0.031776503659784794, -0.09472783373987806, 0.1610954050589418, -0.09059617058399715, -0.1625138819603589, 0.11602717392578803, 0.3566805870112711, -0.3111210984296232, -0.19824120582940663, 0.1293353587932478, -0.26386784400484775, -0.1051713906393196, 0.1718544211516476, -0.1529578682439124, 0.... |
710.191 | Rationalization of EPR Coincidence Experiments | Coincidence experiments on EPR pairs show strong violations of Bell's
Inequalities at certain filter settings which is widely believed to mean that
local hidden variable models cannot explain these results. In this paper it is
shown that the 'non-separable' singlet density matrix can be represented as a
sum of separa... | physics.gen-ph | coincidence experiments on epr pairs show strong violations of bells inequalities at certain filter settings which is widely believed to mean that local hidden variable models cannot explain these results in this paper it is shown that the nonseparable singlet density matrix can be represented as a sum of separable den... | [['coincidence', 'experiments', 'on', 'epr', 'pairs', 'show', 'strong', 'violations', 'of', 'bells', 'inequalities', 'at', 'certain', 'filter', 'settings', 'which', 'is', 'widely', 'believed', 'to', 'mean', 'that', 'local', 'hidden', 'variable', 'models', 'can', 'not', 'explain', 'these', 'results', 'in', 'this', 'pape... | [-0.10134606961618317, 0.1843928334270233, -0.08807946606003474, 0.10227572059658546, -0.03736680083438358, -0.14789592075384164, -0.014789805021260627, 0.3563732216711593, -0.29092012377933857, -0.27055272056548074, 0.09107513382899023, -0.24426985023217687, -0.15126714812575187, 0.14391268361607087, -0.04366592283616... |
710.1911 | Triangulated categories of Gorenstein cyclic quotient singularities | We prove an equivalence of triangulated categories between Orlov's
triangulated category of singularities for a Gorenstein cyclic quotient
singularity and the derived category of representations of a quiver with
relations which is obtained from the McKay quiver by removing one vertex and
half of the arrows.
| math.AG | we prove an equivalence of triangulated categories between orlovs triangulated category of singularities for a gorenstein cyclic quotient singularity and the derived category of representations of a quiver with relations which is obtained from the mckay quiver by removing one vertex and half of the arrows | [['we', 'prove', 'an', 'equivalence', 'of', 'triangulated', 'categories', 'between', 'orlovs', 'triangulated', 'category', 'of', 'singularities', 'for', 'a', 'gorenstein', 'cyclic', 'quotient', 'singularity', 'and', 'the', 'derived', 'category', 'of', 'representations', 'of', 'a', 'quiver', 'with', 'relations', 'which'... | [-0.14718983482326503, -0.02775692355372366, -0.1137083966244498, 0.10412816137692932, -0.08136633289572985, -0.21909206585310723, -0.03654585147033567, 0.3198425607026919, -0.4533781604740121, -0.20216544130412134, 0.06155177427496275, -0.22496878849747387, -0.11736893637672714, 0.09929971477907637, -0.257899181350417... |
710.1912 | Logarithmic vector fields along smooth plane cubic curves | We study the sheaves of logarithmic vector fields along smooth cubic curves
in the projective plane, and prove a Torelli-type theorem in the sense of
Dolgachev-Kapranov for those with non-vanishing j-invariants.
| math.AG | we study the sheaves of logarithmic vector fields along smooth cubic curves in the projective plane and prove a torellitype theorem in the sense of dolgachevkapranov for those with nonvanishing jinvariants | [['we', 'study', 'the', 'sheaves', 'of', 'logarithmic', 'vector', 'fields', 'along', 'smooth', 'cubic', 'curves', 'in', 'the', 'projective', 'plane', 'and', 'prove', 'a', 'torellitype', 'theorem', 'in', 'the', 'sense', 'of', 'dolgachevkapranov', 'for', 'those', 'with', 'nonvanishing', 'jinvariants']] | [-0.2640512591047633, 0.05403575715759108, -0.09328333192294644, 0.07186154474414164, -0.06524268057077162, -0.1157854834361182, -0.01703537609559604, 0.33312016929830274, -0.30421096507099366, -0.15509473307118302, 0.06317029245227816, -0.25617010209469065, -0.1466072035893317, 0.2692229014731223, -0.14290872624804896... |
710.1913 | JVN observations of H2O masers around the evolved star IRAS 22480+6002 | We report on the H2O maser distributions around IRAS 22480+6002 (=IRC+60370)
observed with the Japanese VLBI Network (JVN) at three epochs spanning 2
months. This object was identified as a K-type supergiant in 1970s, which was
unusual as a stellar maser source. The spectrum of H2O masers consists of 5
peaks separate... | astro-ph | we report on the h2o maser distributions around iras 224806002 irc60370 observed with the japanese vlbi network jvn at three epochs spanning 2 months this object was identified as a ktype supergiant in 1970s which was unusual as a stellar maser source the spectrum of h2o masers consists of 5 peaks separated roughly equ... | [['we', 'report', 'on', 'the', 'h2o', 'maser', 'distributions', 'around', 'iras', '224806002', 'irc60370', 'observed', 'with', 'the', 'japanese', 'vlbi', 'network', 'jvn', 'at', 'three', 'epochs', 'spanning', '2', 'months', 'this', 'object', 'was', 'identified', 'as', 'a', 'ktype', 'supergiant', 'in', '1970s', 'which',... | [-0.07937538648032878, 0.09581277210358313, -0.08082136006516792, 0.051954751265935184, -0.09973710987309098, -0.0919283391160873, 0.025075599319816375, 0.46278725146830824, -0.17650226623930546, -0.3331812405843079, 0.048028116826667966, -0.27694748313114137, -0.02046091061863493, 0.17785106998794534, -0.0479097624341... |
710.1914 | Euler Incognito | The nonlinear flow equations discussed recently by Bender and Feinberg are
all reduced to the well-known Euler equation after change of variables.
| hep-th math-ph math.MP physics.flu-dyn | the nonlinear flow equations discussed recently by bender and feinberg are all reduced to the wellknown euler equation after change of variables | [['the', 'nonlinear', 'flow', 'equations', 'discussed', 'recently', 'by', 'bender', 'and', 'feinberg', 'are', 'all', 'reduced', 'to', 'the', 'wellknown', 'euler', 'equation', 'after', 'change', 'of', 'variables']] | [-0.12024857590652326, 0.11487582529133017, -0.07535747311670672, 0.017110459771091966, -0.1063092370221222, -0.15670209657400846, -0.07157789712602441, 0.21994553963569077, -0.3009828213940967, -0.2844947993078015, 0.10259986304762689, -0.27447081021752884, -0.19721811601299455, 0.20782167769291185, -0.093136078889735... |
710.1915 | Nonperturbative quark-gluon dynamics | We summarize recent results on the nonperturbative quark-gluon interaction in
Landau gauge QCD. Our analytical analysis of the infrared behaviour of the
quark-gluon vertex reveals infrared singularities, which lead to an infrared
divergent running coupling and a linear rising quark-antiquark potential when
chiral sym... | hep-ph | we summarize recent results on the nonperturbative quarkgluon interaction in landau gauge qcd our analytical analysis of the infrared behaviour of the quarkgluon vertex reveals infrared singularities which lead to an infrared divergent running coupling and a linear rising quarkantiquark potential when chiral symmetry i... | [['we', 'summarize', 'recent', 'results', 'on', 'the', 'nonperturbative', 'quarkgluon', 'interaction', 'in', 'landau', 'gauge', 'qcd', 'our', 'analytical', 'analysis', 'of', 'the', 'infrared', 'behaviour', 'of', 'the', 'quarkgluon', 'vertex', 'reveals', 'infrared', 'singularities', 'which', 'lead', 'to', 'an', 'infrare... | [-0.17037145170168236, 0.2121009720128943, -0.16741957439658925, 0.05867435220324506, -0.0991298467046223, -0.11263982188822223, 0.02955577979222513, 0.3811102478693311, -0.16470500530722815, -0.1825978188082958, 0.018008907083780147, -0.3054929413379003, -0.16670929396954867, 0.037575910948455714, 0.040663679190075554... |
710.1916 | Evaluate the Word Error Rate of Binary Block Codes with Square Radius
Probability Density Function | The word error rate (WER) of soft-decision-decoded binary block codes rarely
has closed-form. Bounding techniques are widely used to evaluate the
performance of maximum-likelihood decoding algorithm. But the existing bounds
are not tight enough especially for low signal-to-noise ratios and become
looser when a subopt... | cs.IT math.IT | the word error rate wer of softdecisiondecoded binary block codes rarely has closedform bounding techniques are widely used to evaluate the performance of maximumlikelihood decoding algorithm but the existing bounds are not tight enough especially for low signaltonoise ratios and become looser when a suboptimum decodin... | [['the', 'word', 'error', 'rate', 'wer', 'of', 'softdecisiondecoded', 'binary', 'block', 'codes', 'rarely', 'has', 'closedform', 'bounding', 'techniques', 'are', 'widely', 'used', 'to', 'evaluate', 'the', 'performance', 'of', 'maximumlikelihood', 'decoding', 'algorithm', 'but', 'the', 'existing', 'bounds', 'are', 'not'... | [-0.11290242058528362, 0.022257046855167682, -0.07001174792336921, 0.12226507625327389, -0.07521178716066942, -0.24368366063219693, 0.07364700990817227, 0.41582527520332596, -0.24823860740500756, -0.29290950300425966, 0.1318256064939002, -0.20046699504988888, -0.15487109394179602, 0.24987758393575804, -0.10223189650555... |
710.1917 | The heating of the cooling flow (The feedback effervescent heating
model) | The standard cooling flow model has predicted a large amount of cool gas in
the clusters of galaxies. The failure of the Chandra and XXM-Newton telescopes
to detect cooling gas (below 1-2 keV) in clusters of galaxies has suggested
that some heating process must work to suppress the cooling. The most likely
heating so... | astro-ph | the standard cooling flow model has predicted a large amount of cool gas in the clusters of galaxies the failure of the chandra and xxmnewton telescopes to detect cooling gas below 12 kev in clusters of galaxies has suggested that some heating process must work to suppress the cooling the most likely heating source is ... | [['the', 'standard', 'cooling', 'flow', 'model', 'has', 'predicted', 'a', 'large', 'amount', 'of', 'cool', 'gas', 'in', 'the', 'clusters', 'of', 'galaxies', 'the', 'failure', 'of', 'the', 'chandra', 'and', 'xxmnewton', 'telescopes', 'to', 'detect', 'cooling', 'gas', 'below', '12', 'kev', 'in', 'clusters', 'of', 'galaxi... | [-0.07552888690031867, 0.18621772253175026, -0.06621803690002045, 0.07243499178127394, -0.046755980470245984, -0.05469609447896029, 0.050800079446652845, 0.3911483191123063, -0.24272204510599488, -0.32146262614564464, 0.09034641063278259, -0.3056928737032594, -0.008071795766326514, 0.1941360245374116, 0.009204808633887... |
710.1918 | Lithium production on a low-mass secondary in a black hole soft X-ray
transient | We examine production of Li on the surface of a low-mass secondary in a black
hole soft X-ray transient (BHSXT) through the spallation of CNO nuclei by
neutrons which are ejected from a hot (> 10 MeV) advection-dominated accretion
flow (ADAF) around the black hole. Using updated binary parameters, cross
sections of n... | astro-ph | we examine production of li on the surface of a lowmass secondary in a black hole soft xray transient bhsxt through the spallation of cno nuclei by neutrons which are ejected from a hot 10 mev advectiondominated accretion flow adaf around the black hole using updated binary parameters cross sections of neutroninduced s... | [['we', 'examine', 'production', 'of', 'li', 'on', 'the', 'surface', 'of', 'a', 'lowmass', 'secondary', 'in', 'a', 'black', 'hole', 'soft', 'xray', 'transient', 'bhsxt', 'through', 'the', 'spallation', 'of', 'cno', 'nuclei', 'by', 'neutrons', 'which', 'are', 'ejected', 'from', 'a', 'hot', '10', 'mev', 'advectiondominat... | [-0.049946750612714544, 0.17402686708381945, -0.0458661436287502, 0.12200307920715864, -0.010733081398379559, -0.06802458061509162, 0.06294756928704433, 0.3642249985260295, -0.18704728561883363, -0.341283563561584, 0.05532039340411487, -0.32744163617102817, 0.049727488919365945, 0.23885365728938768, -0.0368159756750114... |
710.1919 | Increasing power of the test through pre-test - a robust method | This paper develops robust test procedures for testing the intercept of a
simple regression model when it is \textit{apriori} suspected that the slope
has a specified value. Defining unrestricted test (UT), restricted test (RT)
and pre-test test (PTT) corresponding to the unrestricted (UE), restricted
(RE), and preli... | math.ST stat.TH | this paper develops robust test procedures for testing the intercept of a simple regression model when it is textitapriori suspected that the slope has a specified value defining unrestricted test ut restricted test rt and pretest test ptt corresponding to the unrestricted ue restricted re and preliminary test estimato... | [['this', 'paper', 'develops', 'robust', 'test', 'procedures', 'for', 'testing', 'the', 'intercept', 'of', 'a', 'simple', 'regression', 'model', 'when', 'it', 'is', 'textitapriori', 'suspected', 'that', 'the', 'slope', 'has', 'a', 'specified', 'value', 'defining', 'unrestricted', 'test', 'ut', 'restricted', 'test', 'rt... | [-0.06653291569645739, -0.0013991333865782335, -0.11861239447302761, 0.11824895807076245, -0.06680890045439204, -0.22915078792277546, 0.06695268800415631, 0.3509602132829882, -0.20229302381963601, -0.2818016285237501, 0.11612219141153175, -0.24079937275853894, -0.09573475852874773, 0.20602830855087156, -0.0629374737806... |
710.192 | The Secrecy Capacity of the MIMO Wiretap Channel | We consider the MIMO wiretap channel, that is a MIMO broadcast channel where
the transmitter sends some confidential information to one user which is a
legitimate receiver, while the other user is an eavesdropper. Perfect secrecy
is achieved when the the transmitter and the legitimate receiver can
communicate at some... | cs.IT cs.CR math.IT | we consider the mimo wiretap channel that is a mimo broadcast channel where the transmitter sends some confidential information to one user which is a legitimate receiver while the other user is an eavesdropper perfect secrecy is achieved when the the transmitter and the legitimate receiver can communicate at some posi... | [['we', 'consider', 'the', 'mimo', 'wiretap', 'channel', 'that', 'is', 'a', 'mimo', 'broadcast', 'channel', 'where', 'the', 'transmitter', 'sends', 'some', 'confidential', 'information', 'to', 'one', 'user', 'which', 'is', 'a', 'legitimate', 'receiver', 'while', 'the', 'other', 'user', 'is', 'an', 'eavesdropper', 'perf... | [-0.37711273816724616, 0.043609449651338894, 0.004841452549582207, -0.008428875634181363, -0.12360822147519518, -0.4534808949777676, 0.12319515121885405, 0.3347985075426198, -0.2788402974124878, -0.19041438712187672, 0.10378384529437709, -0.34496623574085133, -0.11260723178675498, 0.02760231382994642, -0.13175893775237... |
710.1921 | Spin Order in Paired Quantum Hall States | We consider quantum Hall states at even-denominator filling fractions,
especially $\nu=5/2$, in the limit of small Zeeman energy. Assuming that a
paired quantum Hall state forms, we study spin ordering and its interplay with
pairing. We give numerical evidence that at $\nu = 5/2$ an incompressible
ground state will e... | cond-mat.mes-hall | we consider quantum hall states at evendenominator filling fractions especially nu52 in the limit of small zeeman energy assuming that a paired quantum hall state forms we study spin ordering and its interplay with pairing we give numerical evidence that at nu 52 an incompressible ground state will exhibit spontaneous ... | [['we', 'consider', 'quantum', 'hall', 'states', 'at', 'evendenominator', 'filling', 'fractions', 'especially', 'nu52', 'in', 'the', 'limit', 'of', 'small', 'zeeman', 'energy', 'assuming', 'that', 'a', 'paired', 'quantum', 'hall', 'state', 'forms', 'we', 'study', 'spin', 'ordering', 'and', 'its', 'interplay', 'with', '... | [-0.2403193278236618, 0.2906840917557929, -0.0691334479238971, 0.0830886889951736, -0.018813269115136273, -0.14794433787964018, 0.0564902655678452, 0.29504605625489994, -0.24233902116040035, -0.2636237933641366, 0.01739414444663063, -0.3024703785444477, -0.1234034701753574, 0.12928147917097835, 0.06791484714735166, -0.... |
710.1922 | On the anomalous dimensions of the multiple pomeron exchanges | High energy hard scattering in large $N_{c}$ limit can be described by the
QCD dipole model. In this paper, single, double and triple BFKL pomeron
exchange amplitudes are computed explicitly within the dipole model. Based on
the calculation, the general formula
$\gamma^{(k)*}_{0}=\chi^{-1}(k\chi({1/2}))$ which govern... | hep-ph | high energy hard scattering in large n_c limit can be described by the qcd dipole model in this paper single double and triple bfkl pomeron exchange amplitudes are computed explicitly within the dipole model based on the calculation the general formula gammak_0chi1kchi12 which governs the anomalous dimension of 1righta... | [['high', 'energy', 'hard', 'scattering', 'in', 'large', 'n_c', 'limit', 'can', 'be', 'described', 'by', 'the', 'qcd', 'dipole', 'model', 'in', 'this', 'paper', 'single', 'double', 'and', 'triple', 'bfkl', 'pomeron', 'exchange', 'amplitudes', 'are', 'computed', 'explicitly', 'within', 'the', 'dipole', 'model', 'based',... | [-0.11840976763946506, 0.1541958861871735, -0.09510676749050617, 0.1297823062158896, -0.059727756275826105, -0.10593659112966813, 0.030430622905451846, 0.32676711029649436, -0.24916090314777997, -0.2869498749048664, 0.014768190299426871, -0.2804572543968539, -0.1418926165654109, 0.12375468510499858, 0.01516773258777243... |
710.1923 | Omni-Lie algebroids | A generalized Courant algebroid structure is defined on the direct sum bundle
D(E) +J(E), where D(E) and J(E) are the gauge Lie algebroid and the jet bundle
of a vector bundle E respectively. Such a structure is called an omni-Lie
algebroid since it is reduced to the omni-Lie algebra introduced by A.Weinstein
if the ... | math-ph math.MP math.SG | a generalized courant algebroid structure is defined on the direct sum bundle de je where de and je are the gauge lie algebroid and the jet bundle of a vector bundle e respectively such a structure is called an omnilie algebroid since it is reduced to the omnilie algebra introduced by aweinstein if the base manifold is... | [['a', 'generalized', 'courant', 'algebroid', 'structure', 'is', 'defined', 'on', 'the', 'direct', 'sum', 'bundle', 'de', 'je', 'where', 'de', 'and', 'je', 'are', 'the', 'gauge', 'lie', 'algebroid', 'and', 'the', 'jet', 'bundle', 'of', 'a', 'vector', 'bundle', 'e', 'respectively', 'such', 'a', 'structure', 'is', 'calle... | [-0.25026798344710294, 0.036912281710058725, -0.09538022613919833, 0.0794351434787078, -0.24036284333971494, -0.12435539839241434, -0.026271165000713047, 0.36190898234353347, -0.3530719239264727, -0.2175635522341027, 0.044556522583041124, -0.19949528466471855, -0.21814771621652385, 0.13809433576157865, -0.1264013905242... |
710.1924 | A Heuristic Routing Mechanism Using a New Addressing Scheme | Current methods of routing are based on network information in the form of
routing tables, in which routing protocols determine how to update the tables
according to the network changes. Despite the variability of data in routing
tables, node addresses are constant. In this paper, we first introduce the new
concept o... | cs.NI cs.AI | current methods of routing are based on network information in the form of routing tables in which routing protocols determine how to update the tables according to the network changes despite the variability of data in routing tables node addresses are constant in this paper we first introduce the new concept of varia... | [['current', 'methods', 'of', 'routing', 'are', 'based', 'on', 'network', 'information', 'in', 'the', 'form', 'of', 'routing', 'tables', 'in', 'which', 'routing', 'protocols', 'determine', 'how', 'to', 'update', 'the', 'tables', 'according', 'to', 'the', 'network', 'changes', 'despite', 'the', 'variability', 'of', 'dat... | [-0.14679824556276175, 0.0029062409815725997, -0.05383352443937268, 0.03705484898493333, -0.11041931942480603, -0.18297005589676105, 0.09390459047307247, 0.4133040892488476, -0.2763988950790198, -0.3235441001563041, 0.11312056169975479, -0.23373192567517287, -0.20188294530415268, 0.18531959098694262, -0.159367792822643... |
710.1925 | Chalker-Coddington model described by an S-matrix with odd dimensions | The Chalker-Coddington network model is often used to describe the transport
properties of quantum Hall systems. By adding an extra channel to this model,
we introduce an asymmetric model with profoundly different transport
properties. We present a numerical analysis of these transport properties and
consider the rel... | cond-mat.mes-hall cond-mat.dis-nn | the chalkercoddington network model is often used to describe the transport properties of quantum hall systems by adding an extra channel to this model we introduce an asymmetric model with profoundly different transport properties we present a numerical analysis of these transport properties and consider the relevance... | [['the', 'chalkercoddington', 'network', 'model', 'is', 'often', 'used', 'to', 'describe', 'the', 'transport', 'properties', 'of', 'quantum', 'hall', 'systems', 'by', 'adding', 'an', 'extra', 'channel', 'to', 'this', 'model', 'we', 'introduce', 'an', 'asymmetric', 'model', 'with', 'profoundly', 'different', 'transport'... | [-0.15265472354367376, 0.08203496176342014, -0.08326846297830343, 0.04246602145954967, -0.015203531915321946, -0.16780813419260085, -0.004646726967766881, 0.3671716302190907, -0.3410821946710348, -0.3017915992392227, 0.07195256249979139, -0.25627563051879404, -0.22532409593462943, 0.17929668402764945, -0.02045184200629... |
710.1926 | Eradication of singularities in the next-to-leading order RG evolution
for the \Delta S = 1 effective Hamiltonian with 3 quark flavours | We consider the renormalization group evolution for the operators in the
$\Delta S=1$ effective Hamiltonian with 3 active quark flavors, which is needed
in the numerical analysis of data sets for $\epsilon'/\epsilon$ calculated in
lattice QCD. Singularities are present in the original solution of Buras et al.
at next... | hep-lat | we consider the renormalization group evolution for the operators in the delta s1 effective hamiltonian with 3 active quark flavors which is needed in the numerical analysis of data sets for epsilonepsilon calculated in lattice qcd singularities are present in the original solution of buras et al at nexttoleading order... | [['we', 'consider', 'the', 'renormalization', 'group', 'evolution', 'for', 'the', 'operators', 'in', 'the', 'delta', 's1', 'effective', 'hamiltonian', 'with', '3', 'active', 'quark', 'flavors', 'which', 'is', 'needed', 'in', 'the', 'numerical', 'analysis', 'of', 'data', 'sets', 'for', 'epsilonepsilon', 'calculated', 'i... | [-0.0927754922710154, 0.10594510700587832, -0.10973148217527282, 0.06723363054574492, -0.042807241950884735, -0.07326633088000187, 0.052641833681664474, 0.35151332403199936, -0.22303694857438222, -0.27369164148721536, 0.09306460392763924, -0.30372556903903636, -0.15889667801627325, 0.14118318142659894, -0.0355802361101... |
710.1927 | Diquarks and \Lambda_{b}\to\Lambda_c weak decays | In this work we investigate the weak $\Lambda_{b}\to\Lambda_c$ semi-leptonic
and non-leptonic decays. The light-front quark model and diquark picture for
heavy baryons are adopted to evaluate the $\Lambda_{b}\to\Lambda_c$ transition
form factors. In the heavy quark limit we study the Isgur-Wise function. By
fitting t... | hep-ph | in this work we investigate the weak lambda_btolambda_c semileptonic and nonleptonic decays the lightfront quark model and diquark picture for heavy baryons are adopted to evaluate the lambda_btolambda_c transition form factors in the heavy quark limit we study the isgurwise function by fitting the data of the semilept... | [['in', 'this', 'work', 'we', 'investigate', 'the', 'weak', 'lambda_btolambda_c', 'semileptonic', 'and', 'nonleptonic', 'decays', 'the', 'lightfront', 'quark', 'model', 'and', 'diquark', 'picture', 'for', 'heavy', 'baryons', 'are', 'adopted', 'to', 'evaluate', 'the', 'lambda_btolambda_c', 'transition', 'form', 'factors... | [-0.0697453078852656, 0.21287437017750124, -0.05351911508210603, 0.15058826309727555, -0.04993300129098807, -0.11122223418527122, 0.09758782226875981, 0.3226044794822904, -0.15390146150649792, -0.19626553060122948, -0.041499272936248575, -0.34489267736930274, -0.00044155967068569416, 0.0778448140494868, 0.1174718441131... |
710.1928 | A Witness of Multipartite Entanglement Strata | We describe an entanglement witness for $N$-qubit mixed states based on the
properties of $N$-point correlation functions. Depending on the degree of
violation, this witness can guarantee that no more than $M$ qubits are
separable from the rest of the state for any $M\leq N$, or that there is some
genuine $M$-party o... | quant-ph | we describe an entanglement witness for nqubit mixed states based on the properties of npoint correlation functions depending on the degree of violation this witness can guarantee that no more than m qubits are separable from the rest of the state for any mleq n or that there is some genuine mparty or greater multipart... | [['we', 'describe', 'an', 'entanglement', 'witness', 'for', 'nqubit', 'mixed', 'states', 'based', 'on', 'the', 'properties', 'of', 'npoint', 'correlation', 'functions', 'depending', 'on', 'the', 'degree', 'of', 'violation', 'this', 'witness', 'can', 'guarantee', 'that', 'no', 'more', 'than', 'm', 'qubits', 'are', 'sepa... | [-0.14959795095724984, 0.218245430841489, -0.10475412992294877, 0.07414320765994489, 0.05676542889792472, -0.17877018954604865, 0.03435880789766088, 0.3335170452110469, -0.188415048699826, -0.24468583991285414, 0.059920368145685646, -0.267993300203234, -0.09231942700920627, 0.19641201387392357, -0.010856331787072121, 0... |
710.1929 | Polynomial splittings of metabelian von Neumann rho-invariants | We show that if the connected sum of two knots with coprime Alexander
polynomials has vanishing von Neumann rho-invariants associated with certain
metabelian representations then so do both knots. As an application, we give a
new example of an infinite family of knots which are linearly independent in
the knot concor... | math.GT | we show that if the connected sum of two knots with coprime alexander polynomials has vanishing von neumann rhoinvariants associated with certain metabelian representations then so do both knots as an application we give a new example of an infinite family of knots which are linearly independent in the knot concordance... | [['we', 'show', 'that', 'if', 'the', 'connected', 'sum', 'of', 'two', 'knots', 'with', 'coprime', 'alexander', 'polynomials', 'has', 'vanishing', 'von', 'neumann', 'rhoinvariants', 'associated', 'with', 'certain', 'metabelian', 'representations', 'then', 'so', 'do', 'both', 'knots', 'as', 'an', 'application', 'we', 'gi... | [-0.24809581954748586, 0.1557588410578319, -0.11406738663880298, 0.013434720986809295, -0.1283348832691375, -0.20094136498832646, -0.07656643779661793, 0.3853841910738713, -0.31885572093037456, -0.20500613225158304, 0.11258498635456468, -0.25080078170419884, -0.1565507919026109, 0.20806279572738837, -0.1296682249253186... |
710.193 | General properties of logarithmically divergent one-loop lattice Feynman
integrals | We prove that logarithmically divergent one-loop lattice Feynman integrals
have the general form I(p,a) = f(p)log(aM)+g(p,M) up to terms which vanish for
lattice spacing a -> 0. Here p denotes collectively the external momenta and M
is an arbitrary mass scale. The f(p) is shown to be universal and to coincide
with th... | hep-lat | we prove that logarithmically divergent oneloop lattice feynman integrals have the general form ipa fplogamgpm up to terms which vanish for lattice spacing a 0 here p denotes collectively the external momenta and m is an arbitrary mass scale the fp is shown to be universal and to coincide with the analogous quantity in... | [['we', 'prove', 'that', 'logarithmically', 'divergent', 'oneloop', 'lattice', 'feynman', 'integrals', 'have', 'the', 'general', 'form', 'ipa', 'fplogamgpm', 'up', 'to', 'terms', 'which', 'vanish', 'for', 'lattice', 'spacing', 'a', '0', 'here', 'p', 'denotes', 'collectively', 'the', 'external', 'momenta', 'and', 'm', '... | [-0.14463295158646183, 0.21313476486605254, -0.11054005607587808, 0.08526856533906657, -0.08952013991311253, -0.11816541783367776, 0.019765441555802416, 0.3596202148260867, -0.23203949731721626, -0.2279239282451146, 0.07737959280507867, -0.2872436496361, -0.13535913150015522, 0.1471529651586557, -0.03197756127598203, 0... |
710.1931 | Strangeness Enhancement: Challenges and Successes | Highly effective conversion of kinetic energy into abundant particle
multiplicity is the remarkable feature discovered in high energy heavy ion
collisions. This short and pedagogic review addresses topical issues related to
the understanding of this phenomenon, originating in the creation of the
deconfined quark--glu... | nucl-th hep-ph nucl-ex physics.hist-ph | highly effective conversion of kinetic energy into abundant particle multiplicity is the remarkable feature discovered in high energy heavy ion collisions this short and pedagogic review addresses topical issues related to the understanding of this phenomenon originating in the creation of the deconfined quarkgluon pla... | [['highly', 'effective', 'conversion', 'of', 'kinetic', 'energy', 'into', 'abundant', 'particle', 'multiplicity', 'is', 'the', 'remarkable', 'feature', 'discovered', 'in', 'high', 'energy', 'heavy', 'ion', 'collisions', 'this', 'short', 'and', 'pedagogic', 'review', 'addresses', 'topical', 'issues', 'related', 'to', 't... | [-0.0873608398432326, 0.26723558952411014, -0.11771478397357794, 0.11909747612533263, -0.05684738258520762, -0.15071637762400011, 0.02877221210963196, 0.3061058177716202, -0.23948183783536983, -0.3008135719431771, -0.03639231807319447, -0.29236197642878525, -0.035296954587101935, 0.07114663214629723, -0.066111641749739... |
710.1932 | A mechanism for Fermi-surface-topology tuned superconductivity in the
cuprates | Based on recent magnetic-quantum-oscillation, ARPES, neutron-scattering and
other data, we propose that superconductivity in the cuprates occurs via a
convenient matching of the spatial distribution of incommensurate spin
fluctuations to the amplitude and phase of the $d_{x^2-y^2}$ Cooper-pair
wavefunction; this esta... | cond-mat.supr-con cond-mat.str-el | based on recent magneticquantumoscillation arpes neutronscattering and other data we propose that superconductivity in the cuprates occurs via a convenient matching of the spatial distribution of incommensurate spin fluctuations to the amplitude and phase of the d_x2y2 cooperpair wavefunction this establishes a robust ... | [['based', 'on', 'recent', 'magneticquantumoscillation', 'arpes', 'neutronscattering', 'and', 'other', 'data', 'we', 'propose', 'that', 'superconductivity', 'in', 'the', 'cuprates', 'occurs', 'via', 'a', 'convenient', 'matching', 'of', 'the', 'spatial', 'distribution', 'of', 'incommensurate', 'spin', 'fluctuations', 't... | [-0.21877729710866148, 0.2496976394557594, -0.07137656289952125, 0.11490073051637288, -0.04648031958371518, -0.1341196350738641, 0.08164667955592392, 0.34214755865620583, -0.25329091980701357, -0.2618536315711699, -0.0072350045748597646, -0.32771286713032743, -0.09024612132027217, 0.14712446481062788, 0.029476791869584... |
710.1933 | Intermediate energy spectrum of five colour QCD at one loop | I consider the monopole condensate of five colour QCD. The naive lowest
energy state is unobtainable at one-loop for five or more colours due to simple
geometry. The consequent adjustment of the vacuum condensate generates a
hierarchy of confinement scales in a natural Higgs-free manner. QCD and
QED-like forces emerg... | hep-th | i consider the monopole condensate of five colour qcd the naive lowest energy state is unobtainable at oneloop for five or more colours due to simple geometry the consequent adjustment of the vacuum condensate generates a hierarchy of confinement scales in a natural higgsfree manner qcd and qedlike forces emerge natura... | [['i', 'consider', 'the', 'monopole', 'condensate', 'of', 'five', 'colour', 'qcd', 'the', 'naive', 'lowest', 'energy', 'state', 'is', 'unobtainable', 'at', 'oneloop', 'for', 'five', 'or', 'more', 'colours', 'due', 'to', 'simple', 'geometry', 'the', 'consequent', 'adjustment', 'of', 'the', 'vacuum', 'condensate', 'gener... | [-0.093372526795561, 0.3108619811069785, -0.11133440724348254, 0.14786914031367016, -0.07399562915617769, -0.10506208725696937, 0.0431209709495306, 0.34398769495909975, -0.19083165738618735, -0.28927538069811737, -7.723311710199624e-06, -0.26599483609651076, -0.020815808033203764, 0.07477453819151517, 0.014402942791948... |
710.1934 | Quantum states with strong positive partial transpose | We construct a large class of bipartite M x N quantum states which defines a
proper subset of states with positive partial transposes (PPT). Any state from
this class is PPT but the positivity of its partial transposition is recognized
with respect to canonical factorization of the original density operator. We
propo... | quant-ph | we construct a large class of bipartite m x n quantum states which defines a proper subset of states with positive partial transposes ppt any state from this class is ppt but the positivity of its partial transposition is recognized with respect to canonical factorization of the original density operator we propose to ... | [['we', 'construct', 'a', 'large', 'class', 'of', 'bipartite', 'm', 'x', 'n', 'quantum', 'states', 'which', 'defines', 'a', 'proper', 'subset', 'of', 'states', 'with', 'positive', 'partial', 'transposes', 'ppt', 'any', 'state', 'from', 'this', 'class', 'is', 'ppt', 'but', 'the', 'positivity', 'of', 'its', 'partial', 't... | [-0.17136576406542875, 0.17100625903639075, -0.03416424170646765, 0.008575299218909382, -0.04772532162932704, -0.1789786926700338, 0.03738274511702563, 0.3313542832046339, -0.2886794775035487, -0.19396772872009124, 0.08346197910109306, -0.31059120271087, -0.10839431169315254, 0.04490281217603957, -0.06215103331647099, ... |
710.1935 | Classification of local realistic theories | Recently, it has shown that an explicit local realistic model for the values
of a correlation function, given in a two-setting Bell experiment (two-setting
model), works only for the specific set of settings in the given experiment,
but cannot construct a local realistic model for the values of a correlation
function... | quant-ph | recently it has shown that an explicit local realistic model for the values of a correlation function given in a twosetting bell experiment twosetting model works only for the specific set of settings in the given experiment but cannot construct a local realistic model for the values of a correlation function given in ... | [['recently', 'it', 'has', 'shown', 'that', 'an', 'explicit', 'local', 'realistic', 'model', 'for', 'the', 'values', 'of', 'a', 'correlation', 'function', 'given', 'in', 'a', 'twosetting', 'bell', 'experiment', 'twosetting', 'model', 'works', 'only', 'for', 'the', 'specific', 'set', 'of', 'settings', 'in', 'the', 'give... | [-0.09190662578155345, 0.08921712929553066, -0.10052187363063539, 0.10877280430282121, -0.01576244811221332, -0.2515619357696155, 0.02271827829389514, 0.3776550338818477, -0.2027076263074015, -0.31617430209384095, 0.05872936192020722, -0.24378572123034017, -0.14072672187813096, 0.22024462122789265, -0.02379365078779263... |
710.1936 | Regular integers modulo n | Let $n=p_1^{\nu_1}... p_r^{\nu_r} >1$ be an integer. An integer $a$ is called
regular (mod $n$) if there is an integer $x$ such that $a^2x\equiv a$ (mod
$n$). Let $\varrho(n)$ denote the number of regular integers $a$ (mod $n$) such
that $1\le a\le n$. Here $\varrho(n)=(\phi(p_1^{\nu_1})+1)...
(\phi(p_r^{\nu_r})+1)$,... | math.NT | let np_1nu_1 p_rnu_r 1 be an integer an integer a is called regular mod n if there is an integer x such that a2xequiv a mod n let varrhon denote the number of regular integers a mod n such that 1le ale n here varrhonphip_1nu_11 phip_rnu_r1 where phin is the euler function in this paper we first summarize some basic pro... | [['let', 'np_1nu_1', 'p_rnu_r', '1', 'be', 'an', 'integer', 'an', 'integer', 'a', 'is', 'called', 'regular', 'mod', 'n', 'if', 'there', 'is', 'an', 'integer', 'x', 'such', 'that', 'a2xequiv', 'a', 'mod', 'n', 'let', 'varrhon', 'denote', 'the', 'number', 'of', 'regular', 'integers', 'a', 'mod', 'n', 'such', 'that', '1le... | [-0.23762268248652474, 0.1639388481021291, -0.050938363145157865, -0.007105029112230358, -0.00019301405553235097, -0.14876452382926023, -0.03805834890913553, 0.2778940765616181, -0.3143783649534322, -0.22164716101722437, 0.0483639015988813, -0.3432312765854589, -0.18052193724675877, 0.1291189328296466, -0.0576536668663... |
710.1937 | Hirzebruch-Riemann-Roch theorem for DG algebras | For an arbitrary proper DG algebra A (i.e. DG algebra with finite dimensional
total cohomology) we introduce a pairing on the Hochschild homology of A and
present an explicit formula for a Chern-type character of an arbitrary perfect
A-module (the Chern characters take values in the Hochschild homology of A).
The Hir... | math.KT math.AG | for an arbitrary proper dg algebra a ie dg algebra with finite dimensional total cohomology we introduce a pairing on the hochschild homology of a and present an explicit formula for a cherntype character of an arbitrary perfect amodule the chern characters take values in the hochschild homology of a the hirzebruchriem... | [['for', 'an', 'arbitrary', 'proper', 'dg', 'algebra', 'a', 'ie', 'dg', 'algebra', 'with', 'finite', 'dimensional', 'total', 'cohomology', 'we', 'introduce', 'a', 'pairing', 'on', 'the', 'hochschild', 'homology', 'of', 'a', 'and', 'present', 'an', 'explicit', 'formula', 'for', 'a', 'cherntype', 'character', 'of', 'an',... | [-0.2321635436670916, 0.048933506141281044, -0.09770691277495083, 0.08862745215167077, -0.10783484953476095, -0.1489221773463414, -0.029099980445327953, 0.32192557831653035, -0.3491922140448958, -0.19802537115782007, 0.07690628633097552, -0.2201051456370176, -0.15403828966165228, 0.17859261061939932, -0.139619744466192... |
710.1938 | Stripe Formation in Fermionic Atoms on 2-D Optical Lattice inside a Box
Trap: DMRG Studies for Repulsive Hubbard Model with Open Boundary Condition | We suggest that box shape trap enables to observe intrinsic properties of the
repulsive Hubbard model in a fixed doping in contrast to the harmonic trap
bringing about spatial variations of atom density profiles. In order to predict
atomic density profile under the box trap, we apply the directly-extended
density-mat... | cond-mat.str-el | we suggest that box shape trap enables to observe intrinsic properties of the repulsive hubbard model in a fixed doping in contrast to the harmonic trap bringing about spatial variations of atom density profiles in order to predict atomic density profile under the box trap we apply the directlyextended densitymatrix re... | [['we', 'suggest', 'that', 'box', 'shape', 'trap', 'enables', 'to', 'observe', 'intrinsic', 'properties', 'of', 'the', 'repulsive', 'hubbard', 'model', 'in', 'a', 'fixed', 'doping', 'in', 'contrast', 'to', 'the', 'harmonic', 'trap', 'bringing', 'about', 'spatial', 'variations', 'of', 'atom', 'density', 'profiles', 'in'... | [-0.13809517394513526, 0.13248460711448962, -0.0694605161217933, 0.059546591342486285, -0.03536695025114884, -0.1550906846920649, 0.11793347480145434, 0.3865634784472327, -0.25417768835017446, -0.2770477935229263, 0.02334884556129258, -0.31632682962792247, -0.09619314905837284, 0.13943410262709865, 0.014195827641755554... |
710.1939 | MARCOS, a numerical tool for the simulation of multiple time-dependent
non-linear diffusive shock acceleration | We present a new code aimed at the simulation of diffusive shock acceleration
(DSA), and discuss various test cases which demonstrate its ability to study
DSA in its full time-dependent and non-linear developments. We present the
numerical methods implemented, coupling the hydrodynamical evolution of a
parallel shock... | astro-ph | we present a new code aimed at the simulation of diffusive shock acceleration dsa and discuss various test cases which demonstrate its ability to study dsa in its full timedependent and nonlinear developments we present the numerical methods implemented coupling the hydrodynamical evolution of a parallel shock in one s... | [['we', 'present', 'a', 'new', 'code', 'aimed', 'at', 'the', 'simulation', 'of', 'diffusive', 'shock', 'acceleration', 'dsa', 'and', 'discuss', 'various', 'test', 'cases', 'which', 'demonstrate', 'its', 'ability', 'to', 'study', 'dsa', 'in', 'its', 'full', 'timedependent', 'and', 'nonlinear', 'developments', 'we', 'pre... | [-0.11218926887594018, 0.05893850360017002, -0.06024850602413899, 0.08207305580274099, -0.08951659901585016, -0.10646122496185545, -0.007000665713004233, 0.3726000371693445, -0.3016099377742244, -0.3212336446310765, 0.050467148213190774, -0.19329479494859889, -0.10173779841530703, 0.21143443043666338, 0.045914791466583... |
710.194 | Spatio-temporal scaling for out-of-equilibrium relaxation dynamics of an
elastic manifold in random media: crossover between the Larkin regime and
thermally activated regime | We study relaxation dynamics of a three dimensional elastic manifold in
random potential from a uniform initial condition by numerically solving the
Langevin equation.We observe growth of roughness of the system up to larger
wavelengths with time.We analyze structure factor in detail and find a compact
scaling ansatz... | cond-mat.dis-nn cond-mat.stat-mech | we study relaxation dynamics of a three dimensional elastic manifold in random potential from a uniform initial condition by numerically solving the langevin equationwe observe growth of roughness of the system up to larger wavelengths with timewe analyze structure factor in detail and find a compact scaling ansatz des... | [['we', 'study', 'relaxation', 'dynamics', 'of', 'a', 'three', 'dimensional', 'elastic', 'manifold', 'in', 'random', 'potential', 'from', 'a', 'uniform', 'initial', 'condition', 'by', 'numerically', 'solving', 'the', 'langevin', 'equationwe', 'observe', 'growth', 'of', 'roughness', 'of', 'the', 'system', 'up', 'to', 'l... | [-0.16191206951899564, 0.20438054774308065, -0.11077128924137238, 0.060613236258801655, -0.024510244852589333, -0.18500615104658566, 0.0039714396333175835, 0.35045328746805443, -0.28452012735400717, -0.2703805796313556, 0.06673047809140283, -0.23908210788652592, -0.13053894269407965, 0.1918042254994861, 0.0569625572831... |
710.1941 | Gamma-Ray Astronomy around 100 TeV with a large Muon Detector operated
at Very High Altitude | Measurements at 100 TeV and above are an important goal for the next
generation of high energy gamma-ray astronomy experiments to solve the still
open problem of the origin of galactic cosmic rays. The most natural
experimental solution to detect very low radiation fluxes is provided by the
Extensive Air Shower (EAS)... | astro-ph | measurements at 100 tev and above are an important goal for the next generation of high energy gammaray astronomy experiments to solve the still open problem of the origin of galactic cosmic rays the most natural experimental solution to detect very low radiation fluxes is provided by the extensive air shower eas array... | [['measurements', 'at', '100', 'tev', 'and', 'above', 'are', 'an', 'important', 'goal', 'for', 'the', 'next', 'generation', 'of', 'high', 'energy', 'gammaray', 'astronomy', 'experiments', 'to', 'solve', 'the', 'still', 'open', 'problem', 'of', 'the', 'origin', 'of', 'galactic', 'cosmic', 'rays', 'the', 'most', 'natural... | [-0.07778553842157447, 0.19169026559463637, 0.01613022878380685, 0.15634348629893544, -0.05121897969812412, -0.06723959564456138, 0.0057760109233766285, 0.4109855470215452, -0.2104669626713891, -0.4520725729008173, 0.08664386977826984, -0.3413236148077352, 0.033026600240504946, 0.22858547444358981, -0.01941000850036226... |
710.1942 | Spatial confinement effects on quantum field theory using nonlinear
coherent states approach | We study some basic quantum confinement effects through investigation a
deformed harmonic oscillator algebra. We show that spatial confinement effects
on a quantum harmonic oscillator can be represented by a deformation function
within the framework of nonlinear coherent states theory. Using the deformed
algebra, we ... | quant-ph | we study some basic quantum confinement effects through investigation a deformed harmonic oscillator algebra we show that spatial confinement effects on a quantum harmonic oscillator can be represented by a deformation function within the framework of nonlinear coherent states theory using the deformed algebra we const... | [['we', 'study', 'some', 'basic', 'quantum', 'confinement', 'effects', 'through', 'investigation', 'a', 'deformed', 'harmonic', 'oscillator', 'algebra', 'we', 'show', 'that', 'spatial', 'confinement', 'effects', 'on', 'a', 'quantum', 'harmonic', 'oscillator', 'can', 'be', 'represented', 'by', 'a', 'deformation', 'funct... | [-0.13491302551029577, 0.19403294562218115, -0.10826077258463987, 0.0692838911692007, -0.05183874028398819, -0.12040447055832627, -0.014877997271562974, 0.39880041079115625, -0.27458518136715154, -0.22325890777709403, 0.012230275454450898, -0.2083359578163507, -0.23627258398445303, 0.18250272977981985, -0.0254730254837... |
710.1943 | Fano Resonances in Stubbed Quantum Waveguides with Impurities | We consider T--shaped, two--dimensional quantum waveguides containing
attractive or repulsive impurities with a smooth, realistic shape, and study
how the resonance behavior of the total conductance depends upon the strength
of the defect potential and the geometry of the device. The resonance
parameters are determin... | cond-mat.mes-hall | we consider tshaped twodimensional quantum waveguides containing attractive or repulsive impurities with a smooth realistic shape and study how the resonance behavior of the total conductance depends upon the strength of the defect potential and the geometry of the device the resonance parameters are determined locatin... | [['we', 'consider', 'tshaped', 'twodimensional', 'quantum', 'waveguides', 'containing', 'attractive', 'or', 'repulsive', 'impurities', 'with', 'a', 'smooth', 'realistic', 'shape', 'and', 'study', 'how', 'the', 'resonance', 'behavior', 'of', 'the', 'total', 'conductance', 'depends', 'upon', 'the', 'strength', 'of', 'the... | [-0.1662998615553783, 0.13272257034055968, -0.051975112333292925, 0.04109034456452856, -0.030223509569662393, -0.11976947390063795, 0.03452009563234144, 0.3381940242183465, -0.24835837924832938, -0.2670753502477241, 0.03276305263247078, -0.3044177811639446, -0.16390863917417503, 0.16966780025501965, 0.05378223357782248... |
710.1944 | Laser-interferometric Detectors for Gravitational Wave Background at 100
MHz : Detector Design and Sensitivity | Recently, observational searches for gravitational wave background (GWB) have
developed and given direct and indirect constraints on the energy density of
GWB in a broad range of frequencies. These constraints have already rejected
some theoretical models of large GWB spectra. However, at 100 MHz, there is no
strict ... | gr-qc | recently observational searches for gravitational wave background gwb have developed and given direct and indirect constraints on the energy density of gwb in a broad range of frequencies these constraints have already rejected some theoretical models of large gwb spectra however at 100 mhz there is no strict upper lim... | [['recently', 'observational', 'searches', 'for', 'gravitational', 'wave', 'background', 'gwb', 'have', 'developed', 'and', 'given', 'direct', 'and', 'indirect', 'constraints', 'on', 'the', 'energy', 'density', 'of', 'gwb', 'in', 'a', 'broad', 'range', 'of', 'frequencies', 'these', 'constraints', 'have', 'already', 're... | [-0.11791818971254837, 0.1440904194135549, -0.026697547524236143, 0.06434846294782678, -0.07450996916756865, -0.12493310493064692, 0.0691134098884209, 0.3758560107278361, -0.1595301910380619, -0.3755115480602694, 0.07344424747547286, -0.27772689498709263, -0.07335002471793543, 0.2529886932021032, 0.060426459974936536, ... |
710.1945 | Measurement of the angular resolution of the ARGO-YBJ detector | The ARGO-YBJ experiment is a full coverage EAS-array installed at the
YangBaJing Cosmic Ray Laboratory (4300 m a.s.l., Tibet, P.R. China). We present
the results on the angular resolution measured with different methods with the
full central carpet. The comparison of experimental results with MC simulations
is discus... | astro-ph | the argoybj experiment is a full coverage easarray installed at the yangbajing cosmic ray laboratory 4300 m asl tibet pr china we present the results on the angular resolution measured with different methods with the full central carpet the comparison of experimental results with mc simulations is discussed | [['the', 'argoybj', 'experiment', 'is', 'a', 'full', 'coverage', 'easarray', 'installed', 'at', 'the', 'yangbajing', 'cosmic', 'ray', 'laboratory', '4300', 'm', 'asl', 'tibet', 'pr', 'china', 'we', 'present', 'the', 'results', 'on', 'the', 'angular', 'resolution', 'measured', 'with', 'different', 'methods', 'with', 'th... | [-0.11825939746415044, 0.12565465917454122, -0.028634773220549872, 0.07825985357185151, -0.014466867276883505, -0.025933178092174707, -0.05135275647935874, 0.3777833864033381, -0.12970293647153897, -0.40543454964744285, 0.04432183277218583, -0.4162836266146537, 0.008151043127191828, 0.2551425367623488, 0.02647076929582... |
710.1946 | A deep, high resolution survey of the low frequency radio sky | We report on the first wide-field, very long baseline interferometry (VLBI)
survey at 90 cm. The survey area consists of two overlapping 28 deg^2 fields
centred on the quasar J0226+3421 and the gravitational lens B0218+357. A total
of 618 sources were targeted in these fields, based on identifications from
Westerbork... | astro-ph | we report on the first widefield very long baseline interferometry vlbi survey at 90 cm the survey area consists of two overlapping 28 deg2 fields centred on the quasar j02263421 and the gravitational lens b0218357 a total of 618 sources were targeted in these fields based on identifications from westerbork northern sk... | [['we', 'report', 'on', 'the', 'first', 'widefield', 'very', 'long', 'baseline', 'interferometry', 'vlbi', 'survey', 'at', '90', 'cm', 'the', 'survey', 'area', 'consists', 'of', 'two', 'overlapping', '28', 'deg2', 'fields', 'centred', 'on', 'the', 'quasar', 'j02263421', 'and', 'the', 'gravitational', 'lens', 'b0218357'... | [-0.10656485364698728, 0.0916276518445538, -0.015969152480591924, 0.05675217062567494, -0.1242880650382603, -0.046610751708171194, 0.059977144147364464, 0.44117902348540267, -0.12417830171975858, -0.39271136728799616, 0.17272171717082455, -0.3523180506011585, -0.0036589503848963247, 0.24446510148082612, 0.0051792064377... |
710.1947 | Results from Droxo. I. The variability of fluorescent Fe 6.4 keV
emission in the young star Elias 29: High-energy electrons in the star's
accretion tubes? | AIMS. We study the variability of the Fe 6.4 KeV emission line from the Class
I young stellar object Elias 29 in the Rho-Oph cloud. METHODS. We analysed the
data from Elias 29 collected by XMM during a nine-day, nearly continuous
observation of the Rho-Oph star-forming region (the Deep Rho-Oph X-ray
Observation, name... | astro-ph | aims we study the variability of the fe 64 kev emission line from the class i young stellar object elias 29 in the rhooph cloud methods we analysed the data from elias 29 collected by xmm during a nineday nearly continuous observation of the rhooph starforming region the deep rhooph xray observation named droxo the dat... | [['aims', 'we', 'study', 'the', 'variability', 'of', 'the', 'fe', '64', 'kev', 'emission', 'line', 'from', 'the', 'class', 'i', 'young', 'stellar', 'object', 'elias', '29', 'in', 'the', 'rhooph', 'cloud', 'methods', 'we', 'analysed', 'the', 'data', 'from', 'elias', '29', 'collected', 'by', 'xmm', 'during', 'a', 'nineda... | [-0.07345124209684709, 0.12474568319191073, -0.021943686678450248, 0.09003790251808155, -0.041687109080408145, -0.07151930758926095, 0.09755874630127855, 0.47059173982402464, -0.1870684384500796, -0.359012212768761, 0.06649162826275692, -0.319617413783258, 0.011242179200053215, 0.163340716137884, -0.008002141743835378,... |
710.1948 | Selection of Surviving Primary Protons at 4300 m a.s.l. with the
ARGO-YBJ experiment | The primary proton spectrum up to 100 TeV has been investigated by balloon-
and satellite-borne instruments. Above this energy range only ground-based air
shower arrays can measure the cosmic ray spectrum with a technique moderately
sensitive to nuclear composition. An array which exploits the full coverage
approach ... | astro-ph | the primary proton spectrum up to 100 tev has been investigated by balloon and satelliteborne instruments above this energy range only groundbased air shower arrays can measure the cosmic ray spectrum with a technique moderately sensitive to nuclear composition an array which exploits the full coverage approach at very... | [['the', 'primary', 'proton', 'spectrum', 'up', 'to', '100', 'tev', 'has', 'been', 'investigated', 'by', 'balloon', 'and', 'satelliteborne', 'instruments', 'above', 'this', 'energy', 'range', 'only', 'groundbased', 'air', 'shower', 'arrays', 'can', 'measure', 'the', 'cosmic', 'ray', 'spectrum', 'with', 'a', 'technique'... | [-0.07567731621785193, 0.23620864683161782, -0.03776199035493173, 0.13671859094642072, -0.0344241694253906, -0.05213494196545157, -0.018220941607627696, 0.39686121985198947, -0.21728340821986006, -0.44319592545351644, 0.021831223195763378, -0.3508568843019994, 0.039803673073238746, 0.22770980460840592, 0.02041661838875... |
710.1949 | Distributed Source Coding Using Continuous-Valued Syndromes | This paper addresses the problem of coding a continuous random source
correlated with another source which is only available at the decoder. The
proposed approach is based on the extension of the channel coding concept of
syndrome from the discrete into the continuous domain. If the correlation
between the sources ca... | cs.IT math.IT | this paper addresses the problem of coding a continuous random source correlated with another source which is only available at the decoder the proposed approach is based on the extension of the channel coding concept of syndrome from the discrete into the continuous domain if the correlation between the sources can be... | [['this', 'paper', 'addresses', 'the', 'problem', 'of', 'coding', 'a', 'continuous', 'random', 'source', 'correlated', 'with', 'another', 'source', 'which', 'is', 'only', 'available', 'at', 'the', 'decoder', 'the', 'proposed', 'approach', 'is', 'based', 'on', 'the', 'extension', 'of', 'the', 'channel', 'coding', 'conce... | [-0.12560151670455794, 0.05415488684192058, -0.09567086094024557, 0.04820963024955105, -0.018558154124076718, -0.21071463960257394, 0.07470035556341625, 0.3875216110437005, -0.3044688953431668, -0.2544033371325996, 0.12468125435946233, -0.24269676557569592, -0.1616937583450366, 0.2103706891682965, -0.1076070244010124, ... |
710.195 | A radiation condition for uniqueness in a wave propagation problem for
2-D open waveguides | We study the uniqueness of solutions of Helmholtz equation for a problem that
concerns wave propagation in waveguides. The classical radiation condition does
not apply to our problem because the inhomogeneity of the index of refraction
extends to infinity in one direction. Also, because of the presence of a
waveguide... | math.AP | we study the uniqueness of solutions of helmholtz equation for a problem that concerns wave propagation in waveguides the classical radiation condition does not apply to our problem because the inhomogeneity of the index of refraction extends to infinity in one direction also because of the presence of a waveguide some... | [['we', 'study', 'the', 'uniqueness', 'of', 'solutions', 'of', 'helmholtz', 'equation', 'for', 'a', 'problem', 'that', 'concerns', 'wave', 'propagation', 'in', 'waveguides', 'the', 'classical', 'radiation', 'condition', 'does', 'not', 'apply', 'to', 'our', 'problem', 'because', 'the', 'inhomogeneity', 'of', 'the', 'ind... | [-0.1482515260420677, 0.09068028383877054, -0.08146008380352199, 0.04304285467985798, -0.121301900935868, -0.1022262820668769, 0.011162104208351058, 0.33376315560880576, -0.2707296237153854, -0.25491279241151543, 0.1023574184368075, -0.23575637009979947, -0.14049231075630875, 0.2160421862274784, -0.03902969356164524, 0... |
710.1951 | Simulation of Tau Decays in the Herwig++ Event Generator | We describe the simulation of tau decays in the Herwig++ event generator,
which includes sophisticated modelling of the hadronic currents and full
treatment of spin correlation effects. The structure of the simulation makes it
easy to add new models of tau decay,change the parameters of the existing
models, and use t... | hep-ph | we describe the simulation of tau decays in the herwig event generator which includes sophisticated modelling of the hadronic currents and full treatment of spin correlation effects the structure of the simulation makes it easy to add new models of tau decaychange the parameters of the existing models and use the model... | [['we', 'describe', 'the', 'simulation', 'of', 'tau', 'decays', 'in', 'the', 'herwig', 'event', 'generator', 'which', 'includes', 'sophisticated', 'modelling', 'of', 'the', 'hadronic', 'currents', 'and', 'full', 'treatment', 'of', 'spin', 'correlation', 'effects', 'the', 'structure', 'of', 'the', 'simulation', 'makes',... | [-0.050868979606189225, 0.1710850259621542, -0.05549432492667907, 0.15508988074664223, -0.052385856956243516, -0.12085919565472164, -0.020621349095170827, 0.3406477783316452, -0.25619523021894947, -0.29627362317160555, 0.054645413423790354, -0.29098415864925636, -0.0377123534287277, 0.18184300341128715, 0.0678627365611... |
710.1952 | Global neutrino parameter estimation using Markov Chain Monte Carlo | We present a Markov Chain Monte Carlo global analysis of neutrino parameters
using both cosmological and experimental data. Results are presented for the
combination of all presently available data from oscillation experiments,
cosmology, and neutrinoless double beta decay. In addition we explicitly study
the interpl... | hep-ph astro-ph | we present a markov chain monte carlo global analysis of neutrino parameters using both cosmological and experimental data results are presented for the combination of all presently available data from oscillation experiments cosmology and neutrinoless double beta decay in addition we explicitly study the interplay bet... | [['we', 'present', 'a', 'markov', 'chain', 'monte', 'carlo', 'global', 'analysis', 'of', 'neutrino', 'parameters', 'using', 'both', 'cosmological', 'and', 'experimental', 'data', 'results', 'are', 'presented', 'for', 'the', 'combination', 'of', 'all', 'presently', 'available', 'data', 'from', 'oscillation', 'experiment... | [-0.009972472870236284, 0.24298735727955187, -0.010235733117212306, 0.19867482626872077, -0.06342975507173074, -0.15859670578348603, 0.053596005332400345, 0.34231609122438744, -0.2623448319282833, -0.2875320654167988, 0.09274712382754373, -0.33170456698184814, -0.04679589025973046, 0.2772855468652119, 0.160474211489270... |
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