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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710.2353 | A Criterion For Ergodicity of Non-uniformly hyperbolic Diffeomorphisms | In this work we exhibit a new criteria for ergodicity of diffeomorphisms
involving conditions on Lyapunov exponents and general position of some
invariant manifolds. On one hand we derive uniqueness of SRB-measures for
transitive surface diffeomorphisms. On the other hand, using recent results on
the existence of ble... | math.DS | in this work we exhibit a new criteria for ergodicity of diffeomorphisms involving conditions on lyapunov exponents and general position of some invariant manifolds on one hand we derive uniqueness of srbmeasures for transitive surface diffeomorphisms on the other hand using recent results on the existence of blenders ... | [['in', 'this', 'work', 'we', 'exhibit', 'a', 'new', 'criteria', 'for', 'ergodicity', 'of', 'diffeomorphisms', 'involving', 'conditions', 'on', 'lyapunov', 'exponents', 'and', 'general', 'position', 'of', 'some', 'invariant', 'manifolds', 'on', 'one', 'hand', 'we', 'derive', 'uniqueness', 'of', 'srbmeasures', 'for', 't... | [-0.20196807024547378, 0.06356831925694605, -0.08580794822223284, 0.07148191412577305, -0.08663287419020324, -0.16615104134748312, 0.029805762982751068, 0.3219981469871552, -0.20750513865700546, -0.20014404379636855, 0.1519324707852148, -0.26377155125531293, -0.15433182635319395, 0.23252589147651215, -0.137862982039616... |
710.2354 | Deformed Quantum Cohomology and (0,2) Mirror Symmetry | We compute instanton corrections to correlators in the genus-zero topological
subsector of a (0,2) supersymmetric gauged linear sigma model with target space
P1xP1, whose left-moving fermions couple to a deformation of the tangent
bundle. We then deduce the theory's chiral ring from these correlators, which
reduces i... | hep-th | we compute instanton corrections to correlators in the genuszero topological subsector of a 02 supersymmetric gauged linear sigma model with target space p1xp1 whose leftmoving fermions couple to a deformation of the tangent bundle we then deduce the theorys chiral ring from these correlators which reduces in the limit... | [['we', 'compute', 'instanton', 'corrections', 'to', 'correlators', 'in', 'the', 'genuszero', 'topological', 'subsector', 'of', 'a', '02', 'supersymmetric', 'gauged', 'linear', 'sigma', 'model', 'with', 'target', 'space', 'p1xp1', 'whose', 'leftmoving', 'fermions', 'couple', 'to', 'a', 'deformation', 'of', 'the', 'tang... | [-0.13735308762356316, 0.10190320098105154, -0.11149449008719428, 0.05127117819780403, -0.06016126597988541, -0.12365986260777825, 0.014846062577461176, 0.3100105060628899, -0.23507399752776584, -0.24055821674688638, 0.0648444202341362, -0.29305070186155324, -0.16075897695112001, 0.10186540392865225, -0.055049083992818... |
710.2355 | Parametric internal waves in a compressible fluid | We describe the effect of vibration on a confined volume of fluid which is
density stratified due to its compressibility. We show that internal
gravity-acoustic waves can be parametrically destabilized by the vibration. The
resulting instability is similar to the classic Faraday instability of surface
waves, albeit m... | physics.flu-dyn physics.gen-ph | we describe the effect of vibration on a confined volume of fluid which is density stratified due to its compressibility we show that internal gravityacoustic waves can be parametrically destabilized by the vibration the resulting instability is similar to the classic faraday instability of surface waves albeit modifie... | [['we', 'describe', 'the', 'effect', 'of', 'vibration', 'on', 'a', 'confined', 'volume', 'of', 'fluid', 'which', 'is', 'density', 'stratified', 'due', 'to', 'its', 'compressibility', 'we', 'show', 'that', 'internal', 'gravityacoustic', 'waves', 'can', 'be', 'parametrically', 'destabilized', 'by', 'the', 'vibration', 't... | [-0.1775635245792342, 0.2558490178886462, -0.1245745991596557, 0.03968275276675933, -0.07960849500853907, -0.08555661283687434, 0.020531968555808293, 0.2824007253811667, -0.3148011249546526, -0.24940564522914815, 0.09638324582413065, -0.2243670987699068, -0.16305999957363715, 0.17918674565964576, -0.02391366051001982, ... |
710.2356 | Patchy sticky hard spheres: analytical study and Monte Carlo simulations | We consider a fluid of hard spheres bearing one or two uniform circular
adhesive patches, distributed so as not to overlap. Two spheres interact via a
``sticky'' Baxter potential if the line joining the centers of the two spheres
intersects a patch on each sphere, and via a hard sphere potential otherwise.
We analyze... | cond-mat.stat-mech cond-mat.soft | we consider a fluid of hard spheres bearing one or two uniform circular adhesive patches distributed so as not to overlap two spheres interact via a sticky baxter potential if the line joining the centers of the two spheres intersects a patch on each sphere and via a hard sphere potential otherwise we analyze the locat... | [['we', 'consider', 'a', 'fluid', 'of', 'hard', 'spheres', 'bearing', 'one', 'or', 'two', 'uniform', 'circular', 'adhesive', 'patches', 'distributed', 'so', 'as', 'not', 'to', 'overlap', 'two', 'spheres', 'interact', 'via', 'a', 'sticky', 'baxter', 'potential', 'if', 'the', 'line', 'joining', 'the', 'centers', 'of', 't... | [-0.12835048657211487, 0.0908822604426766, -0.08731431866317083, 0.038114334559982, -0.02061632396239857, -0.08408985172058935, 0.054856316268631196, 0.37218038774765677, -0.23825778510795784, -0.2846563996749312, 0.08174513262766196, -0.29439847587572987, -0.1149779414969157, 0.12127601738070425, 0.025433805600382543,... |
710.2357 | Overhang | How far off the edge of the table can we reach by stacking $n$ identical,
homogeneous, frictionless blocks of length 1? A classical solution achieves an
overhang of $1/2 H_n$, where $H_n ~ \ln n$ is the $n$th harmonic number. This
solution is widely believed to be optimal. We show, however, that it is, in
fact, expon... | math.HO math-ph math.CO math.MP | how far off the edge of the table can we reach by stacking n identical homogeneous frictionless blocks of length 1 a classical solution achieves an overhang of 12 h_n where h_n ln n is the nth harmonic number this solution is widely believed to be optimal we show however that it is in fact exponentially far from optima... | [['how', 'far', 'off', 'the', 'edge', 'of', 'the', 'table', 'can', 'we', 'reach', 'by', 'stacking', 'n', 'identical', 'homogeneous', 'frictionless', 'blocks', 'of', 'length', '1', 'a', 'classical', 'solution', 'achieves', 'an', 'overhang', 'of', '12', 'h_n', 'where', 'h_n', 'ln', 'n', 'is', 'the', 'nth', 'harmonic', 'n... | [-0.17199117412169773, 0.15186211878162187, -0.03175159948567549, 0.029629801775639255, -0.010527881514281034, -0.1777972041008373, 0.03835310942182938, 0.3761807602643967, -0.3108832106863459, -0.2649279456337293, 0.10594270349790652, -0.301337929541866, -0.1387394269850726, 0.16617661137133838, -0.055406809688235324,... |
710.2358 | Success and failure of programming environments - report on the design
and use of a graphic abstract syntax tree editor | The STAPLE project investigated (at the end of the eighties), a persistent
architecture for functional programming. Work has been done in two directions:
the development of a programming environment for a functional language within a
persistent system and an experiment on transferring the expertise of functional
prot... | cs.PL cs.HC | the staple project investigated at the end of the eighties a persistent architecture for functional programming work has been done in two directions the development of a programming environment for a functional language within a persistent system and an experiment on transferring the expertise of functional prototyping... | [['the', 'staple', 'project', 'investigated', 'at', 'the', 'end', 'of', 'the', 'eighties', 'a', 'persistent', 'architecture', 'for', 'functional', 'programming', 'work', 'has', 'been', 'done', 'in', 'two', 'directions', 'the', 'development', 'of', 'a', 'programming', 'environment', 'for', 'a', 'functional', 'language',... | [-0.09313105635765868, 0.02826379483065886, -0.10390148827662835, 0.07726124805608728, -0.10237382974726363, -0.0822402036910017, 0.03557675592086385, 0.37558541430805165, -0.25919246916265154, -0.3300355362992447, 0.09078543949670767, -0.23708023516855276, -0.1559932408014832, 0.16536053348458013, -0.07791437325067818... |
710.2359 | Stretching of the toroidal field and generation of magnetosonic waves in
differentially rotating plasma | We evaluate the generation of magnetosonic waves in differentially rotating
magnetized plasma. Differential rotation leads to an increase of the azimuthal
field by winding up the poloidal field lines into the toroidal field lines. An
amplification of weak seed perturbations is considered in this time-dependent
backgr... | astro-ph | we evaluate the generation of magnetosonic waves in differentially rotating magnetized plasma differential rotation leads to an increase of the azimuthal field by winding up the poloidal field lines into the toroidal field lines an amplification of weak seed perturbations is considered in this timedependent background ... | [['we', 'evaluate', 'the', 'generation', 'of', 'magnetosonic', 'waves', 'in', 'differentially', 'rotating', 'magnetized', 'plasma', 'differential', 'rotation', 'leads', 'to', 'an', 'increase', 'of', 'the', 'azimuthal', 'field', 'by', 'winding', 'up', 'the', 'poloidal', 'field', 'lines', 'into', 'the', 'toroidal', 'fiel... | [-0.25107749561784265, 0.21613538914148786, -0.02426358361971443, 0.04335719931227884, -0.06314137019217014, -0.020481004759304873, -0.08344316049909178, 0.3172395280967264, -0.2679287852597949, -0.28709020491932397, 0.0566052755305503, -0.20334007825864397, -0.02660011464183259, 0.22062618306676007, -0.001691642500784... |
710.236 | RH Sneutrino Condensate CDM and the Baryon-to-Dark Matter Ratio | The similarity of the observed mass densities of baryons and cold dark matter
may be a sign they have a related origin. The baryon-to-dark matter ratio can
be understood in the MSSM with right-handed (RH) neutrinos if CDM is due to a d
= 4 flat direction condensate of very weakly coupled RH sneutrino LSPs and the
bar... | hep-ph astro-ph hep-th | the similarity of the observed mass densities of baryons and cold dark matter may be a sign they have a related origin the baryontodark matter ratio can be understood in the mssm with righthanded rh neutrinos if cdm is due to a d 4 flat direction condensate of very weakly coupled rh sneutrino lsps and the baryon asymme... | [['the', 'similarity', 'of', 'the', 'observed', 'mass', 'densities', 'of', 'baryons', 'and', 'cold', 'dark', 'matter', 'may', 'be', 'a', 'sign', 'they', 'have', 'a', 'related', 'origin', 'the', 'baryontodark', 'matter', 'ratio', 'can', 'be', 'understood', 'in', 'the', 'mssm', 'with', 'righthanded', 'rh', 'neutrinos', '... | [-0.17109338549130104, 0.34997409195365276, -0.0817690539666835, 0.2136167001335279, -0.1120911334257792, -0.1982276345438817, -0.034534058352822763, 0.31524470212924127, -0.24190286498735933, -0.3159137425190933, 0.00556671304272159, -0.29108127383515237, 0.02661780287128161, 0.051362107581157675, 0.05304281435194699,... |
710.2361 | Response to Nauenberg's "Critique of Quantum Enigma: Physics Encounters
Consciousness" | Nauenberg's extended critique of Quantum Enigma rests on fundamental
misunderstandings.
| quant-ph | nauenbergs extended critique of quantum enigma rests on fundamental misunderstandings | [['nauenbergs', 'extended', 'critique', 'of', 'quantum', 'enigma', 'rests', 'on', 'fundamental', 'misunderstandings']] | [-0.09979881703232725, 0.056734468787908554, -0.25842876277036136, 0.11498284546865357, -0.26624174498849446, -0.23779510044389301, 0.12227448828828831, 0.14060048614111212, -0.14042178872558805, -0.2953195035871532, 0.07067860725025336, -0.21360665890905592, -0.20820170806513894, 0.24684322045909035, -0.27946785899500... |
710.2362 | Application of multifractal wavelet analysis to spontaneous fermentation
processes | An algorithm is presented here to get more detailed information, of mixed
culture type, based exclusively on the biomass concentration data for
fermentation processes. The analysis is performed with only the on-line
measurements of the redox potential being available. It is a two-step procedure
which includes an Arti... | physics.bio-ph | an algorithm is presented here to get more detailed information of mixed culture type based exclusively on the biomass concentration data for fermentation processes the analysis is performed with only the online measurements of the redox potential being available it is a twostep procedure which includes an artificial n... | [['an', 'algorithm', 'is', 'presented', 'here', 'to', 'get', 'more', 'detailed', 'information', 'of', 'mixed', 'culture', 'type', 'based', 'exclusively', 'on', 'the', 'biomass', 'concentration', 'data', 'for', 'fermentation', 'processes', 'the', 'analysis', 'is', 'performed', 'with', 'only', 'the', 'online', 'measureme... | [-0.029431377356353726, 0.059252998782481414, -0.10173601837783691, 0.042929429877359884, -0.02072542546797664, -0.08772585087365681, 0.07072910073217034, 0.37050522007648984, -0.25830432258531333, -0.26405037639121853, 0.12987338763102138, -0.25997459975581977, -0.2111501219483363, 0.21876551115870355, -0.033446941697... |
710.2363 | Global duality, signature calculus and the discrete logarithm problem | We study the discrete logarithm problem for the multiplicative group and for
elliptic curves over a finite field by using a lifting of the corresponding
object to an algebraic number field and global duality. We introduce the
\textit{signature} of a Dirichlet character (in the multiplicative group case)
or principal ... | math.NT | we study the discrete logarithm problem for the multiplicative group and for elliptic curves over a finite field by using a lifting of the corresponding object to an algebraic number field and global duality we introduce the textitsignature of a dirichlet character in the multiplicative group case or principal homogene... | [['we', 'study', 'the', 'discrete', 'logarithm', 'problem', 'for', 'the', 'multiplicative', 'group', 'and', 'for', 'elliptic', 'curves', 'over', 'a', 'finite', 'field', 'by', 'using', 'a', 'lifting', 'of', 'the', 'corresponding', 'object', 'to', 'an', 'algebraic', 'number', 'field', 'and', 'global', 'duality', 'we', 'i... | [-0.14871472086501764, 0.0468420038428032, -0.14048094063650304, 0.06613967401733366, -0.09907489090555292, -0.0979416583363405, 0.03462691983555024, 0.32218202897438813, -0.3712396956067167, -0.25456505508490784, 0.11667172432256241, -0.22300817531661368, -0.1512849350555745, 0.2124643846456071, -0.10211202497000568, ... |
710.2364 | A systematic approach to the solution of the constraints of quantum
gravity: The full theory | This is the third paper in a series outlining an algorithm to construct
finite states of quantum gravity in Ashtekar variables. In this paper we treat
the case of the Klein--Gordon field quantized with gravity on the same footing.
We address the full theory, outlining the solution to the constraints and the
construct... | gr-qc | this is the third paper in a series outlining an algorithm to construct finite states of quantum gravity in ashtekar variables in this paper we treat the case of the kleingordon field quantized with gravity on the same footing we address the full theory outlining the solution to the constraints and the construction of ... | [['this', 'is', 'the', 'third', 'paper', 'in', 'a', 'series', 'outlining', 'an', 'algorithm', 'to', 'construct', 'finite', 'states', 'of', 'quantum', 'gravity', 'in', 'ashtekar', 'variables', 'in', 'this', 'paper', 'we', 'treat', 'the', 'case', 'of', 'the', 'kleingordon', 'field', 'quantized', 'with', 'gravity', 'on', ... | [-0.13545040113908446, 0.09891092681551081, -0.1187241321942788, 0.054077325996405884, -0.06934389295513808, -0.08834841190267126, 0.03831911687465974, 0.26909732596226493, -0.2776657009535298, -0.2568488165032955, 0.08052139776480878, -0.24012205387199564, -0.14049911919068925, 0.12596085106915966, -0.0493127924927073... |
710.2365 | Detection of nuclear magnetic resonance with an anisotropic
magnetoresistive sensor | We report detection of nuclear magnetic resonance (NMR) using an anisotropic
magnetoresistive (AMR) sensor. A ``remote-detection'' arrangement was used, in
which protons in flowing water were pre-polarized in the field of a
superconducting NMR magnet, adiabatically inverted, and subsequently detected
with an AMR sens... | physics.chem-ph physics.atom-ph | we report detection of nuclear magnetic resonance nmr using an anisotropic magnetoresistive amr sensor a remotedetection arrangement was used in which protons in flowing water were prepolarized in the field of a superconducting nmr magnet adiabatically inverted and subsequently detected with an amr sensor situated down... | [['we', 'report', 'detection', 'of', 'nuclear', 'magnetic', 'resonance', 'nmr', 'using', 'an', 'anisotropic', 'magnetoresistive', 'amr', 'sensor', 'a', 'remotedetection', 'arrangement', 'was', 'used', 'in', 'which', 'protons', 'in', 'flowing', 'water', 'were', 'prepolarized', 'in', 'the', 'field', 'of', 'a', 'supercond... | [-0.1397368469172054, 0.1923607403069683, 0.007014257020302235, -0.09097625846449758, -0.05970568038081558, -0.18554934958321234, -0.047973690554499626, 0.42925350965251996, -0.2580768421425351, -0.36063161947660977, 0.04824181824981693, -0.2773202739892498, -0.05908110247008384, 0.25124910398430766, 0.0344343232434420... |
710.2366 | New Worlds on the Horizon: Earth-Sized Planets Close to Other Stars | The search for habitable planets like Earth around other stars fulfils an
ancient imperative to understand our origins and place in the cosmos. The past
decade has seen the discovery of hundreds of planets, but nearly all are gas
giants like Jupiter and Saturn. Recent advances in instrumentation and new
missions are ... | astro-ph | the search for habitable planets like earth around other stars fulfils an ancient imperative to understand our origins and place in the cosmos the past decade has seen the discovery of hundreds of planets but nearly all are gas giants like jupiter and saturn recent advances in instrumentation and new missions are exten... | [['the', 'search', 'for', 'habitable', 'planets', 'like', 'earth', 'around', 'other', 'stars', 'fulfils', 'an', 'ancient', 'imperative', 'to', 'understand', 'our', 'origins', 'and', 'place', 'in', 'the', 'cosmos', 'the', 'past', 'decade', 'has', 'seen', 'the', 'discovery', 'of', 'hundreds', 'of', 'planets', 'but', 'nea... | [-0.08943195875622408, 0.1919939850005785, -0.07618526760034444, 0.09304707517288827, -0.17522798282874189, -0.03847532967726389, 0.06856925049948136, 0.35681192802522727, -0.18360337310629646, -0.36952390994619183, 0.13487994012979382, -0.3313343247504738, -0.11559328320246887, 0.24919052719804874, -0.0782767272084890... |
710.2367 | Rubidium and lead abundances in giant stars of the globular clusters M4
and M5 | We present measurements of the neutron-capture elements Rb and Pb for bright
giants in the globular clusters M4 and M5. The clusters are of similar
metallicity ([Fe/H] = -1.2) but M4 is decidedly s-process enriched relative to
M5: [Ba/Fe] = +0.6 for M4 but 0.0 for M5. The Rb and Pb abundances were derived
by comparin... | astro-ph | we present measurements of the neutroncapture elements rb and pb for bright giants in the globular clusters m4 and m5 the clusters are of similar metallicity feh 12 but m4 is decidedly sprocess enriched relative to m5 bafe 06 for m4 but 00 for m5 the rb and pb abundances were derived by comparing synthetic spectra with... | [['we', 'present', 'measurements', 'of', 'the', 'neutroncapture', 'elements', 'rb', 'and', 'pb', 'for', 'bright', 'giants', 'in', 'the', 'globular', 'clusters', 'm4', 'and', 'm5', 'the', 'clusters', 'are', 'of', 'similar', 'metallicity', 'feh', '12', 'but', 'm4', 'is', 'decidedly', 'sprocess', 'enriched', 'relative', '... | [-0.026936020197563967, 0.17908232912080935, -0.003223487319141546, 0.06336607037911353, 0.058004262165363446, -0.1330028837412381, 0.10836689166339616, 0.4032814823753702, -0.09934004489108562, -0.4248151319763845, -0.020346924338530067, -0.4156713182411085, 0.07124667789657206, 0.13072037634153205, -0.119648267231801... |
710.2368 | Dynamical Mutation of Dark Energy | We discuss the intriguing possibility that dark energy may change its
equation of state in situations where large dark energy fluctuations are
present. We show indications of this dynamical mutation in some generic models
of dark energy.
| astro-ph hep-ph | we discuss the intriguing possibility that dark energy may change its equation of state in situations where large dark energy fluctuations are present we show indications of this dynamical mutation in some generic models of dark energy | [['we', 'discuss', 'the', 'intriguing', 'possibility', 'that', 'dark', 'energy', 'may', 'change', 'its', 'equation', 'of', 'state', 'in', 'situations', 'where', 'large', 'dark', 'energy', 'fluctuations', 'are', 'present', 'we', 'show', 'indications', 'of', 'this', 'dynamical', 'mutation', 'in', 'some', 'generic', 'mode... | [-0.20531576791325132, 0.18612244906457695, -0.13297484876789353, 0.18585213531450545, -0.05929322670390074, -0.11364510482038699, 0.0052455421222524865, 0.32761916631480326, -0.26784906536340714, -0.3440365276828006, 0.03167278621018537, -0.23514064499554602, -0.1301383319738749, 0.13176678272115216, -0.02677180502261... |
710.2369 | Graphene-on-Sapphire and Graphene-on-Glass: Raman Spectroscopy Study | The room-temperature Raman signatures from graphene layers on sapphire and
glass substrates were compared with those from graphene on GaAs substrate and
on the standard Si/SiO2 substrate, which served as a reference. It was found
that while G peak of graphene on Si/SiO2 and GaAs is positioned at 1580 cm-1 it
is down-... | cond-mat.mtrl-sci | the roomtemperature raman signatures from graphene layers on sapphire and glass substrates were compared with those from graphene on gaas substrate and on the standard sisio2 substrate which served as a reference it was found that while g peak of graphene on sisio2 and gaas is positioned at 1580 cm1 it is downshifted b... | [['the', 'roomtemperature', 'raman', 'signatures', 'from', 'graphene', 'layers', 'on', 'sapphire', 'and', 'glass', 'substrates', 'were', 'compared', 'with', 'those', 'from', 'graphene', 'on', 'gaas', 'substrate', 'and', 'on', 'the', 'standard', 'sisio2', 'substrate', 'which', 'served', 'as', 'a', 'reference', 'it', 'wa... | [-0.06531614902325802, 0.13118717319060427, 0.004521261693702804, -0.09652440092371156, 0.04041583585656351, -0.2320603255389465, 0.08671716041862965, 0.5049570204069217, -0.1798086574818525, -0.2975833690311346, 0.04371060769125405, -0.37042263216442534, -0.09905902199550636, 0.2974872938512514, 0.0014604602112538285,... |
710.237 | Using a complete spectroscopic survey to find red quasars and test the
KX method | We present an investigation of quasar colour-redshift parameter space in
order to search for radio-quiet red quasars and to test the ability of a
variant of the KX quasar selection method to detect quasars over a full range
of colour without bias. This is achieved by combining IRIS2 imaging with the
complete Fornax C... | astro-ph | we present an investigation of quasar colourredshift parameter space in order to search for radioquiet red quasars and to test the ability of a variant of the kx quasar selection method to detect quasars over a full range of colour without bias this is achieved by combining iris2 imaging with the complete fornax cluste... | [['we', 'present', 'an', 'investigation', 'of', 'quasar', 'colourredshift', 'parameter', 'space', 'in', 'order', 'to', 'search', 'for', 'radioquiet', 'red', 'quasars', 'and', 'to', 'test', 'the', 'ability', 'of', 'a', 'variant', 'of', 'the', 'kx', 'quasar', 'selection', 'method', 'to', 'detect', 'quasars', 'over', 'a',... | [-0.0037454435330306884, 0.0548450748599841, -0.08509463595893944, 0.08191778601552333, -0.1394536644476062, -0.10256095232732723, 0.11351053456700477, 0.46861325111778485, -0.11261885209719656, -0.3713075160883324, 0.034821313320702166, -0.3241711828340857, -0.02440042878707031, 0.18798387432982339, -0.050477354849198... |
710.2371 | Probing Non-Gaussianity In The Cosmic Microwave Background Anisotropies:
One Point Distribution Function | We analyze WMAP 3 year data using the one-point distribution functions to
probe the non-Gaussianity in the Cosmic Microwave Background (CMB) Anisotropy
data. Computer simulations are performed to determine the uncertainties of the
results. We report the non-Gaussianity parameter f_NL is constrained to
26<f_NL<82 for ... | astro-ph hep-th | we analyze wmap 3 year data using the onepoint distribution functions to probe the nongaussianity in the cosmic microwave background cmb anisotropy data computer simulations are performed to determine the uncertainties of the results we report the nongaussianity parameter f_nl is constrained to 26f_nl82 for qband 12f_n... | [['we', 'analyze', 'wmap', '3', 'year', 'data', 'using', 'the', 'onepoint', 'distribution', 'functions', 'to', 'probe', 'the', 'nongaussianity', 'in', 'the', 'cosmic', 'microwave', 'background', 'cmb', 'anisotropy', 'data', 'computer', 'simulations', 'are', 'performed', 'to', 'determine', 'the', 'uncertainties', 'of', ... | [-0.0962982450185691, 0.06311852241061248, -0.03486849025081275, 0.1470220945242761, -0.06979303781763982, -0.05908039594226974, 0.04009096823253874, 0.34510226528775895, -0.18533466219649478, -0.3553907126188278, 0.09056523745934779, -0.36036529467772627, 0.04516065100620311, 0.2671429412123763, 0.05151923670101974, 0... |
710.2372 | Vista, results of a model-independent search for new physics in 927
pb^-1 at CDF | A global, model-independent search for high-pT exotic phenomena is presented
using 927 pb^-1 of CDF II data. The search algorithms employed in this analysis
are Vista and Sleuth. These proceedings focus on Vista, including a description
of the method and a summary of results.
| hep-ex hep-ph | a global modelindependent search for highpt exotic phenomena is presented using 927 pb1 of cdf ii data the search algorithms employed in this analysis are vista and sleuth these proceedings focus on vista including a description of the method and a summary of results | [['a', 'global', 'modelindependent', 'search', 'for', 'highpt', 'exotic', 'phenomena', 'is', 'presented', 'using', '927', 'pb1', 'of', 'cdf', 'ii', 'data', 'the', 'search', 'algorithms', 'employed', 'in', 'this', 'analysis', 'are', 'vista', 'and', 'sleuth', 'these', 'proceedings', 'focus', 'on', 'vista', 'including', '... | [-0.045612330506132406, 0.04628218516749753, -0.17197364640676163, 0.11831276288086717, -0.12020234966290776, -0.08057791294149039, 0.039688858859749, 0.2865137442184443, -0.14664259137035432, -0.3686618523206562, 0.09917895549601367, -0.33508516128428956, -0.07775473156520589, 0.23657231117249466, 0.03671918660190634,... |
710.2373 | A Silicon-Tungsten ECal with Integrated Electronics | We summarize recent R&D progress for a silicon-tungsten electromagnetic
calorimeter (ECal) with integrated electronics, designed to meet the ILC
physics requirements.
| physics.ins-det | we summarize recent rd progress for a silicontungsten electromagnetic calorimeter ecal with integrated electronics designed to meet the ilc physics requirements | [['we', 'summarize', 'recent', 'rd', 'progress', 'for', 'a', 'silicontungsten', 'electromagnetic', 'calorimeter', 'ecal', 'with', 'integrated', 'electronics', 'designed', 'to', 'meet', 'the', 'ilc', 'physics', 'requirements']] | [-0.06420138834177383, 0.16527814613211722, -0.00010020720462004344, -0.04060412020910354, -0.16085919799904028, -0.1477701462406133, -0.1661476870732648, 0.4217378333920524, -0.144395843946508, -0.3348996850351493, 0.07500631188685518, -0.3511468189812842, -0.007697173527308873, 0.2062309379024165, 0.02579716770421890... |
710.2374 | Star cluster life-times: dependence on mass, radius and environment | The dissolution time (t_dis) of clusters in a tidal field does not scale with
the ``classical'' expression for the relaxation time. First, the scaling with
N, and hence cluster mass, is shallower due to the finite escape time of stars.
Secondly, the cluster half-mass radius is of little importance. This is due to
a b... | astro-ph | the dissolution time t_dis of clusters in a tidal field does not scale with the classical expression for the relaxation time first the scaling with n and hence cluster mass is shallower due to the finite escape time of stars secondly the cluster halfmass radius is of little importance this is due to a balance between t... | [['the', 'dissolution', 'time', 't_dis', 'of', 'clusters', 'in', 'a', 'tidal', 'field', 'does', 'not', 'scale', 'with', 'the', 'classical', 'expression', 'for', 'the', 'relaxation', 'time', 'first', 'the', 'scaling', 'with', 'n', 'and', 'hence', 'cluster', 'mass', 'is', 'shallower', 'due', 'to', 'the', 'finite', 'escap... | [-0.11482686123740977, 0.13161040952581046, -0.08512940813744733, 0.08910729687987132, -0.05688767024637365, -0.009832004432656288, 0.03613765498677619, 0.37177147816507344, -0.23092007515526514, -0.3538995151015632, 0.06078998757783929, -0.23148209344936052, -0.08689618866706296, 0.18407799651004791, -0.00405756018814... |
710.2375 | Surgery, Yamabe invariant, and Seiberg-Witten theory | By using the gluing formula of the Seiberg-Witten invariant, we compute the
Yamabe invariant Y(X) of 4-manifolds X obtained by performing surgeries along
points, circles or tori on compact Kaehler surfaces. For instance, if M is a
compact Kaehler surface of nonnegative Kodaira dimension, and N is a smooth
closed orie... | math.DG | by using the gluing formula of the seibergwitten invariant we compute the yamabe invariant yx of 4manifolds x obtained by performing surgeries along points circles or tori on compact kaehler surfaces for instance if m is a compact kaehler surface of nonnegative kodaira dimension and n is a smooth closed oriented 4manif... | [['by', 'using', 'the', 'gluing', 'formula', 'of', 'the', 'seibergwitten', 'invariant', 'we', 'compute', 'the', 'yamabe', 'invariant', 'yx', 'of', '4manifolds', 'x', 'obtained', 'by', 'performing', 'surgeries', 'along', 'points', 'circles', 'or', 'tori', 'on', 'compact', 'kaehler', 'surfaces', 'for', 'instance', 'if', ... | [-0.26816441934751045, 0.09805320425807769, -0.10446987622567723, 0.07380047365797744, -0.08907091158682541, -0.2518484605205876, -0.029308036014798186, 0.38224511737785033, -0.2223708149826815, -0.2107327588413271, 0.10122034006241348, -0.3019359354605718, -0.17092534184696212, 0.17149321956469887, -0.1530850258535675... |
710.2376 | Characteristic foliation on the discriminantal hypersurface of a
holomorphic Lagrangian fibration | We give a Kodaira-type classification of general singular fibers of a
holomorphic Lagrangian fibration in Fujiki's class $\mathcal C$. Our approach
is based on the study of the characteristic vector field of the discriminantal
hypersurface, which naturally arises from the defining equation of the
hypersurface via the... | math.AG | we give a kodairatype classification of general singular fibers of a holomorphic lagrangian fibration in fujikis class mathcal c our approach is based on the study of the characteristic vector field of the discriminantal hypersurface which naturally arises from the defining equation of the hypersurface via the symplect... | [['we', 'give', 'a', 'kodairatype', 'classification', 'of', 'general', 'singular', 'fibers', 'of', 'a', 'holomorphic', 'lagrangian', 'fibration', 'in', 'fujikis', 'class', 'mathcal', 'c', 'our', 'approach', 'is', 'based', 'on', 'the', 'study', 'of', 'the', 'characteristic', 'vector', 'field', 'of', 'the', 'discriminant... | [-0.23969109609008651, 0.008240316428558277, -0.14349957734142263, 0.023368761582899685, -0.11675108742121965, -0.14554759794973757, -0.0814175838732148, 0.28242665224657587, -0.3314179159598808, -0.17172493691211693, 0.08303552326484749, -0.2399823681948936, -0.19478459869613488, 0.22100942203940901, -0.13095790105680... |
710.2377 | Conversion Efficiencies of Heteronuclear Feshbach Molecules | We study the conversion efficiency of heteronuclear Feshbach molecules in
population imbalanced atomic gases formed by ramping the magnetic field
adiabatically. We extend the recent work [J. E. Williams et al., New J. Phys.,
8, 150 (2006)] on the theory of Feshbach molecule formations to various
combinations of quant... | cond-mat.other | we study the conversion efficiency of heteronuclear feshbach molecules in population imbalanced atomic gases formed by ramping the magnetic field adiabatically we extend the recent work j e williams et al new j phys 8 150 2006 on the theory of feshbach molecule formations to various combinations of quantum statistics o... | [['we', 'study', 'the', 'conversion', 'efficiency', 'of', 'heteronuclear', 'feshbach', 'molecules', 'in', 'population', 'imbalanced', 'atomic', 'gases', 'formed', 'by', 'ramping', 'the', 'magnetic', 'field', 'adiabatically', 'we', 'extend', 'the', 'recent', 'work', 'j', 'e', 'williams', 'et', 'al', 'new', 'j', 'phys', ... | [-0.12652585461369847, 0.1822769019295395, -0.01852485667381968, -0.026801884033983307, -0.0019709456766889033, -0.09571496241060751, 0.11465843288427485, 0.3408791947364807, -0.1780611161980778, -0.3224947591125965, -0.04130374693976981, -0.26665872644899147, -0.049578082742435595, 0.16006580701363937, -0.020146781123... |
710.2378 | Sleuth at CDF, a quasi-model-independent search for new electroweak
scale physics | These proceedings describe Sleuth, a quasi-model-independent search strategy
targeting new electroweak scale physics, and its application to 927 pb^-1 of
CDF II data. Exclusive final states are analyzed for an excess of data beyond
the Standard Model prediction at large summed scalar transverse momentum. This
analysi... | hep-ex hep-ph | these proceedings describe sleuth a quasimodelindependent search strategy targeting new electroweak scale physics and its application to 927 pb1 of cdf ii data exclusive final states are analyzed for an excess of data beyond the standard model prediction at large summed scalar transverse momentum this analysis of highp... | [['these', 'proceedings', 'describe', 'sleuth', 'a', 'quasimodelindependent', 'search', 'strategy', 'targeting', 'new', 'electroweak', 'scale', 'physics', 'and', 'its', 'application', 'to', '927', 'pb1', 'of', 'cdf', 'ii', 'data', 'exclusive', 'final', 'states', 'are', 'analyzed', 'for', 'an', 'excess', 'of', 'data', '... | [-0.031840781356687796, 0.1292528374860095, -0.09451932112587559, 0.14597680885873904, -0.09896169911900704, -0.1324954996428763, 0.03636546973421267, 0.27490318033166905, -0.2199597074597312, -0.3779006470277002, 0.04950202181653091, -0.3321065991044496, 0.0586949324263542, 0.16676119505956938, 0.09548562931630647, 0.... |
710.2379 | Connected sums with HP^n or CaP^2 and the Yamabe invariant | Let $M$ be a smooth closed $4k$-manifold whose Yamabe invariant $Y(M)$ is
nonpositive. We show that $$Y(M\sharp l \Bbb HP^k\sharp m \bar{\Bbb
HP^k})=Y(M),$$ where $l,m$ are nonnegative integers, and $\Bbb HP^k$ is the
quaternionic projective space. When $k=4$, we also have $$Y(M\sharp l
CaP^2\sharp m \bar{CaP^2})=Y(M... | math.DG | let m be a smooth closed 4kmanifold whose yamabe invariant ym is nonpositive we show that ymsharp l bbb hpksharp m barbbb hpkym where lm are nonnegative integers and bbb hpk is the quaternionic projective space when k4 we also have ymsharp l cap2sharp m barcap2ym where cap2 is the cayley plane | [['let', 'm', 'be', 'a', 'smooth', 'closed', '4kmanifold', 'whose', 'yamabe', 'invariant', 'ym', 'is', 'nonpositive', 'we', 'show', 'that', 'ymsharp', 'l', 'bbb', 'hpksharp', 'm', 'barbbb', 'hpkym', 'where', 'lm', 'are', 'nonnegative', 'integers', 'and', 'bbb', 'hpk', 'is', 'the', 'quaternionic', 'projective', 'space',... | [-0.2820817436156578, 0.1867621425799159, -0.049178706763615444, -8.321796316480221e-05, -0.12819699115704658, -0.25720101684808383, -0.1432747968315515, 0.3559612113722535, -0.25035191812487534, -0.1546462256201478, 0.09055644046341957, -0.30530820115534374, -0.1588701049277429, 0.13988816870787982, -0.087530762975125... |
710.238 | Aspects of QCD Vacuum Structure | The impact of dynamical fermions on the vacuum structure of QCD is explored.
Of particular interest is the topological charge correlator, $<q(x) q(0) >$,
where negative values at small $x$ reveal a sign-alternating layered structure
to the topological-charge density of the QCD vacuum. We consider large $28^3
\times 9... | hep-lat | the impact of dynamical fermions on the vacuum structure of qcd is explored of particular interest is the topological charge correlator qx q0 where negative values at small x reveal a signalternating layered structure to the topologicalcharge density of the qcd vacuum we consider large 283 times 96 lattices from the mi... | [['the', 'impact', 'of', 'dynamical', 'fermions', 'on', 'the', 'vacuum', 'structure', 'of', 'qcd', 'is', 'explored', 'of', 'particular', 'interest', 'is', 'the', 'topological', 'charge', 'correlator', 'qx', 'q0', 'where', 'negative', 'values', 'at', 'small', 'x', 'reveal', 'a', 'signalternating', 'layered', 'structure'... | [-0.17209368568373754, 0.21577343902630142, -0.09795931286871343, 0.05894762913273398, -0.03589518762636566, -0.0681431109274499, 0.058652514795184976, 0.32928909691868397, -0.16906033287949224, -0.2691851298143042, 0.052802070220023756, -0.2920397310773274, -0.13728179858582912, 0.08442776546268384, 0.0085407725106584... |
710.2381 | Magnetism and effect of anisotropy with one dimensional monatomic chain
of cobalt by a Monte Carlo simulation | The magnetic properties of the one dimensional (1D) monatomic chain of Co
reported in a previous experimental work are investigated by a classical Monte
Carlo simulation based on the anisotropic Heisenberg model. In our simulation,
the effect of the on-site uniaxial anisotropy, Ku, on each individual Co atom
and the ... | cond-mat.stat-mech cond-mat.mtrl-sci | the magnetic properties of the one dimensional 1d monatomic chain of co reported in a previous experimental work are investigated by a classical monte carlo simulation based on the anisotropic heisenberg model in our simulation the effect of the onsite uniaxial anisotropy ku on each individual co atom and the nearest n... | [['the', 'magnetic', 'properties', 'of', 'the', 'one', 'dimensional', '1d', 'monatomic', 'chain', 'of', 'co', 'reported', 'in', 'a', 'previous', 'experimental', 'work', 'are', 'investigated', 'by', 'a', 'classical', 'monte', 'carlo', 'simulation', 'based', 'on', 'the', 'anisotropic', 'heisenberg', 'model', 'in', 'our',... | [-0.15608719362210774, 0.15864681460273763, -0.040611265215785335, 0.03171893448188712, -0.013911846048180378, -0.10818310419905602, 0.06288390424892629, 0.37654554111627386, -0.2697797607283528, -0.28914660260117814, 0.04805573269407557, -0.28599431899869265, -0.0496343454521825, 0.1983562786281611, 0.0822800023106894... |
710.2382 | Flux Line Lattice Melting and the Formation of a Coherent Quasiparticle
Bloch State in the Ultraclean URu$_2$Si$_2$ Superconductor | We find that in ultraclean heavy-fermion superconductor URu$_2$Si$_2$
($T_{c0}=1.45$ K) a distinct flux line lattice melting transition with
outstanding characters occurs well below the mean-field upper critical fields.
We show that a very small number of carriers with heavy mass in this system
results in exceptional... | cond-mat.supr-con cond-mat.str-el | we find that in ultraclean heavyfermion superconductor uru_2si_2 t_c0145 k a distinct flux line lattice melting transition with outstanding characters occurs well below the meanfield upper critical fields we show that a very small number of carriers with heavy mass in this system results in exceptionally large thermal ... | [['we', 'find', 'that', 'in', 'ultraclean', 'heavyfermion', 'superconductor', 'uru_2si_2', 't_c0145', 'k', 'a', 'distinct', 'flux', 'line', 'lattice', 'melting', 'transition', 'with', 'outstanding', 'characters', 'occurs', 'well', 'below', 'the', 'meanfield', 'upper', 'critical', 'fields', 'we', 'show', 'that', 'a', 'v... | [-0.20026207535660692, 0.28310136808194125, -0.03330292803596477, 0.04264055298907416, 0.013172756994561273, -0.12443526495457152, 0.13988157519262892, 0.368179879616946, -0.21423449755019072, -0.2905660968615997, 0.03295895208756686, -0.31630856948619596, -0.07729212607599187, 0.14513681906902667, 0.025313251677660596... |
710.2383 | Direct Amplification of Sound By Light | A new device, the opto-acoustic parametric amplifier (OAPA), is introduced,
which is analogous to an optical parametric amplifier (OPA). The radiation
pressure reaction of light on the reflective surface of an acoustic resonator
provides nonlinearity similar to the Kerr effect in the OPA. The OAPA can be
tuned to ope... | gr-qc | a new device the optoacoustic parametric amplifier oapa is introduced which is analogous to an optical parametric amplifier opa the radiation pressure reaction of light on the reflective surface of an acoustic resonator provides nonlinearity similar to the kerr effect in the opa the oapa can be tuned to operate in two ... | [['a', 'new', 'device', 'the', 'optoacoustic', 'parametric', 'amplifier', 'oapa', 'is', 'introduced', 'which', 'is', 'analogous', 'to', 'an', 'optical', 'parametric', 'amplifier', 'opa', 'the', 'radiation', 'pressure', 'reaction', 'of', 'light', 'on', 'the', 'reflective', 'surface', 'of', 'an', 'acoustic', 'resonator',... | [-0.14229792004083225, 0.1723310027699443, -0.08785963549751524, -0.014168704240467905, -0.12263371227424086, -0.1759937885907237, 0.009354638450284615, 0.40188997744778054, -0.289514687832123, -0.21084414289712353, 0.03971648010436767, -0.3001861555248867, -0.116517712097661, 0.3112425315251321, -0.07184445569694134, ... |
710.2384 | Long-time limit for a class of quadratic infinite-dimensional dynamical
systems inspired by models of viscoelastic fluids | We study a class of quadratic, infinite-dimensional dynamical systems,
inspired by models for viscoelastic fluids. We prove that these equations
define a semi-flow on the cone of positive, essentially bounded functions. As
time tends to infinity, the solutions tend to an equilibrium manifold in the
$L^2$-norm. Conver... | math.DS math.AP | we study a class of quadratic infinitedimensional dynamical systems inspired by models for viscoelastic fluids we prove that these equations define a semiflow on the cone of positive essentially bounded functions as time tends to infinity the solutions tend to an equilibrium manifold in the l2norm convergence to a part... | [['we', 'study', 'a', 'class', 'of', 'quadratic', 'infinitedimensional', 'dynamical', 'systems', 'inspired', 'by', 'models', 'for', 'viscoelastic', 'fluids', 'we', 'prove', 'that', 'these', 'equations', 'define', 'a', 'semiflow', 'on', 'the', 'cone', 'of', 'positive', 'essentially', 'bounded', 'functions', 'as', 'time'... | [-0.16663664826333072, 0.06106111744024516, -0.11680928193329071, 0.11308107942265148, -0.07760205283535249, -0.15405143192214327, 0.008022046817297285, 0.32178570183389116, -0.32647789900445123, -0.18259865324944258, 0.15384555104802447, -0.2621328754378765, -0.18253511012616483, 0.15461803288340117, -0.09948049171009... |
710.2385 | Effect of initial condition of inflation on power and angular power
spectra in finite slow-roll inflation | The effect of the initial condition of inflation on the power spectra of
scalar and tensor perturbations is estimated assuming a slow-roll inflation
model. By defining a more general initial state in inflation particular
properties of the power spectrum such as oscillation can be revealed. The
behavior of the power s... | astro-ph | the effect of the initial condition of inflation on the power spectra of scalar and tensor perturbations is estimated assuming a slowroll inflation model by defining a more general initial state in inflation particular properties of the power spectrum such as oscillation can be revealed the behavior of the power spectr... | [['the', 'effect', 'of', 'the', 'initial', 'condition', 'of', 'inflation', 'on', 'the', 'power', 'spectra', 'of', 'scalar', 'and', 'tensor', 'perturbations', 'is', 'estimated', 'assuming', 'a', 'slowroll', 'inflation', 'model', 'by', 'defining', 'a', 'more', 'general', 'initial', 'state', 'in', 'inflation', 'particular... | [-0.1425897792298013, 0.1765072555281222, -0.1027090584686948, 0.12413246676233501, -0.05752211531616777, -0.15400965092147134, -0.06309422778626125, 0.30397913150444805, -0.2500350164802396, -0.3060137545349043, 0.08190310079710135, -0.26261039740179637, -0.0857064942384057, 0.17922891009333675, -0.010911440768045377,... |
710.2386 | Local Convexity Properties of j-metric Balls | This paper deals with local convexity properties of the j-metric. We consider
convexity and starlikeness of the j-metric balls in convex, starlike and
general subdomains of R^n.
| math.MG | this paper deals with local convexity properties of the jmetric we consider convexity and starlikeness of the jmetric balls in convex starlike and general subdomains of rn | [['this', 'paper', 'deals', 'with', 'local', 'convexity', 'properties', 'of', 'the', 'jmetric', 'we', 'consider', 'convexity', 'and', 'starlikeness', 'of', 'the', 'jmetric', 'balls', 'in', 'convex', 'starlike', 'and', 'general', 'subdomains', 'of', 'rn']] | [-0.1707483115433543, -0.01124852731892908, -0.007571578991633875, 0.06464754060100487, -0.08303776845611908, -0.06960580366905089, -0.043005853266179284, 0.3541300070506555, -0.31828376499039157, -0.12298616515127597, 0.1481755056409855, -0.35843948261053477, -0.13095430581382028, 0.05467151257174986, -0.2419639093870... |
710.2387 | Characterizing arbitrarily slow convergence in the method of alternating
projections | In 1997, Bauschke, Borwein, and Lewis have stated a trichotomy theorem that
characterizes when the convergence of the method of alternating projections can
be arbitrarily slow. However, there are two errors in their proof of this
theorem. In this note, we show that although one of the errors is critical, the
theorem ... | math.FA math.OC | in 1997 bauschke borwein and lewis have stated a trichotomy theorem that characterizes when the convergence of the method of alternating projections can be arbitrarily slow however there are two errors in their proof of this theorem in this note we show that although one of the errors is critical the theorem itself is ... | [['in', '1997', 'bauschke', 'borwein', 'and', 'lewis', 'have', 'stated', 'a', 'trichotomy', 'theorem', 'that', 'characterizes', 'when', 'the', 'convergence', 'of', 'the', 'method', 'of', 'alternating', 'projections', 'can', 'be', 'arbitrarily', 'slow', 'however', 'there', 'are', 'two', 'errors', 'in', 'their', 'proof',... | [-0.14044461060240437, 0.10334082059134012, -0.15479362317114725, 0.10672494910935733, -0.035756250500850295, -0.1273010729640808, 0.048998865657539546, 0.31795976349505883, -0.26744767644538964, -0.2452449981422945, 0.12911271633467927, -0.207643150432228, -0.17757161095706298, 0.24283947472075193, -0.176426447430845,... |
710.2388 | On Chern-Moser normal forms of strongly pseudoconvex hypersurfaces with
high-dimensional stability group | We explicitly describe germs of strongly pseudoconvex non-spherical
real-analytic hypersurfaces $M$ at the origin in $\CC^{n+1}$ for which the
group of local CR-automorphisms preserving the origin has dimension $d_0(M)$
equal to either $n^2-2n+1$ with $n\ge 2$, or $n^2-2n$ with $n\ge 3$. The
description is given in t... | math.CV | we explicitly describe germs of strongly pseudoconvex nonspherical realanalytic hypersurfaces m at the origin in ccn1 for which the group of local crautomorphisms preserving the origin has dimension d_0m equal to either n22n1 with nge 2 or n22n with nge 3 the description is given in terms of equations defining hypersur... | [['we', 'explicitly', 'describe', 'germs', 'of', 'strongly', 'pseudoconvex', 'nonspherical', 'realanalytic', 'hypersurfaces', 'm', 'at', 'the', 'origin', 'in', 'ccn1', 'for', 'which', 'the', 'group', 'of', 'local', 'crautomorphisms', 'preserving', 'the', 'origin', 'has', 'dimension', 'd_0m', 'equal', 'to', 'either', 'n... | [-0.17959201449507867, 0.04220688620909721, -0.02123539658406606, -0.022431423343912505, -0.057130041818139604, -0.13768626768449013, -0.06618182370336828, 0.3177045161661866, -0.21820785678350008, -0.21747010899963534, 0.08692592073354748, -0.2929779358290054, -0.12727717291000862, 0.14870803088338658, -0.090070776201... |
710.2389 | Entanglement of formation from optimal decomposition | We present a new method of analytically deriving the entanglement of
formation of the bipartite mixed state. The method realizes the optimal
decomposition families of states. Our method can lead to many new results
concerning entanglement of formation, its additivity and entanglement cost. We
illustrate it by investi... | quant-ph | we present a new method of analytically deriving the entanglement of formation of the bipartite mixed state the method realizes the optimal decomposition families of states our method can lead to many new results concerning entanglement of formation its additivity and entanglement cost we illustrate it by investigating... | [['we', 'present', 'a', 'new', 'method', 'of', 'analytically', 'deriving', 'the', 'entanglement', 'of', 'formation', 'of', 'the', 'bipartite', 'mixed', 'state', 'the', 'method', 'realizes', 'the', 'optimal', 'decomposition', 'families', 'of', 'states', 'our', 'method', 'can', 'lead', 'to', 'many', 'new', 'results', 'co... | [-0.12515049605415418, 0.16772979426985749, -0.1176375539543537, 0.05092860986120426, 0.044078524840565826, -0.1612203400152234, 0.0748869507931746, 0.32070469930768014, -0.2562265075170077, -0.2500487777619408, 0.09546866925576558, -0.2338583642312397, -0.10832338507931966, 0.16898620260449557, -0.01788955031392666, 0... |
710.239 | Pion form factor from all-to-all propagators of overlap quarks | We report on our calculation of the pion electromagnetic form factor with
two-flavors of dynamical overlap quarks. Gauge configurations are generated
using the Iwasaki gauge action on a 16^3 \times 32 lattice at the lattice
spacing of 0.12fm with sea quark masses down to m_s/6, where m_s is the
physical strange quark... | hep-lat | we report on our calculation of the pion electromagnetic form factor with twoflavors of dynamical overlap quarks gauge configurations are generated using the iwasaki gauge action on a 163 times 32 lattice at the lattice spacing of 012fm with sea quark masses down to m_s6 where m_s is the physical strange quark mass we ... | [['we', 'report', 'on', 'our', 'calculation', 'of', 'the', 'pion', 'electromagnetic', 'form', 'factor', 'with', 'twoflavors', 'of', 'dynamical', 'overlap', 'quarks', 'gauge', 'configurations', 'are', 'generated', 'using', 'the', 'iwasaki', 'gauge', 'action', 'on', 'a', '163', 'times', '32', 'lattice', 'at', 'the', 'lat... | [-0.101282916909882, 0.33605323916833313, -0.0853194392984733, 0.04005366414951693, -0.027856284413220626, -0.031689055451923714, 0.15381747030187398, 0.3980526494560763, -0.07238487738317677, -0.28415166144924503, 0.027690290879192097, -0.2839882985289608, -0.01739830923200186, 0.09146591520735196, 0.07676879393735102... |
710.2391 | First-principles prediction of coexistence of magnetism and
ferroelectricity in rhombohedral Bi2FeTiO6 | First principles calculations based on the density functional theory within
the local spin density approximation plus U(LSDA+U)scheme, show rhombohedral
Bi$_2$FeTiO$_6$ is a potential multiferroic in which the magnetism and
ferroelectricity coexist . A ferromagnetic configuration with magnetic moment
of 4 $\mu_B$ per... | cond-mat.mtrl-sci | first principles calculations based on the density functional theory within the local spin density approximation plus ulsdauscheme show rhombohedral bi_2fetio_6 is a potential multiferroic in which the magnetism and ferroelectricity coexist a ferromagnetic configuration with magnetic moment of 4 mu_b per formula unit h... | [['first', 'principles', 'calculations', 'based', 'on', 'the', 'density', 'functional', 'theory', 'within', 'the', 'local', 'spin', 'density', 'approximation', 'plus', 'ulsdauscheme', 'show', 'rhombohedral', 'bi_2fetio_6', 'is', 'a', 'potential', 'multiferroic', 'in', 'which', 'the', 'magnetism', 'and', 'ferroelectrici... | [-0.14783779966573302, 0.17240334446900166, -0.04964211425708177, -0.00492452248895111, 0.03171647741244389, -0.0737569565168367, 0.10515610014598888, 0.34811845333494534, -0.23361882243233806, -0.33036218112057003, -0.005871726735495031, -0.3111735673334736, -0.1194516593303818, 0.08849687671933609, 0.0364344287001026... |
710.2392 | Characterization of the Microstructure of Zirconolite-Based
Glass-Ceramics | December 1991 legislation in France has spurred research on enhanced
separation and conditioning or transmutation of long-lived radionuclides from
high level radioactive wastes (HLW). In this field, we have studied
zirconolite-based glass-ceramics in which the crystalline phase (zirconolite:
CaZrTi2O7) aimed to prefe... | cond-mat.mtrl-sci | december 1991 legislation in france has spurred research on enhanced separation and conditioning or transmutation of longlived radionuclides from high level radioactive wastes hlw in this field we have studied zirconolitebased glassceramics in which the crystalline phase zirconolite cazrti2o7 aimed to preferentially in... | [['december', '1991', 'legislation', 'in', 'france', 'has', 'spurred', 'research', 'on', 'enhanced', 'separation', 'and', 'conditioning', 'or', 'transmutation', 'of', 'longlived', 'radionuclides', 'from', 'high', 'level', 'radioactive', 'wastes', 'hlw', 'in', 'this', 'field', 'we', 'have', 'studied', 'zirconolitebased'... | [-0.0447609545869044, 0.23997485162525445, -0.12028537913579988, -0.023884320409094866, -0.007648469204396273, -0.08230488067410424, 0.07286709423879557, 0.3729474476200685, -0.2500893095903824, -0.3003212225528648, 0.10772543695273158, -0.3103006488470509, -0.05727650470201305, 0.12705581082933606, -0.0178093264514036... |
710.2393 | Demailly-Semple jets of orders 4 and 5 in dimension 2 | In view of Kobayashi's hyperbolicity conjecture, Demailly-Semple jets of
orders 4 and 5 in dimension 2 are studied, some expectations about their
algebraic tameness being (dis)proved, after systematic, substantial, formal,
manual calculations.
| math.CV math.AG | in view of kobayashis hyperbolicity conjecture demaillysemple jets of orders 4 and 5 in dimension 2 are studied some expectations about their algebraic tameness being disproved after systematic substantial formal manual calculations | [['in', 'view', 'of', 'kobayashis', 'hyperbolicity', 'conjecture', 'demaillysemple', 'jets', 'of', 'orders', '4', 'and', '5', 'in', 'dimension', '2', 'are', 'studied', 'some', 'expectations', 'about', 'their', 'algebraic', 'tameness', 'being', 'disproved', 'after', 'systematic', 'substantial', 'formal', 'manual', 'calc... | [-0.1991678224876523, 0.08108381765487138, -0.0651093753403984, 0.15775071481766645, -0.06927522736077663, -0.12840365736337844, 0.024613529501948506, 0.350635777489515, -0.21479508611082565, -0.35178587993141264, 0.11333520965854404, -0.27341443564364454, -0.03802011082007084, 0.15886744030285627, -0.15837031725095585... |
710.2394 | Recent Progress in Effective Field Theory in the One-Nucleon Sector | Chiral perturbation theory (ChPT) is the effective field theory of the strong
interactions at low energies. We will address the issue of a consistent power
counting scheme in a manifestly Lorentz-invariant formulation of baryon ChPT.
As applications we show how the inclusion of vector and axial-vector mesons in
the c... | hep-ph | chiral perturbation theory chpt is the effective field theory of the strong interactions at low energies we will address the issue of a consistent power counting scheme in a manifestly lorentzinvariant formulation of baryon chpt as applications we show how the inclusion of vector and axialvector mesons in the calculati... | [['chiral', 'perturbation', 'theory', 'chpt', 'is', 'the', 'effective', 'field', 'theory', 'of', 'the', 'strong', 'interactions', 'at', 'low', 'energies', 'we', 'will', 'address', 'the', 'issue', 'of', 'a', 'consistent', 'power', 'counting', 'scheme', 'in', 'a', 'manifestly', 'lorentzinvariant', 'formulation', 'of', 'b... | [-0.15198301051140709, 0.1631367319224142, -0.11696309504058103, 0.1283428970957175, -0.07008253600284019, -0.0506375440834638, 0.06339867684360155, 0.3264194377971923, -0.18419752447482418, -0.2522835727342788, -0.016056015668436886, -0.3007070776732529, -0.13625932961483211, 0.0825195001986097, 0.029082230935968897, ... |
710.2395 | Stability of Palatini-f(R) cosmology | The evolution of linear cosmological perturbations in modified theories of
gravity is investigated assuming the Palatini formalism. It has been discussed
about the stability problem in this model based on the equivalence between f(R)
gravity and the scalar tensor theory. However, we study this problem in the
physical... | gr-qc astro-ph | the evolution of linear cosmological perturbations in modified theories of gravity is investigated assuming the palatini formalism it has been discussed about the stability problem in this model based on the equivalence between fr gravity and the scalar tensor theory however we study this problem in the physical frame ... | [['the', 'evolution', 'of', 'linear', 'cosmological', 'perturbations', 'in', 'modified', 'theories', 'of', 'gravity', 'is', 'investigated', 'assuming', 'the', 'palatini', 'formalism', 'it', 'has', 'been', 'discussed', 'about', 'the', 'stability', 'problem', 'in', 'this', 'model', 'based', 'on', 'the', 'equivalence', 'b... | [-0.15233346247409899, 0.12785869954516077, -0.1283805456381136, 0.11203179611188788, -0.056788449813168315, -0.11104189636119242, -0.08194022011547719, 0.27062449173351366, -0.2430582221612216, -0.2763611980314766, 0.06239546258242742, -0.25871873123937156, -0.17376813150772322, 0.11276194941629433, -0.028388430046597... |
710.2396 | A peculiar two point boundary value problem | In this paper we consider a one-dimensional diffusion equation on the
interval $[0,1]$ satisfying non-Feller boundary conditions. As a consequence,
the initial value Cauchy problem fails to preserve nonnegativity or
boundedness. Nonetheless, probability theory plays an interesting role in our
analysis and understandi... | math.PR | in this paper we consider a onedimensional diffusion equation on the interval 01 satisfying nonfeller boundary conditions as a consequence the initial value cauchy problem fails to preserve nonnegativity or boundedness nonetheless probability theory plays an interesting role in our analysis and understanding of solutio... | [['in', 'this', 'paper', 'we', 'consider', 'a', 'onedimensional', 'diffusion', 'equation', 'on', 'the', 'interval', '01', 'satisfying', 'nonfeller', 'boundary', 'conditions', 'as', 'a', 'consequence', 'the', 'initial', 'value', 'cauchy', 'problem', 'fails', 'to', 'preserve', 'nonnegativity', 'or', 'boundedness', 'nonet... | [-0.13645973339832076, 0.026118761484212882, -0.0780833743143982, 0.09168191414210014, -0.08207075844499438, -0.10088559856133845, -0.004125470654495682, 0.29199528876536834, -0.30331406187421334, -0.24753728084033355, 0.16234091200264325, -0.26964140209020115, -0.15888582491364409, 0.1325972444465151, -0.0955864552136... |
710.2397 | Initial-Final Mass Relationship for Stars of Different Metallicities | Following Paczy\'{n}ski & Zi\'{o}lkowski (1968) and Han et al. (1994), we
assume that the envelope of an asymptotic giant branch (AGB) or a first giant
branch (FGB) star is lost when the binding energy of the envelope is equal to
zero ($\Delta W=0$) and the core mass of the AGB star or the FGB star at the
point ($\De... | astro-ph | following paczynski ziolkowski 1968 and han et al 1994 we assume that the envelope of an asymptotic giant branch agb or a first giant branch fgb star is lost when the binding energy of the envelope is equal to zero delta w0 and the core mass of the agb star or the fgb star at the point delta w0 is taken as the final ma... | [['following', 'paczynski', 'ziolkowski', '1968', 'and', 'han', 'et', 'al', '1994', 'we', 'assume', 'that', 'the', 'envelope', 'of', 'an', 'asymptotic', 'giant', 'branch', 'agb', 'or', 'a', 'first', 'giant', 'branch', 'fgb', 'star', 'is', 'lost', 'when', 'the', 'binding', 'energy', 'of', 'the', 'envelope', 'is', 'equal... | [-0.054385451441360776, 0.16967340831547187, -0.0655336239091728, 0.10307738096141121, -0.07085737610316795, -0.04901480836037924, 0.11607686111423443, 0.3482042463577312, -0.1160349744246375, -0.3789479976276989, 0.015841464332365635, -0.3268418484607853, 0.01748280532268362, 0.18682497444619978, -0.11234711464519774,... |
710.2398 | Differential Rotation in F Stars | Differential rotation can be detected in single line profiles of stars
rotating more rapidly than about $v \sin{i} = 10$ km s$^{-1}$ with the Fourier
transform technique. This allows to search for differential rotation in large
samples to look for correlations between differential rotation and other
stellar parameter... | astro-ph | differential rotation can be detected in single line profiles of stars rotating more rapidly than about v sini 10 km s1 with the fourier transform technique this allows to search for differential rotation in large samples to look for correlations between differential rotation and other stellar parameters i analyze the ... | [['differential', 'rotation', 'can', 'be', 'detected', 'in', 'single', 'line', 'profiles', 'of', 'stars', 'rotating', 'more', 'rapidly', 'than', 'about', 'v', 'sini', '10', 'km', 's1', 'with', 'the', 'fourier', 'transform', 'technique', 'this', 'allows', 'to', 'search', 'for', 'differential', 'rotation', 'in', 'large',... | [-0.08026686378997629, 0.1822975863662103, -0.09167459721312575, 0.10189584799758766, -0.11265025270049987, -0.10595779728711299, 0.01572075376044149, 0.4103402720845264, -0.20414643079933265, -0.37148672711994984, 0.04901712676712676, -0.3009656532972535, -0.013204882779847021, 0.22752632220761607, -0.1009691108382590... |
710.2399 | Signatures of inflow motion in cores of massive star formation:
Potential collapse candidates | Using the IRAM 30 m telescope, a mapping survey in optically thick and thin
lines was performed towards 46 high mass star-forming regions. The sample
includes UC H{\sc ii} precursors and UC H{\sc ii} regions. Seventeen sources
are found to show "blue profiles", the expected signature of collapsing cores.
The excess o... | astro-ph | using the iram 30 m telescope a mapping survey in optically thick and thin lines was performed towards 46 high mass starforming regions the sample includes uc hsc ii precursors and uc hsc ii regions seventeen sources are found to show blue profiles the expected signature of collapsing cores the excess of sources with b... | [['using', 'the', 'iram', '30', 'm', 'telescope', 'a', 'mapping', 'survey', 'in', 'optically', 'thick', 'and', 'thin', 'lines', 'was', 'performed', 'towards', '46', 'high', 'mass', 'starforming', 'regions', 'the', 'sample', 'includes', 'uc', 'hsc', 'ii', 'precursors', 'and', 'uc', 'hsc', 'ii', 'regions', 'seventeen', '... | [-0.05763595300833569, 0.15546090508735663, 0.02388696418571714, 0.09718488905440412, -0.03193071022176662, -0.08497957244351809, 0.09835529790536778, 0.4131548862778456, -0.09289629494116919, -0.3642202571789558, 0.05838593856016224, -0.2993347277789301, -0.016284173476585263, 0.11620768503210432, -0.00590449602031849... |
710.24 | On invisible plasma content in radio-loud AGNs: The case of TeV blazar
Markarian 421 | Invisible plasma content in blazar jets such as protons and/or thermal
electron-positron ($e^{\pm}$) pairs is explored through combined arguments of
dynamical and radiative processes. By comparing physical quantities required by
the internal shock model with those obtained through the observed broadband
spectra for M... | astro-ph | invisible plasma content in blazar jets such as protons andor thermal electronpositron epm pairs is explored through combined arguments of dynamical and radiative processes by comparing physical quantities required by the internal shock model with those obtained through the observed broadband spectra for mrk 421 we obt... | [['invisible', 'plasma', 'content', 'in', 'blazar', 'jets', 'such', 'as', 'protons', 'andor', 'thermal', 'electronpositron', 'epm', 'pairs', 'is', 'explored', 'through', 'combined', 'arguments', 'of', 'dynamical', 'and', 'radiative', 'processes', 'by', 'comparing', 'physical', 'quantities', 'required', 'by', 'the', 'in... | [-0.07788391668631992, 0.22664491115888288, -0.051902534837406394, 0.12796633309294067, -0.01561029942295739, -0.06903933336068899, 0.02676176753389468, 0.3640098392530852, -0.19428628511777615, -0.32232984702292633, 0.01897962239319326, -0.2906699872297628, 0.04258258514419657, 0.19611649668854947, 0.05759729917483378... |
710.2401 | Tracing non-equilibrium plasma dynamics on the attosecond timescale in
small clusters | It is shown that the energy absorption of a rare-gas cluster from a
vacuum-ultraviolet (VUV) pulse can be traced with time-delayed
extreme-ultraviolet (XUV) attosecond probe pulses by measuring the kinetic
energy of the electrons detached by the probe pulse. By means of this scheme we
demonstrate, that for pump pulse... | physics.atm-clus | it is shown that the energy absorption of a raregas cluster from a vacuumultraviolet vuv pulse can be traced with timedelayed extremeultraviolet xuv attosecond probe pulses by measuring the kinetic energy of the electrons detached by the probe pulse by means of this scheme we demonstrate that for pump pulses as short a... | [['it', 'is', 'shown', 'that', 'the', 'energy', 'absorption', 'of', 'a', 'raregas', 'cluster', 'from', 'a', 'vacuumultraviolet', 'vuv', 'pulse', 'can', 'be', 'traced', 'with', 'timedelayed', 'extremeultraviolet', 'xuv', 'attosecond', 'probe', 'pulses', 'by', 'measuring', 'the', 'kinetic', 'energy', 'of', 'the', 'electr... | [-0.0699044128716306, 0.2627082960301998, -0.10968277166653989, 0.06864707163009426, 0.03321876186369495, -0.1321337842311936, 0.03712481243366545, 0.5214589901663589, -0.2825170105577193, -0.336240974244323, 0.005081305675434343, -0.23797473039788505, 0.0031865460755811496, 0.2807535687743714, 0.016106568354492385, 0.... |
710.2402 | Intraday pattern in bid-ask spreads and its power-law relaxation for
Chinese A-share stocks | We use high-frequency data of 1364 Chinese A-share stocks traded on the
Shanghai Stock Exchange and Shenzhen Stock Exchange to investigate the intraday
patterns in the bid-ask spreads. The daily periodicity in the spread time
series is confirmed by Lomb analysis and the intraday bid-ask spreads are found
to exhibit $... | q-fin.ST physics.soc-ph | we use highfrequency data of 1364 chinese ashare stocks traded on the shanghai stock exchange and shenzhen stock exchange to investigate the intraday patterns in the bidask spreads the daily periodicity in the spread time series is confirmed by lomb analysis and the intraday bidask spreads are found to exhibit lshaped ... | [['we', 'use', 'highfrequency', 'data', 'of', '1364', 'chinese', 'ashare', 'stocks', 'traded', 'on', 'the', 'shanghai', 'stock', 'exchange', 'and', 'shenzhen', 'stock', 'exchange', 'to', 'investigate', 'the', 'intraday', 'patterns', 'in', 'the', 'bidask', 'spreads', 'the', 'daily', 'periodicity', 'in', 'the', 'spread',... | [-0.1139772500216953, 0.1535534268757776, -0.16059896820742223, 0.17248281221854528, -0.05242214722282245, -0.10814790315846474, 0.1384698683873583, 0.46809594252875125, -0.30103309682578355, -0.25077898477196187, 0.15304559379274774, -0.3823875442593016, -0.11175782818538256, 0.19888636563769263, -0.039157090297677256... |
710.2403 | Double quantum dot as a probe of nonequilibrium charge fluctuations at
the quantum point contact | Absorption of energy quanta generated by quantum point contact results in the
inelastic current through the double quantum dot placed nearby. In contrast to
a single quantum dot, the inelastic current through the double quantum dot is
sensitive to the energy dependence of the quantum point contact transmission,
which... | cond-mat.mes-hall | absorption of energy quanta generated by quantum point contact results in the inelastic current through the double quantum dot placed nearby in contrast to a single quantum dot the inelastic current through the double quantum dot is sensitive to the energy dependence of the quantum point contact transmission which can ... | [['absorption', 'of', 'energy', 'quanta', 'generated', 'by', 'quantum', 'point', 'contact', 'results', 'in', 'the', 'inelastic', 'current', 'through', 'the', 'double', 'quantum', 'dot', 'placed', 'nearby', 'in', 'contrast', 'to', 'a', 'single', 'quantum', 'dot', 'the', 'inelastic', 'current', 'through', 'the', 'double'... | [-0.13757108999551207, 0.17364735830494243, -0.04025174719214007, 0.056293113759475884, 0.002306293169765369, -0.17118000253981006, 0.09477907427978041, 0.3282492153778456, -0.31110323111162236, -0.2845196570067302, -0.0362229786131639, -0.32905068448272307, -0.11165234404683545, 0.23096128817026815, 0.0385194178535670... |
710.2404 | Probing the Origin of the Large-angle CMB Anomalies | It has been argued that the large-angle cosmic microwave background
anisotropy has anomalies at 3-sigma level. We review various proposed ideas to
explain the origin of the anomalies and discuss how we can constrain the
proposed models using future observational data.
| astro-ph | it has been argued that the largeangle cosmic microwave background anisotropy has anomalies at 3sigma level we review various proposed ideas to explain the origin of the anomalies and discuss how we can constrain the proposed models using future observational data | [['it', 'has', 'been', 'argued', 'that', 'the', 'largeangle', 'cosmic', 'microwave', 'background', 'anisotropy', 'has', 'anomalies', 'at', '3sigma', 'level', 'we', 'review', 'various', 'proposed', 'ideas', 'to', 'explain', 'the', 'origin', 'of', 'the', 'anomalies', 'and', 'discuss', 'how', 'we', 'can', 'constrain', 'th... | [-0.09147082859786546, 0.09321390339968408, -0.11275559830729191, 0.1585198952475699, -0.1341140650485347, -0.07342158307934679, -0.021366714886048944, 0.3504921229692494, -0.20196982414075515, -0.34221184822708006, 0.09879371780538704, -0.3431233400024655, -0.13483584099789944, 0.17593069946983966, -0.0084839560909242... |
710.2405 | Large deviations and adiabatic transitions for dynamical systems and
Markov processes in fully coupled averaging | The work treats systems combining slow and fast motions depending on each
other where fast motions are perturbations of families of either dynamical
systems or Markov processes with freezed slow variable. In the first case we
consider hyperbolic dynamical systems and in the second case we deal with
random evolutions ... | math.DS math.PR | the work treats systems combining slow and fast motions depending on each other where fast motions are perturbations of families of either dynamical systems or markov processes with freezed slow variable in the first case we consider hyperbolic dynamical systems and in the second case we deal with random evolutions whi... | [['the', 'work', 'treats', 'systems', 'combining', 'slow', 'and', 'fast', 'motions', 'depending', 'on', 'each', 'other', 'where', 'fast', 'motions', 'are', 'perturbations', 'of', 'families', 'of', 'either', 'dynamical', 'systems', 'or', 'markov', 'processes', 'with', 'freezed', 'slow', 'variable', 'in', 'the', 'first',... | [-0.15347683916268784, 0.17838017440131196, -0.05093419267665421, 0.0447624483903017, -0.03862924995248981, -0.12707710090075908, 0.01995780254348625, 0.389412814481445, -0.33167438239955876, -0.23633451179261797, 0.17027599514771044, -0.25806981962278625, -0.12182775494712188, 0.19350064469057474, -0.02506656677105298... |
710.2406 | Quasi-exactly solvable quasinormal modes | We consider quasinormal modes with complex energies from the point of view of
the theory of quasi-exactly solvable (QES) models. We demonstrate that it is
possible to find new potentials which admit exactly solvable or QES quasinormal
modes by suitable complexification of parameters defining the QES potentials.
Parti... | hep-th | we consider quasinormal modes with complex energies from the point of view of the theory of quasiexactly solvable qes models we demonstrate that it is possible to find new potentials which admit exactly solvable or qes quasinormal modes by suitable complexification of parameters defining the qes potentials particularly... | [['we', 'consider', 'quasinormal', 'modes', 'with', 'complex', 'energies', 'from', 'the', 'point', 'of', 'view', 'of', 'the', 'theory', 'of', 'quasiexactly', 'solvable', 'qes', 'models', 'we', 'demonstrate', 'that', 'it', 'is', 'possible', 'to', 'find', 'new', 'potentials', 'which', 'admit', 'exactly', 'solvable', 'or'... | [-0.1278436711881364, 0.08368992126560297, -0.02889949191307676, 0.04844593068591548, -0.1028004097279863, -0.2728851760697106, -0.023679657962402678, 0.3797209498513004, -0.2241958198002607, -0.21663326119491155, 0.052518230991141085, -0.27784057804450824, -0.2326638824812582, 0.2320351814749934, 0.05652924506938544, ... |
710.2407 | Physical implementation of topologically decoherence-protected
superconducting qubits | We propose a scenario to physically implement a kind of topologically
decoherence-protected qubit using superconducting devices coupled to a
micro-wave cavity mode with unconventional geometric operations. It is shown
that the two needed interactions for selective devices, which are required for
implementing such pro... | quant-ph | we propose a scenario to physically implement a kind of topologically decoherenceprotected qubit using superconducting devices coupled to a microwave cavity mode with unconventional geometric operations it is shown that the two needed interactions for selective devices which are required for implementing such protected... | [['we', 'propose', 'a', 'scenario', 'to', 'physically', 'implement', 'a', 'kind', 'of', 'topologically', 'decoherenceprotected', 'qubit', 'using', 'superconducting', 'devices', 'coupled', 'to', 'a', 'microwave', 'cavity', 'mode', 'with', 'unconventional', 'geometric', 'operations', 'it', 'is', 'shown', 'that', 'the', '... | [-0.23582219248153583, 0.18026645979948677, -0.00013693298404157328, -0.023178499352888026, -0.026306661510358702, -0.2621567591219052, 0.07808342289435939, 0.40330821975772635, -0.2042457986560263, -0.35968856513500214, 0.054045260957117834, -0.23052566558164492, -0.12305276715353633, 0.26992883654625227, -0.041007948... |
710.2408 | Triplet Leptogenesis in Left-Right Symmetric Seesaw Models | We discuss scalar triplet leptogenesis in a specific left-right symmetric
seesaw model. We show that the Majorana phases that are present in the model
can be effectively used to saturate the existing upper limit on the
CP-asymmetry of the triplets. We solve the relevant Boltzmann equations and
analyze the viability o... | hep-ph | we discuss scalar triplet leptogenesis in a specific leftright symmetric seesaw model we show that the majorana phases that are present in the model can be effectively used to saturate the existing upper limit on the cpasymmetry of the triplets we solve the relevant boltzmann equations and analyze the viability of trip... | [['we', 'discuss', 'scalar', 'triplet', 'leptogenesis', 'in', 'a', 'specific', 'leftright', 'symmetric', 'seesaw', 'model', 'we', 'show', 'that', 'the', 'majorana', 'phases', 'that', 'are', 'present', 'in', 'the', 'model', 'can', 'be', 'effectively', 'used', 'to', 'saturate', 'the', 'existing', 'upper', 'limit', 'on', ... | [-0.11824503199473452, 0.23261245620329823, -0.0055787992886209906, 0.16836089615821345, -0.07110341590524247, -0.21051660396851005, 0.06126068020284545, 0.33931060394981, -0.2438819109445718, -0.2554668147504264, 0.057934030072466856, -0.24915722847413435, -0.039780503171866974, 0.118150274619559, 0.037210351494923896... |
710.2409 | Precise predictions for MSSM Higgs-boson production in bottom-quark
fusion | The main production mechanism for supersymmetric Higgs particles at hadron
colliders crucially depends on the size of their Yukawa couplings to bottom
quarks. For sufficiently large tan(beta) the total cross section for some of
the neutral Higgs bosons in the MSSM is dominated by bottom-quark fusion. After
an introdu... | hep-ph | the main production mechanism for supersymmetric higgs particles at hadron colliders crucially depends on the size of their yukawa couplings to bottom quarks for sufficiently large tanbeta the total cross section for some of the neutral higgs bosons in the mssm is dominated by bottomquark fusion after an introduction t... | [['the', 'main', 'production', 'mechanism', 'for', 'supersymmetric', 'higgs', 'particles', 'at', 'hadron', 'colliders', 'crucially', 'depends', 'on', 'the', 'size', 'of', 'their', 'yukawa', 'couplings', 'to', 'bottom', 'quarks', 'for', 'sufficiently', 'large', 'tanbeta', 'the', 'total', 'cross', 'section', 'for', 'some... | [-0.07663827976865466, 0.23661069558313516, -0.011242493029209998, 0.16774941067999685, -0.03951951789081489, -0.1530304527555576, 0.04663075358819282, 0.3145651929570656, -0.19002507510390787, -0.26136771437564965, 0.0031467140774781768, -0.313598814485758, 0.02710499721293321, 0.16555261178955175, 0.02742131694072955... |
710.241 | Modified Lattice Landau Gauge | We propose a modified lattice Landau gauge based on stereographically
projecting the link variables on the circle S^1 -> R for compact U(1) or the
3-sphere S^3 -> R^3 for SU(2) before imposing the Landau gauge condition. This
can reduce the number of Gribov copies exponentially and solves the Gribov
problem in compac... | hep-lat | we propose a modified lattice landau gauge based on stereographically projecting the link variables on the circle s1 r for compact u1 or the 3sphere s3 r3 for su2 before imposing the landau gauge condition this can reduce the number of gribov copies exponentially and solves the gribov problem in compact u1 where it is ... | [['we', 'propose', 'a', 'modified', 'lattice', 'landau', 'gauge', 'based', 'on', 'stereographically', 'projecting', 'the', 'link', 'variables', 'on', 'the', 'circle', 's1', 'r', 'for', 'compact', 'u1', 'or', 'the', '3sphere', 's3', 'r3', 'for', 'su2', 'before', 'imposing', 'the', 'landau', 'gauge', 'condition', 'this',... | [-0.18996380634751975, 0.19811287200005323, -0.06843125941097741, 0.0825970435832335, -0.1338052832220188, -0.1350391818365703, 0.09954937141132998, 0.35238860317451115, -0.2149560027847103, -0.2576745751624306, 0.13747732468433313, -0.22156270379748413, -0.0779119167321672, 0.03344727483094104, -0.13507901702770123, 0... |
710.2411 | The Kontsevich weight of a wheel with spokes pointing outward | This is a companion note to ``Hochschild cohomology and Atiyah classes'' by
Damien Calaque and the author. Using elementary methods we compute the
Kontsevich weight of a wheel with spokes pointing outward. The result is in
terms of modified Bernouilli numbers. The same result had been obtained earlier
by Torossian (u... | math.CO | this is a companion note to hochschild cohomology and atiyah classes by damien calaque and the author using elementary methods we compute the kontsevich weight of a wheel with spokes pointing outward the result is in terms of modified bernouilli numbers the same result had been obtained earlier by torossian unpublished... | [['this', 'is', 'a', 'companion', 'note', 'to', 'hochschild', 'cohomology', 'and', 'atiyah', 'classes', 'by', 'damien', 'calaque', 'and', 'the', 'author', 'using', 'elementary', 'methods', 'we', 'compute', 'the', 'kontsevich', 'weight', 'of', 'a', 'wheel', 'with', 'spokes', 'pointing', 'outward', 'the', 'result', 'is',... | [-0.10362441452433181, 0.07546992676916643, -0.13209660136598653, 0.06406317595431929, -0.13769787780435408, -0.11805614278162435, -0.005563755567043515, 0.3287408170369217, -0.22968537595628177, -0.33076832513719545, 0.07986671696772199, -0.2174107527707593, -0.2006121491549647, 0.19962842484651985, -0.187807555894477... |
710.2412 | Nonet symmetry in \eta, \eta^{\prime} and B\to K\eta,K\eta^{\prime}
decays | The nonet symmetry scheme seems to describe rather well the masses and
$\eta-\eta^{\prime}$ mixing angle of the ground state pseudo-scalar mesons. It
is expected that nonet symmetry should also be valid for the matrix elements of
the pseudo-scalar densitty operators which play an important role in charmless
two-body ... | hep-ph hep-ex | the nonet symmetry scheme seems to describe rather well the masses and etaetaprime mixing angle of the ground state pseudoscalar mesons it is expected that nonet symmetry should also be valid for the matrix elements of the pseudoscalar densitty operators which play an important role in charmless twobody b decays with e... | [['the', 'nonet', 'symmetry', 'scheme', 'seems', 'to', 'describe', 'rather', 'well', 'the', 'masses', 'and', 'etaetaprime', 'mixing', 'angle', 'of', 'the', 'ground', 'state', 'pseudoscalar', 'mesons', 'it', 'is', 'expected', 'that', 'nonet', 'symmetry', 'should', 'also', 'be', 'valid', 'for', 'the', 'matrix', 'elements... | [-0.0987796240194068, 0.2707125563971409, -0.03502633072488572, 0.10389181326323557, -0.06567325734067708, -0.12633533300700123, 0.1174967170265758, 0.29975588446074464, -0.19167818144657914, -0.22452160023275833, -0.04582904301252093, -0.3155679816538292, -0.03830163660876559, 0.0825986617172295, 0.07981520711514607, ... |
710.2413 | Inverted Hybrid Inflation as a solution to gravitino problems in Gravity
Mediation | It was recently found that the decay of inflaton and the SUSY breaking field
produces many gravitinos in the gravity mediation scenario. These discoveries
led to an exclusion of many inflation models such as chaotic, (smooth) hybrid,
topological and new inflation models. Under these circumstances we searched for
a su... | hep-ph | it was recently found that the decay of inflaton and the susy breaking field produces many gravitinos in the gravity mediation scenario these discoveries led to an exclusion of many inflation models such as chaotic smooth hybrid topological and new inflation models under these circumstances we searched for a successful... | [['it', 'was', 'recently', 'found', 'that', 'the', 'decay', 'of', 'inflaton', 'and', 'the', 'susy', 'breaking', 'field', 'produces', 'many', 'gravitinos', 'in', 'the', 'gravity', 'mediation', 'scenario', 'these', 'discoveries', 'led', 'to', 'an', 'exclusion', 'of', 'many', 'inflation', 'models', 'such', 'as', 'chaotic'... | [-0.12309219623767884, 0.23030135802781562, -0.1029894315141523, 0.17584912544584216, -0.08546328465845958, -0.19418201825764275, -0.03188195949959978, 0.3156304961314129, -0.2455371262105269, -0.3278004404660053, 0.06813989958843374, -0.22064419387552503, -0.1487094418180532, 0.15854090570132726, -0.03244823369275883,... |
710.2414 | Exchange Reactions with Dick Dalitz | An account is given of the close collaboration of Dick Dalitz with the
European K- Collaboration over many decades in many aspects of hypernuclear
physics. In particular, emphasis is given to the topics of double hypernuclei
and the discovery and resolution of p-wave Lambda strangeness exchange states.
| physics.hist-ph | an account is given of the close collaboration of dick dalitz with the european k collaboration over many decades in many aspects of hypernuclear physics in particular emphasis is given to the topics of double hypernuclei and the discovery and resolution of pwave lambda strangeness exchange states | [['an', 'account', 'is', 'given', 'of', 'the', 'close', 'collaboration', 'of', 'dick', 'dalitz', 'with', 'the', 'european', 'k', 'collaboration', 'over', 'many', 'decades', 'in', 'many', 'aspects', 'of', 'hypernuclear', 'physics', 'in', 'particular', 'emphasis', 'is', 'given', 'to', 'the', 'topics', 'of', 'double', 'hy... | [-0.12649154724513598, 0.19869220824794537, -0.07847500254618044, 0.07440013096152627, -0.06372751131098955, -0.10245498769143795, 0.045399776877875025, 0.28977834235163447, -0.1979186530918517, -0.2984804964842314, -0.026166719894737324, -0.34872414369849447, -0.02840885282196897, 0.16281914150223453, 0.03024306540635... |
710.2415 | Single Production of Doubly Charged Higgsinos at linear e-e- colliders | Several extended supersymmetric models, motivated by either grand
unification, or by neutrino mass generation, predict light doubly charged
higgsinos. We study the production of a single doubly charged higgsino and its
decay channels at the International Linear Collider (ILC) operating in the e-e-
mode. We analyze th... | hep-ph | several extended supersymmetric models motivated by either grand unification or by neutrino mass generation predict light doubly charged higgsinos we study the production of a single doubly charged higgsino and its decay channels at the international linear collider ilc operating in the ee mode we analyze the productio... | [['several', 'extended', 'supersymmetric', 'models', 'motivated', 'by', 'either', 'grand', 'unification', 'or', 'by', 'neutrino', 'mass', 'generation', 'predict', 'light', 'doubly', 'charged', 'higgsinos', 'we', 'study', 'the', 'production', 'of', 'a', 'single', 'doubly', 'charged', 'higgsino', 'and', 'its', 'decay', '... | [-0.06473735275119544, 0.21803757233172655, -0.041985793307423594, 0.1877118779970333, -0.033698124296963214, -0.20426800671964884, 0.0350553485006094, 0.28974937691166996, -0.2527925728261471, -0.2816565649658442, 0.06034602590184659, -0.3047305892929435, 0.017613531397655605, 0.13579114929772915, 0.06804794050380587,... |
710.2416 | Low Scale Leptogenesis and Dark Matter Candidates in an Extended Seesaw
Model | We consider a variant of seesaw mechanism by introducing extra singlet
neutrinos and singlet scalar boson, and show how low scale leptogenesis is
successfully realized in this scenario. We examine if the newly introduced
neutral particles, either singlet Majorana neutrino or singlet scalar boson,
can be a candidate f... | hep-ph | we consider a variant of seesaw mechanism by introducing extra singlet neutrinos and singlet scalar boson and show how low scale leptogenesis is successfully realized in this scenario we examine if the newly introduced neutral particles either singlet majorana neutrino or singlet scalar boson can be a candidate for dar... | [['we', 'consider', 'a', 'variant', 'of', 'seesaw', 'mechanism', 'by', 'introducing', 'extra', 'singlet', 'neutrinos', 'and', 'singlet', 'scalar', 'boson', 'and', 'show', 'how', 'low', 'scale', 'leptogenesis', 'is', 'successfully', 'realized', 'in', 'this', 'scenario', 'we', 'examine', 'if', 'the', 'newly', 'introduced... | [-0.1037261217357949, 0.2697961628078841, -0.08721874299226329, 0.21320767179489708, -0.08625064615849763, -0.20707642251867442, 0.026097180673297353, 0.3022129501645955, -0.2168435384788049, -0.3391411506801468, 0.02546931995759503, -0.23520792833565232, -0.05038226388905269, 0.11626457229543191, 0.09723197681775603, ... |
710.2417 | Finite volume spectrum of N=1 superminimal models perturbed by
$\Phi_{13}$ | We describe an extension of the nonlinear integral equation (NLIE) tehnique
to N=1 superminimal models perturbed by $\Phi_{13}$. Along the way, we also
complete our previous studies of the finite volume spectrum of the N=1
supersymmetric sine-Gordon model by considering the attractive regime and more
specifically, br... | hep-th | we describe an extension of the nonlinear integral equation nlie tehnique to n1 superminimal models perturbed by phi_13 along the way we also complete our previous studies of the finite volume spectrum of the n1 supersymmetric sinegordon model by considering the attractive regime and more specifically breather states | [['we', 'describe', 'an', 'extension', 'of', 'the', 'nonlinear', 'integral', 'equation', 'nlie', 'tehnique', 'to', 'n1', 'superminimal', 'models', 'perturbed', 'by', 'phi_13', 'along', 'the', 'way', 'we', 'also', 'complete', 'our', 'previous', 'studies', 'of', 'the', 'finite', 'volume', 'spectrum', 'of', 'the', 'n1', '... | [-0.12390349175499675, 0.10359194757165824, -0.05629683782656988, 0.08075895101743906, -0.07629730366170406, -0.15419361893630898, -0.026113859727047384, 0.3261127465715011, -0.222755949672622, -0.20751168202453604, 0.08169498011799685, -0.3147717307632168, -0.18477511213859543, 0.15445932479633484, -0.0188572675251634... |
710.2418 | H.E.S.S. Galactic Plane Survey unveils a Milagro Hotspot | We report here on a new VHE source, HESS J1908+063, disovered during the
extended H.E.S.S. survey of the Galactic plane and which coincides with the
recently reported MILAGRO unidentied source MGRO J1908+06. The position,
extension and spectrum measurements of the HESS source are presented and
compared to those of MG... | astro-ph | we report here on a new vhe source hess j1908063 disovered during the extended hess survey of the galactic plane and which coincides with the recently reported milagro unidentied source mgro j190806 the position extension and spectrum measurements of the hess source are presented and compared to those of mgro j190806 p... | [['we', 'report', 'here', 'on', 'a', 'new', 'vhe', 'source', 'hess', 'j1908063', 'disovered', 'during', 'the', 'extended', 'hess', 'survey', 'of', 'the', 'galactic', 'plane', 'and', 'which', 'coincides', 'with', 'the', 'recently', 'reported', 'milagro', 'unidentied', 'source', 'mgro', 'j190806', 'the', 'position', 'ext... | [-0.08261927450770762, 0.08246368590964755, -0.030052302175882593, 0.1219749309682051, -0.16368815327869424, -0.10302257150717413, 0.02211948855321354, 0.4492652574693089, -0.1581135621405582, -0.36956632231820874, 0.09575858186416106, -0.39963712858786776, 0.009574204870958381, 0.29066815388514033, 0.00873902845179050... |
710.2419 | The Variable Hierarchy for the Games mu-Calculus | Parity games are combinatorial representations of closed Boolean mu-terms. By
adding to them draw positions, they have been organized by Arnold and one of
the authors into a mu-calculus. As done by Berwanger et al. for the
propositional modal mu-calculus, it is possible to classify parity games into
levels of a hiera... | cs.LO cs.GT math.LO | parity games are combinatorial representations of closed boolean muterms by adding to them draw positions they have been organized by arnold and one of the authors into a mucalculus as done by berwanger et al for the propositional modal mucalculus it is possible to classify parity games into levels of a hierarchy accor... | [['parity', 'games', 'are', 'combinatorial', 'representations', 'of', 'closed', 'boolean', 'muterms', 'by', 'adding', 'to', 'them', 'draw', 'positions', 'they', 'have', 'been', 'organized', 'by', 'arnold', 'and', 'one', 'of', 'the', 'authors', 'into', 'a', 'mucalculus', 'as', 'done', 'by', 'berwanger', 'et', 'al', 'for... | [-0.07830834714317225, 0.11841243944638144, -0.06574948551322568, 0.13099846191234826, -0.11515143305835564, -0.20584861021791775, 0.10678373595199935, 0.3511018918721172, -0.2963035120363764, -0.33642837966837713, 0.05374159004607397, -0.25838294429931696, -0.09615038012980665, 0.08780283195807076, -0.0912396123981088... |
710.242 | Magnetoplasmons excitations in graphene for filling factors $\nu \leq 6$ | In the frame of the Hartree-Fock approximation, the dispersion of
magnetoplasmons in Graphene is derived for all types of transitions for filling
factors $\nu\leq 6$. The optical conductivity components of the magnetoplasmon
curves are calculated. It is shown that the electron-electron interactions lead
to a strong r... | cond-mat.str-el cond-mat.mes-hall | in the frame of the hartreefock approximation the dispersion of magnetoplasmons in graphene is derived for all types of transitions for filling factors nuleq 6 the optical conductivity components of the magnetoplasmon curves are calculated it is shown that the electronelectron interactions lead to a strong renormalizat... | [['in', 'the', 'frame', 'of', 'the', 'hartreefock', 'approximation', 'the', 'dispersion', 'of', 'magnetoplasmons', 'in', 'graphene', 'is', 'derived', 'for', 'all', 'types', 'of', 'transitions', 'for', 'filling', 'factors', 'nuleq', '6', 'the', 'optical', 'conductivity', 'components', 'of', 'the', 'magnetoplasmon', 'cur... | [-0.20646949674025358, 0.16768252661812208, -0.0696614962033627, 0.055778260235749784, 0.02380634470271968, -0.12021886323758911, 0.03945295051145818, 0.377949133335102, -0.2373085317592467, -0.25465221534813604, -0.03451711686343075, -0.31198031944973814, -0.12118594142638388, 0.1863798228422961, 0.06123317678969714, ... |
710.2421 | Spontaneous emission spectrum of a two-level atom in a very high Q
cavity | In this paper we consider an initially excited two-level system coupled to a
monomode cavity, and compute exact expressions for the spectra spontaneously
emitted by each system in the general case where they have arbitrary linewidths
and frequencies. Our method is based on the fact that this problem has an
easily sol... | quant-ph | in this paper we consider an initially excited twolevel system coupled to a monomode cavity and compute exact expressions for the spectra spontaneously emitted by each system in the general case where they have arbitrary linewidths and frequencies our method is based on the fact that this problem has an easily solvable... | [['in', 'this', 'paper', 'we', 'consider', 'an', 'initially', 'excited', 'twolevel', 'system', 'coupled', 'to', 'a', 'monomode', 'cavity', 'and', 'compute', 'exact', 'expressions', 'for', 'the', 'spectra', 'spontaneously', 'emitted', 'by', 'each', 'system', 'in', 'the', 'general', 'case', 'where', 'they', 'have', 'arbi... | [-0.11682813716975372, 0.1972219337777077, -0.04000224425911534, 0.023331490581256744, -0.02434655708022231, -0.16454874376635537, 0.019553055321943968, 0.44030715121064057, -0.22966509641601304, -0.261918698429815, 0.03245513134612894, -0.2988968496788139, -0.10203368393203997, 0.24199983037330888, 0.01828488687530529... |
710.2422 | Soft-gluon resummation for Higgs differential distributions at the Large
Hadron Collider | We study the transverse-momentum (q_T) and rapidity (y) distributions of the
Higgs boson in perturbative QCD, including the most advanced theoretical
information presently available: fixed-order perturbation theory at
Next-to-Leading Order (NLO) in the large-q_T region (q_T ~ M_H, being M_H the
Higgs mass), and soft-... | hep-ph | we study the transversemomentum q_t and rapidity y distributions of the higgs boson in perturbative qcd including the most advanced theoretical information presently available fixedorder perturbation theory at nexttoleading order nlo in the largeq_t region q_t m_h being m_h the higgs mass and softgluon resummation at t... | [['we', 'study', 'the', 'transversemomentum', 'q_t', 'and', 'rapidity', 'y', 'distributions', 'of', 'the', 'higgs', 'boson', 'in', 'perturbative', 'qcd', 'including', 'the', 'most', 'advanced', 'theoretical', 'information', 'presently', 'available', 'fixedorder', 'perturbation', 'theory', 'at', 'nexttoleading', 'order'... | [-0.04973153231654271, 0.16283127473644823, -0.11870851297582309, 0.21097917203982192, -0.01966835121927132, -0.07844409956919389, -0.017013738904897324, 0.3450385120484125, -0.13349384050928506, -0.18644862209098884, -0.059884987837433006, -0.3762035161840269, 0.14583453083837247, 0.10946376979384706, 0.07031469282039... |
710.2423 | Centrality dependence of some characteristics of relativistic nuclear
interactions and percolation cluster formation | Some of the centrality experiments indicate regime change and saturation in
the behaviour of characteristics of the secondary particles produced in
relativistic nuclear interactions. We discuss that the responsible mechanism to
explain the phenomena could be the percolation cluster formation and we expect
appearance ... | nucl-ex | some of the centrality experiments indicate regime change and saturation in the behaviour of characteristics of the secondary particles produced in relativistic nuclear interactions we discuss that the responsible mechanism to explain the phenomena could be the percolation cluster formation and we expect appearance of ... | [['some', 'of', 'the', 'centrality', 'experiments', 'indicate', 'regime', 'change', 'and', 'saturation', 'in', 'the', 'behaviour', 'of', 'characteristics', 'of', 'the', 'secondary', 'particles', 'produced', 'in', 'relativistic', 'nuclear', 'interactions', 'we', 'discuss', 'that', 'the', 'responsible', 'mechanism', 'to'... | [-0.13092822965462597, 0.21587170584469426, -0.1543510182106952, 0.14835318979065942, -0.03357478626528565, -0.057818441376166076, 0.015733141642139882, 0.35633028405053274, -0.252849618657207, -0.30227358593624465, 0.017540314237169008, -0.26869847498149896, -0.14886140443232596, 0.12653948077741933, 0.029758452523347... |
710.2424 | The Nicolas and Robin inequalities with sums of two squares | In 1984, G. Robin proved that the Riemann hypothesis is true if and only if
the Robin inequality $\sigma(n)<e^\gamma n\log\log n$ holds for every integer
$n>5040$, where $\sigma(n)$ is the sum of divisors function, and $\gamma$ is
the Euler-Mascheroni constant. We exhibit a broad class of subsets $\cS$ of the
natural... | math.NT | in 1984 g robin proved that the riemann hypothesis is true if and only if the robin inequality sigmanegamma nloglog n holds for every integer n5040 where sigman is the sum of divisors function and gamma is the eulermascheroni constant we exhibit a broad class of subsets cs of the natural numbers such that the robin ine... | [['in', '1984', 'g', 'robin', 'proved', 'that', 'the', 'riemann', 'hypothesis', 'is', 'true', 'if', 'and', 'only', 'if', 'the', 'robin', 'inequality', 'sigmanegamma', 'nloglog', 'n', 'holds', 'for', 'every', 'integer', 'n5040', 'where', 'sigman', 'is', 'the', 'sum', 'of', 'divisors', 'function', 'and', 'gamma', 'is', '... | [-0.18551033234580586, 0.11280119156673829, -0.06939290883889962, 0.0698125694789184, -0.05954369026558282, -0.26000409965864685, 0.003204129372993223, 0.2791260546334436, -0.2673980176675125, -0.2662457143974917, 0.10628439580899811, -0.3053636864963571, -0.1339194021823111, 0.23502393604460756, -0.09344822541314447, ... |
710.2425 | A variational principle for hardening elastoplasticity | We present a variational principle governing the quasistatic evolution of a
linearized elastoplastic material. In case of linear hardening, the novel
characterization allows to recover and partly extend some known results and
proves itself to be especially well-suited for discussing general approximation
and converge... | math.AP | we present a variational principle governing the quasistatic evolution of a linearized elastoplastic material in case of linear hardening the novel characterization allows to recover and partly extend some known results and proves itself to be especially wellsuited for discussing general approximation and convergence i... | [['we', 'present', 'a', 'variational', 'principle', 'governing', 'the', 'quasistatic', 'evolution', 'of', 'a', 'linearized', 'elastoplastic', 'material', 'in', 'case', 'of', 'linear', 'hardening', 'the', 'novel', 'characterization', 'allows', 'to', 'recover', 'and', 'partly', 'extend', 'some', 'known', 'results', 'and'... | [-0.0900000742970942, 0.024991533163791664, -0.0932710913893504, 0.10622739560979728, -0.11220164981802018, -0.12067735271576123, 0.03843767183701484, 0.33854372302691144, -0.3307161253327743, -0.26904631432336873, 0.1521339164270709, -0.15873115462902485, -0.1837709115770383, 0.18897326491200006, -0.12606502139272216,... |
710.2426 | Low angular momentum accretion flow model of Sgr A* activity | Sgr A* is a source of strongly variable emission in several energy bands. It
is generally agreed that this emission comes from the material surrounding the
black hole which is either falling in or flowing out. The activity must be
driven by accretion but the character of accretion flow in this object is an
open quest... | astro-ph | sgr a is a source of strongly variable emission in several energy bands it is generally agreed that this emission comes from the material surrounding the black hole which is either falling in or flowing out the activity must be driven by accretion but the character of accretion flow in this object is an open question w... | [['sgr', 'a', 'is', 'a', 'source', 'of', 'strongly', 'variable', 'emission', 'in', 'several', 'energy', 'bands', 'it', 'is', 'generally', 'agreed', 'that', 'this', 'emission', 'comes', 'from', 'the', 'material', 'surrounding', 'the', 'black', 'hole', 'which', 'is', 'either', 'falling', 'in', 'or', 'flowing', 'out', 'th... | [-0.10511219971055727, 0.1300080259181988, -0.07691215712835557, 0.07329816715268231, -0.06696371357045783, -0.08177522984088252, 0.03236350582068136, 0.39338220542399255, -0.28071958654778495, -0.32079664775522415, 0.09614563416845598, -0.3083503599942586, -0.012538494864193518, 0.22691731125397083, -0.023422194726941... |
710.2427 | Helac-Phegas: a generator for all parton level processes | The updated version of the Helac-Phegas event generator is presented. The
matrix elements are calculated through Dyson-Schwinger recursive equations.
Helac-Phegas generates parton-level events with all necessary information, in
the most recent Les Houches Accord format, for the study of any process within
the Standar... | hep-ph hep-ex physics.data-an | the updated version of the helacphegas event generator is presented the matrix elements are calculated through dysonschwinger recursive equations helacphegas generates partonlevel events with all necessary information in the most recent les houches accord format for the study of any process within the standard model in... | [['the', 'updated', 'version', 'of', 'the', 'helacphegas', 'event', 'generator', 'is', 'presented', 'the', 'matrix', 'elements', 'are', 'calculated', 'through', 'dysonschwinger', 'recursive', 'equations', 'helacphegas', 'generates', 'partonlevel', 'events', 'with', 'all', 'necessary', 'information', 'in', 'the', 'most'... | [-0.0585446892073378, 0.13357782404869795, -0.07089956190437079, 0.12063979659131291, -0.07497659948654473, -0.09793309196829796, -0.07286276473198086, 0.2857453428581357, -0.1989273232896812, -0.26840065392665563, 0.08156030233483762, -0.34897155068814756, -0.044610291351564225, 0.15339968498330564, 0.0348960633389651... |
710.2428 | The anomaly in the cosmic-ray positron spectrum | A recent analysis of cosmic-ray data from a space borne experiment by the AMS
collaboration supports the observation of an excess in the cosmic-ray positron
spectrum by previous balloon experiments. The combination of the various
experimental data establishes a deviation from the expected background with a
significan... | astro-ph | a recent analysis of cosmicray data from a space borne experiment by the ams collaboration supports the observation of an excess in the cosmicray positron spectrum by previous balloon experiments the combination of the various experimental data establishes a deviation from the expected background with a significance of... | [['a', 'recent', 'analysis', 'of', 'cosmicray', 'data', 'from', 'a', 'space', 'borne', 'experiment', 'by', 'the', 'ams', 'collaboration', 'supports', 'the', 'observation', 'of', 'an', 'excess', 'in', 'the', 'cosmicray', 'positron', 'spectrum', 'by', 'previous', 'balloon', 'experiments', 'the', 'combination', 'of', 'the... | [-0.06897401436220943, 0.15231009184818028, -0.08576378071946757, 0.10532488068343983, -0.06103777064099198, -0.055163207193393085, 0.03997592223542077, 0.3296634533752998, -0.21198008096377766, -0.3680538819836719, 0.03476110641578478, -0.3448160582310742, -0.0015142377111173812, 0.26705722030074824, -0.01863149739136... |
710.2429 | (g-2)_mu and supersymmetry: status and prospects | The experimental determination of the muon magnetic moment and its
theoretical prediction within the Standard Model and the MSSM are reviewed. A 3
sigma deviation between experiment and Standard Model prediction has been
established, and supersymmetry could provide a natural explation of this
deviation. Possible futu... | hep-ph | the experimental determination of the muon magnetic moment and its theoretical prediction within the standard model and the mssm are reviewed a 3 sigma deviation between experiment and standard model prediction has been established and supersymmetry could provide a natural explation of this deviation possible future im... | [['the', 'experimental', 'determination', 'of', 'the', 'muon', 'magnetic', 'moment', 'and', 'its', 'theoretical', 'prediction', 'within', 'the', 'standard', 'model', 'and', 'the', 'mssm', 'are', 'reviewed', 'a', '3', 'sigma', 'deviation', 'between', 'experiment', 'and', 'standard', 'model', 'prediction', 'has', 'been',... | [-0.05516072199679911, 0.12010034510696477, -0.0378073177723722, 0.155774632898498, -0.06465054713189602, -0.13831248337572272, 0.04169762844579633, 0.3423443381081928, -0.21679512946443125, -0.34275308255614206, 0.11528105674819512, -0.3083919695747847, -0.07108931888572194, 0.20233210793442347, -0.006244153533638878,... |
710.243 | Tackling the SUSY flavour & CP problem - SUGRA versus SU(3) | We comment on the power of the 'standard' solutions to the SUSY flavour and
CP problem based on supergravity and its derivates like mSUGRA in comparison to
the flavour symmetry approach. It is argued that flavour symmetries, and SU(3)
in particular, can not only mimic the situation in supergravity frameworks in
this ... | hep-ph | we comment on the power of the standard solutions to the susy flavour and cp problem based on supergravity and its derivates like msugra in comparison to the flavour symmetry approach it is argued that flavour symmetries and su3 in particular can not only mimic the situation in supergravity frameworks in this respect b... | [['we', 'comment', 'on', 'the', 'power', 'of', 'the', 'standard', 'solutions', 'to', 'the', 'susy', 'flavour', 'and', 'cp', 'problem', 'based', 'on', 'supergravity', 'and', 'its', 'derivates', 'like', 'msugra', 'in', 'comparison', 'to', 'the', 'flavour', 'symmetry', 'approach', 'it', 'is', 'argued', 'that', 'flavour', ... | [-0.08643819198478013, 0.14849175458075478, -0.06849704954074695, 0.14457325122202747, -0.12517092609778047, -0.1944361159694381, 0.05792668709764257, 0.3837385520688258, -0.20427395441802218, -0.2847876760912186, 0.12441966639598831, -0.2731923403509427, -0.0928429699037224, 0.1368349106705864, -0.05359991329023615, 0... |
710.2431 | Control of recollision wave packets for molecular orbital tomography
using short laser pulses | The tomographic imaging of arbitrary molecular orbitals via high-order
harmonic generation requires that electrons recollide from one direction only.
Within a semi-classical model, we show that extremely short phase-stabilized
laser pulses offer control over the momentum distribution of the returning
electrons. By ad... | physics.atom-ph | the tomographic imaging of arbitrary molecular orbitals via highorder harmonic generation requires that electrons recollide from one direction only within a semiclassical model we show that extremely short phasestabilized laser pulses offer control over the momentum distribution of the returning electrons by adjusting ... | [['the', 'tomographic', 'imaging', 'of', 'arbitrary', 'molecular', 'orbitals', 'via', 'highorder', 'harmonic', 'generation', 'requires', 'that', 'electrons', 'recollide', 'from', 'one', 'direction', 'only', 'within', 'a', 'semiclassical', 'model', 'we', 'show', 'that', 'extremely', 'short', 'phasestabilized', 'laser', ... | [-0.11685873089903374, 0.1926411043784422, -0.09426293226254241, 0.04986065636366242, -0.02009754264500083, -0.15306643586287774, 0.024138060688018437, 0.40761213731474993, -0.2892675484053609, -0.2743293028097691, 0.004629980953035467, -0.28646753002071706, -0.034673567520590816, 0.2376775582769613, 0.0426388384757290... |
710.2432 | Isospectral orbifolds with different maximal isotropy orders | We construct pairs of compact Riemannian orbifolds which are isospectral for
the Laplace operator on functions such that the maximal isotropy order of
singular points in one of the orbifolds is higher than in the other. In one
type of examples, isospectrality arises from a version of the famous Sunada
theorem which a... | math.DG | we construct pairs of compact riemannian orbifolds which are isospectral for the laplace operator on functions such that the maximal isotropy order of singular points in one of the orbifolds is higher than in the other in one type of examples isospectrality arises from a version of the famous sunada theorem which also ... | [['we', 'construct', 'pairs', 'of', 'compact', 'riemannian', 'orbifolds', 'which', 'are', 'isospectral', 'for', 'the', 'laplace', 'operator', 'on', 'functions', 'such', 'that', 'the', 'maximal', 'isotropy', 'order', 'of', 'singular', 'points', 'in', 'one', 'of', 'the', 'orbifolds', 'is', 'higher', 'than', 'in', 'the', ... | [-0.11830860357889135, 0.0939755472949797, -0.0592214443783899, 0.1444294816907145, -0.12673916784990438, -0.13731558837654784, -0.06244053645409588, 0.36899148516840113, -0.2407116051203102, -0.2166738938470196, 0.16493943874825745, -0.3085006902876653, -0.1485547138293995, 0.2635995727636382, -0.15471972017039115, -0... |
710.2433 | Astrophysical Condition on the attolensing as a possible probe for a
modified gravity theory | We investigate the wave effect in the gravitational lensing by a black hole
with very tiny mass less than 10^-19 solar mass, which is called attolensing,
motivated by a recent report that the lensing signature might be a possible
probe of a modified gravity theory in the braneworld scenario. We focus on the
finite so... | astro-ph | we investigate the wave effect in the gravitational lensing by a black hole with very tiny mass less than 1019 solar mass which is called attolensing motivated by a recent report that the lensing signature might be a possible probe of a modified gravity theory in the braneworld scenario we focus on the finite source si... | [['we', 'investigate', 'the', 'wave', 'effect', 'in', 'the', 'gravitational', 'lensing', 'by', 'a', 'black', 'hole', 'with', 'very', 'tiny', 'mass', 'less', 'than', '1019', 'solar', 'mass', 'which', 'is', 'called', 'attolensing', 'motivated', 'by', 'a', 'recent', 'report', 'that', 'the', 'lensing', 'signature', 'might'... | [-0.17601179282778417, 0.13565212289609438, -0.10583041497629206, 0.12937257835918264, -0.11896326013331143, -0.09697586192116844, -0.02357259389443569, 0.27577254515281824, -0.20664408379497956, -0.32877697332604033, 0.06262135258348624, -0.27828695789366115, -0.15363999712720233, 0.21154948474206733, -0.0309232004593... |
710.2434 | Integrability of geodesic flows and isospectrality of Riemannian
manifolds | We construct a pair of compact, eight-dimensional, two-step Riemannian
nilmanifolds $M$ and $M'$ which are isospectral for the Laplace operator on
functions and such that $M$ has completely integrable geodesic flow in the
sense of Liouville, while $M'$ has not. Moreover, for both manifolds we analyze
the structure of... | math.DG | we construct a pair of compact eightdimensional twostep riemannian nilmanifolds m and m which are isospectral for the laplace operator on functions and such that m has completely integrable geodesic flow in the sense of liouville while m has not moreover for both manifolds we analyze the structure of the submanifolds o... | [['we', 'construct', 'a', 'pair', 'of', 'compact', 'eightdimensional', 'twostep', 'riemannian', 'nilmanifolds', 'm', 'and', 'm', 'which', 'are', 'isospectral', 'for', 'the', 'laplace', 'operator', 'on', 'functions', 'and', 'such', 'that', 'm', 'has', 'completely', 'integrable', 'geodesic', 'flow', 'in', 'the', 'sense',... | [-0.21001365717139936, 0.12045025531467306, -0.0724481051213168, 0.09308189418422239, -0.09597154823131859, -0.14465975723860244, -0.04548329133540392, 0.3626897229602741, -0.2515141984695689, -0.2149456560972237, 0.11040243012004441, -0.2708870963666648, -0.16282248417095793, 0.19709713616513558, -0.0843999802991147, ... |
710.2435 | Primordial magnetic fields and nonlinear electrodynamics | The creation of large scale magnetic fields is studied in an inflationary
universe where electrodynamics is assumed to be nonlinear. After inflation ends
electrodynamics becomes linear and thus the description of reheating and the
subsequent radiation dominated stage are unaltered. The nonlinear regime of
electrodyna... | astro-ph | the creation of large scale magnetic fields is studied in an inflationary universe where electrodynamics is assumed to be nonlinear after inflation ends electrodynamics becomes linear and thus the description of reheating and the subsequent radiation dominated stage are unaltered the nonlinear regime of electrodynamics... | [['the', 'creation', 'of', 'large', 'scale', 'magnetic', 'fields', 'is', 'studied', 'in', 'an', 'inflationary', 'universe', 'where', 'electrodynamics', 'is', 'assumed', 'to', 'be', 'nonlinear', 'after', 'inflation', 'ends', 'electrodynamics', 'becomes', 'linear', 'and', 'thus', 'the', 'description', 'of', 'reheating', ... | [-0.1768843509695109, 0.2527617356755346, -0.08093158114044105, 0.07134866156368791, -0.09075392401667641, -0.12997918029534905, -0.10548745907897897, 0.3103979383321369, -0.23169610202312468, -0.3107865285128355, 0.05432957161409671, -0.22786788823740448, -0.08235558430280755, 0.22723275437019766, 0.03128268170882674,... |
710.2436 | Optical afterglows of gamma-ray bursts: a bimodal distribution?" | The luminosities of the optical afterglows of Gamma Ray Bursts, 12 hours
(rest frame time) after the trigger, show a surprising clustering, with a
minority of events being at a significant smaller luminosity. If real, this
dichotomy would be a crucial clue to understand the nature of optically dark
afterglows, i.e. b... | astro-ph | the luminosities of the optical afterglows of gamma ray bursts 12 hours rest frame time after the trigger show a surprising clustering with a minority of events being at a significant smaller luminosity if real this dichotomy would be a crucial clue to understand the nature of optically dark afterglows ie bursts that a... | [['the', 'luminosities', 'of', 'the', 'optical', 'afterglows', 'of', 'gamma', 'ray', 'bursts', '12', 'hours', 'rest', 'frame', 'time', 'after', 'the', 'trigger', 'show', 'a', 'surprising', 'clustering', 'with', 'a', 'minority', 'of', 'events', 'being', 'at', 'a', 'significant', 'smaller', 'luminosity', 'if', 'real', 't... | [-0.09427063829192009, 0.15418794770038835, -0.07935941621115872, 0.17236392405558085, -0.06772412876353452, -0.10584591249690244, 0.05854203538650549, 0.442601611038768, -0.20927782818478974, -0.3332439309133119, 0.06066288908784229, -0.31344688266123594, -0.05393074323717309, 0.1980898571617313, -0.015114290023369616... |
710.2437 | Discovery of 18 Jupiter mass RV companion orbiting the brown dwarf
candidate ChaHa8 | We report the discovery of a 16-20 Jupiter mass radial velocity companion
around the very young (3 Myr) brown dwarf candidate ChaHa8. Based on
high-resolution echelle spectra of ChaHa8 taken between 2000 and 2007 with UVES
at the VLT, a companion was detected through RV variability with a
semi-amplitude of 1.6 km/s. ... | astro-ph | we report the discovery of a 1620 jupiter mass radial velocity companion around the very young 3 myr brown dwarf candidate chaha8 based on highresolution echelle spectra of chaha8 taken between 2000 and 2007 with uves at the vlt a companion was detected through rv variability with a semiamplitude of 16 kms a kepler fit... | [['we', 'report', 'the', 'discovery', 'of', 'a', '1620', 'jupiter', 'mass', 'radial', 'velocity', 'companion', 'around', 'the', 'very', 'young', '3', 'myr', 'brown', 'dwarf', 'candidate', 'chaha8', 'based', 'on', 'highresolution', 'echelle', 'spectra', 'of', 'chaha8', 'taken', 'between', '2000', 'and', '2007', 'with', ... | [-0.1086437990021545, 0.12362595769495695, -0.09274360566746954, 0.05416994912957307, -0.12550642890125221, -0.1203731599414502, 0.09850941900638681, 0.34113854222689005, -0.12564161506894628, -0.3904748151270563, 0.09717983598181722, -0.2968838005144076, -0.042077350632205385, 0.2152097884077104, -0.12675354570374825,... |
710.2438 | Stability and leptogenesis in left-right symmetric seesaw models | In left-right symmetric seesaw models an eight-fold degeneracy among the
right-handed neutrino mass matrices is known to exist. We use stability and
viability of leptogenesis as criteria in order to discriminate among the
degenerate solutions and to partially lift the eight-fold degeneracy.
| hep-ph | in leftright symmetric seesaw models an eightfold degeneracy among the righthanded neutrino mass matrices is known to exist we use stability and viability of leptogenesis as criteria in order to discriminate among the degenerate solutions and to partially lift the eightfold degeneracy | [['in', 'leftright', 'symmetric', 'seesaw', 'models', 'an', 'eightfold', 'degeneracy', 'among', 'the', 'righthanded', 'neutrino', 'mass', 'matrices', 'is', 'known', 'to', 'exist', 'we', 'use', 'stability', 'and', 'viability', 'of', 'leptogenesis', 'as', 'criteria', 'in', 'order', 'to', 'discriminate', 'among', 'the', '... | [-0.12614496979152873, 0.17193310877753124, 0.04500504101937016, 0.2060308748373895, -0.10153741212118239, -0.19314018257760576, 0.02227790059433097, 0.3225217318783204, -0.27409985204715104, -0.31059236070307505, 0.09585451605796282, -0.26397279649972916, -0.07424629098247915, 0.05547372189660867, -0.02307404382597832... |
710.2439 | Ab initio molecular and solid state studies of Fe$^{II}$ spin cross-over
system [Fe(btz)$_2$(NCS)$_2$ | Ab initio computations within the density functional theory are reported for
the spin cross-over complex, [Fe(btz)$_{2}$(NCS)$_{2}$], where 3d$^6$ Fe$^{II}$
is characterized by High Spin (HS t$_{2g}^4$, e$_g^2$) and Low Spin (LS
t$_{2g}^6$, e$_g^0$) states. Results of infra red and Raman spectra for the
isolated mole... | cond-mat.soft cond-mat.mtrl-sci | ab initio computations within the density functional theory are reported for the spin crossover complex febtz_2ncs_2 where 3d6 feii is characterized by high spin hs t_2g4 e_g2 and low spin ls t_2g6 e_g0 states results of infra red and raman spectra for the isolated molecule are complemented for the crystalline solid wi... | [['ab', 'initio', 'computations', 'within', 'the', 'density', 'functional', 'theory', 'are', 'reported', 'for', 'the', 'spin', 'crossover', 'complex', 'febtz_2ncs_2', 'where', '3d6', 'feii', 'is', 'characterized', 'by', 'high', 'spin', 'hs', 't_2g4', 'e_g2', 'and', 'low', 'spin', 'ls', 't_2g6', 'e_g0', 'states', 'resul... | [-0.12386255717814662, 0.1636858909028084, -0.037731568773038855, 0.03087526177148183, 0.008287957623102811, -0.10590168091923345, 0.07327644420966375, 0.4112709465891469, -0.21341921369610137, -0.275843545534583, 0.005633285025481221, -0.30902474232797705, -0.08100627805647809, 0.08251851474660514, 0.1026746236548629,... |
710.244 | Study of the electron trigger efficiency of the CMS Experiment using
test beam data | A study of the electron identification and selection efficiency of the L1
Trigger algorithm has been performed using the combined ECAL/HCAL test beam
data. A detailed discussion of the electron isolation and its impact on the
selection efficiency is presented. The L1 electron algorithm is studied for
different beam e... | physics.ins-det | a study of the electron identification and selection efficiency of the l1 trigger algorithm has been performed using the combined ecalhcal test beam data a detailed discussion of the electron isolation and its impact on the selection efficiency is presented the l1 electron algorithm is studied for different beam energi... | [['a', 'study', 'of', 'the', 'electron', 'identification', 'and', 'selection', 'efficiency', 'of', 'the', 'l1', 'trigger', 'algorithm', 'has', 'been', 'performed', 'using', 'the', 'combined', 'ecalhcal', 'test', 'beam', 'data', 'a', 'detailed', 'discussion', 'of', 'the', 'electron', 'isolation', 'and', 'its', 'impact',... | [-0.04090569827501301, 0.15158359669814153, -0.04757477559757476, 0.11398103194458563, 0.011941356479893533, -0.15186300418073578, 0.07756340681879344, 0.4093114949610768, -0.15226993704575817, -0.4188065178008104, 0.06763932824476945, -0.28924988187393363, 0.058518555711441655, 0.22852148112546347, 0.0464700687182497,... |
710.2441 | Pion and $\rho$-meson form factors using four-point functions in N$_F$=2
QCD | Hadron wave functions and form factors can be extracted using four-point
correlators. Stochastic techniques are used to estimate the all to all
propagators, which are required for the exact calculation of four-point
functions. We apply the so called one-end trick to evaluate meson four-point
functions. We demonstrate... | hep-lat | hadron wave functions and form factors can be extracted using fourpoint correlators stochastic techniques are used to estimate the all to all propagators which are required for the exact calculation of fourpoint functions we apply the so called oneend trick to evaluate meson fourpoint functions we demonstrate the effec... | [['hadron', 'wave', 'functions', 'and', 'form', 'factors', 'can', 'be', 'extracted', 'using', 'fourpoint', 'correlators', 'stochastic', 'techniques', 'are', 'used', 'to', 'estimate', 'the', 'all', 'to', 'all', 'propagators', 'which', 'are', 'required', 'for', 'the', 'exact', 'calculation', 'of', 'fourpoint', 'functions... | [-0.049552036117609236, 0.12303461029181538, -0.10133204371859766, 0.15896762436102718, -0.06119192239177758, -0.037579154544701315, 0.01854218004194841, 0.3514652907950421, -0.19211277153904308, -0.20737671487875384, 0.05752213247286232, -0.3087705447376795, -0.1960930329570483, 0.17240161025156714, 0.1008366508639022... |
710.2442 | QCD on the Cell Broadband Engine | We evaluate IBM's Enhanced Cell Broadband Engine (BE) as a possible building
block of a new generation of lattice QCD machines. The Enhanced Cell BE will
provide full support of double-precision floating-point arithmetics, including
IEEE-compliant rounding. We have developed a performance model and applied it
to rele... | hep-lat | we evaluate ibms enhanced cell broadband engine be as a possible building block of a new generation of lattice qcd machines the enhanced cell be will provide full support of doubleprecision floatingpoint arithmetics including ieeecompliant rounding we have developed a performance model and applied it to relevant lattic... | [['we', 'evaluate', 'ibms', 'enhanced', 'cell', 'broadband', 'engine', 'be', 'as', 'a', 'possible', 'building', 'block', 'of', 'a', 'new', 'generation', 'of', 'lattice', 'qcd', 'machines', 'the', 'enhanced', 'cell', 'be', 'will', 'provide', 'full', 'support', 'of', 'doubleprecision', 'floatingpoint', 'arithmetics', 'in... | [-0.08799477281271044, 0.08568808493453266, -0.06579969314123513, 0.03581521461863037, -0.08703260396931901, -0.1625185439089706, 0.06823820138879873, 0.43865885858962295, -0.23210014719003386, -0.2513988510867871, 0.19276856824140484, -0.22957668439784182, -0.1337035769007143, 0.28274500763701665, -0.04491258970538684... |
710.2443 | Observe matter falling into a black hole | It has been well known that in the point of view of a distant observer, all
in-falling matter to a black hole (BH) will be eventually stalled and "frozen"
just outside the event horizon of the BH, although an in-falling observer will
see the matter falling straight through the event horizon. Thus in this "frozen
star... | astro-ph | it has been well known that in the point of view of a distant observer all infalling matter to a black hole bh will be eventually stalled and frozen just outside the event horizon of the bh although an infalling observer will see the matter falling straight through the event horizon thus in this frozen star scenario as... | [['it', 'has', 'been', 'well', 'known', 'that', 'in', 'the', 'point', 'of', 'view', 'of', 'a', 'distant', 'observer', 'all', 'infalling', 'matter', 'to', 'a', 'black', 'hole', 'bh', 'will', 'be', 'eventually', 'stalled', 'and', 'frozen', 'just', 'outside', 'the', 'event', 'horizon', 'of', 'the', 'bh', 'although', 'an',... | [-0.11186106045822557, 0.16752368035858295, -0.1262886118704894, 0.12352428816232502, -0.1347125953609657, -0.13453883270143988, -0.00709135651953729, 0.3763410443828405, -0.1984786535086696, -0.28624326667654604, 0.12233449175440486, -0.3047731677103169, -0.033097577819357175, 0.1909294511955034, -0.03984131191772136,... |
710.2444 | Determining QCD Low-Energy Couplings from lattice simulations | Different strategies for the computation of QCD low-energy couplings by
matching lattice QCD with the chiral effective theory are reviewed. After
recalling the main features of the chiral effective theory in the epsilon- and
p- regimes, the current status of the determination of leading order (Sigma, F)
and next-to-l... | hep-lat hep-ph | different strategies for the computation of qcd lowenergy couplings by matching lattice qcd with the chiral effective theory are reviewed after recalling the main features of the chiral effective theory in the epsilon and p regimes the current status of the determination of leading order sigma f and nexttoleading order... | [['different', 'strategies', 'for', 'the', 'computation', 'of', 'qcd', 'lowenergy', 'couplings', 'by', 'matching', 'lattice', 'qcd', 'with', 'the', 'chiral', 'effective', 'theory', 'are', 'reviewed', 'after', 'recalling', 'the', 'main', 'features', 'of', 'the', 'chiral', 'effective', 'theory', 'in', 'the', 'epsilon', '... | [-0.1370380695854478, 0.24797940301119953, -0.04561488387887092, 0.022039735807886568, -0.012054483337766108, -0.09639118332073421, 0.0380168517551604, 0.3314573097809711, -0.17598628970410893, -0.24977694082019083, 0.06848111063556965, -0.31647171236245947, -0.08653715233701993, 0.0871085433070274, 0.07598999029698247... |
710.2445 | Magnetization of Color-Flavor Locked Matter | We show that the magnetization in color-flavor locked superconductors can be
so strong that homogeneous quark matter becomes metastable for a wide range of
magnetic field values. This indicates that magnetic domains or other type of
magnetic inhomogeneities can be present in the quark cores of magnetars.
| hep-ph | we show that the magnetization in colorflavor locked superconductors can be so strong that homogeneous quark matter becomes metastable for a wide range of magnetic field values this indicates that magnetic domains or other type of magnetic inhomogeneities can be present in the quark cores of magnetars | [['we', 'show', 'that', 'the', 'magnetization', 'in', 'colorflavor', 'locked', 'superconductors', 'can', 'be', 'so', 'strong', 'that', 'homogeneous', 'quark', 'matter', 'becomes', 'metastable', 'for', 'a', 'wide', 'range', 'of', 'magnetic', 'field', 'values', 'this', 'indicates', 'that', 'magnetic', 'domains', 'or', 'o... | [-0.19201423338753112, 0.33238422270230156, -0.060771497957249905, 0.06933286669911777, -0.12719938515665682, -0.04602781031280756, 0.04053593238201389, 0.4029120076844033, -0.23586941621405014, -0.29850365419654135, 0.01923426407627127, -0.17504162180851748, -0.024226822063049422, 0.1847660660377129, 0.014698898474230... |
710.2446 | The structure of verbal sequences analyzed with unsupervised learning
techniques | Data mining allows the exploration of sequences of phenomena, whereas one
usually tends to focus on isolated phenomena or on the relation between two
phenomena. It offers invaluable tools for theoretical analyses and exploration
of the structure of sentences, texts, dialogues, and speech. We report here the
results o... | cs.CL cs.AI cs.LG | data mining allows the exploration of sequences of phenomena whereas one usually tends to focus on isolated phenomena or on the relation between two phenomena it offers invaluable tools for theoretical analyses and exploration of the structure of sentences texts dialogues and speech we report here the results of an att... | [['data', 'mining', 'allows', 'the', 'exploration', 'of', 'sequences', 'of', 'phenomena', 'whereas', 'one', 'usually', 'tends', 'to', 'focus', 'on', 'isolated', 'phenomena', 'or', 'on', 'the', 'relation', 'between', 'two', 'phenomena', 'it', 'offers', 'invaluable', 'tools', 'for', 'theoretical', 'analyses', 'and', 'exp... | [-0.09234036021107049, 0.045849884614775266, -0.11531441202861499, 0.08610394639394212, -0.122778687953811, -0.08183011963825534, 0.10648555832880514, 0.3838082564787732, -0.26119611971080303, -0.3527153337223421, 0.05025352239867465, -0.3200640316519033, -0.13604326404941577, 0.20897225896069022, -0.043522760875661065... |
710.2447 | Enhanced visibility of graphene: effect of one-dimensional photonic
crystal | We investigate theoretically the light reflectance of a graphene layer
prepared on the top of one-dimensional Si/SiO2 photonic crystal (1DPC). It is
shown that the visibility of the graphene layers is enhanced greatly when 1DPC
is added, and the visibility can be tuned by changing the incident angle and
light wavelen... | cond-mat.mtrl-sci | we investigate theoretically the light reflectance of a graphene layer prepared on the top of onedimensional sisio2 photonic crystal 1dpc it is shown that the visibility of the graphene layers is enhanced greatly when 1dpc is added and the visibility can be tuned by changing the incident angle and light wavelengths thi... | [['we', 'investigate', 'theoretically', 'the', 'light', 'reflectance', 'of', 'a', 'graphene', 'layer', 'prepared', 'on', 'the', 'top', 'of', 'onedimensional', 'sisio2', 'photonic', 'crystal', '1dpc', 'it', 'is', 'shown', 'that', 'the', 'visibility', 'of', 'the', 'graphene', 'layers', 'is', 'enhanced', 'greatly', 'when'... | [-0.12704026686074887, 0.2311058450571221, -0.04433051433306241, -0.05720076738499051, 0.0004030146460602249, -0.15578452358022332, 0.09155902046494294, 0.4731935058126523, -0.3269562929112842, -0.29304159038524696, 0.015067030331524818, -0.2983015195021163, -0.17511635052337163, 0.17389909821845914, -0.027586993167473... |
710.2448 | PARNI for importance sampling and density estimation | We present an aid for importance sampling in Monte Carlo integration, which
is of the general-purpose type in the sense that it in principle deals with any
quadratically integrable integrand on a unit hyper-cube of arbitrary dimension.
In contrast to most existing systems of this type, it does not ask for the
integra... | hep-ph | we present an aid for importance sampling in monte carlo integration which is of the generalpurpose type in the sense that it in principle deals with any quadratically integrable integrand on a unit hypercube of arbitrary dimension in contrast to most existing systems of this type it does not ask for the integrand as a... | [['we', 'present', 'an', 'aid', 'for', 'importance', 'sampling', 'in', 'monte', 'carlo', 'integration', 'which', 'is', 'of', 'the', 'generalpurpose', 'type', 'in', 'the', 'sense', 'that', 'it', 'in', 'principle', 'deals', 'with', 'any', 'quadratically', 'integrable', 'integrand', 'on', 'a', 'unit', 'hypercube', 'of', '... | [-0.0749697485138444, 0.05593078064893242, -0.09479563866179806, 0.056775520273551414, -0.08620063037200419, -0.11116059996640763, 0.035391157427970485, 0.3775054296197554, -0.27957158067225907, -0.3197680547128658, 0.15818667410440776, -0.2383641949645034, -0.11206152477628879, 0.25482383734118697, -0.0798890326446895... |
710.2449 | Statistical substantiation of introduction of the distributions
containing lifetime as thermodynamic parameter | By means of an inequality of the information and parametrization of family of
distributions of the probabilities, supposing an effective estimation,
introduction of the distributions containing time of the first achievement of a
level as internal thermodynamic parameter ground.
| physics.data-an | by means of an inequality of the information and parametrization of family of distributions of the probabilities supposing an effective estimation introduction of the distributions containing time of the first achievement of a level as internal thermodynamic parameter ground | [['by', 'means', 'of', 'an', 'inequality', 'of', 'the', 'information', 'and', 'parametrization', 'of', 'family', 'of', 'distributions', 'of', 'the', 'probabilities', 'supposing', 'an', 'effective', 'estimation', 'introduction', 'of', 'the', 'distributions', 'containing', 'time', 'of', 'the', 'first', 'achievement', 'of... | [-0.10775210710543877, 0.12384812925563146, -0.10726533567485137, 0.024702604152620412, 0.0067958668148957, -0.031845175625326544, 0.08324390630691479, 0.26598421503336, -0.25719392177863765, -0.37304798833643776, 0.07520561231873356, -0.2587098811681454, -0.06725724513093248, 0.15155478757925522, 0.003407585434615612,... |
710.245 | Transient Crossing of Phantom divide line $w_{\Lambda}=-1$ under
Gauss-Bonnet interaction | Smooth double crossing of the phantom barrier $w_{\Lambda} = -1$ has been
found possible in cosmological model with Gauss-Bonnet-scalar interaction, in
the presence of background cold dark matter. Such crossing has been observed to
be a sufficiently late time phenomena and independent of the sign of
Gauss-Bonnet-scal... | astro-ph | smooth double crossing of the phantom barrier w_lambda 1 has been found possible in cosmological model with gaussbonnetscalar interaction in the presence of background cold dark matter such crossing has been observed to be a sufficiently late time phenomena and independent of the sign of gaussbonnetscalar interaction t... | [['smooth', 'double', 'crossing', 'of', 'the', 'phantom', 'barrier', 'w_lambda', '1', 'has', 'been', 'found', 'possible', 'in', 'cosmological', 'model', 'with', 'gaussbonnetscalar', 'interaction', 'in', 'the', 'presence', 'of', 'background', 'cold', 'dark', 'matter', 'such', 'crossing', 'has', 'been', 'observed', 'to',... | [-0.12536443741844286, 0.10320062935352325, -0.13707146557816674, 0.08728639524252642, -0.08259444351175002, -0.17750837791356303, -0.028851051127449387, 0.37733163380078855, -0.22086668472796206, -0.3872944179096348, -0.0021767907827678653, -0.2793216562223813, 0.0027181162121927456, 0.13436596813271678, 0.04670317995... |
710.2451 | Reionization: Characteristic Scales, Topology and Observability | Recently the numerical simulations of the process of reionization of the
universe at z>6 have made a qualitative leap forward, reaching sufficient sizes
and dynamic range to determine the characteristic scales of this process. This
allowed making the first realistic predictions for a variety of observational
signatur... | astro-ph | recently the numerical simulations of the process of reionization of the universe at z6 have made a qualitative leap forward reaching sufficient sizes and dynamic range to determine the characteristic scales of this process this allowed making the first realistic predictions for a variety of observational signatures we... | [['recently', 'the', 'numerical', 'simulations', 'of', 'the', 'process', 'of', 'reionization', 'of', 'the', 'universe', 'at', 'z6', 'have', 'made', 'a', 'qualitative', 'leap', 'forward', 'reaching', 'sufficient', 'sizes', 'and', 'dynamic', 'range', 'to', 'determine', 'the', 'characteristic', 'scales', 'of', 'this', 'pr... | [-0.07873392962078056, 0.0785574429213408, -0.04203774059847505, 0.0990171073025191, -0.07468123541382904, -0.03196452594023536, 0.0321635616234165, 0.3942872594026002, -0.23023388686124235, -0.31278528789566323, 0.08439807777970353, -0.2451992384812911, -0.07290429970651696, 0.19930308001031252, 0.08508398935241117, 0... |
710.2452 | EG And: FUSE and HST/STIS Monitoring of an Eclipsing Symbiotic Binary | We present highlights and an overview of 20 FUSE and HST/STIS observations of
the bright symbiotic binary EG And. The main motivation behind this work is to
obtain spatially-resolved information on an evolved giant star in order to
understand the mass-loss processes at work in these objects. The system
consists of a ... | astro-ph | we present highlights and an overview of 20 fuse and hststis observations of the bright symbiotic binary eg and the main motivation behind this work is to obtain spatiallyresolved information on an evolved giant star in order to understand the massloss processes at work in these objects the system consists of a lowlumi... | [['we', 'present', 'highlights', 'and', 'an', 'overview', 'of', '20', 'fuse', 'and', 'hststis', 'observations', 'of', 'the', 'bright', 'symbiotic', 'binary', 'eg', 'and', 'the', 'main', 'motivation', 'behind', 'this', 'work', 'is', 'to', 'obtain', 'spatiallyresolved', 'information', 'on', 'an', 'evolved', 'giant', 'sta... | [-0.04044414143863832, 0.08490893950329337, -0.02122770879456463, 0.06632406420782597, -0.09029297148420785, -0.09134412684361451, 0.04476415238750633, 0.42231628542455535, -0.17325842624365276, -0.34931856356949237, 0.055715242678949534, -0.33276669071444, -0.054833618238626515, 0.159340607720272, -0.04106814696897345... |
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