id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
710.4153 | Quantum Indeterminacy of Emergent Spacetime | It is shown that nearly-flat 3+1D spacetime emerging from a dual quantum
field theory in 2+1D displays quantum fluctuations from classical Euclidean
geometry on macroscopic scales. A covariant holographic mapping is assumed,
where plane wave states with wavevector k on a 2D surface map onto classical
null trajectorie... | gr-qc astro-ph hep-th | it is shown that nearlyflat 31d spacetime emerging from a dual quantum field theory in 21d displays quantum fluctuations from classical euclidean geometry on macroscopic scales a covariant holographic mapping is assumed where plane wave states with wavevector k on a 2d surface map onto classical null trajectories in th... | [['it', 'is', 'shown', 'that', 'nearlyflat', '31d', 'spacetime', 'emerging', 'from', 'a', 'dual', 'quantum', 'field', 'theory', 'in', '21d', 'displays', 'quantum', 'fluctuations', 'from', 'classical', 'euclidean', 'geometry', 'on', 'macroscopic', 'scales', 'a', 'covariant', 'holographic', 'mapping', 'is', 'assumed', 'w... | [-0.15758729675170255, 0.2053500529546215, -0.14255813865876926, 0.07179381269906487, -0.05653094005400381, -0.15297260685939584, -0.01811849259352587, 0.3097785915958987, -0.2776783660619751, -0.23099718099052208, 0.0237279229008003, -0.3149541049820961, -0.10454213613445854, 0.17750278000097128, -0.06098023514456554,... |
710.4154 | Spin phonon coupling in frustrated magnet CdCr$_2$O$_4$ | The infrared phonon spectrum of the spinel CdCr2O4 is measured as a function
temperature from 6 K to 300K. The triply degenerate Cr phonons soften in the
paramagnetic phase as temperature is lowered below 100 K and then split into a
singlet and doublet in the low T antiferromagnetic phase which is tetragonally
distor... | cond-mat.mtrl-sci cond-mat.str-el | the infrared phonon spectrum of the spinel cdcr2o4 is measured as a function temperature from 6 k to 300k the triply degenerate cr phonons soften in the paramagnetic phase as temperature is lowered below 100 k and then split into a singlet and doublet in the low t antiferromagnetic phase which is tetragonally distorted... | [['the', 'infrared', 'phonon', 'spectrum', 'of', 'the', 'spinel', 'cdcr2o4', 'is', 'measured', 'as', 'a', 'function', 'temperature', 'from', '6', 'k', 'to', '300k', 'the', 'triply', 'degenerate', 'cr', 'phonons', 'soften', 'in', 'the', 'paramagnetic', 'phase', 'as', 'temperature', 'is', 'lowered', 'below', '100', 'k', ... | [-0.1484652191069252, 0.29035856285219974, -0.013897008368832953, 0.0254180751304961, -0.051001245763790386, -0.11738381692639634, 0.08321130447380319, 0.3784782463597171, -0.2813224259634258, -0.276246657295015, 0.005384224162268259, -0.34474734041914845, -0.05090063719716448, 0.12262764528562509, 0.057138040999338134... |
710.4155 | Hook-content formulae for symplectic and orthogonal tableaux | By considering the specialisation $s_{\lambda}(1,q,q^2,...,q^{n-1})$ of the
Schur function, Stanley was able to describe a formula for the number of
semistandard Young tableaux of shape $\lambda$ in terms of two properties of
the boxes in the diagram for $\lambda$. Using specialisations of symplectic and
orthogonal S... | math.CO math.RT | by considering the specialisation s_lambda1qq2qn1 of the schur function stanley was able to describe a formula for the number of semistandard young tableaux of shape lambda in terms of two properties of the boxes in the diagram for lambda using specialisations of symplectic and orthogonal schur functions we derive corr... | [['by', 'considering', 'the', 'specialisation', 's_lambda1qq2qn1', 'of', 'the', 'schur', 'function', 'stanley', 'was', 'able', 'to', 'describe', 'a', 'formula', 'for', 'the', 'number', 'of', 'semistandard', 'young', 'tableaux', 'of', 'shape', 'lambda', 'in', 'terms', 'of', 'two', 'properties', 'of', 'the', 'boxes', 'in... | [-0.09496973119676114, 0.06974397544590129, -0.0795493337397392, 0.07616671118885279, -0.0927128500985698, -0.08770593538737068, 0.03581097312271595, 0.32422095663272416, -0.2556799155552513, -0.2889761751374373, 0.03859107612202374, -0.17609465215355158, -0.15758532010591947, 0.17319732225643328, -0.11549470067883913,... |
710.4156 | Search for Neutrinoless Double Beta Decay with NEMO 3 and SuperNEMO | Since 2003 the NEMO~3 experiment has been searching for neutrinoless double
beta decay using about 10 kg of enriched isotopes. A limit of T_(1/2)(0nu) >
5.8 10**23 years at 90 % CL has been obtained for 100-Mo from the first two
years of data. Several measurements of two-neutrino double beta decays have
also been per... | hep-ex | since 2003 the nemo3 experiment has been searching for neutrinoless double beta decay using about 10 kg of enriched isotopes a limit of t_120nu 58 1023 years at 90 cl has been obtained for 100mo from the first two years of data several measurements of twoneutrino double beta decays have also been performed a first nemo... | [['since', '2003', 'the', 'nemo3', 'experiment', 'has', 'been', 'searching', 'for', 'neutrinoless', 'double', 'beta', 'decay', 'using', 'about', '10', 'kg', 'of', 'enriched', 'isotopes', 'a', 'limit', 'of', 't_120nu', '58', '1023', 'years', 'at', '90', 'cl', 'has', 'been', 'obtained', 'for', '100mo', 'from', 'the', 'fi... | [-0.019106895197182894, 0.2157850086907554, -0.028870742324775513, 0.04471431770966424, 0.05737031408800529, -0.1250908437784976, 0.07946225436395392, 0.3043632136048892, -0.11421303995526753, -0.3656201643170789, 0.10689814025961543, -0.37225310131907463, 0.06364232928563769, 0.25258957710152924, 0.04988593772913401, ... |
710.4157 | A Cross-Match of 2MASS and SDSS: Newly-Found L and T Dwarfs and an
Estimate of the Space Densitfy of T Dwarfs | We report new L and T dwarfs found in a cross-match of the SDSS Data Release
1 and 2MASS. Our simultaneous search of the two databases effectively allows us
to relax the criteria for object detection in either survey and to explore the
combined databases to a greater completeness level. We find two new T dwarfs in
ad... | astro-ph | we report new l and t dwarfs found in a crossmatch of the sdss data release 1 and 2mass our simultaneous search of the two databases effectively allows us to relax the criteria for object detection in either survey and to explore the combined databases to a greater completeness level we find two new t dwarfs in additio... | [['we', 'report', 'new', 'l', 'and', 't', 'dwarfs', 'found', 'in', 'a', 'crossmatch', 'of', 'the', 'sdss', 'data', 'release', '1', 'and', '2mass', 'our', 'simultaneous', 'search', 'of', 'the', 'two', 'databases', 'effectively', 'allows', 'us', 'to', 'relax', 'the', 'criteria', 'for', 'object', 'detection', 'in', 'eithe... | [-0.05392531662619868, 0.07897070143279793, -0.05190454313270159, 0.12488389849983038, -0.15224732162997776, -0.0781410504408593, 0.141653041256842, 0.37331331690235925, -0.13635268568000553, -0.3889342004874088, 0.04594682603237024, -0.34006082922273834, -0.00915255560355607, 0.20258262318102532, -0.08387032527944281,... |
710.4158 | The Highest Energy Neutrinos | Measurements of the arrival directions of cosmic rays have not revealed their
sources. High energy neutrino telescopes attempt to resolve the problem by
detecting neutrinos whose directions are not scrambled by magnetic fields. The
key issue is whether the neutrino flux produced in cosmic ray accelerators is
detectab... | astro-ph | measurements of the arrival directions of cosmic rays have not revealed their sources high energy neutrino telescopes attempt to resolve the problem by detecting neutrinos whose directions are not scrambled by magnetic fields the key issue is whether the neutrino flux produced in cosmic ray accelerators is detectable i... | [['measurements', 'of', 'the', 'arrival', 'directions', 'of', 'cosmic', 'rays', 'have', 'not', 'revealed', 'their', 'sources', 'high', 'energy', 'neutrino', 'telescopes', 'attempt', 'to', 'resolve', 'the', 'problem', 'by', 'detecting', 'neutrinos', 'whose', 'directions', 'are', 'not', 'scrambled', 'by', 'magnetic', 'fi... | [-0.1061639063685869, 0.22226009894971738, -0.01798868342684911, 0.1417736071401518, -0.0694978857551692, -0.07364909193299786, -0.02619795991822776, 0.4171310566422163, -0.212164422661781, -0.34907309314932183, 0.06531648757935718, -0.33749283696854054, -0.044292008170312404, 0.23560111751577656, -0.01084716349600278,... |
710.4159 | Phase Bifurcations of Strongly Correlated Electron Gas at the Conditions
of dHvA Effect | In a framework of catastrophe theory we investigate the equilibrium set for
the system of strongly correlated electron gas at the conditions of dHvA effect
and show that the discontinuities accompanied the diamagnetic phase transition
(DPT) is handled by Riemann-Hugoniot catastrophe. We show that applicability of
the... | cond-mat.str-el | in a framework of catastrophe theory we investigate the equilibrium set for the system of strongly correlated electron gas at the conditions of dhva effect and show that the discontinuities accompanied the diamagnetic phase transition dpt is handled by riemannhugoniot catastrophe we show that applicability of the stand... | [['in', 'a', 'framework', 'of', 'catastrophe', 'theory', 'we', 'investigate', 'the', 'equilibrium', 'set', 'for', 'the', 'system', 'of', 'strongly', 'correlated', 'electron', 'gas', 'at', 'the', 'conditions', 'of', 'dhva', 'effect', 'and', 'show', 'that', 'the', 'discontinuities', 'accompanied', 'the', 'diamagnetic', '... | [-0.18608685480700385, 0.136673606565159, -0.0733504226946898, 0.02884425399075183, -0.0324428733609259, -0.08720101168810648, 0.09434494643214311, 0.2846442976977024, -0.23624328009279097, -0.2777668771539199, 0.08600374208736933, -0.2926008939311582, -0.13517834255366593, 0.21081572914190885, -0.005241114567270723, 0... |
710.416 | Raman spectroscopy of graphene on different substrates and influence of
defects | We show the evolution of Raman spectra with number of graphene layers on
different substrates, SiO$_{2}$/Si and conducting indium tin oxide (ITO) plate.
The G mode peak position and the intensity ratio of G and 2D bands depend on
the preparation of sample for the same number of graphene layers. The 2D Raman
band has ... | cond-mat.mtrl-sci cond-mat.other | we show the evolution of raman spectra with number of graphene layers on different substrates sio_2si and conducting indium tin oxide ito plate the g mode peak position and the intensity ratio of g and 2d bands depend on the preparation of sample for the same number of graphene layers the 2d raman band has characterist... | [['we', 'show', 'the', 'evolution', 'of', 'raman', 'spectra', 'with', 'number', 'of', 'graphene', 'layers', 'on', 'different', 'substrates', 'sio_2si', 'and', 'conducting', 'indium', 'tin', 'oxide', 'ito', 'plate', 'the', 'g', 'mode', 'peak', 'position', 'and', 'the', 'intensity', 'ratio', 'of', 'g', 'and', '2d', 'band... | [-0.13611649097789055, 0.12311217872257361, -0.009307400626273244, -0.09080561026473719, 0.00675695222099683, -0.11910799385314133, 0.10920846999331486, 0.47771897768756044, -0.24737413803278327, -0.3079852569745454, -0.007460527612679164, -0.31550305882937335, -0.10389418383500328, 0.19000190424452895, 0.0213961324417... |
710.4161 | Trigger strategies for SUSY searches at the LHC | Supersymmetry will be searched for in a variety of final states at the LHC.
It is crucial that a robust, efficient and unbiased trigger selection for SUSY
is implemented from the very early days of data taking. After a brief
description of the ATLAS and the CMS trigger systems, and a more in-depth
discussion of the A... | hep-ex | supersymmetry will be searched for in a variety of final states at the lhc it is crucial that a robust efficient and unbiased trigger selection for susy is implemented from the very early days of data taking after a brief description of the atlas and the cms trigger systems and a more indepth discussion of the atlas hi... | [['supersymmetry', 'will', 'be', 'searched', 'for', 'in', 'a', 'variety', 'of', 'final', 'states', 'at', 'the', 'lhc', 'it', 'is', 'crucial', 'that', 'a', 'robust', 'efficient', 'and', 'unbiased', 'trigger', 'selection', 'for', 'susy', 'is', 'implemented', 'from', 'the', 'very', 'early', 'days', 'of', 'data', 'taking',... | [-0.08283447994175039, 0.1536951387878245, -0.14292976140818545, 0.15023912081304727, -0.06437777153308123, -0.17754827807067144, -0.0033402355177931382, 0.3438536148046104, -0.16204004336646954, -0.3176341470278485, 0.17104734737970406, -0.23958185286274258, -0.04030375494818452, 0.2051733465419269, 0.0100666618656734... |
710.4162 | Impact of reionization on CMB polarization tests of slow-roll inflation | Estimates of inflationary parameters from the CMB B-mode polarization
spectrum on the largest scales depend on knowledge of the reionization history,
especially at low tensor-to-scalar ratio. Assuming an incorrect reionization
history in the analysis of such polarization data can strongly bias the
inflationary parame... | astro-ph | estimates of inflationary parameters from the cmb bmode polarization spectrum on the largest scales depend on knowledge of the reionization history especially at low tensortoscalar ratio assuming an incorrect reionization history in the analysis of such polarization data can strongly bias the inflationary parameters on... | [['estimates', 'of', 'inflationary', 'parameters', 'from', 'the', 'cmb', 'bmode', 'polarization', 'spectrum', 'on', 'the', 'largest', 'scales', 'depend', 'on', 'knowledge', 'of', 'the', 'reionization', 'history', 'especially', 'at', 'low', 'tensortoscalar', 'ratio', 'assuming', 'an', 'incorrect', 'reionization', 'histo... | [-0.13610928139869907, 0.12629098670053404, -0.08052409768692757, 0.09379814403775827, -0.12621426010588394, -0.09335543256589121, -0.02617993331304226, 0.3541019217748391, -0.223396922930851, -0.3263671113291048, 0.06283555931544729, -0.24649203088330596, -0.08747214001876519, 0.18222745410796898, -0.03546450755215789... |
710.4163 | Achernar: Rapid Polarization Variability as Evidence of Photospheric and
Circumstellar Activity | We present the results of a high accuracy ($\sigma \approx 0.005%$)
polarization monitoring of the Be Star Achernar that was carried out between
July 7th and November 5th, 2006. Our results indicate that, after a near
quiescent phase from 1998 to 2002, Achernar is presently in an active phase and
has built a circumst... | astro-ph | we present the results of a high accuracy sigma approx 0005 polarization monitoring of the be star achernar that was carried out between july 7th and november 5th 2006 our results indicate that after a near quiescent phase from 1998 to 2002 achernar is presently in an active phase and has built a circumstellar disk we ... | [['we', 'present', 'the', 'results', 'of', 'a', 'high', 'accuracy', 'sigma', 'approx', '0005', 'polarization', 'monitoring', 'of', 'the', 'be', 'star', 'achernar', 'that', 'was', 'carried', 'out', 'between', 'july', '7th', 'and', 'november', '5th', '2006', 'our', 'results', 'indicate', 'that', 'after', 'a', 'near', 'qu... | [-0.0955416109302405, 0.12945183518991144, -0.09307420146706136, 0.06215391624664335, -0.05565525510610314, -0.06348483088731882, 0.02086642499307345, 0.4101372484874446, -0.22753905794434104, -0.3674612319464359, 0.16437709124693356, -0.2614397564284445, -0.09240821495745877, 0.20714432676868455, -0.06025449362823565,... |
710.4164 | Morphology of Condon Domains Phase in Plate-Like Sample | Based on Shoenberg assumption of magnetic flux density dependence of
diamagnetic moments which accounts for an instability of strongly correlated
electron gas at the conditions of dHvA effect and diamagnetic phase transition
(DPT) to non-uniform phase, we investigate the morphology of the Condon domains
(CD) in plate... | cond-mat.str-el | based on shoenberg assumption of magnetic flux density dependence of diamagnetic moments which accounts for an instability of strongly correlated electron gas at the conditions of dhva effect and diamagnetic phase transition dpt to nonuniform phase we investigate the morphology of the condon domains cd in platelike sam... | [['based', 'on', 'shoenberg', 'assumption', 'of', 'magnetic', 'flux', 'density', 'dependence', 'of', 'diamagnetic', 'moments', 'which', 'accounts', 'for', 'an', 'instability', 'of', 'strongly', 'correlated', 'electron', 'gas', 'at', 'the', 'conditions', 'of', 'dhva', 'effect', 'and', 'diamagnetic', 'phase', 'transition... | [-0.2083456113377455, 0.2586915461041759, -0.05195168416546889, 0.036663738753808246, -0.012638706203996519, -0.0627717930469508, 0.06393416538980813, 0.3436764990064231, -0.23779780744798173, -0.31945458512506947, 0.024005601665559262, -0.2813687831902307, -0.10625501267596586, 0.16639425826435986, 0.05725132005889553... |
710.4165 | A note on plurisubharmonic defining functions in $\mathbb{C}^n$ | Let D be a smoothly bounded domain in complex space of dimension larger than
2. Suppose that D admits a smooth defining function which is plurisubharmonic
on the boundary of D. Then the Diederich-Fornaess exponent can be chosen
arbitrarily close to 1, and the closure of D admits a Stein neighborhood basis.
| math.CV | let d be a smoothly bounded domain in complex space of dimension larger than 2 suppose that d admits a smooth defining function which is plurisubharmonic on the boundary of d then the diederichfornaess exponent can be chosen arbitrarily close to 1 and the closure of d admits a stein neighborhood basis | [['let', 'd', 'be', 'a', 'smoothly', 'bounded', 'domain', 'in', 'complex', 'space', 'of', 'dimension', 'larger', 'than', '2', 'suppose', 'that', 'd', 'admits', 'a', 'smooth', 'defining', 'function', 'which', 'is', 'plurisubharmonic', 'on', 'the', 'boundary', 'of', 'd', 'then', 'the', 'diederichfornaess', 'exponent', 'c... | [-0.17489705667741454, 0.13373139058239758, -0.1285707086073951, 0.011938266270310404, -0.0957876269206351, -0.22891141267385906, 0.012487827191272607, 0.2997398142917798, -0.3074588217557623, -0.19081590455383635, 0.07812413509460524, -0.24482492570622036, -0.10749414623177682, 0.16906137321180162, -0.0812253082236006... |
710.4166 | Quasilocality of joining/splitting strings from coherent states | Using the coherent state formalism we calculate matrix elements of the
one-loop non-planar dilatation operator of ${\cal N}=4$ SYM between operators
dual to folded Frolov-Tseytlin strings and observe a curious scaling behavior.
We comment on the {\it qualitative} similarity of our matrix elements to the
interaction v... | hep-th | using the coherent state formalism we calculate matrix elements of the oneloop nonplanar dilatation operator of cal n4 sym between operators dual to folded frolovtseytlin strings and observe a curious scaling behavior we comment on the it qualitative similarity of our matrix elements to the interaction vertex of a stri... | [['using', 'the', 'coherent', 'state', 'formalism', 'we', 'calculate', 'matrix', 'elements', 'of', 'the', 'oneloop', 'nonplanar', 'dilatation', 'operator', 'of', 'cal', 'n4', 'sym', 'between', 'operators', 'dual', 'to', 'folded', 'frolovtseytlin', 'strings', 'and', 'observe', 'a', 'curious', 'scaling', 'behavior', 'we'... | [-0.14532498224474655, 0.16619567619380796, -0.08634202427916475, 0.11363159536619435, -0.06710927718789778, -0.12287229109059118, 0.04989209898957307, 0.33208198679590617, -0.2584125177914297, -0.23403316387231207, 0.014185986086306581, -0.3621274799845376, -0.18733070972426744, 0.0873047752781761, 0.00451012532441661... |
710.4167 | A Minkowski Type Trace Inequality and Strong Subadditivity of Quantum
Entropy II: Convexity and Concavity | We revisit and prove some convexity inequalities for trace functions
conjectured in the earlier part I. The main functional considered is
\Phi_{p,q}(A_1,A_2,...,A_m) = (trace((\sum_{j=1}^m A_j^p)^{q/p}))^{1/q} for m
positive definite operators A_j. In part I we only considered the case q=1 and
proved the concavity ... | math.OA math-ph math.MP | we revisit and prove some convexity inequalities for trace functions conjectured in the earlier part i the main functional considered is phi_pqa_1a_2a_m tracesum_j1m a_jpqp1q for m positive definite operators a_j in part i we only considered the case q1 and proved the concavity of phi_p1 for 0 p leq 1 and the convexity... | [['we', 'revisit', 'and', 'prove', 'some', 'convexity', 'inequalities', 'for', 'trace', 'functions', 'conjectured', 'in', 'the', 'earlier', 'part', 'i', 'the', 'main', 'functional', 'considered', 'is', 'phi_pqa_1a_2a_m', 'tracesum_j1m', 'a_jpqp1q', 'for', 'm', 'positive', 'definite', 'operators', 'a_j', 'in', 'part', '... | [-0.1471648577485897, 0.08778230147366492, -0.05610064977372531, 0.11600816602601785, -0.023902490912069096, -0.1927688720776406, 0.004894492160592688, 0.3258570722521168, -0.2918390742605169, -0.21961247590242897, 0.10080605120340694, -0.31063186023894646, -0.09422606842158592, 0.15471226757564518, -0.0855740059505229... |
710.4168 | Fitting Pulsar Wind Tori. II. Error Analysis and Applications | We have applied the torus fitting procedure described in Ng & Romani (2004)
to PWNe observations in the Chandra data archive. This study provides
quantitative measurement of the PWN geometry and we characterize the
uncertainties in the fits, with statistical errors coming from the fit
uncertainties and systematic err... | astro-ph | we have applied the torus fitting procedure described in ng romani 2004 to pwne observations in the chandra data archive this study provides quantitative measurement of the pwn geometry and we characterize the uncertainties in the fits with statistical errors coming from the fit uncertainties and systematic errors esti... | [['we', 'have', 'applied', 'the', 'torus', 'fitting', 'procedure', 'described', 'in', 'ng', 'romani', '2004', 'to', 'pwne', 'observations', 'in', 'the', 'chandra', 'data', 'archive', 'this', 'study', 'provides', 'quantitative', 'measurement', 'of', 'the', 'pwn', 'geometry', 'and', 'we', 'characterize', 'the', 'uncertai... | [-0.0766027603697564, 0.059768324171440027, -0.07991771131982, 0.11865194605625405, -0.0996807980902341, -0.10188191773474445, 0.05289213060477407, 0.42992808411315997, -0.22451934936617937, -0.36434329602373194, 0.10109941736433883, -0.2610144588445332, -0.03026271547780049, 0.2069157855870316, -0.063624382769803, 0.0... |
710.4169 | Charged Higgs boson phenomenology in Supersymmetric models with Higgs
triplets | We present a detailed study of the Higgs sector within an extension of the
Minimal Supersymmetric Standard Model that includes one Complex Higgs Triplet
(MSSM+1CHT). The model spectrum includes three singly charged Higgs bosons as
well as three CP-even (or scalar) and two CP-odd (or pseudoscalar) neutral
Higgs bosons... | hep-ph | we present a detailed study of the higgs sector within an extension of the minimal supersymmetric standard model that includes one complex higgs triplet mssm1cht the model spectrum includes three singly charged higgs bosons as well as three cpeven or scalar and two cpodd or pseudoscalar neutral higgs bosons we present ... | [['we', 'present', 'a', 'detailed', 'study', 'of', 'the', 'higgs', 'sector', 'within', 'an', 'extension', 'of', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'that', 'includes', 'one', 'complex', 'higgs', 'triplet', 'mssm1cht', 'the', 'model', 'spectrum', 'includes', 'three', 'singly', 'charged', 'higgs', 'b... | [-0.04644940177042207, 0.26508855770639045, 0.018555429904319517, 0.18519060346774163, -0.05027909413712967, -0.22286736363788473, 0.03289272224488245, 0.30885647295376245, -0.15595327683496923, -0.25911382443419745, 0.029415654222909572, -0.3206607646954415, 0.02858201949592595, 0.15205860897904958, 0.1078645391204521... |
710.417 | STACEE Observations of 1ES 1218+304 | We present the analysis and results of recent high-energy gamma-ray
observations of the high energy-peaked BL Lac (HBL) object 1ES 1218+304 with
the Solar Tower Atmospheric Cherenkov Effect Experiment (STACEE). 1ES 1218+304
is an X-ray bright HBL at a redshift z=0.182. It has been predicted to be a
gamma-ray emitter ... | astro-ph | we present the analysis and results of recent highenergy gammaray observations of the high energypeaked bl lac hbl object 1es 1218304 with the solar tower atmospheric cherenkov effect experiment stacee 1es 1218304 is an xray bright hbl at a redshift z0182 it has been predicted to be a gammaray emitter above 100 gev det... | [['we', 'present', 'the', 'analysis', 'and', 'results', 'of', 'recent', 'highenergy', 'gammaray', 'observations', 'of', 'the', 'high', 'energypeaked', 'bl', 'lac', 'hbl', 'object', '1es', '1218304', 'with', 'the', 'solar', 'tower', 'atmospheric', 'cherenkov', 'effect', 'experiment', 'stacee', '1es', '1218304', 'is', 'a... | [0.006196624412301129, 0.23348305354959717, -0.03194512611454619, 0.21537310383220237, -0.15337331905694945, -0.14206348057320742, 0.008723611405002885, 0.5319199643230864, -0.0662198134533745, -0.4893806852466826, 0.04269037659417206, -0.35600921411670633, 0.030048002873497483, 0.2759298915043473, -0.04686697484742451... |
710.4171 | Interference Cancelation in Coherent CDMA Systems Using Parallel
Iterative Algorithms | Least mean square-partial parallel interference cancelation (LMS-PPIC) is a
partial interference cancelation using adaptive multistage structure in which
the normalized least mean square (NLMS) adaptive algorithm is engaged to obtain
the cancelation weights. The performance of the NLMS algorithm is mostly
dependent t... | stat.AP | least mean squarepartial parallel interference cancelation lmsppic is a partial interference cancelation using adaptive multistage structure in which the normalized least mean square nlms adaptive algorithm is engaged to obtain the cancelation weights the performance of the nlms algorithm is mostly dependent to its ste... | [['least', 'mean', 'squarepartial', 'parallel', 'interference', 'cancelation', 'lmsppic', 'is', 'a', 'partial', 'interference', 'cancelation', 'using', 'adaptive', 'multistage', 'structure', 'in', 'which', 'the', 'normalized', 'least', 'mean', 'square', 'nlms', 'adaptive', 'algorithm', 'is', 'engaged', 'to', 'obtain', ... | [-0.17071842427176784, 0.055234109345226996, -0.05955061601974022, 0.012084129119590168, -0.06678041734343115, -0.190910072802426, 0.058811010111098974, 0.4239284072582628, -0.2738068985411885, -0.2900738866476257, 0.11065989222341016, -0.25044586125980406, -0.15519982288223297, 0.12659583396576587, -0.0761892143758683... |
710.4172 | Interference Cancelation in Non-coherent CDMA Systems Using Parallel
Iterative Algorithms | Parallel least mean square-partial parallel interference cancelation
(PLMS-PPIC) is a partial interference cancelation which employs adaptive
multistage structure. In this algorithm the channel phases for all users are
assumed to be known. Having only their quarters in (0,2\pi), a modified version
of PLMS-PPIC is pro... | stat.AP | parallel least mean squarepartial parallel interference cancelation plmsppic is a partial interference cancelation which employs adaptive multistage structure in this algorithm the channel phases for all users are assumed to be known having only their quarters in 02pi a modified version of plmsppic is proposed in this ... | [['parallel', 'least', 'mean', 'squarepartial', 'parallel', 'interference', 'cancelation', 'plmsppic', 'is', 'a', 'partial', 'interference', 'cancelation', 'which', 'employs', 'adaptive', 'multistage', 'structure', 'in', 'this', 'algorithm', 'the', 'channel', 'phases', 'for', 'all', 'users', 'are', 'assumed', 'to', 'be... | [-0.21320972439134495, 0.09086626635398716, -0.06023600584594533, 0.05294381960993633, -0.05730368685326539, -0.19546788431471213, 0.05268401994690066, 0.394704161118716, -0.26721149719669485, -0.3029291016748175, 0.08658031548256986, -0.23124100039713086, -0.18003159431755195, 0.10814022331032902, -0.10044304657494649... |
710.4173 | Full MIMO Channel Estimation Using A Simple Adaptive Partial Feedback
Method | Partial feedback in multiple-input multiple-output (MIMO) communication
systems provides tremendous capacity gain and enables the transmitter to
exploit channel condition and to eliminate channel interference. In the case of
severely limited feedback, constructing a quantized partial feedback is an
important issue. T... | stat.AP | partial feedback in multipleinput multipleoutput mimo communication systems provides tremendous capacity gain and enables the transmitter to exploit channel condition and to eliminate channel interference in the case of severely limited feedback constructing a quantized partial feedback is an important issue to reduce ... | [['partial', 'feedback', 'in', 'multipleinput', 'multipleoutput', 'mimo', 'communication', 'systems', 'provides', 'tremendous', 'capacity', 'gain', 'and', 'enables', 'the', 'transmitter', 'to', 'exploit', 'channel', 'condition', 'and', 'to', 'eliminate', 'channel', 'interference', 'in', 'the', 'case', 'of', 'severely',... | [-0.21708697151633904, 0.02057064515017157, -0.04887886559121686, 0.0024955110061618923, -0.13037165036766704, -0.2607677467971397, 0.09703194242047829, 0.3834505812901494, -0.30263092493464194, -0.2639214286058069, 0.1189121343388068, -0.22149638392419801, -0.1581861275661127, 0.12634318450586401, -0.14554221908019171... |
710.4174 | Structural Conditions for Full MHD Equations | In this paper, we investigate the characteristic structure of the full
equations of magnetohydrodynamics (MHD) and show that it satisfies the
hypotheses of a general variable-multiplicity stability frame- work introduced
by Metivier and Zumbrun, thereby extending to the general case various results
obtained by Metivi... | math.AP | in this paper we investigate the characteristic structure of the full equations of magnetohydrodynamics mhd and show that it satisfies the hypotheses of a general variablemultiplicity stability frame work introduced by metivier and zumbrun thereby extending to the general case various results obtained by metivier and z... | [['in', 'this', 'paper', 'we', 'investigate', 'the', 'characteristic', 'structure', 'of', 'the', 'full', 'equations', 'of', 'magnetohydrodynamics', 'mhd', 'and', 'show', 'that', 'it', 'satisfies', 'the', 'hypotheses', 'of', 'a', 'general', 'variablemultiplicity', 'stability', 'frame', 'work', 'introduced', 'by', 'metiv... | [-0.13028037458514938, 0.04451100340184684, -0.05220681979083635, 0.04660381475920216, -0.0522537763731984, -0.061230609291949525, -0.05667043844228969, 0.20929579054847217, -0.26845050408827287, -0.25005629680191094, 0.09791485036839731, -0.17801635518956643, -0.14427115109104377, 0.22111120325728104, -0.0490191359825... |
710.4175 | Integral means spectrum of random conformal snowflakes | In this paper we construct random conformal snowflakes with large integral
means spectrum at different points. These new estimates are significant
improvement over previously known lower bound of the universal spectrum. Our
estimates are within 5-10 percent from the conjectured value of the universal
spectrum.
| math.CV math.PR | in this paper we construct random conformal snowflakes with large integral means spectrum at different points these new estimates are significant improvement over previously known lower bound of the universal spectrum our estimates are within 510 percent from the conjectured value of the universal spectrum | [['in', 'this', 'paper', 'we', 'construct', 'random', 'conformal', 'snowflakes', 'with', 'large', 'integral', 'means', 'spectrum', 'at', 'different', 'points', 'these', 'new', 'estimates', 'are', 'significant', 'improvement', 'over', 'previously', 'known', 'lower', 'bound', 'of', 'the', 'universal', 'spectrum', 'our', ... | [-0.08123460602235152, 0.10751235702385505, -0.06916550651399625, 0.052192052730566096, -0.038905344406763714, -0.07855669224841727, 0.040887253837556474, 0.32443389147520063, -0.23940003224545056, -0.37393654733896253, 0.09577608093774567, -0.29190123577912647, -0.13278167206380104, 0.2753075086408191, -0.067598905046... |
710.4176 | Hochschild and cyclic (co)homology of preprojective algebras of quivers
of type T | We calculate the additive and multiplicative structure (together with the
grading) of the Hochschild homology and cohomology and the cyclic homology of
preprojective algebras of types T. We also compute the calculus structure which
is formed by the Hochschild homology/cohomology pair.
| math.RT math.QA | we calculate the additive and multiplicative structure together with the grading of the hochschild homology and cohomology and the cyclic homology of preprojective algebras of types t we also compute the calculus structure which is formed by the hochschild homologycohomology pair | [['we', 'calculate', 'the', 'additive', 'and', 'multiplicative', 'structure', 'together', 'with', 'the', 'grading', 'of', 'the', 'hochschild', 'homology', 'and', 'cohomology', 'and', 'the', 'cyclic', 'homology', 'of', 'preprojective', 'algebras', 'of', 'types', 't', 'we', 'also', 'compute', 'the', 'calculus', 'structur... | [-0.22922392045147716, 0.05974838170222938, -0.10527725969441235, 0.0863354016240919, -0.10087734461412765, -0.12850034383591263, -0.05277266507036984, 0.3459778151474893, -0.4927663069218397, -0.23206913378089666, 0.08670640110503883, -0.18465378694236279, -0.2272318058181554, 0.07370703807100654, -0.14781861868686974... |
710.4177 | Consistent Truncation to Three Dimensional (Super-)gravity | For a general three dimensional theory of (super-)gravity coupled to
arbitrary matter fields with arbitrary set of higher derivative terms in the
effective action, we give an algorithm for consistently truncating the theory
to a theory of pure (super-)gravity with the gravitational sector containing
only Einstein-Hil... | hep-th | for a general three dimensional theory of supergravity coupled to arbitrary matter fields with arbitrary set of higher derivative terms in the effective action we give an algorithm for consistently truncating the theory to a theory of pure supergravity with the gravitational sector containing only einsteinhilbert cosmo... | [['for', 'a', 'general', 'three', 'dimensional', 'theory', 'of', 'supergravity', 'coupled', 'to', 'arbitrary', 'matter', 'fields', 'with', 'arbitrary', 'set', 'of', 'higher', 'derivative', 'terms', 'in', 'the', 'effective', 'action', 'we', 'give', 'an', 'algorithm', 'for', 'consistently', 'truncating', 'the', 'theory',... | [-0.10891148619841606, 0.10758752409795609, -0.03479273899657918, 0.07285381146994907, -0.05330667818807775, -0.11455134725464242, -0.04902696249163931, 0.2512299965357497, -0.17642384952022916, -0.29111386755747454, 0.08761706779200938, -0.2625042779548537, -0.19451338775633348, 0.11343835108869132, -0.063782547928747... |
710.4178 | Composition-dependent polarization switching behaviors of
(111)-preferred polycrystalline Pb(Zr_{x}Ti_{1-x})O_{3} thin films | We investigated the time-dependent polarization switching behaviors of
(111)-preferred polycrystalline Pb(ZrxTi1-x)O3 thin films with various Zr
concentrations. We could explain all the polarization switching behaviors well
by assuming Lorentzian distributions in the logarithmic polarization switching
time [Refer to ... | cond-mat.mtrl-sci | we investigated the timedependent polarization switching behaviors of 111preferred polycrystalline pbzrxti1xo3 thin films with various zr concentrations we could explain all the polarization switching behaviors well by assuming lorentzian distributions in the logarithmic polarization switching time refer to j y jo et a... | [['we', 'investigated', 'the', 'timedependent', 'polarization', 'switching', 'behaviors', 'of', '111preferred', 'polycrystalline', 'pbzrxti1xo3', 'thin', 'films', 'with', 'various', 'zr', 'concentrations', 'we', 'could', 'explain', 'all', 'the', 'polarization', 'switching', 'behaviors', 'well', 'by', 'assuming', 'loren... | [-0.11394861279259202, 0.146057867386844, -0.016110201203264295, -0.042308665743621535, -0.06455098380683921, -0.12852556859143077, 0.07917385059008666, 0.4520162070519291, -0.21505068584810944, -0.2967805540887639, -0.0582264592681895, -0.2590749323600903, -0.13983425987535156, 0.156741601601243, -0.09075950441765598,... |
710.4179 | On a Connection between Entropy, Extensive Measurement and Memoryless
Characterization | We define an entropy based on a chosen governing probability distribution. If
a certain kind of measurements follow such a distribution it also gives us a
suitable scale to study it with. This scale will appear as a link function that
is applied to the measurements. A link function can also be used to define an
alter... | physics.data-an | we define an entropy based on a chosen governing probability distribution if a certain kind of measurements follow such a distribution it also gives us a suitable scale to study it with this scale will appear as a link function that is applied to the measurements a link function can also be used to define an alternativ... | [['we', 'define', 'an', 'entropy', 'based', 'on', 'a', 'chosen', 'governing', 'probability', 'distribution', 'if', 'a', 'certain', 'kind', 'of', 'measurements', 'follow', 'such', 'a', 'distribution', 'it', 'also', 'gives', 'us', 'a', 'suitable', 'scale', 'to', 'study', 'it', 'with', 'this', 'scale', 'will', 'appear', '... | [-0.0971305607445538, 0.12619849564459099, -0.1898104639351368, 0.11866983325065424, -0.09447633397920678, -0.12089354124075423, 0.02917944828979671, 0.34964519462237753, -0.29385214152590683, -0.27744727650346857, 0.10445354819918672, -0.2576547440265616, -0.14515719324350357, 0.21062297674361616, -0.06365209681292375... |
710.418 | A quick search method for audio signals based on a piecewise linear
representation of feature trajectories | This paper presents a new method for a quick similarity-based search through
long unlabeled audio streams to detect and locate audio clips provided by
users. The method involves feature-dimension reduction based on a piecewise
linear representation of a sequential feature trajectory extracted from a long
audio stream... | cs.MM cs.DB | this paper presents a new method for a quick similaritybased search through long unlabeled audio streams to detect and locate audio clips provided by users the method involves featuredimension reduction based on a piecewise linear representation of a sequential feature trajectory extracted from a long audio stream two ... | [['this', 'paper', 'presents', 'a', 'new', 'method', 'for', 'a', 'quick', 'similaritybased', 'search', 'through', 'long', 'unlabeled', 'audio', 'streams', 'to', 'detect', 'and', 'locate', 'audio', 'clips', 'provided', 'by', 'users', 'the', 'method', 'involves', 'featuredimension', 'reduction', 'based', 'on', 'a', 'piec... | [-0.05232089353376068, -0.030219612440334692, -0.12962381650821395, 0.04417598811860737, -0.10584847948273583, -0.14159056576224224, 0.10782058391956642, 0.3960029278250952, -0.2921291948559003, -0.37055704255978905, 0.07172242676812945, -0.2590513702016324, -0.1602907316898176, 0.24613389992455562, -0.0413155806055592... |
710.4181 | Thermodynamic and structural consensus principle predicts mature miRNA
location and structure, categorizes conserved interspecies miRNA subgroups,
and hints new possible mechanisms of miRNA maturization | Although conservation of thermodynamics is much less studied than of
sequences and structures, thermodynamic details are biophysical features
different from but as important as structural features. As a succession of
previous research which revealed the important relationships between
thermodynamic features and miRNA... | q-bio.BM q-bio.GN | although conservation of thermodynamics is much less studied than of sequences and structures thermodynamic details are biophysical features different from but as important as structural features as a succession of previous research which revealed the important relationships between thermodynamic features and mirna mat... | [['although', 'conservation', 'of', 'thermodynamics', 'is', 'much', 'less', 'studied', 'than', 'of', 'sequences', 'and', 'structures', 'thermodynamic', 'details', 'are', 'biophysical', 'features', 'different', 'from', 'but', 'as', 'important', 'as', 'structural', 'features', 'as', 'a', 'succession', 'of', 'previous', '... | [-0.0836732782067625, 0.11006507117867212, -0.07654168756580032, 0.12295685007570054, -0.05382283483026171, -0.1458504404027935, 0.055865524217440954, 0.3714282428580753, -0.2594648628988742, -0.28939351592046336, 0.038344690181992616, -0.2923705350793141, -0.1908039960355263, 0.14538785270169166, -0.04457117215450096,... |
710.4182 | Beyond Feedforward Models Trained by Backpropagation: a Practical
Training Tool for a More Efficient Universal Approximator | Cellular Simultaneous Recurrent Neural Network (SRN) has been shown to be a
function approximator more powerful than the MLP. This means that the
complexity of MLP would be prohibitively large for some problems while SRN
could realize the desired mapping with acceptable computational constraints.
The speed of trainin... | cs.NE | cellular simultaneous recurrent neural network srn has been shown to be a function approximator more powerful than the mlp this means that the complexity of mlp would be prohibitively large for some problems while srn could realize the desired mapping with acceptable computational constraints the speed of training of c... | [['cellular', 'simultaneous', 'recurrent', 'neural', 'network', 'srn', 'has', 'been', 'shown', 'to', 'be', 'a', 'function', 'approximator', 'more', 'powerful', 'than', 'the', 'mlp', 'this', 'means', 'that', 'the', 'complexity', 'of', 'mlp', 'would', 'be', 'prohibitively', 'large', 'for', 'some', 'problems', 'while', 's... | [-0.08582742003285956, -0.0005859774244252405, -0.04137114139622171, 0.0546929145109565, -0.0871328924156109, -0.17924280619087943, 0.01663370930804141, 0.4262320491210591, -0.2679106703450193, -0.3041651672503589, 0.12154997067221125, -0.209709205775247, -0.21761849434148495, 0.24056573646317284, -0.09946960330063062,... |
710.4183 | Late time tails in the Kerr spacetime | Outside a black hole, perturbation fields die off in time as $1/t^n$. For
spherical holes $n=2\ell+3$ where $\ell$ is the multipole index. In the
nonspherical Kerr spacetime there is no coordinate-independent meaning of
"multipole," and a common sense viewpoint is to set $\ell$ to the lowest
radiatiable index, althou... | gr-qc | outside a black hole perturbation fields die off in time as 1tn for spherical holes n2ell3 where ell is the multipole index in the nonspherical kerr spacetime there is no coordinateindependent meaning of multipole and a common sense viewpoint is to set ell to the lowest radiatiable index although theoretical studies ha... | [['outside', 'a', 'black', 'hole', 'perturbation', 'fields', 'die', 'off', 'in', 'time', 'as', '1tn', 'for', 'spherical', 'holes', 'n2ell3', 'where', 'ell', 'is', 'the', 'multipole', 'index', 'in', 'the', 'nonspherical', 'kerr', 'spacetime', 'there', 'is', 'no', 'coordinateindependent', 'meaning', 'of', 'multipole', 'a... | [-0.12281365688127208, 0.09157617551874908, -0.10291258035317423, 0.06364551204374531, -0.1314732158074088, -0.12520290023636027, 0.028621709362760813, 0.37186489613300344, -0.15116971760359874, -0.266416513304933, 0.06811620464761663, -0.3198753106127302, -0.10577681740319514, 0.22673131010483905, -0.05057035878101498... |
710.4184 | Critical charge dynamics of superconducting LSCO thin films probed by
complex microwave spectroscopy: Anomalous changes of the universality class
by hole doping | We study the critical charge dynamics of the superconducting to the
normal-state transition for LSCO thin films with a wide range of the Sr
concentration, by measuring the frequency-dependent excess parts of the complex
microwave conductivity, which is induced by the superconducting fluctuations.
We present a dynamic... | cond-mat.supr-con | we study the critical charge dynamics of the superconducting to the normalstate transition for lsco thin films with a wide range of the sr concentration by measuring the frequencydependent excess parts of the complex microwave conductivity which is induced by the superconducting fluctuations we present a dynamic scalin... | [['we', 'study', 'the', 'critical', 'charge', 'dynamics', 'of', 'the', 'superconducting', 'to', 'the', 'normalstate', 'transition', 'for', 'lsco', 'thin', 'films', 'with', 'a', 'wide', 'range', 'of', 'the', 'sr', 'concentration', 'by', 'measuring', 'the', 'frequencydependent', 'excess', 'parts', 'of', 'the', 'complex',... | [-0.11718910659478485, 0.19232264073247385, -0.02292271009312518, 0.0040499090370276995, -0.03646978477327673, -0.133185521896367, 0.11183874721652554, 0.3196389239096521, -0.24141240432072664, -0.28607043311828473, 0.021609846722105218, -0.34699477672213963, -0.12361581244605237, 0.18106339849563322, -0.01266202097459... |
710.4185 | Baryonium, tetra-quark state and glue-ball in large N_c QCD | From the large-N_c QCD point of view, baryonia, tetra-quark states, hybrids,
and glueballs are studied. The existence of these states is argued for. They
are constructed from baryons. In N_f=1 large N_c QCD, a baryonium is always
identical to a glueball with N_c valence gluons. The ground state 0^{-+}
glueball has a ... | hep-ph | from the largen_c qcd point of view baryonia tetraquark states hybrids and glueballs are studied the existence of these states is argued for they are constructed from baryons in n_f1 large n_c qcd a baryonium is always identical to a glueball with n_c valence gluons the ground state 0 glueball has a mass about 2450 mev... | [['from', 'the', 'largen_c', 'qcd', 'point', 'of', 'view', 'baryonia', 'tetraquark', 'states', 'hybrids', 'and', 'glueballs', 'are', 'studied', 'the', 'existence', 'of', 'these', 'states', 'is', 'argued', 'for', 'they', 'are', 'constructed', 'from', 'baryons', 'in', 'n_f1', 'large', 'n_c', 'qcd', 'a', 'baryonium', 'is'... | [-0.09451164632628206, 0.3877921487340548, -0.12082599062947945, 0.21014781184567255, -0.02114190909590737, -0.158469109267268, 0.08974664681954891, 0.32702099268014234, -0.07332941037990774, -0.18062879016360966, -0.08606705992739687, -0.38849350436551805, 0.041650725856015924, -0.045650646284533046, 0.113443364049696... |
710.4186 | Reflection of microwave from energy deposit by X-ray irradiation in rock
salt: Implication of an ultra high energy salt neutrino detector to act like
a radio bubble chamber | Existence of GZK neutrinos (ultra high energy neutrinos) have been justified
although the flux is very low. A new method is desired to use a huge mass of a
detector medium to detect them. A fundamental study of radar method was carried
out to measure microwave reflection from electromagnetic energy deposit by
X-ray i... | astro-ph | existence of gzk neutrinos ultra high energy neutrinos have been justified although the flux is very low a new method is desired to use a huge mass of a detector medium to detect them a fundamental study of radar method was carried out to measure microwave reflection from electromagnetic energy deposit by xray irradiat... | [['existence', 'of', 'gzk', 'neutrinos', 'ultra', 'high', 'energy', 'neutrinos', 'have', 'been', 'justified', 'although', 'the', 'flux', 'is', 'very', 'low', 'a', 'new', 'method', 'is', 'desired', 'to', 'use', 'a', 'huge', 'mass', 'of', 'a', 'detector', 'medium', 'to', 'detect', 'them', 'a', 'fundamental', 'study', 'of... | [-0.07780279577173133, 0.21595598534258897, -0.08597476967224793, 0.12942221174034785, -0.09122126196052704, -0.09026436578096764, 0.051277420885526226, 0.39542508743761573, -0.2214715885638725, -0.3734957454871619, 0.08166743944912014, -0.2933366172364913, -0.02000595780555159, 0.18036295167257776, -0.0143289439474756... |
710.4187 | Universal coding for correlated sources with complementary delivery | This paper deals with a universal coding problem for a certain kind of
multiterminal source coding system that we call the complementary delivery
coding system. In this system, messages from two correlated sources are jointly
encoded, and each decoder has access to one of the two messages to enable it to
reproduce th... | cs.IT math.IT | this paper deals with a universal coding problem for a certain kind of multiterminal source coding system that we call the complementary delivery coding system in this system messages from two correlated sources are jointly encoded and each decoder has access to one of the two messages to enable it to reproduce the oth... | [['this', 'paper', 'deals', 'with', 'a', 'universal', 'coding', 'problem', 'for', 'a', 'certain', 'kind', 'of', 'multiterminal', 'source', 'coding', 'system', 'that', 'we', 'call', 'the', 'complementary', 'delivery', 'coding', 'system', 'in', 'this', 'system', 'messages', 'from', 'two', 'correlated', 'sources', 'are', ... | [-0.23673435237220267, 0.04141003622183787, -0.04947431337510802, 0.0905914894886046, -0.028510278378872527, -0.3272374985864405, 0.09584947766798559, 0.3922715895261961, -0.34131490065687403, -0.2120021271336939, 0.12728424189665077, -0.2852401010375278, -0.16560516006185147, 0.1972742246214262, -0.13944898743528067, ... |
710.4188 | Mode-coupling theory of sheared dense granular liquids | Mode-coupling theory (MCT) of sheared dense granular liquids %in the vicinity
of jamming transition is formulated. Starting from the Liouville equation of
granular particles, the generalized Langevin equation is derived with the aid
of the projection operator technique. The MCT equation for the density
correlation fu... | cond-mat.stat-mech | modecoupling theory mct of sheared dense granular liquids in the vicinity of jamming transition is formulated starting from the liouville equation of granular particles the generalized langevin equation is derived with the aid of the projection operator technique the mct equation for the density correlation function ob... | [['modecoupling', 'theory', 'mct', 'of', 'sheared', 'dense', 'granular', 'liquids', 'in', 'the', 'vicinity', 'of', 'jamming', 'transition', 'is', 'formulated', 'starting', 'from', 'the', 'liouville', 'equation', 'of', 'granular', 'particles', 'the', 'generalized', 'langevin', 'equation', 'is', 'derived', 'with', 'the',... | [-0.10406066672518276, 0.17775235668970987, -0.21487747849180147, 0.06699072052008258, -0.01782875161809035, -0.1309876307988396, -0.0609215582222439, 0.2760284097196582, -0.3011337935160368, -0.21161997333192864, 0.019612115894396525, -0.3136042329715565, -0.2125352471589278, 0.1061246941009393, 0.05687549906090284, 0... |
710.4189 | Structural relaxation around substitutional Cr3+ in pyrope garnet | The structural environment of substitutional Cr3+ ion in a natural pyrope
Mg3Al2Si3O12 has been investigated by Cr K-edge Extended X-ray Absorption Fine
Structure (EXAFS) and X-ray Absorption Near Edge Structure (XANES) coupled with
first-principles computations. The Cr-O distance is close to that in
knorringite Mg3C... | cond-mat.mtrl-sci | the structural environment of substitutional cr3 ion in a natural pyrope mg3al2si3o12 has been investigated by cr kedge extended xray absorption fine structure exafs and xray absorption near edge structure xanes coupled with firstprinciples computations the cro distance is close to that in knorringite mg3cr2si3o12 indi... | [['the', 'structural', 'environment', 'of', 'substitutional', 'cr3', 'ion', 'in', 'a', 'natural', 'pyrope', 'mg3al2si3o12', 'has', 'been', 'investigated', 'by', 'cr', 'kedge', 'extended', 'xray', 'absorption', 'fine', 'structure', 'exafs', 'and', 'xray', 'absorption', 'near', 'edge', 'structure', 'xanes', 'coupled', 'w... | [-0.11086245790562209, 0.1438930539332111, 0.030754009891739664, -0.0021136964091519805, -0.033994726626677255, -0.13437265747993746, 0.08735841816729482, 0.47889066516768697, -0.32201985025084484, -0.2489487397867967, 0.01887794732636608, -0.3403589100777811, -0.09665046387589445, -0.0020610991518433186, 0.06549245892... |
710.419 | Parameter estimation of ODE's via nonparametric estimators | Ordinary differential equations (ODE's) are widespread models in physics,
chemistry and biology. In particular, this mathematical formalism is used for
describing the evolution of complex systems and it might consist of
high-dimensional sets of coupled nonlinear differential equations. In this
setting, we propose a g... | math.ST stat.TH | ordinary differential equations odes are widespread models in physics chemistry and biology in particular this mathematical formalism is used for describing the evolution of complex systems and it might consist of highdimensional sets of coupled nonlinear differential equations in this setting we propose a general meth... | [['ordinary', 'differential', 'equations', 'odes', 'are', 'widespread', 'models', 'in', 'physics', 'chemistry', 'and', 'biology', 'in', 'particular', 'this', 'mathematical', 'formalism', 'is', 'used', 'for', 'describing', 'the', 'evolution', 'of', 'complex', 'systems', 'and', 'it', 'might', 'consist', 'of', 'highdimens... | [-0.06563691356088092, 0.0003931412525864118, -0.1030218584162977, 0.1059031312200772, -0.06647071413439543, -0.11811793117077658, -0.0049102194732267585, 0.3286485414477003, -0.28709936683259957, -0.2720369227268052, 0.12960779860665733, -0.2316103072230698, -0.1968273905187145, 0.22117253525288863, -0.139020400415580... |
710.4191 | Anisotropic Magnification Distortion of the 3D Galaxy Correlation: II.
Fourier and Redshift Space | In paper I of this series we discuss how magnification bias distorts the 3D
correlation function by enhancing the observed correlation in the line-of-sight
(LOS) orientation, especially on large scales. This lensing anisotropy is
distinctive, making it possible to separately measure the galaxy-galaxy,
galaxy-magnific... | astro-ph | in paper i of this series we discuss how magnification bias distorts the 3d correlation function by enhancing the observed correlation in the lineofsight los orientation especially on large scales this lensing anisotropy is distinctive making it possible to separately measure the galaxygalaxy galaxymagnification it and... | [['in', 'paper', 'i', 'of', 'this', 'series', 'we', 'discuss', 'how', 'magnification', 'bias', 'distorts', 'the', '3d', 'correlation', 'function', 'by', 'enhancing', 'the', 'observed', 'correlation', 'in', 'the', 'lineofsight', 'los', 'orientation', 'especially', 'on', 'large', 'scales', 'this', 'lensing', 'anisotropy'... | [-0.16031458705644278, 0.14107514997897308, -0.09884530722430741, 0.13052828038876602, -0.1371084194343407, -0.07706625390682341, -0.05257103180597616, 0.3907138341063157, -0.2610568926243704, -0.28870522683890637, 0.05393168573491564, -0.29057729055982284, -0.09292728518241432, 0.2058842519411904, -0.00687255434531270... |
710.4192 | Nuclear Matter and Neutron stars in a Parity Doublet Model | We investigate the properties of isospin-symmetric nuclear matter and neutron
stars in a chiral model approach adopting the SU(2) parity doublet formulation.
This ansatz explicitly incorporates chiral symmetry restoration with the limit
of degenerate masses of the nucleons and their parity partners. Instead of
search... | nucl-th | we investigate the properties of isospinsymmetric nuclear matter and neutron stars in a chiral model approach adopting the su2 parity doublet formulation this ansatz explicitly incorporates chiral symmetry restoration with the limit of degenerate masses of the nucleons and their parity partners instead of searching for... | [['we', 'investigate', 'the', 'properties', 'of', 'isospinsymmetric', 'nuclear', 'matter', 'and', 'neutron', 'stars', 'in', 'a', 'chiral', 'model', 'approach', 'adopting', 'the', 'su2', 'parity', 'doublet', 'formulation', 'this', 'ansatz', 'explicitly', 'incorporates', 'chiral', 'symmetry', 'restoration', 'with', 'the'... | [-0.07932168279733995, 0.19158635105644783, -0.09329306672873866, 0.13069638633042696, -0.08094719333736144, -0.07687604726980561, 0.05482361552750935, 0.33713652999342786, -0.16634956075880758, -0.35861917178187036, 0.016451718813344916, -0.2733435412544919, -0.019392262253424396, 0.08478472039164246, 0.05010249509739... |
710.4193 | Reaction cross sections of carbon isotopes incident on a proton | We systematically study total reaction cross sections of carbon isotopes with
N=6-16 on a proton target for wide range of incident energies, putting an
emphasis on the difference from the case of a carbon target. The analysis
includes the reaction cross sections of ^{19,20,22}C at 40 AMeV, the data of
which have rece... | nucl-th | we systematically study total reaction cross sections of carbon isotopes with n616 on a proton target for wide range of incident energies putting an emphasis on the difference from the case of a carbon target the analysis includes the reaction cross sections of 192022c at 40 amev the data of which have recently been me... | [['we', 'systematically', 'study', 'total', 'reaction', 'cross', 'sections', 'of', 'carbon', 'isotopes', 'with', 'n616', 'on', 'a', 'proton', 'target', 'for', 'wide', 'range', 'of', 'incident', 'energies', 'putting', 'an', 'emphasis', 'on', 'the', 'difference', 'from', 'the', 'case', 'of', 'a', 'carbon', 'target', 'the... | [-0.01661356945645393, 0.10617566158447624, -0.09254628587201724, 0.12499091395447441, 0.0348957319271422, -0.09857645657158333, 0.04414101789948558, 0.3748062744818847, -0.19456386511720827, -0.28548302033039574, -0.031560914965024604, -0.3422253318884246, -0.03938568843638196, 0.15961840893450083, 0.06564590616054534... |
710.4194 | On the Hodge-Newton filtration for p-divisible O-modules | The notions Hodge-Newton decomposition and Hodge-Newton filtration for
F-crystals are due to Katz and generalize Messing's result on the existence of
the local-\'etale filtration for p-divisible groups. Recently, some of Katz's
classical results have been generalized by Kottwitz to the context of
F-crystals with addi... | math.AG | the notions hodgenewton decomposition and hodgenewton filtration for fcrystals are due to katz and generalize messings result on the existence of the localetale filtration for pdivisible groups recently some of katzs classical results have been generalized by kottwitz to the context of fcrystals with additional structu... | [['the', 'notions', 'hodgenewton', 'decomposition', 'and', 'hodgenewton', 'filtration', 'for', 'fcrystals', 'are', 'due', 'to', 'katz', 'and', 'generalize', 'messings', 'result', 'on', 'the', 'existence', 'of', 'the', 'localetale', 'filtration', 'for', 'pdivisible', 'groups', 'recently', 'some', 'of', 'katzs', 'classic... | [-0.1450100785990556, 0.06888782196988662, -0.15229313706358275, 0.047423134810912114, -0.10446872770786285, -0.08744159016758203, -0.012162878623542686, 0.33260627085963884, -0.3518523851533731, -0.2657181212306023, 0.11586444382711003, -0.20697216728702186, -0.18498219605535268, 0.20112518578767777, -0.23033950135111... |
710.4195 | Simple helices on Fano threefolds | Building on the work of Nogin \cite{Nogin}, we prove that the braid group
$B_4$ acts transitively on full exceptional collections of vector bundles on
Fano threefolds with $b_2=1$ and $b_3=0$. Equivalently, this group acts
transitively on the set of simple helices (considered up to a shift in the
derived category) on... | math.AG | building on the work of nogin citenogin we prove that the braid group b_4 acts transitively on full exceptional collections of vector bundles on fano threefolds with b_21 and b_30 equivalently this group acts transitively on the set of simple helices considered up to a shift in the derived category on such a fano three... | [['building', 'on', 'the', 'work', 'of', 'nogin', 'citenogin', 'we', 'prove', 'that', 'the', 'braid', 'group', 'b_4', 'acts', 'transitively', 'on', 'full', 'exceptional', 'collections', 'of', 'vector', 'bundles', 'on', 'fano', 'threefolds', 'with', 'b_21', 'and', 'b_30', 'equivalently', 'this', 'group', 'acts', 'transi... | [-0.22277301914785821, 0.04502519575658905, -0.04365964354436896, 0.04035536246214776, -0.15432962530279812, -0.17400077599011463, 0.041601012942496025, 0.4266632331968987, -0.267843127040167, -0.1574948678456553, 0.0874407390620534, -0.2671741331378891, -0.1840648956864766, 0.24628596352285717, -0.18511156605122842, -... |
710.4196 | Magnitude Uncertainties Impact Seismic Rate Estimates, Forecasts and
Predictability Experiments | The Collaboratory for the Study of Earthquake Predictability (CSEP) aims to
prospectively test time-dependent earthquake probability forecasts on their
consistency with observations. To compete, time-dependent seismicity models are
calibrated on earthquake catalog data. But catalogs contain much observational
uncerta... | physics.geo-ph | the collaboratory for the study of earthquake predictability csep aims to prospectively test timedependent earthquake probability forecasts on their consistency with observations to compete timedependent seismicity models are calibrated on earthquake catalog data but catalogs contain much observational uncertainty we s... | [['the', 'collaboratory', 'for', 'the', 'study', 'of', 'earthquake', 'predictability', 'csep', 'aims', 'to', 'prospectively', 'test', 'timedependent', 'earthquake', 'probability', 'forecasts', 'on', 'their', 'consistency', 'with', 'observations', 'to', 'compete', 'timedependent', 'seismicity', 'models', 'are', 'calibra... | [-0.08481279176970323, 0.08427768927746608, -0.10305549662663704, 0.16771499525289982, -0.0530349609716278, -0.08079870135419899, 0.06670307236206201, 0.3597748109325767, -0.1891374501006471, -0.3348569547591938, 0.14289805164819377, -0.3225435238621301, -0.08775003388006654, 0.22037396719679236, -0.08282119953177042, ... |
710.4197 | The equation of state at high temperatures from lattice QCD | We present results for the equation of state upto previously unreachable,
high temperatures. Since the temperature range is quite large, a comparison
with perturbation theory can be done directly.
| hep-lat | we present results for the equation of state upto previously unreachable high temperatures since the temperature range is quite large a comparison with perturbation theory can be done directly | [['we', 'present', 'results', 'for', 'the', 'equation', 'of', 'state', 'upto', 'previously', 'unreachable', 'high', 'temperatures', 'since', 'the', 'temperature', 'range', 'is', 'quite', 'large', 'a', 'comparison', 'with', 'perturbation', 'theory', 'can', 'be', 'done', 'directly']] | [-0.09063705225507247, 0.180365153219037, -0.11344088978487356, 0.043589043611628485, -0.046625576977585924, -0.10699706471621476, 0.035745643019066034, 0.35858687989670657, -0.23376302074255614, -0.3931128931199682, 0.12883516258142633, -0.25426048647355415, -0.035670002087436876, 0.23139995702638708, 0.01456953087371... |
710.4198 | Topological Classification of Gapped Spin Chains :Quantized Berry Phase
as a Local Order Parameter | We characterize several phases of gapped spin systems by local order
parameters defined by quantized Berry phases. This characterization is
topologically stable against any small perturbation as long as the energy gap
remains finite. The models we pick up are $S=1,2$ dimerized Heisenberg chains
and S=2 Heisenberg cha... | cond-mat.str-el cond-mat.stat-mech | we characterize several phases of gapped spin systems by local order parameters defined by quantized berry phases this characterization is topologically stable against any small perturbation as long as the energy gap remains finite the models we pick up are s12 dimerized heisenberg chains and s2 heisenberg chains with ... | [['we', 'characterize', 'several', 'phases', 'of', 'gapped', 'spin', 'systems', 'by', 'local', 'order', 'parameters', 'defined', 'by', 'quantized', 'berry', 'phases', 'this', 'characterization', 'is', 'topologically', 'stable', 'against', 'any', 'small', 'perturbation', 'as', 'long', 'as', 'the', 'energy', 'gap', 'rema... | [-0.24392490620659882, 0.28552993820292527, -0.006074209854569893, 0.08581740766503783, -0.0347832917603989, -0.17978638343426379, 0.022193495999090374, 0.38715964466939834, -0.28483596506940073, -0.25741803629843646, 0.10174303072326016, -0.29429497277813554, -0.14186271281674678, 0.10981732358625375, 0.07017314360412... |
710.4199 | Observation of Orbitally Excited B_s Mesons | We report the first observation of two narrow resonances consistent with
states of orbitally excited (L=1) B_s mesons using 1 fb^{-1} of ppbar
collisions at sqrt{s} = 1.96 TeV collected with the CDF II detector at the
Fermilab Tevatron. We use two-body decays into K^- and B^+ mesons reconstructed
as B^+ \to J/\psi K^... | hep-ex | we report the first observation of two narrow resonances consistent with states of orbitally excited l1 b_s mesons using 1 fb1 of ppbar collisions at sqrts 196 tev collected with the cdf ii detector at the fermilab tevatron we use twobody decays into k and b mesons reconstructed as b to jpsi k jpsi to mu mu or b to bar... | [['we', 'report', 'the', 'first', 'observation', 'of', 'two', 'narrow', 'resonances', 'consistent', 'with', 'states', 'of', 'orbitally', 'excited', 'l1', 'b_s', 'mesons', 'using', '1', 'fb1', 'of', 'ppbar', 'collisions', 'at', 'sqrts', '196', 'tev', 'collected', 'with', 'the', 'cdf', 'ii', 'detector', 'at', 'the', 'fer... | [-0.06616860701714034, 0.29880415909222247, -0.08980723751570892, 0.09218440478506648, -0.03340092099007265, -0.1920009492494074, 0.08455810480446405, 0.314133354474181, -0.18701779430755128, -0.2706557380288471, -0.1391770918738603, -0.46749783900600894, 0.16400275922978275, 0.033868251379901244, 0.1565610316041627, 0... |
710.42 | Global L2-Boundedness Theorems for Semiclassical Fourier Integral
Operators with Complex Phase | In this work, a class of semiclassical Fourier Integral Operators (FIOs) with
complex phase associated to some canonical transformation of the phase space
$T^*\R^d$ is constructed. Upon some general boundedness assumptions on the
symbol and the canonical transformation, their continuity (as operators) from
the Schwar... | math-ph math.FA math.MP | in this work a class of semiclassical fourier integral operators fios with complex phase associated to some canonical transformation of the phase space trd is constructed upon some general boundedness assumptions on the symbol and the canonical transformation their continuity as operators from the schwartz class into i... | [['in', 'this', 'work', 'a', 'class', 'of', 'semiclassical', 'fourier', 'integral', 'operators', 'fios', 'with', 'complex', 'phase', 'associated', 'to', 'some', 'canonical', 'transformation', 'of', 'the', 'phase', 'space', 'trd', 'is', 'constructed', 'upon', 'some', 'general', 'boundedness', 'assumptions', 'on', 'the',... | [-0.07379558245566759, 0.11395616222342307, -0.11482071182267233, 0.09186897719786925, -0.12754462497647512, -0.06881243379109285, 0.010866363346576691, 0.3395171789960428, -0.3368967808698389, -0.18045374365015462, 0.1425264425723898, -0.2486709775403142, -0.1818540855903517, 0.2085588497109711, -0.10235565750097686, ... |
710.4201 | The role of energy-momentum conservation in emission of Cherenkov gluons | The famous formula for the emission angle of Cherenkov radiation should be
modified when applied to hadronic reactions because of recoil effects. They
impose the upper limit on the energy of the gluon emitted at a given angle.
Also, it leads to essential corrections to the nuclear refractive index value
as determined... | hep-ph nucl-th | the famous formula for the emission angle of cherenkov radiation should be modified when applied to hadronic reactions because of recoil effects they impose the upper limit on the energy of the gluon emitted at a given angle also it leads to essential corrections to the nuclear refractive index value as determined from... | [['the', 'famous', 'formula', 'for', 'the', 'emission', 'angle', 'of', 'cherenkov', 'radiation', 'should', 'be', 'modified', 'when', 'applied', 'to', 'hadronic', 'reactions', 'because', 'of', 'recoil', 'effects', 'they', 'impose', 'the', 'upper', 'limit', 'on', 'the', 'energy', 'of', 'the', 'gluon', 'emitted', 'at', 'a... | [-0.04543388237134885, 0.20538976452297578, -0.12785972254666483, 0.12214700810333035, -0.08152676837802944, -0.09308124639062305, 0.010386831547386186, 0.343165508187297, -0.24802539442365956, -0.3265968307979026, 0.037245236179333625, -0.2879427715946557, 0.0034961897437855347, 0.22428184937117462, 0.0030855528962940... |
710.4202 | Sub-millimeter Observations of Giant Molecular Clouds in the Large
Magellanic Cloud: Temperature and Density as Determined from J=3-2 and J=1-0
transitions of CO | We have carried out sub-mm 12CO(J=3-2) observations of 6 giant molecular
clouds (GMCs) in the Large Magellanic Cloud (LMC) with the ASTE 10m sub-mm
telescope at a spatial resolution of 5 pc and very high sensitivity. We have
identified 32 molecular clumps in the GMCs and revealed significant details of
the warm and d... | astro-ph | we have carried out submm 12coj32 observations of 6 giant molecular clouds gmcs in the large magellanic cloud lmc with the aste 10m submm telescope at a spatial resolution of 5 pc and very high sensitivity we have identified 32 molecular clumps in the gmcs and revealed significant details of the warm and dense molecula... | [['we', 'have', 'carried', 'out', 'submm', '12coj32', 'observations', 'of', '6', 'giant', 'molecular', 'clouds', 'gmcs', 'in', 'the', 'large', 'magellanic', 'cloud', 'lmc', 'with', 'the', 'aste', '10m', 'submm', 'telescope', 'at', 'a', 'spatial', 'resolution', 'of', '5', 'pc', 'and', 'very', 'high', 'sensitivity', 'we'... | [-0.08193040841229818, 0.11413198119826032, -0.019206452104690425, 0.0748419851663068, -0.021647199433845816, -0.015478689904866857, 0.053433890933067434, 0.46152695470853994, -0.10723581704072618, -0.3582982407333914, 0.01837276186623075, -0.26719276679022874, -0.015652665645693956, 0.10050005219924008, 0.009789665612... |
710.4203 | Baryon to Meson Ratios on the Near and Away-Side of Jets and their
Centrality Dependence at STAR | We measure relative abundances of $K_{S}^{0}$, $\Lambda$ and $\bar{\Lambda}$
in near-side and away-side cones correlated with triggered high-$p_{T}$
particles in $^{197}$Au + $^{197}$Au collisions at $\sqrt{s_{NN}}$ = 200 GeV.
The centrality dependence of identified particles in the triggered particle
cones is also p... | nucl-ex | we measure relative abundances of k_s0 lambda and barlambda in nearside and awayside cones correlated with triggered highp_t particles in 197au 197au collisions at sqrts_nn 200 gev the centrality dependence of identified particles in the triggered particle cones is also presented particle yields and ratios are extracte... | [['we', 'measure', 'relative', 'abundances', 'of', 'k_s0', 'lambda', 'and', 'barlambda', 'in', 'nearside', 'and', 'awayside', 'cones', 'correlated', 'with', 'triggered', 'highp_t', 'particles', 'in', '197au', '197au', 'collisions', 'at', 'sqrts_nn', '200', 'gev', 'the', 'centrality', 'dependence', 'of', 'identified', '... | [-0.09184800756937715, 0.24932876850053778, -0.16922049245819354, 0.16426463615275946, 0.030254165162606275, -0.07778943046886365, -0.10312766043010496, 0.4070336984056185, -0.2426818080164273, -0.304124898979139, -0.0800536042678526, -0.3910312430919422, 0.06273661407313365, 0.12000065159586751, 0.05005337899852106, 0... |
710.4204 | Chirality sensitive effect on surface states in chiral p-wave
superconductors | We study the local density of states at the surface of a chiral p-wave
superconductor in the presence of a weak magnetic field. As a result, the
formation of low-energy Andreev bound states is either suppressed or enhanced
by an applied magnetic field, depending on its orientation with respect to the
chirality of the... | cond-mat.supr-con | we study the local density of states at the surface of a chiral pwave superconductor in the presence of a weak magnetic field as a result the formation of lowenergy andreev bound states is either suppressed or enhanced by an applied magnetic field depending on its orientation with respect to the chirality of the pwave ... | [['we', 'study', 'the', 'local', 'density', 'of', 'states', 'at', 'the', 'surface', 'of', 'a', 'chiral', 'pwave', 'superconductor', 'in', 'the', 'presence', 'of', 'a', 'weak', 'magnetic', 'field', 'as', 'a', 'result', 'the', 'formation', 'of', 'lowenergy', 'andreev', 'bound', 'states', 'is', 'either', 'suppressed', 'or... | [-0.2019084181700801, 0.197910355141834, -0.09536233318343373, 0.06377462741862662, -0.07559680105347572, -0.12269611795962757, 0.08959003740917602, 0.3253505948031771, -0.2233403123883081, -0.2822948920059797, 0.018083199966048565, -0.2622889551045052, -0.09400761843827585, 0.12761614088506984, 0.0142520512133066, -0.... |
710.4205 | Factorization Approach for Top Mass Reconstruction at High Energies | Using effective theories for jets and heavy quarks it is possible to prove
that the double differential top-antitop invariant mass distribution for the
process $e^+e^-\to t\bar t$ in the resonance region for c.m. energies $Q$ much
larger than the top mass can factorized into perturbatively computable hard
coefficient... | hep-ph | using effective theories for jets and heavy quarks it is possible to prove that the double differential topantitop invariant mass distribution for the process eeto tbar t in the resonance region for cm energies q much larger than the top mass can factorized into perturbatively computable hard coefficients and jet funct... | [['using', 'effective', 'theories', 'for', 'jets', 'and', 'heavy', 'quarks', 'it', 'is', 'possible', 'to', 'prove', 'that', 'the', 'double', 'differential', 'topantitop', 'invariant', 'mass', 'distribution', 'for', 'the', 'process', 'eeto', 'tbar', 't', 'in', 'the', 'resonance', 'region', 'for', 'cm', 'energies', 'q', ... | [-0.018011817602408036, 0.1988612176899455, -0.12335363421752527, 0.1743206980934127, -0.0711796359943324, -0.10984709116899849, 0.02265290107390141, 0.36721841533455934, -0.22010147464134844, -0.3109465611495053, -0.03198010544496866, -0.27473024679401487, 0.03525768145469524, 0.1869029897886018, 0.025161901000517486,... |
710.4206 | Measurement of 25Mg(p; gamma)26Al resonance strengths via gamma
spectrometry | The COMPTEL instrument performed the first mapping of the 1.809 MeV photons
in the Galaxy, triggering considerable interest in determing the sources of
interstellar 26Al. The predicted 26Al is too low compared to the observation,
for a better understanding more accurate rates for the 25Mg(p; gamma)26Al
reaction are r... | nucl-ex | the comptel instrument performed the first mapping of the 1809 mev photons in the galaxy triggering considerable interest in determing the sources of interstellar 26al the predicted 26al is too low compared to the observation for a better understanding more accurate rates for the 25mgp gamma26al reaction are required t... | [['the', 'comptel', 'instrument', 'performed', 'the', 'first', 'mapping', 'of', 'the', '1809', 'mev', 'photons', 'in', 'the', 'galaxy', 'triggering', 'considerable', 'interest', 'in', 'determing', 'the', 'sources', 'of', 'interstellar', '26al', 'the', 'predicted', '26al', 'is', 'too', 'low', 'compared', 'to', 'the', 'o... | [-0.04490318189040878, 0.13313490518503973, -0.060568118560402055, 0.09800584287938452, -0.005228575141846968, -0.13507919897505594, 0.00697515290155406, 0.37884638674046484, -0.12042772877330502, -0.38481449350083785, 0.024286946293056732, -0.37223345417183856, 0.04930546753589184, 0.22659149536329712, 0.0291573258432... |
710.4207 | Low degree bounded cohomology and l^2-invariants for negatively curved
groups | We study the subgroup structure of discrete groups which share cohomological
properties which resemble non-negative curvature. Examples include all Gromov
hyperbolic groups.
We provide strong restrictions on the possible s-normal subgroups of a Gromov
hyperbolic group, or more generally a 'negatively curved' group.... | math.GR math.DS | we study the subgroup structure of discrete groups which share cohomological properties which resemble nonnegative curvature examples include all gromov hyperbolic groups we provide strong restrictions on the possible snormal subgroups of a gromov hyperbolic group or more generally a negatively curved group another res... | [['we', 'study', 'the', 'subgroup', 'structure', 'of', 'discrete', 'groups', 'which', 'share', 'cohomological', 'properties', 'which', 'resemble', 'nonnegative', 'curvature', 'examples', 'include', 'all', 'gromov', 'hyperbolic', 'groups', 'we', 'provide', 'strong', 'restrictions', 'on', 'the', 'possible', 'snormal', 's... | [-0.16184608914264817, 0.1400399382591353, -0.14923962239279515, 0.07465196242149447, -0.13919173965289716, -0.11223992453296742, 0.02185490963211845, 0.4152022639200801, -0.29272831976413727, -0.211644790135324, 0.1378381316455835, -0.2477537444053543, -0.15822172600088552, 0.2260244558842498, -0.18240609337827043, -0... |
710.4208 | Structure factor of Bose-condensed systems | The structure factor for a Bose system with Bose-Einstein condensate is
considered in the frame of the self-consistent mean-field approximation. The
accomplished analysis demonstrates the principal importance of the following
three points: the necessity of preserving the approximation order, the
necessity of taking i... | cond-mat.stat-mech | the structure factor for a bose system with boseeinstein condensate is considered in the frame of the selfconsistent meanfield approximation the accomplished analysis demonstrates the principal importance of the following three points the necessity of preserving the approximation order the necessity of taking into acco... | [['the', 'structure', 'factor', 'for', 'a', 'bose', 'system', 'with', 'boseeinstein', 'condensate', 'is', 'considered', 'in', 'the', 'frame', 'of', 'the', 'selfconsistent', 'meanfield', 'approximation', 'the', 'accomplished', 'analysis', 'demonstrates', 'the', 'principal', 'importance', 'of', 'the', 'following', 'three... | [-0.19374429974704982, 0.12190339249723098, -0.11946278431984919, 0.0775896164780373, -0.02748637333895792, -0.0715220357181833, 0.042754234053084955, 0.2902586597510997, -0.20590463366140338, -0.26280473207726196, 0.05453147340757663, -0.23849849812686444, -0.10822344588882783, 0.09257497657364344, 0.0401485916446237,... |
710.4209 | Chow motives of universal families over some Shimura surfaces | We prove an absolute Chow-Kuenneth decomposition for the motive of universal
families A of abelian varieties over some compact Shimura surface. We
furthermore prove the Hodge conjecture for general fibres of A, extending
results of Ribet.
| math.AG math.NT | we prove an absolute chowkuenneth decomposition for the motive of universal families a of abelian varieties over some compact shimura surface we furthermore prove the hodge conjecture for general fibres of a extending results of ribet | [['we', 'prove', 'an', 'absolute', 'chowkuenneth', 'decomposition', 'for', 'the', 'motive', 'of', 'universal', 'families', 'a', 'of', 'abelian', 'varieties', 'over', 'some', 'compact', 'shimura', 'surface', 'we', 'furthermore', 'prove', 'the', 'hodge', 'conjecture', 'for', 'general', 'fibres', 'of', 'a', 'extending', '... | [-0.21582446767327687, 0.018703210895586783, -0.20478195986813968, 0.08877176077415545, -0.105958869215101, -0.09456933121610847, 0.005889977871750792, 0.2917086619676815, -0.31567115129696, -0.15914089791476727, 0.09096741856127563, -0.13606480135866958, -0.14829389988962147, 0.3322066602607568, -0.2558786713828643, -... |
710.421 | Conductance of a tunnel point-contact of noble metals in the presence of
a single defect | In paper [1] (Avotina et al. Phys. Rev. B,74, 085411 (2006)) the effect of
Fermi surface anisotropy to the conductance of a tunnel point contact, in the
vicinity of which a single point-like defect is situated, has been investigated
theoretically. The oscillatory dependence of the conductance on the distance
between ... | cond-mat.mes-hall | in paper 1 avotina et al phys rev b74 085411 2006 the effect of fermi surface anisotropy to the conductance of a tunnel point contact in the vicinity of which a single pointlike defect is situated has been investigated theoretically the oscillatory dependence of the conductance on the distance between the contact and t... | [['in', 'paper', '1', 'avotina', 'et', 'al', 'phys', 'rev', 'b74', '085411', '2006', 'the', 'effect', 'of', 'fermi', 'surface', 'anisotropy', 'to', 'the', 'conductance', 'of', 'a', 'tunnel', 'point', 'contact', 'in', 'the', 'vicinity', 'of', 'which', 'a', 'single', 'pointlike', 'defect', 'is', 'situated', 'has', 'been'... | [-0.1362201697939566, 0.10119181005952911, -0.10127110098922298, -0.017294992066258636, -0.004392079027895709, -0.12642743048890856, 0.056210663487320726, 0.33774277860057034, -0.2312782222506384, -0.33014174133098423, -0.04529554664711859, -0.29591414059746923, -0.19751752739530484, 0.23118171671704027, -0.04011922334... |
710.4211 | Dispersion relations and QCD factorization in hard reactions | We study analytical properties of the hard exclusive process amplitudes. We
found that QCD factorization for deeply virtual Compton scattering and hard
exclusive vector meson production results in the subtracted dispersion relation
with the subtraction constant determined by the Polyakov-Weiss $D$-term.
| hep-ph | we study analytical properties of the hard exclusive process amplitudes we found that qcd factorization for deeply virtual compton scattering and hard exclusive vector meson production results in the subtracted dispersion relation with the subtraction constant determined by the polyakovweiss dterm | [['we', 'study', 'analytical', 'properties', 'of', 'the', 'hard', 'exclusive', 'process', 'amplitudes', 'we', 'found', 'that', 'qcd', 'factorization', 'for', 'deeply', 'virtual', 'compton', 'scattering', 'and', 'hard', 'exclusive', 'vector', 'meson', 'production', 'results', 'in', 'the', 'subtracted', 'dispersion', 're... | [-0.08198753846227191, 0.22765797694446518, -0.14204887324012816, 0.18783698967476994, -0.08887503203004599, -0.0988625306636095, 0.08106228434480726, 0.4342566004022956, -0.24464085253421217, -0.1503429975826293, -0.02863348188402597, -0.29242991395294665, -0.09245710400864482, 0.09826836418360471, 0.10476766891079023... |
710.4212 | $\pi N\to \eta N$ process in a $\chi$QM approach | A chiral quark model approach is used to investigate the $\pi^{-}p \to \eta
n$ process at low energies. The roles of the most relevant nucleon resonances
in $n\leq 2$ shells are briefly discussed.
| nucl-th | a chiral quark model approach is used to investigate the pip to eta n process at low energies the roles of the most relevant nucleon resonances in nleq 2 shells are briefly discussed | [['a', 'chiral', 'quark', 'model', 'approach', 'is', 'used', 'to', 'investigate', 'the', 'pip', 'to', 'eta', 'n', 'process', 'at', 'low', 'energies', 'the', 'roles', 'of', 'the', 'most', 'relevant', 'nucleon', 'resonances', 'in', 'nleq', '2', 'shells', 'are', 'briefly', 'discussed']] | [-0.10966299412151177, 0.2448039771706769, -0.023647560328809603, 0.1596493695734821, 0.013736570744323686, -0.1477498009264695, 0.009166121398183432, 0.3596489695888577, -0.1602904551387341, -0.24474173400438193, -0.02822271682618355, -0.3131890692324801, -0.08475412375463004, 0.08602761691012843, 0.08904724892680392,... |
710.4213 | On the Integrable Structure of the Ising Model | Starting from the lattice $A_3$ realization of the Ising model defined on a
strip with integrable boundary conditions, the exact spectrum (including
excited states) of all the local integrals of motion is derived in the
continuum limit by means of TBA techniques. It is also possible to follow the
massive flow of this... | hep-th cond-mat.stat-mech | starting from the lattice a_3 realization of the ising model defined on a strip with integrable boundary conditions the exact spectrum including excited states of all the local integrals of motion is derived in the continuum limit by means of tba techniques it is also possible to follow the massive flow of this spectru... | [['starting', 'from', 'the', 'lattice', 'a_3', 'realization', 'of', 'the', 'ising', 'model', 'defined', 'on', 'a', 'strip', 'with', 'integrable', 'boundary', 'conditions', 'the', 'exact', 'spectrum', 'including', 'excited', 'states', 'of', 'all', 'the', 'local', 'integrals', 'of', 'motion', 'is', 'derived', 'in', 'the'... | [-0.13994384407124016, 0.13259083449067371, -0.08376312689012233, 0.03896586938963254, -0.03978363033120503, -0.10978697382247532, 0.028253053772957327, 0.3174530195669745, -0.24831534038245115, -0.2337308375797463, 0.09902811458747271, -0.296373678336166, -0.13669541001293528, 0.1676800553577091, -0.000300798099488019... |
710.4214 | Typicality for Generalized Microcanonical Ensembles | For a macroscopic, isolated quantum system in an unknown pure state, the
expectation value of any given observable is shown to hardly deviate from the
ensemble average with extremely high probability under generic equilibrium and
nonequilibrium conditions. Special care is devoted to the uncontrollable
microscopic det... | cond-mat.stat-mech | for a macroscopic isolated quantum system in an unknown pure state the expectation value of any given observable is shown to hardly deviate from the ensemble average with extremely high probability under generic equilibrium and nonequilibrium conditions special care is devoted to the uncontrollable microscopic details ... | [['for', 'a', 'macroscopic', 'isolated', 'quantum', 'system', 'in', 'an', 'unknown', 'pure', 'state', 'the', 'expectation', 'value', 'of', 'any', 'given', 'observable', 'is', 'shown', 'to', 'hardly', 'deviate', 'from', 'the', 'ensemble', 'average', 'with', 'extremely', 'high', 'probability', 'under', 'generic', 'equili... | [-0.09871519927942563, 0.16004501458214795, -0.09809854144750293, 0.09975678230998604, 0.0019131003537886711, -0.17788675486659739, 0.029931483321909813, 0.3144525993225533, -0.22939533418380156, -0.27204230706055843, 0.06458019510420515, -0.26673503103395274, -0.052648818507509, 0.17498256325678424, -0.039029417830237... |
710.4215 | On Majorana fermions on the lattice | The construction of massless Majorana fermions with chiral Yukawa couplings
on the lattice is considered. We find topological obstructions tightly linked
to those underlying the Nielsen-Ninomiya no-go theorem. In contradistinction to
chiral fermions the obstructions originate only from the combination of the
Dirac ac... | hep-lat | the construction of massless majorana fermions with chiral yukawa couplings on the lattice is considered we find topological obstructions tightly linked to those underlying the nielsenninomiya nogo theorem in contradistinction to chiral fermions the obstructions originate only from the combination of the dirac action a... | [['the', 'construction', 'of', 'massless', 'majorana', 'fermions', 'with', 'chiral', 'yukawa', 'couplings', 'on', 'the', 'lattice', 'is', 'considered', 'we', 'find', 'topological', 'obstructions', 'tightly', 'linked', 'to', 'those', 'underlying', 'the', 'nielsenninomiya', 'nogo', 'theorem', 'in', 'contradistinction', '... | [-0.1822340133464119, 0.24457052349297997, -0.057107245752540156, 0.09199506976456644, -0.11207967855107899, -0.15044065356517258, 0.03426597123362649, 0.31945593065271777, -0.22161018232313487, -0.25458543284390217, 0.03212384425121574, -0.3060709854396872, -0.2167102126046442, 0.0799834290996958, -0.01993573855799742... |
710.4216 | Anomalous GPDs in the photon | We consider deeply virtual Compton scattering (DVCS) on a photon target, in
the generalized Bjorken limit, at the Born order and in the leading logarithmic
approximation. This leads us to the extraction of the photon anomalous
generalized parton distributions (GPDs) \cite{url, DVCSphoton}.
| hep-ph | we consider deeply virtual compton scattering dvcs on a photon target in the generalized bjorken limit at the born order and in the leading logarithmic approximation this leads us to the extraction of the photon anomalous generalized parton distributions gpds citeurl dvcsphoton | [['we', 'consider', 'deeply', 'virtual', 'compton', 'scattering', 'dvcs', 'on', 'a', 'photon', 'target', 'in', 'the', 'generalized', 'bjorken', 'limit', 'at', 'the', 'born', 'order', 'and', 'in', 'the', 'leading', 'logarithmic', 'approximation', 'this', 'leads', 'us', 'to', 'the', 'extraction', 'of', 'the', 'photon', '... | [-0.038632362801581624, 0.20671201173681766, -0.18269345484441146, 0.20181632291933055, -0.0629808937665075, -0.010944428096991032, 0.10810712158636307, 0.30625348291359844, -0.2274719055276364, -0.14258484463207424, -0.09928286740905605, -0.32510356078855696, 0.0062508626841008665, 0.12717794361524284, 0.0345463764620... |
710.4217 | Optimal rate of convergence for nonparametric change-point estimators
for nonstationary sequences | Let $(X_i)_{i=1,...,n}$ be a possibly nonstationary sequence such that
$\mathscr{L}(X_i)=P_n$ if $i\leq n\theta$ and $\mathscr{L}(X_i)=Q_n$ if
$i>n\theta$, where $0<\theta <1$ is the location of the change-point to be
estimated. We construct a class of estimators based on the empirical measures
and a seminorm on the ... | math.ST stat.TH | let x_i_i1n be a possibly nonstationary sequence such that mathscrlx_ip_n if ileq ntheta and mathscrlx_iq_n if intheta where 0theta 1 is the location of the changepoint to be estimated we construct a class of estimators based on the empirical measures and a seminorm on the space of measures defined through a family of ... | [['let', 'x_i_i1n', 'be', 'a', 'possibly', 'nonstationary', 'sequence', 'such', 'that', 'mathscrlx_ip_n', 'if', 'ileq', 'ntheta', 'and', 'mathscrlx_iq_n', 'if', 'intheta', 'where', '0theta', '1', 'is', 'the', 'location', 'of', 'the', 'changepoint', 'to', 'be', 'estimated', 'we', 'construct', 'a', 'class', 'of', 'estima... | [-0.09451808111142304, 0.08179524780045878, -0.08016468890768996, 0.08373598947872456, -0.02939002914156891, -0.15473233654668903, 0.032341377423894674, 0.36963783390820026, -0.2616620038328219, -0.2274519325109688, 0.13835946043609973, -0.2473537844874091, -0.12798755714606683, 0.2388744008790512, -0.09586804186909507... |
710.4218 | Foldy-Wouthyusen Transformation and Semiclassical Limit for Relativistic
Particles in Strong External Fields | A general method of the Foldy-Wouthyusen (FW) transformation for relativistic
particles of arbitrary spin in strong external fields has been developed. The
use of the found transformation operator is not restricted by any definite
commutation relations between even and odd operators. The final FW Hamiltonian
can be e... | math-ph hep-th math.MP | a general method of the foldywouthyusen fw transformation for relativistic particles of arbitrary spin in strong external fields has been developed the use of the found transformation operator is not restricted by any definite commutation relations between even and odd operators the final fw hamiltonian can be expanded... | [['a', 'general', 'method', 'of', 'the', 'foldywouthyusen', 'fw', 'transformation', 'for', 'relativistic', 'particles', 'of', 'arbitrary', 'spin', 'in', 'strong', 'external', 'fields', 'has', 'been', 'developed', 'the', 'use', 'of', 'the', 'found', 'transformation', 'operator', 'is', 'not', 'restricted', 'by', 'any', '... | [-0.1329196886558618, 0.1800647405052067, -0.10406689014094549, 0.08988301713169286, -0.0696047551281351, -0.14321882722017887, -0.030925029775659953, 0.31430334323751075, -0.22170128584174173, -0.3042518000035281, 0.02524324520740525, -0.2580582453221723, -0.1083454481159736, 0.18795893608060266, 0.03423408222318228, ... |
710.4219 | Arithmetic of rationaly connected quintic 3-folds over finite and
function fields | We prove that both classical Chevalley-Warning-Ax and Tsen theorems hold for
the blowing up of a quintic 3-fold along a line of multiplicity 3. Both proofs,
which are of the same spirit than the original ones, involve the description of
this blowing-up as a subvariety of a toric variety.
| math.NT math.AG | we prove that both classical chevalleywarningax and tsen theorems hold for the blowing up of a quintic 3fold along a line of multiplicity 3 both proofs which are of the same spirit than the original ones involve the description of this blowingup as a subvariety of a toric variety | [['we', 'prove', 'that', 'both', 'classical', 'chevalleywarningax', 'and', 'tsen', 'theorems', 'hold', 'for', 'the', 'blowing', 'up', 'of', 'a', 'quintic', '3fold', 'along', 'a', 'line', 'of', 'multiplicity', '3', 'both', 'proofs', 'which', 'are', 'of', 'the', 'same', 'spirit', 'than', 'the', 'original', 'ones', 'invol... | [-0.16681033873588758, -0.013296848935808273, -0.10239071807170168, 0.09129264862326152, -0.049556415845104985, -0.1550373603451125, 0.0026642251363460053, 0.26097932866120593, -0.24450116823526455, -0.2232511864499526, 0.14338541811857214, -0.24067309742516024, -0.08785070185648634, 0.2619440337405243, -0.091165418320... |
710.422 | Ultracold atoms in optical lattices generated by quantized light fields | We study an ultracold gas of neutral atoms subject to the periodic optical
potential generated by a high-$Q$ cavity mode. In the limit of very low
temperatures, cavity field and atomic dynamics require a quantum description.
Starting from a cavity QED single atom Hamiltonian we use different routes to
derive approxim... | quant-ph | we study an ultracold gas of neutral atoms subject to the periodic optical potential generated by a highq cavity mode in the limit of very low temperatures cavity field and atomic dynamics require a quantum description starting from a cavity qed single atom hamiltonian we use different routes to derive approximative mu... | [['we', 'study', 'an', 'ultracold', 'gas', 'of', 'neutral', 'atoms', 'subject', 'to', 'the', 'periodic', 'optical', 'potential', 'generated', 'by', 'a', 'highq', 'cavity', 'mode', 'in', 'the', 'limit', 'of', 'very', 'low', 'temperatures', 'cavity', 'field', 'and', 'atomic', 'dynamics', 'require', 'a', 'quantum', 'descr... | [-0.14303855223503584, 0.2436311607370788, -0.07493169889135198, 0.04385889923256455, 0.007475188505751166, -0.18445129481525244, 0.05323097390602484, 0.35992761284790253, -0.24541632315623715, -0.26281302841803567, 0.0367033272695897, -0.2672133979190028, -0.07768453581145766, 0.18563478972170164, 0.044603046774864194... |
710.4221 | The dynamical rigid body with memory | In the present paper we describe the dynamics of the revised rigid body, the
dynamics of the rigid body with distributed delays and the dynamics of the
fractional rigid body. We analyze the stationary states for given values of the
rigid body's parameters.
| math.DS | in the present paper we describe the dynamics of the revised rigid body the dynamics of the rigid body with distributed delays and the dynamics of the fractional rigid body we analyze the stationary states for given values of the rigid bodys parameters | [['in', 'the', 'present', 'paper', 'we', 'describe', 'the', 'dynamics', 'of', 'the', 'revised', 'rigid', 'body', 'the', 'dynamics', 'of', 'the', 'rigid', 'body', 'with', 'distributed', 'delays', 'and', 'the', 'dynamics', 'of', 'the', 'fractional', 'rigid', 'body', 'we', 'analyze', 'the', 'stationary', 'states', 'for', ... | [-0.1804204738677241, 0.12821897821024406, -0.06876114688727052, -0.044476271585323086, 0.004359947041023609, -0.04697276231681192, -0.010588497489279265, 0.31593340721934343, -0.3100754348344581, -0.2523854681572249, 0.07941532644800582, -0.2368266364386262, -0.1578824098200299, 0.10681133816928365, -0.144866560412527... |
710.4222 | Action of Hecke operators on Siegel theta series II | Given a Siegel theta series and a prime p not dividing the level of the theta
series, we apply to the theta series the n+1 Hecke operators that generate the
local Hecke algebra at p. We show that the average theta series is an eigenform
and we compute the eigenvalues.
| math.NT | given a siegel theta series and a prime p not dividing the level of the theta series we apply to the theta series the n1 hecke operators that generate the local hecke algebra at p we show that the average theta series is an eigenform and we compute the eigenvalues | [['given', 'a', 'siegel', 'theta', 'series', 'and', 'a', 'prime', 'p', 'not', 'dividing', 'the', 'level', 'of', 'the', 'theta', 'series', 'we', 'apply', 'to', 'the', 'theta', 'series', 'the', 'n1', 'hecke', 'operators', 'that', 'generate', 'the', 'local', 'hecke', 'algebra', 'at', 'p', 'we', 'show', 'that', 'the', 'ave... | [-0.23194523513317108, 0.05109469336719485, -0.1561914184782654, 0.05254366026492789, -0.08527055267710239, -0.10071658870205283, 0.008970775101333857, 0.28725096937268974, -0.3592453937977552, -0.21291984372772277, 0.04078858328051865, -0.30021412381902335, -0.1827182611078024, 0.183653086386621, -0.04866187460720539,... |
710.4223 | Time Scaling of Chaotic Systems: Application to Secure Communications | The paper deals with time-scaling transformations of dynamical systems. Such
scaling functions operate a change of coordinates on the time axis of the
system trajectories preserving its phase portrait. Exploiting this property, a
chaos encryption technique to transmit a binary signal through an analog
channel is prop... | nlin.CD | the paper deals with timescaling transformations of dynamical systems such scaling functions operate a change of coordinates on the time axis of the system trajectories preserving its phase portrait exploiting this property a chaos encryption technique to transmit a binary signal through an analog channel is proposed t... | [['the', 'paper', 'deals', 'with', 'timescaling', 'transformations', 'of', 'dynamical', 'systems', 'such', 'scaling', 'functions', 'operate', 'a', 'change', 'of', 'coordinates', 'on', 'the', 'time', 'axis', 'of', 'the', 'system', 'trajectories', 'preserving', 'its', 'phase', 'portrait', 'exploiting', 'this', 'property'... | [-0.2862331987945018, 0.02857967323992246, -0.14099378523382325, 0.028209126896489366, -0.053363058526344875, -0.21755682737825233, 0.0816498481751891, 0.31355062183740057, -0.31432990748205303, -0.2295000829998358, 0.13705811835250553, -0.23666862568553584, -0.1956133146735805, 0.2053019991259516, -0.10540015001516835... |
710.4224 | Hecke operators on Hilbert-Siegel modular forms | We define Hilbert-Siegel modular forms and Hecke "operators" acting on them.
As with Hilbert modular forms, these linear transformations are not linear
operators until we consider a direct product of spaces of modular forms (with
varying groups), modulo natural identifications we can make between certain
spaces. With... | math.NT | we define hilbertsiegel modular forms and hecke operators acting on them as with hilbert modular forms these linear transformations are not linear operators until we consider a direct product of spaces of modular forms with varying groups modulo natural identifications we can make between certain spaces with hilbertsie... | [['we', 'define', 'hilbertsiegel', 'modular', 'forms', 'and', 'hecke', 'operators', 'acting', 'on', 'them', 'as', 'with', 'hilbert', 'modular', 'forms', 'these', 'linear', 'transformations', 'are', 'not', 'linear', 'operators', 'until', 'we', 'consider', 'a', 'direct', 'product', 'of', 'spaces', 'of', 'modular', 'forms... | [-0.20818520925628642, 0.1049918971140869, -0.09770080815457428, 0.03611089419282507, -0.12586853279305313, -0.08277015681766595, -0.007683593003700177, 0.3517664437337468, -0.3304724831134081, -0.21210326388342463, 0.11249571710650344, -0.24745870111510157, -0.19816796689798746, 0.2530932262695084, -0.0586738841996217... |
710.4225 | Exploring the chiral regime with dynamical overlap fermions | I report the status of the dynamical overlap fermion project by the JLQCD and
TWQCD collaborations. So far, the simulations have been completed with two
flavors of overlap sea quarks in a wide range of sea quark mass corresponding
the $p$-regime and the $\epsilon$-regime on a $16^3\times 32$ lattice at
$a=$0.12 fm. M... | hep-lat | i report the status of the dynamical overlap fermion project by the jlqcd and twqcd collaborations so far the simulations have been completed with two flavors of overlap sea quarks in a wide range of sea quark mass corresponding the pregime and the epsilonregime on a 163times 32 lattice at a012 fm more recently runs wi... | [['i', 'report', 'the', 'status', 'of', 'the', 'dynamical', 'overlap', 'fermion', 'project', 'by', 'the', 'jlqcd', 'and', 'twqcd', 'collaborations', 'so', 'far', 'the', 'simulations', 'have', 'been', 'completed', 'with', 'two', 'flavors', 'of', 'overlap', 'sea', 'quarks', 'in', 'a', 'wide', 'range', 'of', 'sea', 'quark... | [-0.06742004856393423, 0.3150348511351295, -0.08923479609571897, 0.056790279247230145, 0.014398130968712815, -0.056670231286084234, 0.10152751904139977, 0.3535730926456248, -0.06978857835255019, -0.3088406019122908, 0.11048374464451449, -0.33214162586529444, -0.05286788306179138, 0.06932918073200597, 0.0568960747431691... |
710.4226 | NGC3147: a "true" Seyfert 2 without the broad-line region | We report on simultaneous optical and X-ray observations of the Seyfert
galaxy, NGC3147. The XMM-Newton spectrum shows that the source is unabsorbed in
the X-rays ($N_H<5\times10^{20}$ cm$^{-2}$). On the other hand, no broad lines
are present in the optical spectrum. The origin of this optical/X-rays
misclassificatio... | astro-ph | we report on simultaneous optical and xray observations of the seyfert galaxy ngc3147 the xmmnewton spectrum shows that the source is unabsorbed in the xrays n_h5times1020 cm2 on the other hand no broad lines are present in the optical spectrum the origin of this opticalxrays misclassification with respect to the unifi... | [['we', 'report', 'on', 'simultaneous', 'optical', 'and', 'xray', 'observations', 'of', 'the', 'seyfert', 'galaxy', 'ngc3147', 'the', 'xmmnewton', 'spectrum', 'shows', 'that', 'the', 'source', 'is', 'unabsorbed', 'in', 'the', 'xrays', 'n_h5times1020', 'cm2', 'on', 'the', 'other', 'hand', 'no', 'broad', 'lines', 'are', ... | [-0.06021690480713922, 0.04172582255498453, -0.016307506399850052, 0.11277117144138499, -0.09156873387027138, -0.1392255745093694, 0.05885535731676936, 0.505909281835808, -0.15464811712291424, -0.32676538316451575, 0.08890960426202302, -0.308196836113324, -0.0019004626532759124, 0.17972059169504034, -0.0365557563701754... |
710.4227 | New developments in PHOKHARA Monte Carlo generator | The present status of the physics program, which led to the development of
the Monte Carlo event generator PHOKHARA is described. The possibility of using
the radiative return method in various aspects of hadronic physics, from the
measurement of the hadronic cross section, to detailed investigations of the
hadronic ... | hep-ph hep-ex | the present status of the physics program which led to the development of the monte carlo event generator phokhara is described the possibility of using the radiative return method in various aspects of hadronic physics from the measurement of the hadronic cross section to detailed investigations of the hadronic dynami... | [['the', 'present', 'status', 'of', 'the', 'physics', 'program', 'which', 'led', 'to', 'the', 'development', 'of', 'the', 'monte', 'carlo', 'event', 'generator', 'phokhara', 'is', 'described', 'the', 'possibility', 'of', 'using', 'the', 'radiative', 'return', 'method', 'in', 'various', 'aspects', 'of', 'hadronic', 'phy... | [-0.02466799730124573, 0.15556150695309043, -0.11931751956542333, 0.08982718542528649, -0.056615412275617324, -0.025870548461874327, 0.014539296790802231, 0.30551136543353397, -0.2328602713594834, -0.3178141539047162, 0.038645216063596305, -0.29056748325626053, -0.04360172999401887, 0.20098842440793913, 0.0809762590378... |
710.4228 | Retrospective Markov chain Monte Carlo methods for Dirichlet process
hierarchical model | Inference for Dirichlet process hierarchical models is typically performed
using Markov chain Monte Carlo methods, which can be roughly categorised into
marginal and conditional methods. The former integrate out analytically the
infinite-dimensional component of the hierarchical model and sample from the
marginal dis... | stat.ME stat.CO | inference for dirichlet process hierarchical models is typically performed using markov chain monte carlo methods which can be roughly categorised into marginal and conditional methods the former integrate out analytically the infinitedimensional component of the hierarchical model and sample from the marginal distribu... | [['inference', 'for', 'dirichlet', 'process', 'hierarchical', 'models', 'is', 'typically', 'performed', 'using', 'markov', 'chain', 'monte', 'carlo', 'methods', 'which', 'can', 'be', 'roughly', 'categorised', 'into', 'marginal', 'and', 'conditional', 'methods', 'the', 'former', 'integrate', 'out', 'analytically', 'the'... | [0.004612560327871737, 0.05882472897319092, -0.14555831536011074, 0.12169702826454395, -0.05779215474949634, -0.11547810070115669, 0.08915865510009252, 0.43912088805921823, -0.30153193093656777, -0.3105353367827336, 0.12683033053160095, -0.22376543115361605, -0.09909542136775128, 0.1785009982238288, -0.0406623603102852... |
710.4229 | Robust non-adiabatic molecular dynamics for metals and insulators | We present a new formulation of the correlated electron-ion dynamics (CEID)
scheme, which systematically improves Ehrenfest dynamics by including quantum
fluctuations around the mean-field atomic trajectories. We show that the method
can simulate models of non-adiabatic electronic transitions, and test it
against exa... | cond-mat.mtrl-sci | we present a new formulation of the correlated electronion dynamics ceid scheme which systematically improves ehrenfest dynamics by including quantum fluctuations around the meanfield atomic trajectories we show that the method can simulate models of nonadiabatic electronic transitions and test it against exact integra... | [['we', 'present', 'a', 'new', 'formulation', 'of', 'the', 'correlated', 'electronion', 'dynamics', 'ceid', 'scheme', 'which', 'systematically', 'improves', 'ehrenfest', 'dynamics', 'by', 'including', 'quantum', 'fluctuations', 'around', 'the', 'meanfield', 'atomic', 'trajectories', 'we', 'show', 'that', 'the', 'method... | [-0.16161493612435152, 0.11936145160143496, -0.10844951832041261, 0.08150299010867457, 0.0061757706353091635, -0.14364659153216053, 0.0660993872807012, 0.3232928559064021, -0.24937337451046915, -0.2896554103208473, 0.00023448372667189687, -0.23702109322039178, -0.13265719272567367, 0.1975792490056847, 0.023320352323935... |
710.423 | Trees, linear orders and G\^ateaux smooth norms | We introduce a linearly ordered set Z and use it to prove a necessity
condition for the existence of a G\^ateaux smooth norm on C(T), where T is a
tree. This criterion is directly analogous to the corresponding equivalent
condition for Fr\'echet smooth norms. In addition, we prove that if C(T) admits
a G\^ateaux smoo... | math.FA | we introduce a linearly ordered set z and use it to prove a necessity condition for the existence of a gateaux smooth norm on ct where t is a tree this criterion is directly analogous to the corresponding equivalent condition for frechet smooth norms in addition we prove that if ct admits a gateaux smooth lattice norm ... | [['we', 'introduce', 'a', 'linearly', 'ordered', 'set', 'z', 'and', 'use', 'it', 'to', 'prove', 'a', 'necessity', 'condition', 'for', 'the', 'existence', 'of', 'a', 'gateaux', 'smooth', 'norm', 'on', 'ct', 'where', 't', 'is', 'a', 'tree', 'this', 'criterion', 'is', 'directly', 'analogous', 'to', 'the', 'corresponding',... | [-0.08521446032260639, 0.10841674348035746, -0.11627984589701383, 0.11539517701569729, -0.10264648303416544, -0.1541293970565649, 0.02405099738119305, 0.4257471638367228, -0.3596331936077795, -0.09091034477603609, 0.14563647010937278, -0.2449487199925858, -0.15640437465323054, 0.11847659808489075, -0.12450342414819676,... |
710.4231 | Analyzing covert social network foundation behind terrorism disaster | This paper addresses a method to analyze the covert social network foundation
hidden behind the terrorism disaster. It is to solve a node discovery problem,
which means to discover a node, which functions relevantly in a social network,
but escaped from monitoring on the presence and mutual relationship of nodes.
The... | cs.AI | this paper addresses a method to analyze the covert social network foundation hidden behind the terrorism disaster it is to solve a node discovery problem which means to discover a node which functions relevantly in a social network but escaped from monitoring on the presence and mutual relationship of nodes the method... | [['this', 'paper', 'addresses', 'a', 'method', 'to', 'analyze', 'the', 'covert', 'social', 'network', 'foundation', 'hidden', 'behind', 'the', 'terrorism', 'disaster', 'it', 'is', 'to', 'solve', 'a', 'node', 'discovery', 'problem', 'which', 'means', 'to', 'discover', 'a', 'node', 'which', 'functions', 'relevantly', 'in... | [-0.1077369547370472, -0.035490290375892075, -0.09072298655752092, 0.08443434177548624, -0.15809397858567537, -0.16255937457084657, 0.13832181203644722, 0.3484097526222467, -0.2921930944453925, -0.353056425191462, 0.08034667326835915, -0.29468037489335985, -0.26206316163763405, 0.14202240345068276, -0.08253442847169935... |
710.4232 | Path Integral Representations on the Complex Sphere | In this paper we discuss the path integral representations for the coordinate
systems on the complex sphere S3C. The Schroedinger equation, respectively the
path integral, separates in exactly 21 orthogonal coordinate systems. We
enumerate these coordinate systems and we are able to present the path integral
represen... | quant-ph | in this paper we discuss the path integral representations for the coordinate systems on the complex sphere s3c the schroedinger equation respectively the path integral separates in exactly 21 orthogonal coordinate systems we enumerate these coordinate systems and we are able to present the path integral representation... | [['in', 'this', 'paper', 'we', 'discuss', 'the', 'path', 'integral', 'representations', 'for', 'the', 'coordinate', 'systems', 'on', 'the', 'complex', 'sphere', 's3c', 'the', 'schroedinger', 'equation', 'respectively', 'the', 'path', 'integral', 'separates', 'in', 'exactly', '21', 'orthogonal', 'coordinate', 'systems',... | [-0.1661653556134347, 0.04321535252377514, -0.08457640867557499, 0.05617514359099524, -0.05601729752731274, -0.03917171497020747, -0.019168776914139617, 0.38983168586024214, -0.2810612729709636, -0.2043866936199285, 0.10806046968459018, -0.2828455323885594, -0.17875183798925398, 0.17864888128671016, -0.0513830332924704... |
710.4233 | Hamiltonian stationary Lagrangian tori contained in a hypersphere | The Clifford torus is a torus in a three-dimensional sphere. Homogeneous tori
are simple generalization of the Clifford torus which still in a
three-dimensional sphere. There is a way to construct tori in a
three-dimensional sphere using the Hopf fibration. In this paper, all
Hamiltonian stationary Lagrangian tori wh... | math.DG | the clifford torus is a torus in a threedimensional sphere homogeneous tori are simple generalization of the clifford torus which still in a threedimensional sphere there is a way to construct tori in a threedimensional sphere using the hopf fibration in this paper all hamiltonian stationary lagrangian tori which is co... | [['the', 'clifford', 'torus', 'is', 'a', 'torus', 'in', 'a', 'threedimensional', 'sphere', 'homogeneous', 'tori', 'are', 'simple', 'generalization', 'of', 'the', 'clifford', 'torus', 'which', 'still', 'in', 'a', 'threedimensional', 'sphere', 'there', 'is', 'a', 'way', 'to', 'construct', 'tori', 'in', 'a', 'threedimensi... | [-0.2075973050268658, 0.08783897278666093, -0.07538415958212379, 0.10190670573016784, -0.07060576179355849, -0.12982290209523248, -0.07396505283031729, 0.39042966389873374, -0.24443564302055165, -0.17679828926702612, 0.13385524322560136, -0.23881339810031932, -0.20679359912173823, 0.22445346133220787, -0.13615918364181... |
710.4234 | Stability of the Gibbs Sampler for Bayesian Hierarchical Models | We characterise the convergence of the Gibbs sampler which samples from the
joint posterior distribution of parameters and missing data in hierarchical
linear models with arbitrary symmetric error distributions. We show that the
convergence can be uniform, geometric or sub-geometric depending on the
relative tail beh... | stat.ME stat.CO | we characterise the convergence of the gibbs sampler which samples from the joint posterior distribution of parameters and missing data in hierarchical linear models with arbitrary symmetric error distributions we show that the convergence can be uniform geometric or subgeometric depending on the relative tail behaviou... | [['we', 'characterise', 'the', 'convergence', 'of', 'the', 'gibbs', 'sampler', 'which', 'samples', 'from', 'the', 'joint', 'posterior', 'distribution', 'of', 'parameters', 'and', 'missing', 'data', 'in', 'hierarchical', 'linear', 'models', 'with', 'arbitrary', 'symmetric', 'error', 'distributions', 'we', 'show', 'that'... | [-0.01676624933845067, 0.09227738247930327, -0.1944361864800819, 0.14648387753560532, -0.04677442875055766, -0.10046900460623544, 0.04885535024566872, 0.4312423709568314, -0.29805603015913884, -0.2869093653941739, 0.08877398669243451, -0.21322790093042635, -0.10418941957124678, 0.1673119490389416, -0.09436325264290314,... |
710.4235 | Top-Down Causation by Information Control: From a Philosophical Problem
to a Scientific Research Program | It has been claimed that different types of causes must be considered in
biological systems, including top-down as well as same-level and bottom-up
causation, thus enabling the top levels to be causally efficacious in their own
right. To clarify this issue, important distinctions between information and
signs are int... | q-bio.OT | it has been claimed that different types of causes must be considered in biological systems including topdown as well as samelevel and bottomup causation thus enabling the top levels to be causally efficacious in their own right to clarify this issue important distinctions between information and signs are introduced h... | [['it', 'has', 'been', 'claimed', 'that', 'different', 'types', 'of', 'causes', 'must', 'be', 'considered', 'in', 'biological', 'systems', 'including', 'topdown', 'as', 'well', 'as', 'samelevel', 'and', 'bottomup', 'causation', 'thus', 'enabling', 'the', 'top', 'levels', 'to', 'be', 'causally', 'efficacious', 'in', 'th... | [-0.08398404451006132, 0.13764965819275898, -0.05440941210836172, 0.12123394834647036, -0.062889530947027, -0.16689039092591923, 0.05682063877744519, 0.386260722545178, -0.30395399144162305, -0.32731528985314073, 0.11075727087141865, -0.2536935511652542, -0.15936234870966037, 0.17405831152168305, -0.09150720536506371, ... |
710.4236 | NNNLO correction to the toponium and bottomonium wave-functions at the
origin | We report new results of the NNNLO correction to the S-wave quarkonium
wave-functions at the origin, which also provide an estimate of the resonance
cross section in t-tbar threshold production at the ILC.
| hep-ph | we report new results of the nnnlo correction to the swave quarkonium wavefunctions at the origin which also provide an estimate of the resonance cross section in ttbar threshold production at the ilc | [['we', 'report', 'new', 'results', 'of', 'the', 'nnnlo', 'correction', 'to', 'the', 'swave', 'quarkonium', 'wavefunctions', 'at', 'the', 'origin', 'which', 'also', 'provide', 'an', 'estimate', 'of', 'the', 'resonance', 'cross', 'section', 'in', 'ttbar', 'threshold', 'production', 'at', 'the', 'ilc']] | [-0.06241470554871767, 0.12148923240998886, -0.11960497981106694, 0.14090813854427048, -0.016384631113121002, -0.10380352502970984, 0.03624310284486097, 0.299521670084108, -0.20207609924854655, -0.2172891836274754, -0.05401491131421856, -0.3745583229218469, 0.01836883336496116, 0.15860798675566912, 0.1203012117608027, ... |
710.4237 | Free energy of static quarks and the renormalized Polyakov loop in full
QCD | We present results from a detailed study of singlet free energies in full QCD
with realistic quark masses. An improved scheme for the non-perturbative
renormalization of the Polyakov loop is used and we compare its temperature
dependence for QCD with different flavor content. We also analyze screening
masses extracte... | hep-lat | we present results from a detailed study of singlet free energies in full qcd with realistic quark masses an improved scheme for the nonperturbative renormalization of the polyakov loop is used and we compare its temperature dependence for qcd with different flavor content we also analyze screening masses extracted fro... | [['we', 'present', 'results', 'from', 'a', 'detailed', 'study', 'of', 'singlet', 'free', 'energies', 'in', 'full', 'qcd', 'with', 'realistic', 'quark', 'masses', 'an', 'improved', 'scheme', 'for', 'the', 'nonperturbative', 'renormalization', 'of', 'the', 'polyakov', 'loop', 'is', 'used', 'and', 'we', 'compare', 'its', ... | [-0.059958696992208176, 0.2522062798270781, -0.10526498939053944, 0.11354814380487929, -0.03171573610206206, -0.10922392297876425, 0.07337082541982035, 0.3912202415880389, -0.17551647853822663, -0.31386215508414, 0.012110902702820918, -0.2902061535188785, -0.007016197773807038, 0.15303882403084293, 0.08087849535233825,... |
710.4238 | Multi-line (sub)millimetre observations of the high-mass proto cluster
IRAS 05358+3543 | Since most high- and intermediate-mass protostars are at great distance and
form in clusters, high linear resolution observations are needed to investigate
their physical properties. To study the gas in the innermost region around the
protostars in the proto-cluster IRAS 05358+3543, we observed the source in
several ... | astro-ph | since most high and intermediatemass protostars are at great distance and form in clusters high linear resolution observations are needed to investigate their physical properties to study the gas in the innermost region around the protostars in the protocluster iras 053583543 we observed the source in several transitio... | [['since', 'most', 'high', 'and', 'intermediatemass', 'protostars', 'are', 'at', 'great', 'distance', 'and', 'form', 'in', 'clusters', 'high', 'linear', 'resolution', 'observations', 'are', 'needed', 'to', 'investigate', 'their', 'physical', 'properties', 'to', 'study', 'the', 'gas', 'in', 'the', 'innermost', 'region',... | [-0.10496660847046552, 0.11705818290160516, -0.041457328677931726, 0.03225170636178218, -0.04906361674108689, -0.06480861473289773, 0.002403510020553204, 0.43668332682106614, -0.16156618476870338, -0.3185192789701545, 0.0896094217761766, -0.273001340887517, -0.0038267407106420347, 0.12374380813076445, 0.037609026165874... |
710.4239 | Unparticle Physics in Single Top Signals | We study the single production of top quarks in $e^+e^-, ep$ and $pp$
collisions in the context of unparticle physics through the Flavor Violating
(FV) unparticle vertices and compute the total cross sections for single top
production as functions of scale dimension $d_{\U}$. We find that among all,
LHC is the most p... | hep-ph | we study the single production of top quarks in ee ep and pp collisions in the context of unparticle physics through the flavor violating fv unparticle vertices and compute the total cross sections for single top production as functions of scale dimension d_u we find that among all lhc is the most promising facility to... | [['we', 'study', 'the', 'single', 'production', 'of', 'top', 'quarks', 'in', 'ee', 'ep', 'and', 'pp', 'collisions', 'in', 'the', 'context', 'of', 'unparticle', 'physics', 'through', 'the', 'flavor', 'violating', 'fv', 'unparticle', 'vertices', 'and', 'compute', 'the', 'total', 'cross', 'sections', 'for', 'single', 'top... | [-0.03814407197328714, 0.24450527710410264, -0.057538264316435044, 0.16361921165729515, -0.05495811164952241, -0.14514031671345806, 0.0371366372009596, 0.24341486404076793, -0.24503493282693223, -0.25569755953664963, -0.08850583070530914, -0.38640233622147485, 0.00483621689849175, 0.1259048304305627, 0.1729014476904502... |
710.424 | Universality and massive excitations in 3d 3-state Potts model | The mass spectrum of the 3d 3-state Potts model is considered in the broken
phase (a) near the second order Ising critical point in the
temperature-magnetic field plane and (b) near the weakly first order transition
point at zero magnetic field. In the case (a), the mass spectrum is compared
with the prediction from ... | hep-lat | the mass spectrum of the 3d 3state potts model is considered in the broken phase a near the second order ising critical point in the temperaturemagnetic field plane and b near the weakly first order transition point at zero magnetic field in the case a the mass spectrum is compared with the prediction from universality... | [['the', 'mass', 'spectrum', 'of', 'the', '3d', '3state', 'potts', 'model', 'is', 'considered', 'in', 'the', 'broken', 'phase', 'a', 'near', 'the', 'second', 'order', 'ising', 'critical', 'point', 'in', 'the', 'temperaturemagnetic', 'field', 'plane', 'and', 'b', 'near', 'the', 'weakly', 'first', 'order', 'transition', ... | [-0.12177521064786204, 0.20364774277264835, -0.02195786135887508, 0.03600873547839001, 0.029912111463536527, -0.10623443087873359, 0.02816008206105371, 0.317862425081651, -0.19425088693113887, -0.2750336924093027, 0.07440614452307094, -0.30622916226731794, -0.04981633107287481, 0.09662396507109423, 0.06503531843533411,... |
710.4241 | BCS-BEC crossover of neutron pairs in symmetric and asymmetric nuclear
matter | We propose new types of density dependent contact pairing interaction which
reproduce the pairing gaps in symmetric and neutron matter obtained by a
microscopic treatment based on the nucleon-nucleon interaction. These
interactions are able to simulate the pairing gaps of either the bare
interaction or the interactio... | nucl-th | we propose new types of density dependent contact pairing interaction which reproduce the pairing gaps in symmetric and neutron matter obtained by a microscopic treatment based on the nucleonnucleon interaction these interactions are able to simulate the pairing gaps of either the bare interaction or the interaction sc... | [['we', 'propose', 'new', 'types', 'of', 'density', 'dependent', 'contact', 'pairing', 'interaction', 'which', 'reproduce', 'the', 'pairing', 'gaps', 'in', 'symmetric', 'and', 'neutron', 'matter', 'obtained', 'by', 'a', 'microscopic', 'treatment', 'based', 'on', 'the', 'nucleonnucleon', 'interaction', 'these', 'interac... | [-0.1485033331204622, 0.23173758038175032, -0.12500460234127928, 0.12362534522732592, -0.04292793468982907, -0.15380985957356344, -0.004083559475260677, 0.3319352790481926, -0.2268679148592749, -0.28591953796444475, -0.06900543892200782, -0.3062008364322763, -0.07667105136171123, 0.06540364759789075, 0.1142506435027589... |
710.4242 | Adaptive Importance Sampling in General Mixture Classes | In this paper, we propose an adaptive algorithm that iteratively updates both
the weights and component parameters of a mixture importance sampling density
so as to optimise the importance sampling performances, as measured by an
entropy criterion. The method is shown to be applicable to a wide class of
importance sa... | stat.CO | in this paper we propose an adaptive algorithm that iteratively updates both the weights and component parameters of a mixture importance sampling density so as to optimise the importance sampling performances as measured by an entropy criterion the method is shown to be applicable to a wide class of importance samplin... | [['in', 'this', 'paper', 'we', 'propose', 'an', 'adaptive', 'algorithm', 'that', 'iteratively', 'updates', 'both', 'the', 'weights', 'and', 'component', 'parameters', 'of', 'a', 'mixture', 'importance', 'sampling', 'density', 'so', 'as', 'to', 'optimise', 'the', 'importance', 'sampling', 'performances', 'as', 'measured... | [-0.03745327750588522, 0.09041034165604384, -0.1012571775856869, 0.04659075213498191, -0.0486579547391126, -0.1309930993391103, 0.051652320750106714, 0.4260158550582434, -0.28348700967862417, -0.31254538995654957, 0.09225055030792167, -0.18082434350722715, -0.17624737647803207, 0.20501696381129716, -0.10559950329755483... |
710.4243 | Heun and Mathieu functions as solutions of the Dirac equation | We give examples of where the Heun function exists as solutions of wave
equations encountered in general relativity. While the Dirac equation written
in the background of Nutku helicoid metric yields Mathieu functions as its
solutions in four spacetime dimensions, the trivial generalization to five
dimensions results... | gr-qc | we give examples of where the heun function exists as solutions of wave equations encountered in general relativity while the dirac equation written in the background of nutku helicoid metric yields mathieu functions as its solutions in four spacetime dimensions the trivial generalization to five dimensions results in ... | [['we', 'give', 'examples', 'of', 'where', 'the', 'heun', 'function', 'exists', 'as', 'solutions', 'of', 'wave', 'equations', 'encountered', 'in', 'general', 'relativity', 'while', 'the', 'dirac', 'equation', 'written', 'in', 'the', 'background', 'of', 'nutku', 'helicoid', 'metric', 'yields', 'mathieu', 'functions', 'a... | [-0.16444809310676822, 0.011557483608015331, -0.09238126086834145, 0.08425428825767195, -0.10050894686088235, -0.14502706238438925, -0.04498945270855743, 0.28845670881557717, -0.237625373145902, -0.24411040805392417, 0.08542383000456605, -0.3216800972067538, -0.20995101202503744, 0.1775839548917061, -0.0764236425621861... |
710.4244 | Near-Field Radio Holography of Large Reflector Antennas | We summarise the mathematical foundation of the holographic method of
measuring the reflector profile of an antenna or radio telescope. In
particular, we treat the case, where the signal source is located at a finite
distance from the antenna under test, necessitating the inclusion of the
so-called Fresnel field term... | astro-ph | we summarise the mathematical foundation of the holographic method of measuring the reflector profile of an antenna or radio telescope in particular we treat the case where the signal source is located at a finite distance from the antenna under test necessitating the inclusion of the socalled fresnel field terms in th... | [['we', 'summarise', 'the', 'mathematical', 'foundation', 'of', 'the', 'holographic', 'method', 'of', 'measuring', 'the', 'reflector', 'profile', 'of', 'an', 'antenna', 'or', 'radio', 'telescope', 'in', 'particular', 'we', 'treat', 'the', 'case', 'where', 'the', 'signal', 'source', 'is', 'located', 'at', 'a', 'finite',... | [-0.16090063887285228, 0.05190380744084073, -0.06768457501755744, 0.009533329240354252, -0.07062494531037065, -0.12914038549761397, 0.016481030010223642, 0.37649521200870306, -0.17916829110975613, -0.2797099543514393, 0.1066220465986358, -0.27621988709068906, -0.12672833567366826, 0.20335644585972304, -0.03193279573599... |
710.4245 | Particle Filters for Partially Observed Diffusions | In this paper we introduce a novel particle filter scheme for a class of
partially-observed multivariate diffusions. %continuous-time dynamic models
where the %signal is given by a multivariate diffusion process. We consider a
variety of observation schemes, including diffusion observed with error,
observation of a s... | stat.ME stat.CO | in this paper we introduce a novel particle filter scheme for a class of partiallyobserved multivariate diffusions continuoustime dynamic models where the signal is given by a multivariate diffusion process we consider a variety of observation schemes including diffusion observed with error observation of a subset of t... | [['in', 'this', 'paper', 'we', 'introduce', 'a', 'novel', 'particle', 'filter', 'scheme', 'for', 'a', 'class', 'of', 'partiallyobserved', 'multivariate', 'diffusions', 'continuoustime', 'dynamic', 'models', 'where', 'the', 'signal', 'is', 'given', 'by', 'a', 'multivariate', 'diffusion', 'process', 'we', 'consider', 'a'... | [-0.06309668926422941, 0.05536423136408512, -0.09726233520275036, 0.042046898979627864, -0.040538936013014185, -0.1237007813836784, 0.056071152880280854, 0.40230977658689376, -0.28123736205185657, -0.2648258058673884, 0.12125045525326157, -0.22598827547619682, -0.16549798482533037, 0.1759159358097075, -0.07075638121776... |
710.4246 | Critical properties of the four-state Commutative Random Permutation
Glassy Potts model in three and four dimensions | We investigate the critical properties of the four-state commutative random
permutation glassy Potts model in three and four dimensions by means of Monte
Carlo simulation and of a finite size scaling analysis. Thanks to the use of a
field programmable gate array we have been able to thermalize a large number of
sampl... | cond-mat.dis-nn | we investigate the critical properties of the fourstate commutative random permutation glassy potts model in three and four dimensions by means of monte carlo simulation and of a finite size scaling analysis thanks to the use of a field programmable gate array we have been able to thermalize a large number of samples o... | [['we', 'investigate', 'the', 'critical', 'properties', 'of', 'the', 'fourstate', 'commutative', 'random', 'permutation', 'glassy', 'potts', 'model', 'in', 'three', 'and', 'four', 'dimensions', 'by', 'means', 'of', 'monte', 'carlo', 'simulation', 'and', 'of', 'a', 'finite', 'size', 'scaling', 'analysis', 'thanks', 'to'... | [-0.12124973593981357, 0.19894357821442657, -0.07334350821402696, 0.023788830612551187, -0.02303189956708937, -0.14495136036730563, 0.08399711252475443, 0.33757563042748084, -0.19886473447151548, -0.3079895360986828, 0.1244355809155365, -0.2871351090201118, -0.12029735895024764, 0.15630799973895354, 0.00141455939559786... |
710.4247 | Chiral dynamics of few-nucleon systems | I discuss some recent developments in chiral effective field theory for
few-nucleon systems.
| nucl-th | i discuss some recent developments in chiral effective field theory for fewnucleon systems | [['i', 'discuss', 'some', 'recent', 'developments', 'in', 'chiral', 'effective', 'field', 'theory', 'for', 'fewnucleon', 'systems']] | [-0.1805626851363251, 0.21081335068895266, -0.023967611531798657, 0.07473729020701005, -0.055028076928395495, -0.1333107681801686, -0.08648453120034762, 0.35113818442019135, -0.17440365398159394, -0.2000109043258887, 0.09309736838958298, -0.2916659310889932, -0.28867468954278874, 0.1340323153596658, -0.0463214066739265... |
710.4248 | INTEGRAL - operating high-energy detectors for five years in space | The INTEGRAL satellite, which studies the Universe in the hard X-ray and soft
Gamma-ray domain, has been operational for 5 years now. The X-ray telescopes,
which use the coded mask technique, provide unprecedented spectral and imaging
resolution. This led to a number of discoveries, such as the distribution of
diffus... | astro-ph | the integral satellite which studies the universe in the hard xray and soft gammaray domain has been operational for 5 years now the xray telescopes which use the coded mask technique provide unprecedented spectral and imaging resolution this led to a number of discoveries such as the distribution of diffuse emission i... | [['the', 'integral', 'satellite', 'which', 'studies', 'the', 'universe', 'in', 'the', 'hard', 'xray', 'and', 'soft', 'gammaray', 'domain', 'has', 'been', 'operational', 'for', '5', 'years', 'now', 'the', 'xray', 'telescopes', 'which', 'use', 'the', 'coded', 'mask', 'technique', 'provide', 'unprecedented', 'spectral', '... | [-0.0381478490264162, 0.10877777874089875, -0.06395538580687926, 0.11696536628060267, -0.11192115987090856, -0.0576995385467614, 0.029606383101300413, 0.44087551049958157, -0.1994129828513509, -0.4272266109859137, 0.12026217356114123, -0.37958635959802267, -0.01534010939426104, 0.26846090096742253, 0.004021106546926767... |
710.4249 | Complex Kerr Geometry, Twistors and the Dirac Electron | The Kerr-Newman spinning particle displays some remarkable relations to the
Dirac electron and has a reach spinor structure which is based on a twistorial
description of the Kerr congruence determined by the Kerr theorem. We consider
the relation between this spinor-twistorial structure and spinors of the Dirac
equat... | hep-th gr-qc quant-ph | the kerrnewman spinning particle displays some remarkable relations to the dirac electron and has a reach spinor structure which is based on a twistorial description of the kerr congruence determined by the kerr theorem we consider the relation between this spinortwistorial structure and spinors of the dirac equation a... | [['the', 'kerrnewman', 'spinning', 'particle', 'displays', 'some', 'remarkable', 'relations', 'to', 'the', 'dirac', 'electron', 'and', 'has', 'a', 'reach', 'spinor', 'structure', 'which', 'is', 'based', 'on', 'a', 'twistorial', 'description', 'of', 'the', 'kerr', 'congruence', 'determined', 'by', 'the', 'kerr', 'theore... | [-0.19570786596552744, 0.11673167962883757, -0.08834148086749043, 0.0793832957444121, -0.14911426571701225, -0.13182790399013036, -0.04139048247944211, 0.28996385386798884, -0.23297829299396677, -0.2507413971061642, -0.010469323301033394, -0.2871802827922275, -0.19688541798323794, 0.1906211181155192, 0.0308131426132309... |
710.425 | Four-nucleon force using the method of unitary transformation | We discuss in detail the derivation of the leading four-nucleon force in
chiral effective field theory using the method of unitary transformation. The
resulting four-nucleon force is given in both momentum and configuration space.
It does not contain any unknown parameters and can be used in few- and
many-nucleon stu... | nucl-th | we discuss in detail the derivation of the leading fournucleon force in chiral effective field theory using the method of unitary transformation the resulting fournucleon force is given in both momentum and configuration space it does not contain any unknown parameters and can be used in few and manynucleon studies | [['we', 'discuss', 'in', 'detail', 'the', 'derivation', 'of', 'the', 'leading', 'fournucleon', 'force', 'in', 'chiral', 'effective', 'field', 'theory', 'using', 'the', 'method', 'of', 'unitary', 'transformation', 'the', 'resulting', 'fournucleon', 'force', 'is', 'given', 'in', 'both', 'momentum', 'and', 'configuration'... | [-0.10661220647394658, 0.17203652953729034, -0.09980879629030824, 0.05775226378114894, -0.056568768471479416, -0.08002706347033381, -0.018437225436791778, 0.3925974164530635, -0.20963203662075103, -0.2913713490962982, 0.02199449230916798, -0.23230326462537051, -0.18148099537938833, 0.16042145892977713, -0.0013220816664... |
710.4251 | Group Analysis of Variable Coefficient Diffusion-Convection Equations.
IV. Potential Symmetries | This paper completes investigation of symmetry properties of nonlinear
variable coefficient diffusion-convection equations of the form
$f(x)u_t=(g(x)A(u)u_x)_x+h(x)B(u)u_x$. Potential symmetries of equations from
the considered class are found and the connection of them with Lie symmetries
of diffusion-type equations... | math-ph math.MP | this paper completes investigation of symmetry properties of nonlinear variable coefficient diffusionconvection equations of the form fxu_tgxauu_x_xhxbuu_x potential symmetries of equations from the considered class are found and the connection of them with lie symmetries of diffusiontype equations is shown exact solut... | [['this', 'paper', 'completes', 'investigation', 'of', 'symmetry', 'properties', 'of', 'nonlinear', 'variable', 'coefficient', 'diffusionconvection', 'equations', 'of', 'the', 'form', 'fxu_tgxauu_x_xhxbuu_x', 'potential', 'symmetries', 'of', 'equations', 'from', 'the', 'considered', 'class', 'are', 'found', 'and', 'the... | [-0.19798866367869158, 0.04782341375075122, -0.06454001474095152, 0.006712852625493357, -0.1485393271246489, -0.12339698923553558, -0.07030574903833343, 0.26800201671195534, -0.27387025972154544, -0.2689337160517561, 0.09662794008197144, -0.29431727084707704, -0.19973610293992022, 0.14760085710502685, 0.028928517066734... |
710.4252 | Scattering of Long-Wavelength Gravitational Waves | We consider the scattering of a low-frequency gravitational wave by a massive
compact body in vacuum. We apply partial-wave methods to compute amplitudes for
the helicity-conserving and helicity-reversing contributions to the cross
section, accurate to first order in $M\omega$. Contrary to previous claims, we
find th... | gr-qc astro-ph | we consider the scattering of a lowfrequency gravitational wave by a massive compact body in vacuum we apply partialwave methods to compute amplitudes for the helicityconserving and helicityreversing contributions to the cross section accurate to first order in momega contrary to previous claims we find that the partia... | [['we', 'consider', 'the', 'scattering', 'of', 'a', 'lowfrequency', 'gravitational', 'wave', 'by', 'a', 'massive', 'compact', 'body', 'in', 'vacuum', 'we', 'apply', 'partialwave', 'methods', 'to', 'compute', 'amplitudes', 'for', 'the', 'helicityconserving', 'and', 'helicityreversing', 'contributions', 'to', 'the', 'cro... | [-0.11488676500699387, 0.06140435597827208, -0.0809184932952811, 0.09377532927640553, -0.06038594197738787, -0.0008310003141904699, 0.01435134105448579, 0.3521977004049153, -0.13838621736343565, -0.20165804640695068, -0.023460053658145, -0.32767040072137427, -0.1147037313223399, 0.22622590842817364, 0.0357756518341344,... |
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