id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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709.1035 | Scaling and aging in the homogeneous cooling state of a granular fluid
of hard particles | The presence of the aging phenomenon in the homogeneous cooling state (HCS)
of a granular fluid composed of inelastic hard spheres or disks is
investigated. As a consequence of the scaling property of the $N$-particle
distribution function, it is obtained that the decay of the normalized two-time
correlation function... | cond-mat.stat-mech | the presence of the aging phenomenon in the homogeneous cooling state hcs of a granular fluid composed of inelastic hard spheres or disks is investigated as a consequence of the scaling property of the nparticle distribution function it is obtained that the decay of the normalized twotime correlation functions slows do... | [['the', 'presence', 'of', 'the', 'aging', 'phenomenon', 'in', 'the', 'homogeneous', 'cooling', 'state', 'hcs', 'of', 'a', 'granular', 'fluid', 'composed', 'of', 'inelastic', 'hard', 'spheres', 'or', 'disks', 'is', 'investigated', 'as', 'a', 'consequence', 'of', 'the', 'scaling', 'property', 'of', 'the', 'nparticle', '... | [-0.13425950568914413, 0.12789288983226288, -0.11292903955467046, 0.07593414933141321, 0.02400355695746839, -0.04174284034967422, 0.02021925588697195, 0.29899337713420393, -0.24446275877393783, -0.28084319376945494, 0.09179102492891252, -0.27728035107627513, -0.11504198540188372, 0.17304226684756577, 0.0658947262614965... |
709.1036 | Longitudinal and Transverse Form Factors from $^{12}$C | Electron scattering form factors from $^{12}$C have been studied in the
framework of the particle-hole shell model. Higher configurations are taken
into account by allowing particle-hole excitations from the 1$s$ and 1$p$
shells core orbits up to the 1$f-2p$ shell. The inclusion of the higher
configurations modifies ... | nucl-th | electron scattering form factors from 12c have been studied in the framework of the particlehole shell model higher configurations are taken into account by allowing particlehole excitations from the 1s and 1p shells core orbits up to the 1f2p shell the inclusion of the higher configurations modifies the form factors m... | [['electron', 'scattering', 'form', 'factors', 'from', '12c', 'have', 'been', 'studied', 'in', 'the', 'framework', 'of', 'the', 'particlehole', 'shell', 'model', 'higher', 'configurations', 'are', 'taken', 'into', 'account', 'by', 'allowing', 'particlehole', 'excitations', 'from', 'the', '1s', 'and', '1p', 'shells', 'c... | [-0.07906452824376643, 0.1534202957916404, -0.060558545455757166, 0.11232989601370308, 0.0352377081815634, -0.08087408924174885, 0.03916868768752583, 0.3667582516227999, -0.18987506787262617, -0.2966219955274174, -0.035275287272769115, -0.3246570864632245, -0.033977525368813544, 0.10198377496037152, 0.09140268564149137... |
709.1037 | The joint large-scale foreground-CMB posteriors of the 3-year WMAP data | Using a Gibbs sampling algorithm for joint CMB estimation and component
separation, we compute the large-scale CMB and foreground posteriors of the
3-yr WMAP temperature data. Our parametric data model includes the cosmological
CMB signal and instrumental noise, a single power law foreground component with
free ampli... | astro-ph | using a gibbs sampling algorithm for joint cmb estimation and component separation we compute the largescale cmb and foreground posteriors of the 3yr wmap temperature data our parametric data model includes the cosmological cmb signal and instrumental noise a single power law foreground component with free amplitude an... | [['using', 'a', 'gibbs', 'sampling', 'algorithm', 'for', 'joint', 'cmb', 'estimation', 'and', 'component', 'separation', 'we', 'compute', 'the', 'largescale', 'cmb', 'and', 'foreground', 'posteriors', 'of', 'the', '3yr', 'wmap', 'temperature', 'data', 'our', 'parametric', 'data', 'model', 'includes', 'the', 'cosmologic... | [-0.0654334639869553, 0.08159829551524085, -0.0728009326520658, 0.06873187624039785, -0.07708496126999376, -0.1121285303661994, 0.040920792819924376, 0.39715517406579864, -0.24309796553116708, -0.34472156426564043, 0.09232252546928096, -0.2946326513009057, -0.0629448068514901, 0.220965139095428, -0.04765499871479216, 0... |
709.1038 | Emergent charge ordering in near half doped Na$_{0.46}$CoO$_{2}$ | We have utilized neutron powder diffraction to probe the crystal structure of
layered Na$_{x}$CoO$_{2}$ near the half doping composition of $x=$0.46 over the
temperature range of 2 to 600K. Our measurements show evidence of a dynamic
transition in the motion of Na-ions at 300K which coincides with the onset of a
near... | cond-mat.str-el cond-mat.supr-con | we have utilized neutron powder diffraction to probe the crystal structure of layered na_xcoo_2 near the half doping composition of x046 over the temperature range of 2 to 600k our measurements show evidence of a dynamic transition in the motion of naions at 300k which coincides with the onset of a near zero thermal ex... | [['we', 'have', 'utilized', 'neutron', 'powder', 'diffraction', 'to', 'probe', 'the', 'crystal', 'structure', 'of', 'layered', 'na_xcoo_2', 'near', 'the', 'half', 'doping', 'composition', 'of', 'x046', 'over', 'the', 'temperature', 'range', 'of', '2', 'to', '600k', 'our', 'measurements', 'show', 'evidence', 'of', 'a', ... | [-0.1589981322441765, 0.2193310830848125, -0.0363384705582043, -0.0074320085236908705, 0.007921367550526208, -0.06258333538378763, 0.10841915669010543, 0.40566016848736663, -0.2991799164934432, -0.27843330611997263, 0.044114900861745625, -0.34811134734077426, -0.06850055721777726, 0.1293326361195707, 0.0730819080812417... |
709.1039 | Critical scaling of stochastic epidemic models | In the simple mean-field SIS and SIR epidemic models, infection is
transmitted from infectious to susceptible members of a finite population by
independent $p-$coin tosses. Spatial variants of these models are proposed, in
which finite populations of size $N$ are situated at the sites of a lattice and
infectious cont... | math.PR | in the simple meanfield sis and sir epidemic models infection is transmitted from infectious to susceptible members of a finite population by independent pcoin tosses spatial variants of these models are proposed in which finite populations of size n are situated at the sites of a lattice and infectious contacts are li... | [['in', 'the', 'simple', 'meanfield', 'sis', 'and', 'sir', 'epidemic', 'models', 'infection', 'is', 'transmitted', 'from', 'infectious', 'to', 'susceptible', 'members', 'of', 'a', 'finite', 'population', 'by', 'independent', 'pcoin', 'tosses', 'spatial', 'variants', 'of', 'these', 'models', 'are', 'proposed', 'in', 'wh... | [-0.11194525300711393, 0.21200687170028687, -0.04641630274802446, 0.1010203336878476, -0.0007289830334484578, -0.22285387417674066, 0.1189098084717989, 0.35831860402226445, -0.23653588764742017, -0.23552429653704166, 0.10681394973769784, -0.3399001601487398, -0.13838797463662922, 0.10791413725912571, -0.022983115814626... |
709.104 | What is Minimal Model of 3He Adsorbed on Graphite? -Importance of
Density Fluctuations in 4/7 Registered Solid - | We show theoretically that the second layer of 3He adsorbed on graphite and
solidified at 4/7 of the first-layer density is close to the fluid-solid
boundary with substantial density fluctuations on the third layer. The solid
shows a translational symmetry breaking as in charge-ordered insulators of
electronic system... | cond-mat.str-el | we show theoretically that the second layer of 3he adsorbed on graphite and solidified at 47 of the firstlayer density is close to the fluidsolid boundary with substantial density fluctuations on the third layer the solid shows a translational symmetry breaking as in chargeordered insulators of electronic systems we co... | [['we', 'show', 'theoretically', 'that', 'the', 'second', 'layer', 'of', '3he', 'adsorbed', 'on', 'graphite', 'and', 'solidified', 'at', '47', 'of', 'the', 'firstlayer', 'density', 'is', 'close', 'to', 'the', 'fluidsolid', 'boundary', 'with', 'substantial', 'density', 'fluctuations', 'on', 'the', 'third', 'layer', 'the... | [-0.14414430545177312, 0.22451006045695976, -0.04952625886071473, 0.0502191578631755, 0.03038250397890806, -0.11457736297510564, 0.06905563795706257, 0.3374248321726918, -0.2706125717237592, -0.28609269430598944, 0.03904114421689883, -0.3003590624639764, -0.11386250594630837, 0.10772575031674933, 0.025501861018128694, ... |
709.1041 | Rainich theory applied to m-rank tensors in n-dimensions | We show a tensorial-computational way to find out conditions that must fulfil
an m-rank tensor in arbitrary dimension in order to be algebraically the
energy-momentum tensor of some field. We apply in this paper our method to
three 2-rank tensors: electromagnetic, mass less scalar field and perfect fluid
tensors. Fin... | gr-qc | we show a tensorialcomputational way to find out conditions that must fulfil an mrank tensor in arbitrary dimension in order to be algebraically the energymomentum tensor of some field we apply in this paper our method to three 2rank tensors electromagnetic mass less scalar field and perfect fluid tensors finally we ap... | [['we', 'show', 'a', 'tensorialcomputational', 'way', 'to', 'find', 'out', 'conditions', 'that', 'must', 'fulfil', 'an', 'mrank', 'tensor', 'in', 'arbitrary', 'dimension', 'in', 'order', 'to', 'be', 'algebraically', 'the', 'energymomentum', 'tensor', 'of', 'some', 'field', 'we', 'apply', 'in', 'this', 'paper', 'our', '... | [-0.14659553454992802, 0.13226130506122818, -0.08552586545416138, 0.04768222327581035, -0.1357216427731736, -0.08996011139498207, -0.09665077512168832, 0.38917770609259605, -0.22644747466894619, -0.2388460546764627, 0.0778499371719367, -0.23263442651123592, -0.2216276028234381, 0.12241244851509436, -0.03114151177323309... |
709.1042 | Quantized vortices in atomic Bose-Einstein condensates | In this review, we give an overview of the experimental and theoretical
advances in the physics of quantized vortices in dilute atomic-gas
Bose--Einstein condensates in a trapping potential, especially focusing on
experimental research activities and their theoretical interpretations. Making
good use of the atom opti... | cond-mat.other cond-mat.mes-hall | in this review we give an overview of the experimental and theoretical advances in the physics of quantized vortices in dilute atomicgas boseeinstein condensates in a trapping potential especially focusing on experimental research activities and their theoretical interpretations making good use of the atom optical tech... | [['in', 'this', 'review', 'we', 'give', 'an', 'overview', 'of', 'the', 'experimental', 'and', 'theoretical', 'advances', 'in', 'the', 'physics', 'of', 'quantized', 'vortices', 'in', 'dilute', 'atomicgas', 'boseeinstein', 'condensates', 'in', 'a', 'trapping', 'potential', 'especially', 'focusing', 'on', 'experimental', ... | [-0.14759173210121743, 0.19678523109202312, -0.09820611200605829, 0.027824504390850456, -0.026445970525188992, -0.08796736729176094, 0.01408455039943672, 0.3468001877733817, -0.2436610691818512, -0.26882583813728866, 0.05014299105484194, -0.2669946300279763, -0.09778524910196008, 0.1883916010743835, 0.022004787517815, ... |
709.1043 | Signals of the QCD Phase Transition in the Heavens | The modern phase diagram of strongly interacting matter reveals a rich
structure at high-densities due to phase transitions related to the chiral
symmetry of quantum chromodynamics (QCD) and the phenomenon of color
superconductivity. These exotic phases have significant impacts on high-density
astrophysics as the pro... | astro-ph nucl-th | the modern phase diagram of strongly interacting matter reveals a rich structure at highdensities due to phase transitions related to the chiral symmetry of quantum chromodynamics qcd and the phenomenon of color superconductivity these exotic phases have significant impacts on highdensity astrophysics as the properties... | [['the', 'modern', 'phase', 'diagram', 'of', 'strongly', 'interacting', 'matter', 'reveals', 'a', 'rich', 'structure', 'at', 'highdensities', 'due', 'to', 'phase', 'transitions', 'related', 'to', 'the', 'chiral', 'symmetry', 'of', 'quantum', 'chromodynamics', 'qcd', 'and', 'the', 'phenomenon', 'of', 'color', 'supercond... | [-0.09942933559129365, 0.24218713785634935, -0.1278345144020635, 0.12484379746867383, -0.15503540800331028, -0.024030508820326008, 0.0785607978965596, 0.32729922432187464, -0.15827054916793348, -0.30776105697605777, 0.04387430695838307, -0.31967509930337695, -0.017153685467286527, 0.18974612698847404, 0.020418958112013... |
709.1044 | Weak-field limit of conformal Weyl gravity | We study the weak-field limit of the conformal Weyl gravity suggested by
Mannheim as an alternative to Einstein's General Relativity modeling both dark
matter and dark energy. We solve the field equations of the theory in the
weak-field approximation for an arbitrary spherically symmetric static
distribution of matte... | astro-ph | we study the weakfield limit of the conformal weyl gravity suggested by mannheim as an alternative to einsteins general relativity modeling both dark matter and dark energy we solve the field equations of the theory in the weakfield approximation for an arbitrary spherically symmetric static distribution of matter in t... | [['we', 'study', 'the', 'weakfield', 'limit', 'of', 'the', 'conformal', 'weyl', 'gravity', 'suggested', 'by', 'mannheim', 'as', 'an', 'alternative', 'to', 'einsteins', 'general', 'relativity', 'modeling', 'both', 'dark', 'matter', 'and', 'dark', 'energy', 'we', 'solve', 'the', 'field', 'equations', 'of', 'the', 'theory... | [-0.1660243827862212, 0.09069781778482532, -0.1256050746447432, 0.12728116555120544, -0.122256043228648, -0.1342296747843156, -0.06043672412193406, 0.2720484414603561, -0.1823241383189688, -0.3187374515912017, 0.009842783952056355, -0.24149233742138823, -0.10694045969914343, 0.11452390319774733, -0.006877276687756987, ... |
709.1045 | Rotational Modulation of M/L Dwarfs due to Magnetic Spots | We find periodic I-band variability in two ultracool dwarfs, TVLM 513-46546
and 2MASS J00361617+1821104, on either side of the M/L dwarf boundary. Both of
these targets are short-period radio transients, with the detected I-band
periods matching those found at radio wavelengths (P=1.96 hr for TVLM
513-46546, and P=3 ... | astro-ph | we find periodic iband variability in two ultracool dwarfs tvlm 51346546 and 2mass j003616171821104 on either side of the ml dwarf boundary both of these targets are shortperiod radio transients with the detected iband periods matching those found at radio wavelengths p196 hr for tvlm 51346546 and p3 hr for 2mass j0036... | [['we', 'find', 'periodic', 'iband', 'variability', 'in', 'two', 'ultracool', 'dwarfs', 'tvlm', '51346546', 'and', '2mass', 'j003616171821104', 'on', 'either', 'side', 'of', 'the', 'ml', 'dwarf', 'boundary', 'both', 'of', 'these', 'targets', 'are', 'shortperiod', 'radio', 'transients', 'with', 'the', 'detected', 'iband... | [-0.14063845922038715, 0.12714154836780664, -0.05635568369887298, 0.07706267674029156, -0.15740018556059537, -0.10230024434667363, 0.07291869277169905, 0.46883820648646995, -0.1447048648680513, -0.3275115161403259, 0.10565299620406844, -0.3007663025102973, -0.08871591773732931, 0.24592319182768652, -0.11384133297560996... |
709.1046 | Exploring the Physical Basis of Solar Cycle Predictions: Flux Transport
Dynamics and Persistence of Memory in Advection versus Diffusion Dominated
Solar Convection Zones | The predictability, or lack thereof, of the solar cycle is governed by
numerous separate physical processes that act in unison in the interior of the
Sun. Magnetic flux transport and the finite time delay it introduces,
specifically in the so-called Babcock-Leighton models of the solar cycle with
spatially segregated... | astro-ph | the predictability or lack thereof of the solar cycle is governed by numerous separate physical processes that act in unison in the interior of the sun magnetic flux transport and the finite time delay it introduces specifically in the socalled babcockleighton models of the solar cycle with spatially segregated source ... | [['the', 'predictability', 'or', 'lack', 'thereof', 'of', 'the', 'solar', 'cycle', 'is', 'governed', 'by', 'numerous', 'separate', 'physical', 'processes', 'that', 'act', 'in', 'unison', 'in', 'the', 'interior', 'of', 'the', 'sun', 'magnetic', 'flux', 'transport', 'and', 'the', 'finite', 'time', 'delay', 'it', 'introdu... | [-0.1746639044468031, 0.225247314804564, -0.01139057900829416, 0.08439540807798745, 0.006424094241127553, -0.08064619465335178, 0.048243367081123444, 0.32868861439939484, -0.2894166510039375, -0.3196629408279411, 0.08716979658283927, -0.21617192361383183, -0.15326233659795513, 0.23802998998091152, -0.03816979673506338,... |
709.1047 | A Dirac type result on Hamilton cycles in oriented graphs | We show that for each \alpha>0 every sufficiently large oriented graph G with
\delta^+(G),\delta^-(G)\ge 3|G|/8+ \alpha |G| contains a Hamilton cycle. This
gives an approximate solution to a problem of Thomassen. In fact, we prove the
stronger result that G is still Hamiltonian if
\delta(G)+\delta^+(G)+\delta^-(G)\ge... | math.CO | we show that for each alpha0 every sufficiently large oriented graph g with deltagdeltagge 3g8 alpha g contains a hamilton cycle this gives an approximate solution to a problem of thomassen in fact we prove the stronger result that g is still hamiltonian if deltagdeltagdeltaggeq 3g2 alpha g up to the term alpha g this ... | [['we', 'show', 'that', 'for', 'each', 'alpha0', 'every', 'sufficiently', 'large', 'oriented', 'graph', 'g', 'with', 'deltagdeltagge', '3g8', 'alpha', 'g', 'contains', 'a', 'hamilton', 'cycle', 'this', 'gives', 'an', 'approximate', 'solution', 'to', 'a', 'problem', 'of', 'thomassen', 'in', 'fact', 'we', 'prove', 'the',... | [-0.24718577380884776, 0.10815549698952853, -0.08046809737711694, 0.027654634582259776, -0.08283867801285603, -0.1563101754679034, 0.016720428314963072, 0.3892197293709173, -0.2707224400206046, -0.29303779580037703, 0.023572291076451427, -0.27615191044187115, -0.167267918304512, 0.16062400219115344, -0.136120139663531,... |
709.1048 | Generalized squeezing operators, bipartite Wigner functions and
entanglement via Wehrl's entropy functionals | We introduce a new class of unitary transformations based on the su(1,1) Lie
algebra that generalizes, for certain particular representations of its
generators, well-known squeezing transformations in quantum optics. To
illustrate our results, we focus on the two-mode bosonic representation and
show how the parametri... | quant-ph | we introduce a new class of unitary transformations based on the su11 lie algebra that generalizes for certain particular representations of its generators wellknown squeezing transformations in quantum optics to illustrate our results we focus on the twomode bosonic representation and show how the parametric amplifier... | [['we', 'introduce', 'a', 'new', 'class', 'of', 'unitary', 'transformations', 'based', 'on', 'the', 'su11', 'lie', 'algebra', 'that', 'generalizes', 'for', 'certain', 'particular', 'representations', 'of', 'its', 'generators', 'wellknown', 'squeezing', 'transformations', 'in', 'quantum', 'optics', 'to', 'illustrate', '... | [-0.0821376345419419, 0.15024226437826907, -0.126388278779939, 0.08323589256118744, -0.06848167920583398, -0.14811781603402946, 0.02511244131585395, 0.3606044962968028, -0.26315974014802673, -0.21410374877624078, 0.049713130150665315, -0.24319992704253426, -0.20145805273044837, 0.22617033965364441, -0.08913153021622004... |
709.1049 | Introduction to Tropical Geometry (notes from the IMPA lectures in
Summer 2007) | These condensed notes treat some basic notions in Tropical Geometry
(varieties, cycles, modifications, equivalence). These topics are to be
extended, illustrated and included to the upcoming book project
http://www.math.toronto.edu/mikha/book.pdf .
| math.AG math.GT | these condensed notes treat some basic notions in tropical geometry varieties cycles modifications equivalence these topics are to be extended illustrated and included to the upcoming book project httpwwwmathtorontoedumikhabookpdf | [['these', 'condensed', 'notes', 'treat', 'some', 'basic', 'notions', 'in', 'tropical', 'geometry', 'varieties', 'cycles', 'modifications', 'equivalence', 'these', 'topics', 'are', 'to', 'be', 'extended', 'illustrated', 'and', 'included', 'to', 'the', 'upcoming', 'book', 'project', 'httpwwwmathtorontoedumikhabookpdf']] | [-0.09128505317494273, 0.1281175838251199, -0.06618895958776452, 0.2567907876800746, -0.12280136067420244, -0.16057986812666059, -0.06774265292499747, 0.30698870015995844, -0.34322599042207, -0.29406753794423174, 0.19510262785063656, -0.2888072302032794, -0.1716787540374623, 0.19848226609506778, -0.19433253910392523, -... |
709.105 | A template bank to search for gravitational waves from inspiralling
compact binaries: II. Phenomenological model | Matched filtering is used to search for gravitational waves emitted by
inspiralling compact binaries in data from ground-based interferometers. One of
the key aspects of the detection process is the deployment of a set of
templates, also called a template bank, to cover the astrophysically
interesting region of the p... | gr-qc | matched filtering is used to search for gravitational waves emitted by inspiralling compact binaries in data from groundbased interferometers one of the key aspects of the detection process is the deployment of a set of templates also called a template bank to cover the astrophysically interesting region of the paramet... | [['matched', 'filtering', 'is', 'used', 'to', 'search', 'for', 'gravitational', 'waves', 'emitted', 'by', 'inspiralling', 'compact', 'binaries', 'in', 'data', 'from', 'groundbased', 'interferometers', 'one', 'of', 'the', 'key', 'aspects', 'of', 'the', 'detection', 'process', 'is', 'the', 'deployment', 'of', 'a', 'set',... | [-0.10088689482258358, 0.03132886389827014, -0.06653133045727684, 0.11193587221902908, -0.1326428230565328, -0.07343592894636922, 0.045721870005962895, 0.35523349339329807, -0.1505942646380977, -0.34644600337911285, 0.09709257788655827, -0.3012116069701561, -0.11795975824476347, 0.2620227384345176, -0.04013173125519626... |
709.1051 | Disproof of modularity of moduli space of CY 3-folds of double covers of
P3 ramified along eight planes in general positions | We prove that the moduli space of Calabi-Yau 3-folds coming from eight planes
of $P^3$ in general positions is not modular. In fact we show the stronger
statement that the Zariski closure of the monodromy group is actually the whole
$Sp(20,R)$. We construct an interesting submoduli, which we call
\emph{hyperelliptic ... | math.AG | we prove that the moduli space of calabiyau 3folds coming from eight planes of p3 in general positions is not modular in fact we show the stronger statement that the zariski closure of the monodromy group is actually the whole sp20r we construct an interesting submoduli which we call emphhyperelliptic locus over which ... | [['we', 'prove', 'that', 'the', 'moduli', 'space', 'of', 'calabiyau', '3folds', 'coming', 'from', 'eight', 'planes', 'of', 'p3', 'in', 'general', 'positions', 'is', 'not', 'modular', 'in', 'fact', 'we', 'show', 'the', 'stronger', 'statement', 'that', 'the', 'zariski', 'closure', 'of', 'the', 'monodromy', 'group', 'is',... | [-0.2369826352329586, 0.03728703524277741, -0.13548021533113735, 0.08999461204935373, -0.10365655153079635, -0.09560827932992569, 0.0038009384562346068, 0.30652294533369556, -0.3384276249403642, -0.16897637011821975, 0.08385416311053136, -0.22678492282284424, -0.17428296226584775, 0.22299651444402777, -0.16285121457820... |
709.1052 | Possibility of a modification of life time of radioactive elements by
magnetic monopoles | A simple explanation of the fact that light magnetic monopoles have not been
observed at accelerator experiments is given. It is based on a possibility of
violation of C invariance in the electromagnetic interactions. Because of the
difficulty of monopole registration, two interconnected problems arise: to
formulate ... | hep-ph | a simple explanation of the fact that light magnetic monopoles have not been observed at accelerator experiments is given it is based on a possibility of violation of c invariance in the electromagnetic interactions because of the difficulty of monopole registration two interconnected problems arise to formulate a theo... | [['a', 'simple', 'explanation', 'of', 'the', 'fact', 'that', 'light', 'magnetic', 'monopoles', 'have', 'not', 'been', 'observed', 'at', 'accelerator', 'experiments', 'is', 'given', 'it', 'is', 'based', 'on', 'a', 'possibility', 'of', 'violation', 'of', 'c', 'invariance', 'in', 'the', 'electromagnetic', 'interactions', ... | [-0.14985046393315618, 0.17536906921925643, -0.06474230419951103, 0.09098889836265395, -0.11813253947844107, -0.10712967969787618, 0.03733913821633905, 0.31188428808624546, -0.2352402702718973, -0.29502222714014353, 0.05555880261119455, -0.2789390516777833, -0.13889526998779425, 0.18182237213477492, 0.00778872920200228... |
709.1053 | Exact Solutions of the Equations of Relativistic Hydrodynamics
Representing Potential Flows | We use a connection between relativistic hydrodynamics and scalar field
theory to generate exact analytic solutions describing non-stationary
inhomogeneous flows of the perfect fluid with one-parametric equation of state
(EOS) $p = p(\epsilon)$. For linear EOS $p = \kappa \epsilon$ we obtain
self-similar solutions in... | math-ph astro-ph math.MP nucl-th | we use a connection between relativistic hydrodynamics and scalar field theory to generate exact analytic solutions describing nonstationary inhomogeneous flows of the perfect fluid with oneparametric equation of state eos p pepsilon for linear eos p kappa epsilon we obtain selfsimilar solutions in the case of plane cy... | [['we', 'use', 'a', 'connection', 'between', 'relativistic', 'hydrodynamics', 'and', 'scalar', 'field', 'theory', 'to', 'generate', 'exact', 'analytic', 'solutions', 'describing', 'nonstationary', 'inhomogeneous', 'flows', 'of', 'the', 'perfect', 'fluid', 'with', 'oneparametric', 'equation', 'of', 'state', 'eos', 'p', ... | [-0.18906551730948723, 0.1077972542276441, -0.12292337768911561, 0.10775407299081076, -0.15052416064788268, -0.18166900590604432, -0.06962906389609215, 0.3149371132301756, -0.16577920344764296, -0.24825142995937716, 0.019881989697843223, -0.2621768148545223, -0.0953076053970741, 0.12932449049033412, 0.08224701965625598... |
709.1054 | Computational details on the disproof of modularity | The purpose of these notes is to provide the details of the Jacobian ring
computations carried out in [1], based on the computer algebra system Magma
[2].
| math.AG | the purpose of these notes is to provide the details of the jacobian ring computations carried out in 1 based on the computer algebra system magma 2 | [['the', 'purpose', 'of', 'these', 'notes', 'is', 'to', 'provide', 'the', 'details', 'of', 'the', 'jacobian', 'ring', 'computations', 'carried', 'out', 'in', '1', 'based', 'on', 'the', 'computer', 'algebra', 'system', 'magma', '2']] | [-0.16066817173527348, -0.03101999878331467, -0.12679975169400373, 0.00584232443684919, -0.034942390776618766, -0.11820436142065942, -0.04477400315442571, 0.30187384549666335, -0.28950753614858343, -0.2551848143339157, 0.23223546983380974, -0.19652693472043783, -0.14143435670821755, 0.23896497826057453, -0.049923020242... |
709.1055 | Mass transport in a strongly sheared binary mixture of Maxwell molecules | Transport coefficients associated with the mass flux of a binary mixture of
Maxwell molecules under uniform shear flow are exactly determined from the
Boltzmann kinetic equation. A normal solution is obtained via a
Chapman--Enskog-like expansion around a local shear flow distribution that
retains all the hydrodynamic... | cond-mat.stat-mech | transport coefficients associated with the mass flux of a binary mixture of maxwell molecules under uniform shear flow are exactly determined from the boltzmann kinetic equation a normal solution is obtained via a chapmanenskoglike expansion around a local shear flow distribution that retains all the hydrodynamics orde... | [['transport', 'coefficients', 'associated', 'with', 'the', 'mass', 'flux', 'of', 'a', 'binary', 'mixture', 'of', 'maxwell', 'molecules', 'under', 'uniform', 'shear', 'flow', 'are', 'exactly', 'determined', 'from', 'the', 'boltzmann', 'kinetic', 'equation', 'a', 'normal', 'solution', 'is', 'obtained', 'via', 'a', 'chap... | [-0.14370102723351802, 0.15759045988803416, -0.0717053787175404, 0.005332922699618275, -0.019058565068585068, -0.05873182791730632, -0.01610965879391069, 0.304683929098689, -0.3165639789086645, -0.2653656412493033, 0.07623830409467464, -0.2941940357220238, -0.09571904317354378, 0.19062107514498916, 0.035907799156342186... |
709.1056 | A Sudoku Game for People with Motor Impairments | Computer games are motivating and beneficial in learning different
educational skills. Most people use their fingers, hands, and arms when using a
computer game. However, for people with motor disabilities this task can be a
barrier. We present a new Sudoku game for people whose motion is impaired,
called Sudoku 4ALL... | cs.HC cs.CY | computer games are motivating and beneficial in learning different educational skills most people use their fingers hands and arms when using a computer game however for people with motor disabilities this task can be a barrier we present a new sudoku game for people whose motion is impaired called sudoku 4all with thi... | [['computer', 'games', 'are', 'motivating', 'and', 'beneficial', 'in', 'learning', 'different', 'educational', 'skills', 'most', 'people', 'use', 'their', 'fingers', 'hands', 'and', 'arms', 'when', 'using', 'a', 'computer', 'game', 'however', 'for', 'people', 'with', 'motor', 'disabilities', 'this', 'task', 'can', 'be'... | [-0.06610768887492799, 0.09304733402527791, -0.1183487078770227, 0.08203594218795524, -0.20789155293947337, -0.27843185960670414, 0.08486134711276144, 0.44098490046471667, -0.2467057623086766, -0.35824376187220064, 0.09427181085974899, -0.2568507500103262, -0.2112680432727541, 0.1474211346214042, -0.20325139590260602, ... |
709.1057 | Spin-orbit coupling effects in one-dimensional ballistic quantum wires | We study the spin-dependent electronic transport through a one-dimensional
ballistic quantum wire in the presence of Rashba spin-orbit interaction. In
particular, we consider the effect of the spin-orbit interaction resulting from
the lateral confinement of the two-dimensional electron gas to the
one-dimensional wire... | cond-mat.mes-hall | we study the spindependent electronic transport through a onedimensional ballistic quantum wire in the presence of rashba spinorbit interaction in particular we consider the effect of the spinorbit interaction resulting from the lateral confinement of the twodimensional electron gas to the onedimensional wire geometry ... | [['we', 'study', 'the', 'spindependent', 'electronic', 'transport', 'through', 'a', 'onedimensional', 'ballistic', 'quantum', 'wire', 'in', 'the', 'presence', 'of', 'rashba', 'spinorbit', 'interaction', 'in', 'particular', 'we', 'consider', 'the', 'effect', 'of', 'the', 'spinorbit', 'interaction', 'resulting', 'from', ... | [-0.18173881418196663, 0.12893283526125957, -0.05310644259203828, -0.00012585371458793387, -0.021918803960194484, -0.1304585778270848, 0.057777784391552865, 0.3567056726760176, -0.26239841456031976, -0.27142783650539487, -0.06282239527054652, -0.27616390946283953, -0.1476517155636376, 0.18412725696929128, 0.02250033493... |
709.1058 | Joint Bayesian component separation and CMB power spectrum estimation | We describe and implement an exact, flexible, and computationally efficient
algorithm for joint component separation and CMB power spectrum estimation,
building on a Gibbs sampling framework. Two essential new features are 1)
conditional sampling of foreground spectral parameters, and 2) joint sampling
of all amplitu... | astro-ph | we describe and implement an exact flexible and computationally efficient algorithm for joint component separation and cmb power spectrum estimation building on a gibbs sampling framework two essential new features are 1 conditional sampling of foreground spectral parameters and 2 joint sampling of all amplitudetype de... | [['we', 'describe', 'and', 'implement', 'an', 'exact', 'flexible', 'and', 'computationally', 'efficient', 'algorithm', 'for', 'joint', 'component', 'separation', 'and', 'cmb', 'power', 'spectrum', 'estimation', 'building', 'on', 'a', 'gibbs', 'sampling', 'framework', 'two', 'essential', 'new', 'features', 'are', '1', '... | [-0.06254200948799243, 0.0462151635928834, -0.09157026594484358, 0.09711363912646562, -0.09583292571481704, -0.11390679998099397, 0.03370162416783879, 0.4117869929782028, -0.24296329593886443, -0.32898065637888724, 0.08664262972968055, -0.264091949937916, -0.09282958386192362, 0.1728996494975796, -0.048610415754972096,... |
709.1059 | A new semilocal convergence theorem for the Weierstrass method from data
at one point | In this paper we present a new semilocal convergence theorem from data at one
point for the Weierstrass iterative method for the simultaneous computation of
polynomial zeros. The main result generalizes and improves all previous ones in
this area.
| math.NA | in this paper we present a new semilocal convergence theorem from data at one point for the weierstrass iterative method for the simultaneous computation of polynomial zeros the main result generalizes and improves all previous ones in this area | [['in', 'this', 'paper', 'we', 'present', 'a', 'new', 'semilocal', 'convergence', 'theorem', 'from', 'data', 'at', 'one', 'point', 'for', 'the', 'weierstrass', 'iterative', 'method', 'for', 'the', 'simultaneous', 'computation', 'of', 'polynomial', 'zeros', 'the', 'main', 'result', 'generalizes', 'and', 'improves', 'all... | [-0.1071264714671251, -0.07508250910979815, -0.11815134687826802, 0.04777488035436433, -0.031606182300796114, -0.0966980730374463, 0.09068754009412935, 0.2871226546808313, -0.2673375129293746, -0.26297830359246105, 0.08292165752619696, -0.2682273739901109, -0.15267412474331182, 0.2603636357742242, -0.13090218062652872,... |
709.106 | Spitzer-MIPS survey of the young stellar content in the Vela Molecular
Cloud-D | A new, unbiased Spitzer-MIPS imaging survey (~1.8 square degs) of the young
stellar content of the Vela Molecular Cloud-D is presented. The survey is
complete down to 5mJy and 250mJy at 24micron (mu) and 70mu, respectively. 849
sources are detected at 24mu and 52 of them also have a 70mu counterpart. The
VMR-D region... | astro-ph | a new unbiased spitzermips imaging survey 18 square degs of the young stellar content of the vela molecular cloudd is presented the survey is complete down to 5mjy and 250mjy at 24micron mu and 70mu respectively 849 sources are detected at 24mu and 52 of them also have a 70mu counterpart the vmrd region is one that we ... | [['a', 'new', 'unbiased', 'spitzermips', 'imaging', 'survey', '18', 'square', 'degs', 'of', 'the', 'young', 'stellar', 'content', 'of', 'the', 'vela', 'molecular', 'cloudd', 'is', 'presented', 'the', 'survey', 'is', 'complete', 'down', 'to', '5mjy', 'and', '250mjy', 'at', '24micron', 'mu', 'and', '70mu', 'respectively'... | [-0.07497745000485641, 0.08400435798646495, -0.03045360446368984, 0.07332330138093407, -0.05487056081575981, -0.05572734630655452, 0.08803385358159319, 0.4444534851604676, -0.1576018609526384, -0.35896710229917883, 0.12016197273285169, -0.32082007450975447, -0.012884155315081459, 0.17880044889591454, -0.015205207887904... |
709.1061 | Fermionic Quasi-free States and Maps in Information Theory | This paper and the results therein are geared towards building a basic
toolbox for calculations in quantum information theory of quasi-free fermionic
systems. Various entropy and relative entropy measures are discussed and the
calculation of these reduced to evaluating functions on the one-particle
component of quasi... | quant-ph | this paper and the results therein are geared towards building a basic toolbox for calculations in quantum information theory of quasifree fermionic systems various entropy and relative entropy measures are discussed and the calculation of these reduced to evaluating functions on the oneparticle component of quasifree ... | [['this', 'paper', 'and', 'the', 'results', 'therein', 'are', 'geared', 'towards', 'building', 'a', 'basic', 'toolbox', 'for', 'calculations', 'in', 'quantum', 'information', 'theory', 'of', 'quasifree', 'fermionic', 'systems', 'various', 'entropy', 'and', 'relative', 'entropy', 'measures', 'are', 'discussed', 'and', '... | [-0.11042125538786811, 0.16479553247990317, -0.047499266044979685, 0.07282948144973161, 0.06394469792944159, -0.11472474265152986, 0.023989520140327094, 0.34002102088978453, -0.27241683659258853, -0.19605343274541953, 0.08805805987029681, -0.3048678520606475, -0.12184897845276119, 0.21713335565919203, -0.02315144857131... |
709.1062 | A complex semigroup approach to group algebras of infinite dimensional
Lie groups | A host algebra of a topological group G is a C^*-algebra whose
representations are in one-to-one correspondence with certain continuous
unitary representations of G. In this paper we present an approach to host
algebras for infinite dimensional Lie groups which is based on complex
involutive semigroups. Any locally b... | math.OA math.RT | a host algebra of a topological group g is a calgebra whose representations are in onetoone correspondence with certain continuous unitary representations of g in this paper we present an approach to host algebras for infinite dimensional lie groups which is based on complex involutive semigroups any locally bounded ab... | [['a', 'host', 'algebra', 'of', 'a', 'topological', 'group', 'g', 'is', 'a', 'calgebra', 'whose', 'representations', 'are', 'in', 'onetoone', 'correspondence', 'with', 'certain', 'continuous', 'unitary', 'representations', 'of', 'g', 'in', 'this', 'paper', 'we', 'present', 'an', 'approach', 'to', 'host', 'algebras', 'f... | [-0.14621836799260687, 0.09262884666601814, -0.11764855119272148, 0.03559830009599203, -0.18475872039322883, -0.12173720800687801, 0.004675569979965126, 0.4148879579638373, -0.3683153861393667, -0.20460811100759838, 0.11020119263701243, -0.23810614387453724, -0.15814864593526118, 0.1744583386844917, -0.1722687789978944... |
709.1063 | Lie groups of bundle automorphisms and their extensions | We describe natural abelian extensions of the Lie algebra $\aut(P)$ of
infinitesimal automorphisms of a principal bundle over a compact manifold $M$
and discuss their integrability to corresponding Lie group extensions. Already
the case of a trivial bundle $P = M \times K$ is quite interesting. In this
case, we show ... | math.DG | we describe natural abelian extensions of the lie algebra autp of infinitesimal automorphisms of a principal bundle over a compact manifold m and discuss their integrability to corresponding lie group extensions already the case of a trivial bundle p m times k is quite interesting in this case we show that essentially ... | [['we', 'describe', 'natural', 'abelian', 'extensions', 'of', 'the', 'lie', 'algebra', 'autp', 'of', 'infinitesimal', 'automorphisms', 'of', 'a', 'principal', 'bundle', 'over', 'a', 'compact', 'manifold', 'm', 'and', 'discuss', 'their', 'integrability', 'to', 'corresponding', 'lie', 'group', 'extensions', 'already', 't... | [-0.1788966410793364, 0.07755662284549684, -0.07029243293576516, 0.0818634484294587, -0.13590566268226562, -0.12100474633491383, -0.012033675575199035, 0.3824763387011794, -0.31913470623011775, -0.1992746802834937, 0.14371306480159265, -0.2166020046059902, -0.17022528929653793, 0.20667478122318594, -0.11372184801416901... |
709.1064 | On convexity of the frequency response of a stable polynomial | In the complex plane, the frequency response of a univariate polynomial is
the set of values taken by the polynomial when evaluated along the imaginary
axis. This is an algebraic curve partitioning the plane into several connected
components. In this note it is shown that the component including the origin is
exactly... | math.OC math.AG | in the complex plane the frequency response of a univariate polynomial is the set of values taken by the polynomial when evaluated along the imaginary axis this is an algebraic curve partitioning the plane into several connected components in this note it is shown that the component including the origin is exactly repr... | [['in', 'the', 'complex', 'plane', 'the', 'frequency', 'response', 'of', 'a', 'univariate', 'polynomial', 'is', 'the', 'set', 'of', 'values', 'taken', 'by', 'the', 'polynomial', 'when', 'evaluated', 'along', 'the', 'imaginary', 'axis', 'this', 'is', 'an', 'algebraic', 'curve', 'partitioning', 'the', 'plane', 'into', 's... | [-0.16683210758945916, 0.09569598196619401, -0.09089922669113844, 0.010451718740007998, -0.09126791630738548, -0.09399995260702615, -0.045225660038458834, 0.34044201822056397, -0.3435212267296655, -0.1717820528035911, 0.13157224122513472, -0.26764899415762294, -0.18205848124555565, 0.21339667183891325, -0.0062266979729... |
709.1065 | Broadband dielectric response of CaCu3Ti4O12: From dc to the electronic
transition regime | We report on phonon properties and electronic transitions in CaCu3Ti4O12, a
material which reveals a colossal dielectric constant at room temperature
without any ferroelectric transition. The results of far- and mid-infrared
measurements are compared to those obtained by broadband dielectric and
millimeter-wave spect... | cond-mat.str-el cond-mat.mtrl-sci | we report on phonon properties and electronic transitions in cacu3ti4o12 a material which reveals a colossal dielectric constant at room temperature without any ferroelectric transition the results of far and midinfrared measurements are compared to those obtained by broadband dielectric and millimeterwave spectroscopy... | [['we', 'report', 'on', 'phonon', 'properties', 'and', 'electronic', 'transitions', 'in', 'cacu3ti4o12', 'a', 'material', 'which', 'reveals', 'a', 'colossal', 'dielectric', 'constant', 'at', 'room', 'temperature', 'without', 'any', 'ferroelectric', 'transition', 'the', 'results', 'of', 'far', 'and', 'midinfrared', 'mea... | [-0.11936683580487235, 0.2210977723454042, 0.025445670874822617, -0.002858482613061954, -0.032321705675453165, -0.15701693159228722, 0.14195440791497407, 0.4797594797730978, -0.20463850251897903, -0.31354924218196956, 0.007137468544117708, -0.37647883258094744, -0.08907378911161297, 0.17184491476967065, 0.0796035522029... |
709.1066 | Direct measurements of the effects of salt and surfactant on interaction
forces between colloidal particles at water-oil interfaces | The forces between colloidal particles at a decane-water interface, in the
presence of low concentrations of a monovalent salt (NaCl) and of the
surfactant sodium dodecylsulfate (SDS) in the aqueous subphase, have been
studied using laser tweezers. In the absence of electrolyte and surfactant,
particle interactions e... | cond-mat.soft | the forces between colloidal particles at a decanewater interface in the presence of low concentrations of a monovalent salt nacl and of the surfactant sodium dodecylsulfate sds in the aqueous subphase have been studied using laser tweezers in the absence of electrolyte and surfactant particle interactions exhibit a lo... | [['the', 'forces', 'between', 'colloidal', 'particles', 'at', 'a', 'decanewater', 'interface', 'in', 'the', 'presence', 'of', 'low', 'concentrations', 'of', 'a', 'monovalent', 'salt', 'nacl', 'and', 'of', 'the', 'surfactant', 'sodium', 'dodecylsulfate', 'sds', 'in', 'the', 'aqueous', 'subphase', 'have', 'been', 'studie... | [-0.1266635231495379, 0.17517961732599824, -0.07061533545158764, 0.012173826767111871, 0.027171005877329315, -0.1343977352822239, 0.02067965777303548, 0.3520015342676259, -0.22988385370476766, -0.33637622366151576, 0.0086604247763852, -0.32022361189444015, -0.09379337798962567, 0.11168966545436056, 0.017773841792083484... |
709.1067 | Wrong Priors | All priors are not created equal. There are right and there are wrong priors.
That is the main conclusion of this contribution. I use, a cooked-up example
designed to create drama, and a typical textbook example to show the
pervasiveness of wrong priors in standard statistical practice.
| physics.data-an | all priors are not created equal there are right and there are wrong priors that is the main conclusion of this contribution i use a cookedup example designed to create drama and a typical textbook example to show the pervasiveness of wrong priors in standard statistical practice | [['all', 'priors', 'are', 'not', 'created', 'equal', 'there', 'are', 'right', 'and', 'there', 'are', 'wrong', 'priors', 'that', 'is', 'the', 'main', 'conclusion', 'of', 'this', 'contribution', 'i', 'use', 'a', 'cookedup', 'example', 'designed', 'to', 'create', 'drama', 'and', 'a', 'typical', 'textbook', 'example', 'to'... | [-0.02395846354446131, 0.0761972743531932, -0.0883235355798641, 0.15889379055158276, -0.12977946078931185, -0.18263281288597247, 0.016458428181383922, 0.42550869107894274, -0.24580864405826383, -0.3097990838729817, 0.11777449525518181, -0.2980080437036636, -0.15027326033653124, 0.17598754518827342, -0.12863158724149285... |
709.1068 | Semilocal convergence of two iterative methods for simultaneous
computation of polynomial zeros | In this paper we study some iterative methods for simultaneous approximation
of polynomial zeros. We give new semilocal convergence theorems with error
bounds for Ehrlich's and Nourein's iterations. Our theorems generalize and
improve recent results of Zheng and Huang [J. Comput. Math. 18 (2000),
113--122], Petkovi\'... | math.NA | in this paper we study some iterative methods for simultaneous approximation of polynomial zeros we give new semilocal convergence theorems with error bounds for ehrlichs and noureins iterations our theorems generalize and improve recent results of zheng and huang j comput math 18 2000 113122 petkovic and herceg j comp... | [['in', 'this', 'paper', 'we', 'study', 'some', 'iterative', 'methods', 'for', 'simultaneous', 'approximation', 'of', 'polynomial', 'zeros', 'we', 'give', 'new', 'semilocal', 'convergence', 'theorems', 'with', 'error', 'bounds', 'for', 'ehrlichs', 'and', 'noureins', 'iterations', 'our', 'theorems', 'generalize', 'and',... | [-0.027482637721631262, -0.04470912729933237, -0.06080986016442896, -0.01059278419739308, -0.09031324551647736, -0.1108796404409481, 0.12016969276818498, 0.31602270407084787, -0.14605434020308572, -0.36541992709195864, 0.10928501444221991, -0.2359843404394471, -0.18635439893437755, 0.18658998683289005, -0.2018653934161... |
709.1069 | A Compromise between Neutrino Masses and Collider Signatures in the
Type-II Seesaw Model | A natural extension of the standard $SU(2)_{\rm L} \times U(1)_{\rm Y}$ gauge
model to accommodate massive neutrinos is to introduce one Higgs triplet and
three right-handed Majorana neutrinos, leading to a $6\times 6$ neutrino mass
matrix which contains three $3\times 3$ sub-matrices $M_{\rm L}$, $M_{\rm D}$
and $M_... | hep-ph hep-ex | a natural extension of the standard su2_rm l times u1_rm y gauge model to accommodate massive neutrinos is to introduce one higgs triplet and three righthanded majorana neutrinos leading to a 6times 6 neutrino mass matrix which contains three 3times 3 submatrices m_rm l m_rm d and m_rm r we show that three light majora... | [['a', 'natural', 'extension', 'of', 'the', 'standard', 'su2_rm', 'l', 'times', 'u1_rm', 'y', 'gauge', 'model', 'to', 'accommodate', 'massive', 'neutrinos', 'is', 'to', 'introduce', 'one', 'higgs', 'triplet', 'and', 'three', 'righthanded', 'majorana', 'neutrinos', 'leading', 'to', 'a', '6times', '6', 'neutrino', 'mass'... | [-0.13768140014683553, 0.3600475549645597, 0.08235324972473015, 0.22332279093259583, -0.06812901788011745, -0.27513454573151347, 0.028189308792611376, 0.29704966450420517, -0.17747220708729905, -0.3133607688963551, 0.0005656278894834772, -0.3121437205657087, -0.00015518685621726845, 0.10761627755063172, 0.0555732210670... |
709.107 | A Synthetical Weights' Dynamic Mechanism for Weighted Networks | We propose a synthetical weights' dynamic mechanism for weighted networks
which takes into account the influences of strengths of nodes, weights of links
and incoming new vertices. Strength/Weight preferential strategies are used in
these weights' dynamic mechanisms, which depict the evolving strategies of many
real-... | physics.soc-ph | we propose a synthetical weights dynamic mechanism for weighted networks which takes into account the influences of strengths of nodes weights of links and incoming new vertices strengthweight preferential strategies are used in these weights dynamic mechanisms which depict the evolving strategies of many realworld net... | [['we', 'propose', 'a', 'synthetical', 'weights', 'dynamic', 'mechanism', 'for', 'weighted', 'networks', 'which', 'takes', 'into', 'account', 'the', 'influences', 'of', 'strengths', 'of', 'nodes', 'weights', 'of', 'links', 'and', 'incoming', 'new', 'vertices', 'strengthweight', 'preferential', 'strategies', 'are', 'use... | [-0.1556048813663357, 0.1327119272334122, -0.055701136646742845, 0.05850548123942693, -0.10755861137449675, -0.21682953140162656, 0.06168121193840572, 0.47562643094400386, -0.33070757285386854, -0.30325320008647655, -0.0020669713787388353, -0.25066636154114935, -0.21854013619960938, 0.10462269334913751, 0.0110419079562... |
709.1071 | Maximum Entropy Principle for the Microcanonical Ensemble | We derive the microcanonical ensemble from the Maximum Entropy Principle
(MEP) using the phase space volume entropy of P. Hertz. Maximizing this entropy
with respect to the probability distribution with the constraints of
normalization and average energy, we obtain the condition of constant energy.
This approach is c... | cond-mat.stat-mech | we derive the microcanonical ensemble from the maximum entropy principle mep using the phase space volume entropy of p hertz maximizing this entropy with respect to the probability distribution with the constraints of normalization and average energy we obtain the condition of constant energy this approach is complemen... | [['we', 'derive', 'the', 'microcanonical', 'ensemble', 'from', 'the', 'maximum', 'entropy', 'principle', 'mep', 'using', 'the', 'phase', 'space', 'volume', 'entropy', 'of', 'p', 'hertz', 'maximizing', 'this', 'entropy', 'with', 'respect', 'to', 'the', 'probability', 'distribution', 'with', 'the', 'constraints', 'of', '... | [-0.06402568858558018, 0.12112679086797136, -0.14454287153938294, 0.07034803027483194, 0.01203260994761398, -0.10451970716913868, 0.13336986653034968, 0.2774486534640585, -0.2671451184923123, -0.3012372861764896, 0.03530676163408268, -0.30346780467631396, -0.05152999977336118, 0.12261328563449513, -0.05444140805813827,... |
709.1072 | Total angular momentum from Dirac eigenspinors | The eigenvalue problem for Dirac operators, constructed from two connections
on the spinor bundle over closed spacelike 2-surfaces, is investigated. A class
of divergence free vector fields, built from the eigenspinors, are found,
which, for the lowest eigenvalue, reproduce the rotation Killing vectors of
metric sphe... | gr-qc | the eigenvalue problem for dirac operators constructed from two connections on the spinor bundle over closed spacelike 2surfaces is investigated a class of divergence free vector fields built from the eigenspinors are found which for the lowest eigenvalue reproduce the rotation killing vectors of metric spheres and pro... | [['the', 'eigenvalue', 'problem', 'for', 'dirac', 'operators', 'constructed', 'from', 'two', 'connections', 'on', 'the', 'spinor', 'bundle', 'over', 'closed', 'spacelike', '2surfaces', 'is', 'investigated', 'a', 'class', 'of', 'divergence', 'free', 'vector', 'fields', 'built', 'from', 'the', 'eigenspinors', 'are', 'fou... | [-0.168001395650208, 0.14935991958000067, -0.06144905123257577, 0.13351799033445805, -0.12667278588203845, -0.13597369320617725, -0.03675744458186356, 0.3341194275728982, -0.23900719361868922, -0.2192498689395084, 0.04644092257843691, -0.26114965768324006, -0.08411989833272093, 0.15999875096322008, 0.005194423033507785... |
709.1073 | On the Metallicity-Color Relations and Bimodal Color Distributions in
Extragalactic Globular Cluster Systems | We perform a series of numerical experiments to study how the nonlinear
metallicity--color relations predicted by different stellar population models
affect the color distributions observed in extragalactic globular cluster
systems. % We present simulations in the $UBVRIJHK$ bandpasses based on five
different sets of... | astro-ph | we perform a series of numerical experiments to study how the nonlinear metallicitycolor relations predicted by different stellar population models affect the color distributions observed in extragalactic globular cluster systems we present simulations in the ubvrijhk bandpasses based on five different sets of simple s... | [['we', 'perform', 'a', 'series', 'of', 'numerical', 'experiments', 'to', 'study', 'how', 'the', 'nonlinear', 'metallicitycolor', 'relations', 'predicted', 'by', 'different', 'stellar', 'population', 'models', 'affect', 'the', 'color', 'distributions', 'observed', 'in', 'extragalactic', 'globular', 'cluster', 'systems'... | [-0.007778218599972639, 0.0800121119427202, -0.1372711081207197, 0.15873986581853405, -0.06180216314490227, -0.09767651198840237, 0.03806639734511189, 0.4760248177151948, -0.20620663803230155, -0.35887674554493926, 0.030323567512609503, -0.26884337754192994, -0.09450646628094041, 0.1736862828337493, -0.0943970290027598... |
709.1074 | Johnson Type Bounds on Constant Dimension Codes | Very recently, an operator channel was defined by Koetter and Kschischang
when they studied random network coding. They also introduced constant
dimension codes and demonstrated that these codes can be employed to correct
errors and/or erasures over the operator channel. Constant dimension codes are
equivalent to the... | cs.IT math.IT | very recently an operator channel was defined by koetter and kschischang when they studied random network coding they also introduced constant dimension codes and demonstrated that these codes can be employed to correct errors andor erasures over the operator channel constant dimension codes are equivalent to the socal... | [['very', 'recently', 'an', 'operator', 'channel', 'was', 'defined', 'by', 'koetter', 'and', 'kschischang', 'when', 'they', 'studied', 'random', 'network', 'coding', 'they', 'also', 'introduced', 'constant', 'dimension', 'codes', 'and', 'demonstrated', 'that', 'these', 'codes', 'can', 'be', 'employed', 'to', 'correct',... | [-0.17956085484746295, 0.10570911145877976, -0.0020412388543364097, 0.08754515157444002, -0.02625020038753611, -0.3134945924422401, 0.07700171614811396, 0.3564574066492403, -0.29876836032629517, -0.26321299911524526, 0.14465658326541855, -0.23483109128221505, -0.201983396281014, 0.186787412988959, -0.1475306733217136, ... |
709.1075 | Techniques for the calculation of electroweak radiative corrections at
the one-loop level and results for W-physics at LEP200 | We review the techniques necessary for the calculation of virtual electroweak
and soft photonic corrections at the one-loop level. In particular we describe
renormalization, calculation of one-loop integrals and evaluation of one-loop
Feynman amplitudes. We summarize many explicit results of general relevance. We
giv... | hep-ph | we review the techniques necessary for the calculation of virtual electroweak and soft photonic corrections at the oneloop level in particular we describe renormalization calculation of oneloop integrals and evaluation of oneloop feynman amplitudes we summarize many explicit results of general relevance we give the fey... | [['we', 'review', 'the', 'techniques', 'necessary', 'for', 'the', 'calculation', 'of', 'virtual', 'electroweak', 'and', 'soft', 'photonic', 'corrections', 'at', 'the', 'oneloop', 'level', 'in', 'particular', 'we', 'describe', 'renormalization', 'calculation', 'of', 'oneloop', 'integrals', 'and', 'evaluation', 'of', 'on... | [-0.11385344076988986, 0.15861375954141294, -0.05745777240081225, 0.14878207502770238, -0.06415775754139759, -0.0643273908237461, 0.07107119885768043, 0.3631732860463671, -0.1726030205070856, -0.25163252954371274, 0.045964927348541094, -0.3051154892425984, -0.11835341452097055, 0.17526274032497896, 0.08104188159632031,... |
709.1076 | Brane backreactions and the Fischler-Susskind mechanism in conformal
field theory | The backreaction of D-branes on closed string moduli is studied in perturbed
conformal field theory. To this end we analyse the divergences in the modular
integral of the annulus diagram. By the Fischler-Susskind mechanism, these
divergences lead to additional terms in the bulk renormalisation group
equations. We der... | hep-th | the backreaction of dbranes on closed string moduli is studied in perturbed conformal field theory to this end we analyse the divergences in the modular integral of the annulus diagram by the fischlersusskind mechanism these divergences lead to additional terms in the bulk renormalisation group equations we derive expl... | [['the', 'backreaction', 'of', 'dbranes', 'on', 'closed', 'string', 'moduli', 'is', 'studied', 'in', 'perturbed', 'conformal', 'field', 'theory', 'to', 'this', 'end', 'we', 'analyse', 'the', 'divergences', 'in', 'the', 'modular', 'integral', 'of', 'the', 'annulus', 'diagram', 'by', 'the', 'fischlersusskind', 'mechanism... | [-0.20355928823540825, 0.11757061311273255, -0.14731801438914693, 0.13151162024587393, -0.09065404488448647, -0.07344090369651499, 0.00425058352065853, 0.32624841732499393, -0.2401886801606557, -0.2815538751150387, 0.08321075912807947, -0.2591889053515658, -0.17088797460040211, 0.14013181431421443, -0.09550607846914858... |
709.1077 | Growth of Subharmonic Functions | In this course of lectures we give an account of the growth theory of
subharmonic functions, which is directed towards its applications to entire
functions of one and several complex variables.
| math.CV math.DS | in this course of lectures we give an account of the growth theory of subharmonic functions which is directed towards its applications to entire functions of one and several complex variables | [['in', 'this', 'course', 'of', 'lectures', 'we', 'give', 'an', 'account', 'of', 'the', 'growth', 'theory', 'of', 'subharmonic', 'functions', 'which', 'is', 'directed', 'towards', 'its', 'applications', 'to', 'entire', 'functions', 'of', 'one', 'and', 'several', 'complex', 'variables']] | [-0.13113997935227328, 0.12161402724685162, -0.12187865093320367, 0.05275819991384783, -0.08528235266285558, -0.04451797204092145, -0.016531340285925376, 0.3269154595721874, -0.2764157590366179, -0.23349191338544892, 0.13119753915441013, -0.2227035950749151, -0.1908062761949916, 0.2374594311019586, -0.04479234770576201... |
709.1078 | Angular momentum of isolated systems | Penrose's twistorial approach to the definition of angular momentum at null
infinity is developed so that angular momenta at different cuts can be
meaningfully compared. This is done by showing that the twistor spaces
associated with different cuts of scri can be identified as manifolds (but not
as vector spaces). Th... | gr-qc | penroses twistorial approach to the definition of angular momentum at null infinity is developed so that angular momenta at different cuts can be meaningfully compared this is done by showing that the twistor spaces associated with different cuts of scri can be identified as manifolds but not as vector spaces the resul... | [['penroses', 'twistorial', 'approach', 'to', 'the', 'definition', 'of', 'angular', 'momentum', 'at', 'null', 'infinity', 'is', 'developed', 'so', 'that', 'angular', 'momenta', 'at', 'different', 'cuts', 'can', 'be', 'meaningfully', 'compared', 'this', 'is', 'done', 'by', 'showing', 'that', 'the', 'twistor', 'spaces', ... | [-0.1022536950834383, 0.15392135425577028, -0.13251587144105426, 0.11540835202693464, -0.13752382493659154, -0.10302139668344151, -0.039786399173356544, 0.35752297499085833, -0.26364586448559424, -0.3039864913479194, 0.05044448889257549, -0.23704921060097997, -0.0866653007773945, 0.17442110147102166, -0.091464901889905... |
709.1079 | Two-scale homogenization of piezoelectric perforated structures | We are interested in the homogenization of elastic-electric coupling
equation, with rapidly oscillating coefficients, in periodically perforated
piezoelectric body. We justify the two first terms in the usual asymptotic
development of the problem solution. For the main convergence results of this
paper, we use the no... | math.NA math.CA | we are interested in the homogenization of elasticelectric coupling equation with rapidly oscillating coefficients in periodically perforated piezoelectric body we justify the two first terms in the usual asymptotic development of the problem solution for the main convergence results of this paper we use the notion of ... | [['we', 'are', 'interested', 'in', 'the', 'homogenization', 'of', 'elasticelectric', 'coupling', 'equation', 'with', 'rapidly', 'oscillating', 'coefficients', 'in', 'periodically', 'perforated', 'piezoelectric', 'body', 'we', 'justify', 'the', 'two', 'first', 'terms', 'in', 'the', 'usual', 'asymptotic', 'development', ... | [-0.12832099633912245, 0.043169189776693075, -0.08559731074741908, 0.009025024072754951, -0.053493509434961846, -0.06987954872948605, 0.01056482801851373, 0.3097226566945513, -0.31918179105490535, -0.20479076408914157, 0.15360728473890395, -0.30917306468334227, -0.17339017492208986, 0.18038182457288107, -0.095515088266... |
709.108 | On the Protocol Composition Logic PCL | A recent development in formal security protocol analysis is the Protocol
Composition Logic (PCL). We identify a number of problems with this logic as
well as with extensions of the logic, as defined in
[DDMP05,HSD+05,He05,Dat05,Der06,DDMR07]. The identified problems imply strong
restrictions on the scope of PCL, and... | cs.CR cs.LO | a recent development in formal security protocol analysis is the protocol composition logic pcl we identify a number of problems with this logic as well as with extensions of the logic as defined in ddmp05hsd05he05dat05der06ddmr07 the identified problems imply strong restrictions on the scope of pcl and imply that some... | [['a', 'recent', 'development', 'in', 'formal', 'security', 'protocol', 'analysis', 'is', 'the', 'protocol', 'composition', 'logic', 'pcl', 'we', 'identify', 'a', 'number', 'of', 'problems', 'with', 'this', 'logic', 'as', 'well', 'as', 'with', 'extensions', 'of', 'the', 'logic', 'as', 'defined', 'in', 'ddmp05hsd05he05d... | [-0.09334526812214076, 0.002946967334562057, -0.07278074681557514, 0.08818910983265252, -0.10856984843298592, -0.16551100195863763, 0.06112323873802214, 0.3572538081254508, -0.2794141327786083, -0.3160012767625016, 0.16416015817997726, -0.19934654532856233, -0.13070647053835863, 0.235218716587091, -0.13201401230715518,... |
709.1081 | Examining exotic structure of proton-rich nucleus $^{23}$Al | The longitudinal momentum distribution (P_{//}) of fragments after one-proton
removal from ^{23} Al and reaction cross sections (\sigma_R) for
^{23,24} Al on carbon target at 74A MeV have been measured. The ^{23,24} Al
ions were produced through projectile fragmentation of 135 A MeV ^{28} Si
primary beam using RIPS... | nucl-ex | the longitudinal momentum distribution p_ of fragments after oneproton removal from 23 al and reaction cross sections sigma_r for 2324 al on carbon target at 74a mev have been measured the 2324 al ions were produced through projectile fragmentation of 135 a mev 28 si primary beam using rips fragment separator at riken ... | [['the', 'longitudinal', 'momentum', 'distribution', 'p_', 'of', 'fragments', 'after', 'oneproton', 'removal', 'from', '23', 'al', 'and', 'reaction', 'cross', 'sections', 'sigma_r', 'for', '2324', 'al', 'on', 'carbon', 'target', 'at', '74a', 'mev', 'have', 'been', 'measured', 'the', '2324', 'al', 'ions', 'were', 'produ... | [-0.016071294075809418, 0.19633326312924812, -0.07420667105373771, 0.04511286711630722, 0.05494597551839737, -0.08582242290101325, 0.04749042508658022, 0.39854524306952954, -0.16991709324065596, -0.37951803363859654, -0.05032263565342873, -0.3467254474200308, 0.05591005569323897, 0.1804542731291925, 0.01723943833455753... |
709.1082 | Microcanonical phase transitions in small systems | When studying the thermodynamic properties of mesoscopic systems the most
appropriate microcanonical entropy is the volume entropy, i.e. the logarithm of
the volume of phase space enclosed by the hypersurface of constant energy. For
systems with broken ergodicity, the volume entropy has discontinuous jumps at
values ... | cond-mat.stat-mech | when studying the thermodynamic properties of mesoscopic systems the most appropriate microcanonical entropy is the volume entropy ie the logarithm of the volume of phase space enclosed by the hypersurface of constant energy for systems with broken ergodicity the volume entropy has discontinuous jumps at values of ener... | [['when', 'studying', 'the', 'thermodynamic', 'properties', 'of', 'mesoscopic', 'systems', 'the', 'most', 'appropriate', 'microcanonical', 'entropy', 'is', 'the', 'volume', 'entropy', 'ie', 'the', 'logarithm', 'of', 'the', 'volume', 'of', 'phase', 'space', 'enclosed', 'by', 'the', 'hypersurface', 'of', 'constant', 'ene... | [-0.15778504843090443, 0.19216256198334566, -0.08110372168309193, 0.056758237389619756, 0.023105869800387386, -0.14122775968590237, 0.06570761602253039, 0.28511645195094193, -0.26225152989463046, -0.25751498819110874, 0.06941960153462207, -0.32985744388536253, -0.0751672270806863, 0.15676640135364883, -0.01649192568723... |
709.1083 | Phase diagram of two-flavor quark matter: Gluonic phase at nonzero
temperature | The phase structure of neutral two-flavor quark matter at nonzero temperature
is studied. Our analysis is performed within the framework of a gauged
Nambu--Jona-Lasinio model and the mean-field approximation. We compute the free
energy of the gluonic phase (gluonic cylindrical phase II) in a self-consistent
manner an... | hep-ph | the phase structure of neutral twoflavor quark matter at nonzero temperature is studied our analysis is performed within the framework of a gauged nambujonalasinio model and the meanfield approximation we compute the free energy of the gluonic phase gluonic cylindrical phase ii in a selfconsistent manner and investigat... | [['the', 'phase', 'structure', 'of', 'neutral', 'twoflavor', 'quark', 'matter', 'at', 'nonzero', 'temperature', 'is', 'studied', 'our', 'analysis', 'is', 'performed', 'within', 'the', 'framework', 'of', 'a', 'gauged', 'nambujonalasinio', 'model', 'and', 'the', 'meanfield', 'approximation', 'we', 'compute', 'the', 'free... | [-0.16115839754724326, 0.2922245908528566, -0.0977578622946406, 0.051623861855991625, 0.009842292663148221, -0.05663246558431317, 0.11907429557074518, 0.3326024688122904, -0.1840769598041387, -0.240818070138202, 0.026918179396649495, -0.2579102232504417, -0.08464816694750506, -0.004543341786655433, 0.09193542742937365,... |
709.1084 | On some asymptotically flat manifolds with non maximal volume growth | Asymptotically flat manifolds with Euclidean volume growth are known to be
ALE. In this paper, we consider a class of asymptotically flat manifolds with
slower volume growth and prove that their asymptotic geometry is that of a
fibration over an ALE manifold. In particular, we show that gravitational
instantons with ... | math.DG | asymptotically flat manifolds with euclidean volume growth are known to be ale in this paper we consider a class of asymptotically flat manifolds with slower volume growth and prove that their asymptotic geometry is that of a fibration over an ale manifold in particular we show that gravitational instantons with cubic ... | [['asymptotically', 'flat', 'manifolds', 'with', 'euclidean', 'volume', 'growth', 'are', 'known', 'to', 'be', 'ale', 'in', 'this', 'paper', 'we', 'consider', 'a', 'class', 'of', 'asymptotically', 'flat', 'manifolds', 'with', 'slower', 'volume', 'growth', 'and', 'prove', 'that', 'their', 'asymptotic', 'geometry', 'is', ... | [-0.17061884186484597, 0.1224475173388121, -0.06395461362871256, 0.06322700360959227, -0.0710805167528716, -0.11423598842864686, -0.08313286178110336, 0.4127051328139549, -0.17902172126553276, -0.2082166109699756, 0.18056265702471136, -0.2661267043514685, -0.22558255378495562, 0.16620438119227235, -0.18414911302653225,... |
709.1085 | Linear response subordination to intermittent energy release in
off-equilibrium aging dynamics | The interpretation of experimental and numerical data describing
off-equilibrium aging dynamics crucially depends on the connection between
spontaneous and induced fluctuations. The hypothesis that linear response
fluctuations are statistically subordinated to irreversible outbursts of
energy, so-called quakes, leads... | cond-mat.stat-mech cond-mat.soft | the interpretation of experimental and numerical data describing offequilibrium aging dynamics crucially depends on the connection between spontaneous and induced fluctuations the hypothesis that linear response fluctuations are statistically subordinated to irreversible outbursts of energy socalled quakes leads to pre... | [['the', 'interpretation', 'of', 'experimental', 'and', 'numerical', 'data', 'describing', 'offequilibrium', 'aging', 'dynamics', 'crucially', 'depends', 'on', 'the', 'connection', 'between', 'spontaneous', 'and', 'induced', 'fluctuations', 'the', 'hypothesis', 'that', 'linear', 'response', 'fluctuations', 'are', 'stat... | [-0.11870823647368925, 0.16418105780126546, -0.1202791804683799, 0.10225862934980746, -0.06175846270295781, -0.08570862885636206, 0.03576712393787802, 0.3638262799531631, -0.2361690480995074, -0.3138881304536711, 0.05112226032536825, -0.2998388395107423, -0.14715562220841932, 0.2053410426667472, -0.024040850329693858, ... |
709.1086 | Flux saturation number of superconducting rings | The distributions of electrical current and magnetic field in a thin-film
superconductor ring is calculated by solving the London equation. The maximum
amount of flux trapped by the hole, the fluxoid saturation number, is obtained
by limiting the current density by the depairing current. The results are
compare it wi... | cond-mat.supr-con | the distributions of electrical current and magnetic field in a thinfilm superconductor ring is calculated by solving the london equation the maximum amount of flux trapped by the hole the fluxoid saturation number is obtained by limiting the current density by the depairing current the results are compare it with simi... | [['the', 'distributions', 'of', 'electrical', 'current', 'and', 'magnetic', 'field', 'in', 'a', 'thinfilm', 'superconductor', 'ring', 'is', 'calculated', 'by', 'solving', 'the', 'london', 'equation', 'the', 'maximum', 'amount', 'of', 'flux', 'trapped', 'by', 'the', 'hole', 'the', 'fluxoid', 'saturation', 'number', 'is'... | [-0.15601049771581868, 0.14339252679716422, 0.020312277352915402, 0.003451177499059225, -0.020095254616004175, -0.08404180976207805, 0.054875940339952974, 0.287989742938528, -0.19765051924087831, -0.33936797591766954, 0.04998880698535163, -0.3107662218070663, -0.031828096070516426, 0.2185317034528187, -0.04100952836153... |
709.1087 | Spin asymmetries in jet-hyperon production at LHC | We consider polarized Lambda hyperon production in proton-proton scattering,
p p -> (\Lambda^\uparrow jet) jet X, in the kinematical region of the LHC
experiments, in particular the ALICE experiment. We present a new Lambda
polarization observable that arises from the Sivers effect in the fragmentation
process. It ca... | hep-ph | we consider polarized lambda hyperon production in protonproton scattering p p lambdauparrow jet jet x in the kinematical region of the lhc experiments in particular the alice experiment we present a new lambda polarization observable that arises from the sivers effect in the fragmentation process it can be large even ... | [['we', 'consider', 'polarized', 'lambda', 'hyperon', 'production', 'in', 'protonproton', 'scattering', 'p', 'p', 'lambdauparrow', 'jet', 'jet', 'x', 'in', 'the', 'kinematical', 'region', 'of', 'the', 'lhc', 'experiments', 'in', 'particular', 'the', 'alice', 'experiment', 'we', 'present', 'a', 'new', 'lambda', 'polariz... | [-0.08931851599508107, 0.23265429868924994, -0.1821605564212544, 0.12987322993700087, -0.07969856892318071, -0.11161352746893426, -0.011880711247506845, 0.3667173639846009, -0.2844407486116832, -0.21754619749346832, -0.05023547801658981, -0.3008991007354616, 0.03639463506437637, 0.15737017870855494, 0.0748222612223676,... |
709.1088 | The Horn conjecture for compact selfadjoint operators | We determine the possible eigenvalues of compact selfadjoint operators
A,B,C... with the property that A=B+C+... When all these operators are
positive, the eigenvalues were known to be subject to certain inequalities
which extend Horn's inequalities from the finite-dimensional case when A=B+C.
We find the proper exte... | math.FA | we determine the possible eigenvalues of compact selfadjoint operators abc with the property that abc when all these operators are positive the eigenvalues were known to be subject to certain inequalities which extend horns inequalities from the finitedimensional case when abc we find the proper extension of the horn i... | [['we', 'determine', 'the', 'possible', 'eigenvalues', 'of', 'compact', 'selfadjoint', 'operators', 'abc', 'with', 'the', 'property', 'that', 'abc', 'when', 'all', 'these', 'operators', 'are', 'positive', 'the', 'eigenvalues', 'were', 'known', 'to', 'be', 'subject', 'to', 'certain', 'inequalities', 'which', 'extend', '... | [-0.10125492996303365, 0.08270333643537015, -0.03939394718501717, 0.08037466549896635, -0.11614535953151062, -0.1826813797838986, 0.012122628996148705, 0.3487470942735672, -0.2665008259064052, -0.22532275687903167, 0.15263525187037885, -0.29076290035387503, -0.15216383046470583, 0.21276569227688014, -0.0538040720741264... |
709.1089 | Universality of the diffusion wake in the gauge-string duality | As a particle moves through a fluid, it may generate a laminar wake behind
it. In the gauge-string duality, we show that such a diffusion wake is created
by a heavy quark moving through a thermal plasma and that it has a universal
strength when compared to the total drag force exerted on the quark by the
plasma. The ... | hep-th hep-ph nucl-th | as a particle moves through a fluid it may generate a laminar wake behind it in the gaugestring duality we show that such a diffusion wake is created by a heavy quark moving through a thermal plasma and that it has a universal strength when compared to the total drag force exerted on the quark by the plasma the univers... | [['as', 'a', 'particle', 'moves', 'through', 'a', 'fluid', 'it', 'may', 'generate', 'a', 'laminar', 'wake', 'behind', 'it', 'in', 'the', 'gaugestring', 'duality', 'we', 'show', 'that', 'such', 'a', 'diffusion', 'wake', 'is', 'created', 'by', 'a', 'heavy', 'quark', 'moving', 'through', 'a', 'thermal', 'plasma', 'and', '... | [-0.08298696425368952, 0.26296956726282683, -0.1685703790941055, 0.08897447542253804, -0.053058046554743325, -0.11897720173289328, -0.01997874208309534, 0.32700448305065233, -0.22406389594999784, -0.24245820518045388, 0.021793455833607575, -0.27960296423107234, -0.10422936256149228, 0.1606635509368474, -0.0059591556188... |
709.109 | Thermodynamic scaling of diffusion in supercooled Lennard-Jones liquids | The manner in which the intermolecular potential u(r) governs structural
relaxation in liquids is a long standing problem in condensed matter physics.
Herein we show that diffusion coefficients for simulated Lennard-Jones m-6
liquids (8<m<36) in normal and moderately supercooled states are a unique
function of the va... | cond-mat.stat-mech cond-mat.soft | the manner in which the intermolecular potential ur governs structural relaxation in liquids is a long standing problem in condensed matter physics herein we show that diffusion coefficients for simulated lennardjones m6 liquids 8m36 in normal and moderately supercooled states are a unique function of the variable rhog... | [['the', 'manner', 'in', 'which', 'the', 'intermolecular', 'potential', 'ur', 'governs', 'structural', 'relaxation', 'in', 'liquids', 'is', 'a', 'long', 'standing', 'problem', 'in', 'condensed', 'matter', 'physics', 'herein', 'we', 'show', 'that', 'diffusion', 'coefficients', 'for', 'simulated', 'lennardjones', 'm6', '... | [-0.13130732192475275, 0.1959574812493634, -0.12140922578435172, 0.036682271470507496, -0.002791512564084876, -0.15724175546190464, 7.902935156416075e-05, 0.3409170566729325, -0.30373821402078166, -0.2600481363433395, 0.040989062399032765, -0.30022566775590476, -0.15144046429115549, 0.1432157846752043, 0.01581958755531... |
709.1091 | Geometry of invariant domains in complex semi-simple Lie groups | We investigate the joint action of two real forms of a semi-simple complex
Lie group S by left and right multiplication. After analyzing the orbit
structure, we study the CR structure of closed orbits. The main results are an
explicit formula of the Levi form of closed orbits and the determination of the
Levi cone of... | math.CV | we investigate the joint action of two real forms of a semisimple complex lie group s by left and right multiplication after analyzing the orbit structure we study the cr structure of closed orbits the main results are an explicit formula of the levi form of closed orbits and the determination of the levi cone of gener... | [['we', 'investigate', 'the', 'joint', 'action', 'of', 'two', 'real', 'forms', 'of', 'a', 'semisimple', 'complex', 'lie', 'group', 's', 'by', 'left', 'and', 'right', 'multiplication', 'after', 'analyzing', 'the', 'orbit', 'structure', 'we', 'study', 'the', 'cr', 'structure', 'of', 'closed', 'orbits', 'the', 'main', 're... | [-0.2526549848295014, 0.057250005827805116, -0.07032325592311756, 0.03913970323095859, -0.09638186127052341, -0.07654845202341676, 0.00018736069143133265, 0.3590020721148647, -0.2906618589194308, -0.2020066819993228, 0.09697682987800209, -0.21108999981157134, -0.16994855082003582, 0.22535980012084186, -0.06531089749252... |
709.1092 | Persistence in a Random Bond Ising Model of Socio-Econo Dynamics | We study the persistence phenomenon in a socio-econo dynamics model using
computer simulations at a finite temperature on hypercubic lattices in
dimensions up to 5. The model includes a ` social\rq local field which contains
the magnetization at time $t$. The nearest neighbour quenched interactions are
drawn from a b... | q-fin.GN cond-mat.dis-nn physics.comp-ph physics.soc-ph q-fin.ST | we study the persistence phenomenon in a socioecono dynamics model using computer simulations at a finite temperature on hypercubic lattices in dimensions up to 5 the model includes a socialrq local field which contains the magnetization at time t the nearest neighbour quenched interactions are drawn from a binary dist... | [['we', 'study', 'the', 'persistence', 'phenomenon', 'in', 'a', 'socioecono', 'dynamics', 'model', 'using', 'computer', 'simulations', 'at', 'a', 'finite', 'temperature', 'on', 'hypercubic', 'lattices', 'in', 'dimensions', 'up', 'to', '5', 'the', 'model', 'includes', 'a', 'socialrq', 'local', 'field', 'which', 'contain... | [-0.11939038742263984, 0.12536762943298843, -0.09019561348286802, 0.08736627292727656, -0.007874550998181575, -0.10028575632471855, 0.08546385823888338, 0.3653353472555599, -0.24883359418375287, -0.2735253220834718, 0.09003910797054139, -0.2687944867464853, -0.14983604647270513, 0.17015503152955588, 0.02069855879581584... |
709.1093 | Holographic description of glueballs in a deformed AdS-dilaton
background | We investigate the mass spectra of scalar and vector glueballs in the
so-called bottom-up approach of the AdS/QCD correspondence. The holographic
model of QCD includes a static dilaton background field. We study the
constraints on the masses coming from perturbing the dilaton field and the
geometry of the bulk.
| hep-ph | we investigate the mass spectra of scalar and vector glueballs in the socalled bottomup approach of the adsqcd correspondence the holographic model of qcd includes a static dilaton background field we study the constraints on the masses coming from perturbing the dilaton field and the geometry of the bulk | [['we', 'investigate', 'the', 'mass', 'spectra', 'of', 'scalar', 'and', 'vector', 'glueballs', 'in', 'the', 'socalled', 'bottomup', 'approach', 'of', 'the', 'adsqcd', 'correspondence', 'the', 'holographic', 'model', 'of', 'qcd', 'includes', 'a', 'static', 'dilaton', 'background', 'field', 'we', 'study', 'the', 'constra... | [-0.12240204796651188, 0.14919432871309773, -0.11572501774193072, 0.09265176890113828, -0.0915489981749228, -0.08675213740682419, -0.005616793123891159, 0.30120167951099575, -0.1752906045211213, -0.261824768316951, 0.018320239118148327, -0.29013664606122336, -0.10142497103946398, 0.0824976034072817, 0.01547625601975893... |
709.1094 | Response Uniformity of the ATLAS Liquid Argon Electromagnetic
Calorimeter | The construction of the ATLAS electromagnetic liquid argon calorimeter
modules is completed and all the modules are assembled and inserted in the
cryostats. During the production period four barrel and three endcap modules
were exposed to test beams in order to assess their performance, ascertain the
production quali... | physics.ins-det | the construction of the atlas electromagnetic liquid argon calorimeter modules is completed and all the modules are assembled and inserted in the cryostats during the production period four barrel and three endcap modules were exposed to test beams in order to assess their performance ascertain the production quality a... | [['the', 'construction', 'of', 'the', 'atlas', 'electromagnetic', 'liquid', 'argon', 'calorimeter', 'modules', 'is', 'completed', 'and', 'all', 'the', 'modules', 'are', 'assembled', 'and', 'inserted', 'in', 'the', 'cryostats', 'during', 'the', 'production', 'period', 'four', 'barrel', 'and', 'three', 'endcap', 'modules... | [-0.07855143091352336, 0.10730876645137524, -0.023659663917175656, 0.030594432945282937, 0.0047500552007414655, -0.11874000468805175, -0.04871842362677101, 0.3747922149005121, -0.23860120763681059, -0.38742587317166655, 0.13485730313174105, -0.32178681505972456, 0.029249460500632894, 0.1683303948957473, -0.010096495517... |
709.1095 | HST/NICMOS Observations of Fast Infrared Flickering in the Microquasar
GRS 1915+105 | We report infrared observations of the microquasar GRS 1915+105 using the
NICMOS instrument of the Hubble Space Telescope during 9 visits in April-June
2003. During epochs of high X-ray/radio activity near the beginning and end of
this period, we find that the $1.87 $\um infrared flux is generally low ($\sim
2$ mJy) ... | astro-ph | we report infrared observations of the microquasar grs 1915105 using the nicmos instrument of the hubble space telescope during 9 visits in apriljune 2003 during epochs of high xrayradio activity near the beginning and end of this period we find that the 187 um infrared flux is generally low sim 2 mjy and relatively st... | [['we', 'report', 'infrared', 'observations', 'of', 'the', 'microquasar', 'grs', '1915105', 'using', 'the', 'nicmos', 'instrument', 'of', 'the', 'hubble', 'space', 'telescope', 'during', '9', 'visits', 'in', 'apriljune', '2003', 'during', 'epochs', 'of', 'high', 'xrayradio', 'activity', 'near', 'the', 'beginning', 'and... | [-0.09023640607732701, 0.15388922790511458, -0.07478243625538553, 0.10620181022378751, -0.05083055558031111, -0.06941091808375907, 0.06593703712152446, 0.43652371375916155, -0.17655910600106267, -0.3525317970839644, 0.13675441665286672, -0.27996159533915277, -0.07489104165551178, 0.22270973794844579, -0.067641544673731... |
709.1096 | Remarks on Our Understanding of Quantum Mechanics | Interpretations of key concepts, such as uncertainty relations, kinetic
energy, value of an observable, probability distributions, the projection or
collapse of a wave function postulate, and discrete versus continuous values,
that appear in several excellent textbooks on quantum mechanics are reviewed
and found not ... | quant-ph | interpretations of key concepts such as uncertainty relations kinetic energy value of an observable probability distributions the projection or collapse of a wave function postulate and discrete versus continuous values that appear in several excellent textbooks on quantum mechanics are reviewed and found not to be con... | [['interpretations', 'of', 'key', 'concepts', 'such', 'as', 'uncertainty', 'relations', 'kinetic', 'energy', 'value', 'of', 'an', 'observable', 'probability', 'distributions', 'the', 'projection', 'or', 'collapse', 'of', 'a', 'wave', 'function', 'postulate', 'and', 'discrete', 'versus', 'continuous', 'values', 'that', ... | [-0.06602803062936612, 0.14799116204461638, -0.1113894762118058, 0.1474329405624805, -0.05284014922277681, -0.10719744294303758, 0.013354296312298113, 0.349730953766868, -0.25347555846232794, -0.3230253082764303, 0.06423803640264568, -0.26506014013309676, -0.12669115277922488, 0.21713243917449668, -0.04338567792277398,... |
709.1097 | Characterizations of Sobolev inequalities on metric spaces | We present isocapacitary characterizations of Sobolev inequalities in very
general metric measure spaces.
| math.AP math.FA | we present isocapacitary characterizations of sobolev inequalities in very general metric measure spaces | [['we', 'present', 'isocapacitary', 'characterizations', 'of', 'sobolev', 'inequalities', 'in', 'very', 'general', 'metric', 'measure', 'spaces']] | [-0.1259931825244656, 0.024577573496991627, -0.08128156756552365, 0.27401770708652645, -0.08872732018622068, -0.17168476461217955, -0.01132232489852378, 0.4255716777764834, -0.28088698937342715, -0.16054603930276173, 0.11664621058242539, -0.30524985320292986, -0.12646593554661825, 0.23784254412524974, -0.25190504482732... |
709.1098 | I-V analysis of high-energy lithium-ion-irradiated Si and GaAs solar
cells | Space-grade Si and GaAs solar cells were irradiated with 15 and 40 MeV
lithium ions. Dark-IV analysis (with and without illumination) reveals
differences in the effects of such irradiation on the different cell types
| cond-mat.mtrl-sci nucl-ex physics.space-ph | spacegrade si and gaas solar cells were irradiated with 15 and 40 mev lithium ions darkiv analysis with and without illumination reveals differences in the effects of such irradiation on the different cell types | [['spacegrade', 'si', 'and', 'gaas', 'solar', 'cells', 'were', 'irradiated', 'with', '15', 'and', '40', 'mev', 'lithium', 'ions', 'darkiv', 'analysis', 'with', 'and', 'without', 'illumination', 'reveals', 'differences', 'in', 'the', 'effects', 'of', 'such', 'irradiation', 'on', 'the', 'different', 'cell', 'types']] | [0.007711195023148321, 0.22835270201903768, 0.10057652572868392, 0.001171636744402349, 0.09757181325676356, -0.1602298239195079, 0.09375966694642557, 0.4688944125082344, -0.1682460878510028, -0.48446184815838933, 0.031209146920446074, -0.38858720174175687, -0.040890105767175555, 0.2049962650053203, -0.08229923636827152... |
709.1099 | Multi-Sensor Fusion Method using Dynamic Bayesian Network for Precise
Vehicle Localization and Road Matching | This paper presents a multi-sensor fusion strategy for a novel road-matching
method designed to support real-time navigational features within advanced
driving-assistance systems. Managing multihypotheses is a useful strategy for
the road-matching problem. The multi-sensor fusion and multi-modal estimation
are realiz... | cs.AI cs.RO | this paper presents a multisensor fusion strategy for a novel roadmatching method designed to support realtime navigational features within advanced drivingassistance systems managing multihypotheses is a useful strategy for the roadmatching problem the multisensor fusion and multimodal estimation are realized using dy... | [['this', 'paper', 'presents', 'a', 'multisensor', 'fusion', 'strategy', 'for', 'a', 'novel', 'roadmatching', 'method', 'designed', 'to', 'support', 'realtime', 'navigational', 'features', 'within', 'advanced', 'drivingassistance', 'systems', 'managing', 'multihypotheses', 'is', 'a', 'useful', 'strategy', 'for', 'the',... | [-0.11795464024503922, -0.02653900284086477, -0.09610565892782891, 0.05269842006641233, -0.09017747172038071, -0.19762764287265278, 0.04769378842158605, 0.4011623077094555, -0.25787135562859476, -0.30058404172046316, 0.13759318342555263, -0.22725330011194778, -0.2183630855805758, 0.25114868371747434, -0.173354319675127... |
709.11 | Lagrangian Investigation of Auto-ignition in a Hydrogen Jet Flame in a
Vitiated Co-flow: Animations of Particle Trajectories in Composition Space
from PDF Model Calculations | PDF model calculations have been performed of the Cabra lifted hydrogen flame
in a vitiated co-flow. Particle trajectories are extracted from the Lagrangian
particle method used to solve the modeled PDF equation. The particle
trajectories in the mixture fraction-temperature plane reveal (at successive
downstream loca... | physics.flu-dyn | pdf model calculations have been performed of the cabra lifted hydrogen flame in a vitiated coflow particle trajectories are extracted from the lagrangian particle method used to solve the modeled pdf equation the particle trajectories in the mixture fractiontemperature plane reveal at successive downstream locations e... | [['pdf', 'model', 'calculations', 'have', 'been', 'performed', 'of', 'the', 'cabra', 'lifted', 'hydrogen', 'flame', 'in', 'a', 'vitiated', 'coflow', 'particle', 'trajectories', 'are', 'extracted', 'from', 'the', 'lagrangian', 'particle', 'method', 'used', 'to', 'solve', 'the', 'modeled', 'pdf', 'equation', 'the', 'part... | [-0.053307145185182606, 0.20451166543565438, -0.13383488155923667, 0.044178418815135956, 0.01832898505544813, -0.11377530900259199, -0.004060288254182074, 0.3345850482792332, -0.2923587039008402, -0.31938080286628073, 0.014435904710082693, -0.2610120643348841, -0.015503301421243154, 0.1360868070473413, 0.03586694371122... |
709.1101 | Surprises in the suddenly-expanded infinite well | I study the time-evolution of a particle prepared in the ground state of an
infinite well after the latter is suddenly expanded. It turns out that the
probability density $|\Psi(x, t)|^{2}$ shows up quite a surprising behaviour:
for definite times, {\it plateaux} appear for which $|\Psi(x, t)|^{2}$ is
constant on fin... | quant-ph cond-mat.other | i study the timeevolution of a particle prepared in the ground state of an infinite well after the latter is suddenly expanded it turns out that the probability density psix t2 shows up quite a surprising behaviour for definite times it plateaux appear for which psix t2 is constant on finite intervals for x elements of... | [['i', 'study', 'the', 'timeevolution', 'of', 'a', 'particle', 'prepared', 'in', 'the', 'ground', 'state', 'of', 'an', 'infinite', 'well', 'after', 'the', 'latter', 'is', 'suddenly', 'expanded', 'it', 'turns', 'out', 'that', 'the', 'probability', 'density', 'psix', 't2', 'shows', 'up', 'quite', 'a', 'surprising', 'beha... | [-0.1302780126020762, 0.1789141444996168, -0.12081760479506619, 0.06752209327392408, -0.017023837893944363, -0.12043728234872607, 0.03675233082331974, 0.3389326495311127, -0.23013427159267252, -0.249596629953333, 0.11429590868506709, -0.2762647221442954, -0.09056205336518329, 0.19220328862248953, 0.012207519224491613, ... |
709.1102 | Light fermion masses and chiral freedom | Within the scenario of chiral freedom we compute the quark and lepton masses
of the first two generations in terms of their chiral couplings. This allows us
to make a rough estimate of the size of the chiral couplings, narrowing down
the uncertainty in the chiron contribution to low energy observables, like the
anoma... | hep-ph | within the scenario of chiral freedom we compute the quark and lepton masses of the first two generations in terms of their chiral couplings this allows us to make a rough estimate of the size of the chiral couplings narrowing down the uncertainty in the chiron contribution to low energy observables like the anomalous ... | [['within', 'the', 'scenario', 'of', 'chiral', 'freedom', 'we', 'compute', 'the', 'quark', 'and', 'lepton', 'masses', 'of', 'the', 'first', 'two', 'generations', 'in', 'terms', 'of', 'their', 'chiral', 'couplings', 'this', 'allows', 'us', 'to', 'make', 'a', 'rough', 'estimate', 'of', 'the', 'size', 'of', 'the', 'chiral... | [-0.11545817525340961, 0.22343457129616767, -0.08280981075352965, 0.11589890003699857, -0.10006053549034569, -0.043864476112410046, 0.059672627091342106, 0.27381904769497806, -0.23594426604895255, -0.3434364559988563, 0.033031538215418085, -0.2943764811604454, -0.013944862426097434, 0.09811030257827578, 0.0232742512150... |
709.1103 | CR-Invariants and the Scattering Operator for Complex Manifolds with
Boundary | The purpose of this paper is to describe certain CR-covariant differential
operators on a strictly pseudoconvex CR manifold $M$ as residues of the
scattering operator for the Laplacian on an ambient complex K\"{a}hler manifold
$X$ having $M$ as a `CR-infinity.' We also characterize the CR $Q$-curvature in
terms of th... | math.AP math.CV | the purpose of this paper is to describe certain crcovariant differential operators on a strictly pseudoconvex cr manifold m as residues of the scattering operator for the laplacian on an ambient complex kahler manifold x having m as a crinfinity we also characterize the cr qcurvature in terms of the scattering operato... | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'describe', 'certain', 'crcovariant', 'differential', 'operators', 'on', 'a', 'strictly', 'pseudoconvex', 'cr', 'manifold', 'm', 'as', 'residues', 'of', 'the', 'scattering', 'operator', 'for', 'the', 'laplacian', 'on', 'an', 'ambient', 'complex', 'kahler', 'manifol... | [-0.1894986585314785, 0.07996998353046365, -0.057857411212864376, 0.05476470788319906, -0.08275517682500538, -0.12508565413189077, -0.03665706076925354, 0.3428120534512259, -0.21914525997071038, -0.20875226520001888, 0.09177649978747858, -0.34392799124831247, -0.19028955451878055, 0.15907192337770193, -0.12226680832959... |
709.1104 | Monolithic or hierarchical star formation? A new statistical analysis | We consider an analytic model of cosmic star formation which incorporates
supernova feedback, gas accretion and enriched outflows, reproducing the
history of cosmic star formation, metallicity, supernovae type II rates and the
fraction of baryons allocated to structures. We present a new statistical
treatment of the ... | astro-ph | we consider an analytic model of cosmic star formation which incorporates supernova feedback gas accretion and enriched outflows reproducing the history of cosmic star formation metallicity supernovae type ii rates and the fraction of baryons allocated to structures we present a new statistical treatment of the availab... | [['we', 'consider', 'an', 'analytic', 'model', 'of', 'cosmic', 'star', 'formation', 'which', 'incorporates', 'supernova', 'feedback', 'gas', 'accretion', 'and', 'enriched', 'outflows', 'reproducing', 'the', 'history', 'of', 'cosmic', 'star', 'formation', 'metallicity', 'supernovae', 'type', 'ii', 'rates', 'and', 'the',... | [-0.07832682007867608, 0.09786585674350227, -0.044043110696960694, 0.11313487862055893, -0.10062813130542368, -0.08263459445727761, 0.058244325326949946, 0.38256070506507733, -0.16956416160042445, -0.3430722159829339, 0.05579958633199776, -0.2333315282410158, -0.04273153168129192, 0.17637728468813135, -0.01433411727933... |
709.1105 | Classification of nonproduct states with maximum stabilizer dimension | Nonproduct n-qubit pure states with maximum dimensional stabilizer subgroups
of the group of local unitary transformations are precisely the generalized
n-qubit Greenberger-Horne-Zeilinger states and their local unitary equivalents,
for n greater than or equal to 3 but not equal to 4. We characterize the Lie
algebra ... | quant-ph | nonproduct nqubit pure states with maximum dimensional stabilizer subgroups of the group of local unitary transformations are precisely the generalized nqubit greenbergerhornezeilinger states and their local unitary equivalents for n greater than or equal to 3 but not equal to 4 we characterize the lie algebra of the s... | [['nonproduct', 'nqubit', 'pure', 'states', 'with', 'maximum', 'dimensional', 'stabilizer', 'subgroups', 'of', 'the', 'group', 'of', 'local', 'unitary', 'transformations', 'are', 'precisely', 'the', 'generalized', 'nqubit', 'greenbergerhornezeilinger', 'states', 'and', 'their', 'local', 'unitary', 'equivalents', 'for',... | [-0.1094321741860498, 0.20497517366652854, -0.04123533873554365, 0.06849930286522449, -0.009361875128506877, -0.22672218222883933, 0.03974704435210169, 0.3494125028359301, -0.2589894886025124, -0.24457461320806617, 0.09022353098578291, -0.24993418882612461, -0.050735863149855974, 0.14328429503021417, -0.088489012390283... |
709.1106 | Quantifying the Cosmic Web I: The large-scale halo
ellipticity-ellipticity and ellipticity-direction correlations | The formation of dark matter halos tends to occur anisotropically along the
filaments of the Cosmic Web, which induces both ellipticity-ellipticity (EE)
correlations between the shapes of halos, as well as ellipticity-direction (ED)
cross-correlations between halo shapes and the directions to neighboring halos.
We an... | astro-ph | the formation of dark matter halos tends to occur anisotropically along the filaments of the cosmic web which induces both ellipticityellipticity ee correlations between the shapes of halos as well as ellipticitydirection ed crosscorrelations between halo shapes and the directions to neighboring halos we analyze the ha... | [['the', 'formation', 'of', 'dark', 'matter', 'halos', 'tends', 'to', 'occur', 'anisotropically', 'along', 'the', 'filaments', 'of', 'the', 'cosmic', 'web', 'which', 'induces', 'both', 'ellipticityellipticity', 'ee', 'correlations', 'between', 'the', 'shapes', 'of', 'halos', 'as', 'well', 'as', 'ellipticitydirection', ... | [-0.10192498348610167, 0.12926505407186775, -0.06786723110400514, 0.16462827569348415, -0.03351600781356391, -0.08273865209629896, -0.019419683294521796, 0.38698826747511345, -0.22661737335709187, -0.35404726745862813, 0.004808114333667983, -0.38224485801428587, -0.013319201180423722, 0.1672183874577399, 0.132851143709... |
709.1107 | High-energy black hole production | Black hole production in high-energy collisions is briefly surveyed. Included
is a summary of recent developments and open problems relevant to collider
(LHC) production, as well as of some theoretical issues pointing towards
fundamental principles of quantum gravity.
| hep-ph gr-qc hep-th | black hole production in highenergy collisions is briefly surveyed included is a summary of recent developments and open problems relevant to collider lhc production as well as of some theoretical issues pointing towards fundamental principles of quantum gravity | [['black', 'hole', 'production', 'in', 'highenergy', 'collisions', 'is', 'briefly', 'surveyed', 'included', 'is', 'a', 'summary', 'of', 'recent', 'developments', 'and', 'open', 'problems', 'relevant', 'to', 'collider', 'lhc', 'production', 'as', 'well', 'as', 'of', 'some', 'theoretical', 'issues', 'pointing', 'towards'... | [-0.08903064504020701, 0.16764161652444223, -0.05389808554594454, 0.15985985720946796, -0.10500614575453494, -0.1628711568069105, -0.015230989163300316, 0.2922864720519436, -0.22378295189455935, -0.27253744045370504, 0.1254983341266205, -0.36897811999446467, -0.028970443472070128, 0.25403624439710065, -0.04362962757510... |
709.1108 | Spike synchronization of a chaotic array as a phase transition | We study how a coupled array of spiking chaotic systems synchronizes to an
external driving in a short time. Synchronization means spike separation at
adjacent sites much shorter than the average inter-spike interval; a local lack
of synchronization is called a defect. The system displays sudden spontaneous
defect di... | nlin.CD | we study how a coupled array of spiking chaotic systems synchronizes to an external driving in a short time synchronization means spike separation at adjacent sites much shorter than the average interspike interval a local lack of synchronization is called a defect the system displays sudden spontaneous defect disappea... | [['we', 'study', 'how', 'a', 'coupled', 'array', 'of', 'spiking', 'chaotic', 'systems', 'synchronizes', 'to', 'an', 'external', 'driving', 'in', 'a', 'short', 'time', 'synchronization', 'means', 'spike', 'separation', 'at', 'adjacent', 'sites', 'much', 'shorter', 'than', 'the', 'average', 'interspike', 'interval', 'a',... | [-0.25182233836037266, 0.16727018056839388, -0.03210876530001514, 0.06630705937168727, -0.017990561004153617, -0.18892470363497071, 0.07207752633883366, 0.3957947757460664, -0.2622602563699551, -0.2691030779279002, 0.0725674504375033, -0.2773472435041287, -0.14771074662311437, 0.15225927541728748, 0.012134727730337426,... |
709.1109 | Density Perturbations in the Universe from Massive Vector Fields | I discuss the possibility of using a massive vector field to generate the
density perturbation in the Universe. I find that a scale-invariant
superhorizon spectrum of vector field perturbations is possible to generate
during inflation. The associated curvature perturbation is imprinted onto the
Universe following the... | hep-th astro-ph hep-ph | i discuss the possibility of using a massive vector field to generate the density perturbation in the universe i find that a scaleinvariant superhorizon spectrum of vector field perturbations is possible to generate during inflation the associated curvature perturbation is imprinted onto the universe following the curv... | [['i', 'discuss', 'the', 'possibility', 'of', 'using', 'a', 'massive', 'vector', 'field', 'to', 'generate', 'the', 'density', 'perturbation', 'in', 'the', 'universe', 'i', 'find', 'that', 'a', 'scaleinvariant', 'superhorizon', 'spectrum', 'of', 'vector', 'field', 'perturbations', 'is', 'possible', 'to', 'generate', 'du... | [-0.21882601660292814, 0.23860492236310485, -0.11599892466876875, 0.11753839493030682, -0.13020243835361564, -0.1225077722714666, -0.1308313194415806, 0.30076093144495697, -0.2638963965890819, -0.21522982872556895, 0.04113390524563489, -0.2312940368291867, -0.1238899234244052, 0.08950591531089123, 0.035483143182800096,... |
709.111 | Deformation quantization for actions of the affine group | We define a universal deformation formula (UDF) for the actions of the affine
group on Frechet algebras. More precisely, starting with any associative
Frechet algebra which the affine group acts on in a strongly continuous and
isometrical manner, the UDF produces a family of topological associative
algebra structures... | math.QA math.OA | we define a universal deformation formula udf for the actions of the affine group on frechet algebras more precisely starting with any associative frechet algebra which the affine group acts on in a strongly continuous and isometrical manner the udf produces a family of topological associative algebra structures on the... | [['we', 'define', 'a', 'universal', 'deformation', 'formula', 'udf', 'for', 'the', 'actions', 'of', 'the', 'affine', 'group', 'on', 'frechet', 'algebras', 'more', 'precisely', 'starting', 'with', 'any', 'associative', 'frechet', 'algebra', 'which', 'the', 'affine', 'group', 'acts', 'on', 'in', 'a', 'strongly', 'continu... | [-0.14862215172983165, 0.10562055497060109, -0.1022875079098474, 0.024444126539854606, -0.15821811406945502, -0.07004982793253837, -0.0178651167441485, 0.38887978709773025, -0.3242830910258791, -0.1882050506662107, 0.1289615350418263, -0.20900775603407507, -0.19017440167445582, 0.22592349686813587, -0.13390213127238948... |
709.1111 | On the oscillations in Mercury's obliquity | One major objective of MESSENGER and BepiColombo spatial missions is to
accurately measure Mercury's rotation and its obliquity in order to obtain
constraints on internal structure of the planet. Which is the obliquity's
dynamical behavior deriving from a complete spin-orbit motion of Mercury
simultaneously integrate... | astro-ph | one major objective of messenger and bepicolombo spatial missions is to accurately measure mercurys rotation and its obliquity in order to obtain constraints on internal structure of the planet which is the obliquitys dynamical behavior deriving from a complete spinorbit motion of mercury simultaneously integrated with... | [['one', 'major', 'objective', 'of', 'messenger', 'and', 'bepicolombo', 'spatial', 'missions', 'is', 'to', 'accurately', 'measure', 'mercurys', 'rotation', 'and', 'its', 'obliquity', 'in', 'order', 'to', 'obtain', 'constraints', 'on', 'internal', 'structure', 'of', 'the', 'planet', 'which', 'is', 'the', 'obliquitys', '... | [-0.1477917562466391, 0.1173656587844171, -0.051225788947863206, 0.05755053692347616, -0.08232660270597035, -0.08019087604953493, 0.026805462119144745, 0.35741764175291296, -0.22193716317665332, -0.3484923203516497, 0.09093292997291262, -0.266802244200442, -0.0851494062987613, 0.23232915432603157, -0.062064176343006046... |
709.1112 | Rotating surface solitons | We introduce a novel type of surface waves that form at the edge of guiding
structures consisting of several concentric rings. Such surface waves rotate
steadily upon propagation and, in contrast to nonrotating waves, for high
rotation frequencies they do not exhibit power thresholds for their existence.
There exists... | physics.optics nlin.PS | we introduce a novel type of surface waves that form at the edge of guiding structures consisting of several concentric rings such surface waves rotate steadily upon propagation and in contrast to nonrotating waves for high rotation frequencies they do not exhibit power thresholds for their existence there exists an up... | [['we', 'introduce', 'a', 'novel', 'type', 'of', 'surface', 'waves', 'that', 'form', 'at', 'the', 'edge', 'of', 'guiding', 'structures', 'consisting', 'of', 'several', 'concentric', 'rings', 'such', 'surface', 'waves', 'rotate', 'steadily', 'upon', 'propagation', 'and', 'in', 'contrast', 'to', 'nonrotating', 'waves', '... | [-0.2112434448580542, 0.173770844265568, -0.04856539343018085, 0.006718811388256856, -0.08916288654371682, -0.07273511941699932, 0.024306795391668048, 0.38926855871816063, -0.24395748597776723, -0.2468047212007352, 0.10997166939745916, -0.24808085466631585, -0.11757585905595785, 0.2509553927504587, -0.01833250593820897... |
709.1113 | Redshift Distortions as a Probe of Gravity | Redshift distortion measurements from galaxy surveys include sensitivity to
the gravitational growth index distinguishing other theories from Einstein
gravity. This gravitational sensitivity is substantially free from uncertainty
in the effective equation of state of the cosmic expansion history. We also
illustrate t... | astro-ph | redshift distortion measurements from galaxy surveys include sensitivity to the gravitational growth index distinguishing other theories from einstein gravity this gravitational sensitivity is substantially free from uncertainty in the effective equation of state of the cosmic expansion history we also illustrate the b... | [['redshift', 'distortion', 'measurements', 'from', 'galaxy', 'surveys', 'include', 'sensitivity', 'to', 'the', 'gravitational', 'growth', 'index', 'distinguishing', 'other', 'theories', 'from', 'einstein', 'gravity', 'this', 'gravitational', 'sensitivity', 'is', 'substantially', 'free', 'from', 'uncertainty', 'in', 't... | [-0.055069855332635996, 0.09484836879071959, -0.13747236394862594, 0.10372398484890398, -0.1410990718490722, -0.032548311313516216, 7.397377569424479e-05, 0.3060579279584712, -0.25768214024668723, -0.3598347835961664, 0.07850950710851241, -0.3103672258572228, -0.09192941237339064, 0.19746074403979277, -0.01906984827170... |
709.1114 | H3+ in Diffuse Interstellar Clouds: a Tracer for the Cosmic-Ray
Ionization Rate | Using high resolution infrared spectroscopy we have surveyed twenty
sightlines for H3+ absorption. H3+ is detected in eight diffuse cloud
sightlines with column densities varying from 0.6x10^14 cm^-2 to 3.9x10^14
cm^-2. This brings to fourteen the total number of diffuse cloud sightlines
where H3+ has been detected. ... | astro-ph | using high resolution infrared spectroscopy we have surveyed twenty sightlines for h3 absorption h3 is detected in eight diffuse cloud sightlines with column densities varying from 06x1014 cm2 to 39x1014 cm2 this brings to fourteen the total number of diffuse cloud sightlines where h3 has been detected these detections... | [['using', 'high', 'resolution', 'infrared', 'spectroscopy', 'we', 'have', 'surveyed', 'twenty', 'sightlines', 'for', 'h3', 'absorption', 'h3', 'is', 'detected', 'in', 'eight', 'diffuse', 'cloud', 'sightlines', 'with', 'column', 'densities', 'varying', 'from', '06x1014', 'cm2', 'to', '39x1014', 'cm2', 'this', 'brings',... | [-0.06510059154033661, 0.1245029532603221, 0.027765720834955574, 0.029915491299703716, -0.010959932383149863, -0.04442933608032763, 0.030793691709637642, 0.43649391825683415, -0.17983990999875824, -0.3581878533549607, 0.058866892891936, -0.31954514083266256, 0.02965562879954814, 0.20141706095915288, -0.0012242608945816... |
709.1115 | Possible co-existence of local itinerancy and global localization in a
quasi-one-dimensional conductor | In the chain compound PrBa$_2$Cu$_4$O$_8$ localization appears simultaneously
with a dimensional crossover in the electronic ground state when the scattering
rate in the chains exceeds the hopping rate between the chains. Here we report
the discovery of a large, transverse magnetoresistance in PrBa$_2$Cu$_4$O$_8$
in ... | cond-mat.str-el | in the chain compound prba_2cu_4o_8 localization appears simultaneously with a dimensional crossover in the electronic ground state when the scattering rate in the chains exceeds the hopping rate between the chains here we report the discovery of a large transverse magnetoresistance in prba_2cu_4o_8 in the localized re... | [['in', 'the', 'chain', 'compound', 'prba_2cu_4o_8', 'localization', 'appears', 'simultaneously', 'with', 'a', 'dimensional', 'crossover', 'in', 'the', 'electronic', 'ground', 'state', 'when', 'the', 'scattering', 'rate', 'in', 'the', 'chains', 'exceeds', 'the', 'hopping', 'rate', 'between', 'the', 'chains', 'here', 'w... | [-0.22007562902260136, 0.25152944990240234, -0.045047402442372465, 0.020983155434285954, 0.019926098021134347, -0.14452719374245346, 0.06979152398764507, 0.3599598395166459, -0.29384910087887345, -0.20282825648591116, 0.020930841122149164, -0.2956796835430644, -0.1294988054395109, 0.15583628097960314, 0.058228496202062... |
709.1116 | Bifurcation of the ACT map | In this paper, we study the Arneodo-Coullet-Tresser map $
F(x,y,z)=(ax-b(y-z), bx+a(y-z), cx-dx^k+e z)$ where $a,b,c,d,e$ are real with
$bd\neq 0$ and $k>1$ is an integer. We obtain stability regions for fixed
points of $F$ and symmetric period-2 points while $c$ and $e$ vary as
parameters. Varying $a$ and $e$ as par... | math.DS | in this paper we study the arneodocoullettresser map fxyzaxbyz bxayz cxdxke z where abcde are real with bdneq 0 and k1 is an integer we obtain stability regions for fixed points of f and symmetric period2 points while c and e vary as parameters varying a and e as parameters we show that there is a hyperbolic invariant ... | [['in', 'this', 'paper', 'we', 'study', 'the', 'arneodocoullettresser', 'map', 'fxyzaxbyz', 'bxayz', 'cxdxke', 'z', 'where', 'abcde', 'are', 'real', 'with', 'bdneq', '0', 'and', 'k1', 'is', 'an', 'integer', 'we', 'obtain', 'stability', 'regions', 'for', 'fixed', 'points', 'of', 'f', 'and', 'symmetric', 'period2', 'poin... | [-0.2188919037404769, 0.12930170782948272, -0.051373342350828195, 0.019821914657511097, -0.03467141397358885, -0.1649007026659641, 0.06017051846830104, 0.3466029311969595, -0.2700901978455906, -0.23656970547552808, 0.09807034963104909, -0.30734048413885934, -0.17412344163573645, 0.19795466273943982, -0.0441479783215261... |
709.1117 | Theory of Electromotive Force Induced by Domain Wall Motion | We formulate a theory on the dynamics of conduction electrons in the presence
of moving magnetic textures in ferromagnetic materials. We show that the
variation of local magnetization in both space and time gives rise to
topological fields, which induce electromotive forces on the electrons.
Universal results are obt... | cond-mat.mtrl-sci cond-mat.mes-hall | we formulate a theory on the dynamics of conduction electrons in the presence of moving magnetic textures in ferromagnetic materials we show that the variation of local magnetization in both space and time gives rise to topological fields which induce electromotive forces on the electrons universal results are obtained... | [['we', 'formulate', 'a', 'theory', 'on', 'the', 'dynamics', 'of', 'conduction', 'electrons', 'in', 'the', 'presence', 'of', 'moving', 'magnetic', 'textures', 'in', 'ferromagnetic', 'materials', 'we', 'show', 'that', 'the', 'variation', 'of', 'local', 'magnetization', 'in', 'both', 'space', 'and', 'time', 'gives', 'ris... | [-0.20132792412739578, 0.20739892600811546, -0.0495691075331614, 0.038480299418862864, -0.07892601319317576, -0.05015894353295429, 0.024448038579504113, 0.4054539005826168, -0.2779286892261633, -0.3146728895887544, 0.026934824262073713, -0.2509032523118054, -0.10600170349301416, 0.23150757924193824, 0.00771228226986301... |
709.1118 | On the uniqueness of certain families of holomorphic disks | A Zoll metric is a Riemannian metric whose geodesics are all circles of equal
length. Via the twistor correspondence of LeBrun and Mason, a Zoll metric on
the 2 dimensional sphere corresponds to a family of holomorphic disks in CP_2
with boundary in a totally real submanifold P. In this paper, we show that for
a fixe... | math.DG math.GT | a zoll metric is a riemannian metric whose geodesics are all circles of equal length via the twistor correspondence of lebrun and mason a zoll metric on the 2 dimensional sphere corresponds to a family of holomorphic disks in cp_2 with boundary in a totally real submanifold p in this paper we show that for a fixed tota... | [['a', 'zoll', 'metric', 'is', 'a', 'riemannian', 'metric', 'whose', 'geodesics', 'are', 'all', 'circles', 'of', 'equal', 'length', 'via', 'the', 'twistor', 'correspondence', 'of', 'lebrun', 'and', 'mason', 'a', 'zoll', 'metric', 'on', 'the', '2', 'dimensional', 'sphere', 'corresponds', 'to', 'a', 'family', 'of', 'holo... | [-0.22434266197561015, 0.09092929791141716, -0.10372422036310339, 0.07231476388264899, -0.09703463016576463, -0.14315899183522118, -0.0306476146979916, 0.3113011062672042, -0.2309216283581624, -0.179828555652439, 0.09206594005897359, -0.3102529920735208, -0.22897647065345686, 0.17160257147248797, -0.1550294976502732, 0... |
709.1119 | Can rigidly rotating polytropes be sources of the Kerr metric? | We use a recent result by Cabezas et al. to build up an approximate solution
to the gravitational field created by a rigidly rotating polytrope. We solve
the linearized Einstein equations inside and outside the surface of zero
pressure including second-order corrections due to rotational motion to get an
asymptotical... | gr-qc | we use a recent result by cabezas et al to build up an approximate solution to the gravitational field created by a rigidly rotating polytrope we solve the linearized einstein equations inside and outside the surface of zero pressure including secondorder corrections due to rotational motion to get an asymptotically fl... | [['we', 'use', 'a', 'recent', 'result', 'by', 'cabezas', 'et', 'al', 'to', 'build', 'up', 'an', 'approximate', 'solution', 'to', 'the', 'gravitational', 'field', 'created', 'by', 'a', 'rigidly', 'rotating', 'polytrope', 'we', 'solve', 'the', 'linearized', 'einstein', 'equations', 'inside', 'and', 'outside', 'the', 'sur... | [-0.10282948258100078, 0.07394230298117084, -0.09200248114939313, 0.027731568637439825, -0.11439617273087303, -0.05911818337093185, 0.0034600023354869336, 0.3463628023940449, -0.2703967329095273, -0.2908766830259992, 0.07218859180162933, -0.2858544813740688, -0.12616333244174407, 0.14734242536360398, -0.076454947404272... |
709.112 | Quasi-one-dimensional polarized Fermi superfluids | We calculate the zero temperature phase diagram of a polarized two-component
Fermi gas in an array of weakly-coupled parallel one-dimensional (1D) 'tubes'
produced by a two-dimensional optical lattice. Increasing the lattice strength
drives a crossover from three-dimensional (3D) to 1D behavior, stabilizing the
Fulde... | cond-mat.other cond-mat.supr-con | we calculate the zero temperature phase diagram of a polarized twocomponent fermi gas in an array of weaklycoupled parallel onedimensional 1d tubes produced by a twodimensional optical lattice increasing the lattice strength drives a crossover from threedimensional 3d to 1d behavior stabilizing the fuldeferrelllarkinov... | [['we', 'calculate', 'the', 'zero', 'temperature', 'phase', 'diagram', 'of', 'a', 'polarized', 'twocomponent', 'fermi', 'gas', 'in', 'an', 'array', 'of', 'weaklycoupled', 'parallel', 'onedimensional', '1d', 'tubes', 'produced', 'by', 'a', 'twodimensional', 'optical', 'lattice', 'increasing', 'the', 'lattice', 'strength... | [-0.22999966684146783, 0.30123851477626223, -0.045765862055122855, 0.005765800546875901, -0.025541459261016412, -0.19311777270737696, 0.06257997384845194, 0.37322654019702567, -0.27440866925224494, -0.16608142064545642, 0.0072791698632169175, -0.2965679372152822, -0.10771152028305964, 0.14190709460526704, 0.08340882720... |
709.1121 | Integral cohomology of certain Picard modular surfaces | Let Gamma be a congruence subgroup of the Picard modular group of an
imaginary number field k, and let D be the associated symmetric space. We
describe a method to compute the integral cohomology of the locally symmetric
space Gamma\D. The method is implemented for the case k=Q(i) and k=Q(sqrt(-3)),
and the cohomolog... | math.NT | let gamma be a congruence subgroup of the picard modular group of an imaginary number field k and let d be the associated symmetric space we describe a method to compute the integral cohomology of the locally symmetric space gammad the method is implemented for the case kqi and kqsqrt3 and the cohomology is computed fo... | [['let', 'gamma', 'be', 'a', 'congruence', 'subgroup', 'of', 'the', 'picard', 'modular', 'group', 'of', 'an', 'imaginary', 'number', 'field', 'k', 'and', 'let', 'd', 'be', 'the', 'associated', 'symmetric', 'space', 'we', 'describe', 'a', 'method', 'to', 'compute', 'the', 'integral', 'cohomology', 'of', 'the', 'locally'... | [-0.204629715788981, 0.10034713038501274, -0.12729147095875493, 0.026503890483832823, -0.10893617758270481, -0.12654561615259996, -0.03545049924788804, 0.3388981058358632, -0.3455992602454177, -0.21959085756077848, 0.09067805255522374, -0.22918273076607748, -0.08395265485160053, 0.2325275518513959, -0.04709547363093187... |
709.1122 | Takai Duality for Crossed Products by Hilbert C*-bimodules | We discuss the crossed product by the dual action of the circle on the
crossed product of a C*-algebra A by a Hilbert C*-bimodule X. When X is an A-A
Morita equivalence bimodule, the double crossed product is shown to be Morita
equivalent to the C*-algebra A.
| math.OA | we discuss the crossed product by the dual action of the circle on the crossed product of a calgebra a by a hilbert cbimodule x when x is an aa morita equivalence bimodule the double crossed product is shown to be morita equivalent to the calgebra a | [['we', 'discuss', 'the', 'crossed', 'product', 'by', 'the', 'dual', 'action', 'of', 'the', 'circle', 'on', 'the', 'crossed', 'product', 'of', 'a', 'calgebra', 'a', 'by', 'a', 'hilbert', 'cbimodule', 'x', 'when', 'x', 'is', 'an', 'aa', 'morita', 'equivalence', 'bimodule', 'the', 'double', 'crossed', 'product', 'is', 's... | [-0.16807803836344007, 0.13819786770785714, -0.06220715693099067, 0.04282439411419662, -0.02776215572227189, -0.13945912450869033, -0.03998771916203042, 0.4523101588512989, -0.439526212342242, -0.09681184695875074, 0.09253830319032708, -0.22362565691087474, -0.06742022012142425, 0.1266955542080897, -0.1990192792120766,... |
709.1123 | Monte-Carlo simulation for fragment mass and kinetic energy
distributions from neutron induced fission of 235U | The mass and kinetic energy distribution of nuclear fragments from thermal
neutron induced fission of 235U have been studied using a Monte-Carlo
simulation. Besides reproducing the pronounced broadening on the standard
deviation of the final fragment kinetic energy distribution $\sigma_{e}(m)$
around the mass number ... | physics.comp-ph | the mass and kinetic energy distribution of nuclear fragments from thermal neutron induced fission of 235u have been studied using a montecarlo simulation besides reproducing the pronounced broadening on the standard deviation of the final fragment kinetic energy distribution sigma_em around the mass number m 109 our s... | [['the', 'mass', 'and', 'kinetic', 'energy', 'distribution', 'of', 'nuclear', 'fragments', 'from', 'thermal', 'neutron', 'induced', 'fission', 'of', '235u', 'have', 'been', 'studied', 'using', 'a', 'montecarlo', 'simulation', 'besides', 'reproducing', 'the', 'pronounced', 'broadening', 'on', 'the', 'standard', 'deviati... | [-0.050264579796030655, 0.16434153969658866, -0.09584860705780153, 0.11292828037283509, 0.014336500787320211, 0.012672862182035274, 0.005080995783593851, 0.3331875041914509, -0.20294869786546058, -0.4130315344358228, -0.0019135429960742746, -0.3086838249846832, 0.011793849029645477, 0.21893612275706584, 0.0155164512407... |
709.1124 | The Adiabatic Instability on Cosmology's Dark Side | We consider theories with a nontrivial coupling between the matter and dark
energy sectors. We describe a small scale instability that can occur in such
models when the coupling is strong compared to gravity, generalizing and
correcting earlier treatments. The instability is characterized by a negative
sound speed sq... | astro-ph | we consider theories with a nontrivial coupling between the matter and dark energy sectors we describe a small scale instability that can occur in such models when the coupling is strong compared to gravity generalizing and correcting earlier treatments the instability is characterized by a negative sound speed squared... | [['we', 'consider', 'theories', 'with', 'a', 'nontrivial', 'coupling', 'between', 'the', 'matter', 'and', 'dark', 'energy', 'sectors', 'we', 'describe', 'a', 'small', 'scale', 'instability', 'that', 'can', 'occur', 'in', 'such', 'models', 'when', 'the', 'coupling', 'is', 'strong', 'compared', 'to', 'gravity', 'generali... | [-0.13581317746013935, 0.13604878792220482, -0.09969406007079497, 0.1133139434736222, -0.1049757367266076, -0.17523712007816702, -0.006757730845406297, 0.3311896091238374, -0.2294258317865786, -0.34859800237630095, 0.07273315423656078, -0.24785360888622346, -0.11062631041166328, 0.21706003903278281, -0.0045708678973217... |
709.1125 | Pyroxenes: A new class of multiferroics | Pyroxenes with the general formula $AM$Si$_2$O$_6$ ($A$ = mono- or divalent
metal, $M$ = di- or trivalent metal) are shown to be a new class of
multiferroic materials. In particular, we have found so far that
NaFeSi$_2$O$_6$ becomes ferroelectric in a magnetically ordered state below
$\simeq 6$ K. Similarly, magnetic... | cond-mat.str-el | pyroxenes with the general formula amsi_2o_6 a mono or divalent metal m di or trivalent metal are shown to be a new class of multiferroic materials in particular we have found so far that nafesi_2o_6 becomes ferroelectric in a magnetically ordered state below simeq 6 k similarly magnetically driven ferroelectricity is ... | [['pyroxenes', 'with', 'the', 'general', 'formula', 'amsi_2o_6', 'a', 'mono', 'or', 'divalent', 'metal', 'm', 'di', 'or', 'trivalent', 'metal', 'are', 'shown', 'to', 'be', 'a', 'new', 'class', 'of', 'multiferroic', 'materials', 'in', 'particular', 'we', 'have', 'found', 'so', 'far', 'that', 'nafesi_2o_6', 'becomes', 'f... | [-0.16846152313825624, 0.23148944420980497, -0.007296610608893006, -0.014442223603347022, -0.07987837555303581, -0.1399999382758611, 0.09087967356470855, 0.42999720919485157, -0.253413385846407, -0.29929279338960585, 0.027825318388395796, -0.3098027709626446, -0.13850027701915488, 0.19518599477841667, 0.063590966520438... |
709.1126 | Some Monotonicity Properties of Gamma and $q$-gamma Functions | We prove some properties of completely monotonic functions and apply them to
obtain results on gamma and $q$-gamma functions.
| math.CA | we prove some properties of completely monotonic functions and apply them to obtain results on gamma and qgamma functions | [['we', 'prove', 'some', 'properties', 'of', 'completely', 'monotonic', 'functions', 'and', 'apply', 'them', 'to', 'obtain', 'results', 'on', 'gamma', 'and', 'qgamma', 'functions']] | [-0.05211379447657811, 0.06421843845103133, -0.13049947166521297, 0.13997509217772044, -0.08314785380896769, -0.14110025381179234, 0.09933701883021154, 0.4507390092078008, -0.32283029705286026, -0.14474422036130963, 0.0745250180510706, -0.3081673058730207, -0.19509287492225044, 0.2795430892392209, -0.011337972491195327... |
709.1127 | Spectral numbers in Floer theories | The chain complexes underlying Floer homology theories typically carry a
real-valued filtration, allowing one to associate to each Floer homology class
a spectral number defined as the infimum of the filtration levels of chains
representing that class. These spectral numbers have been studied extensively
in the case ... | math.SG math.AT | the chain complexes underlying floer homology theories typically carry a realvalued filtration allowing one to associate to each floer homology class a spectral number defined as the infimum of the filtration levels of chains representing that class these spectral numbers have been studied extensively in the case of ha... | [['the', 'chain', 'complexes', 'underlying', 'floer', 'homology', 'theories', 'typically', 'carry', 'a', 'realvalued', 'filtration', 'allowing', 'one', 'to', 'associate', 'to', 'each', 'floer', 'homology', 'class', 'a', 'spectral', 'number', 'defined', 'as', 'the', 'infimum', 'of', 'the', 'filtration', 'levels', 'of', ... | [-0.20988538567129625, 0.07935558527742335, -0.08657837980512552, 0.106403944316103, -0.0739783992150947, -0.15932595953231027, -0.045607708323821196, 0.31972865355800995, -0.3380012091226373, -0.249865322127764, 0.09088302132505009, -0.21028128559444031, -0.1360789123534059, 0.17017939986741068, -0.15226969398283885, ... |
709.1128 | Adiabatic instability in coupled dark energy-dark matter models | We consider theories in which there exists a nontrivial coupling between the
dark matter sector and the sector responsible for the acceleration of the
universe. Such theories can possess an adiabatic regime in which the
quintessence field always sits at the minimum of its effective potential, which
is set by the loca... | astro-ph | we consider theories in which there exists a nontrivial coupling between the dark matter sector and the sector responsible for the acceleration of the universe such theories can possess an adiabatic regime in which the quintessence field always sits at the minimum of its effective potential which is set by the local da... | [['we', 'consider', 'theories', 'in', 'which', 'there', 'exists', 'a', 'nontrivial', 'coupling', 'between', 'the', 'dark', 'matter', 'sector', 'and', 'the', 'sector', 'responsible', 'for', 'the', 'acceleration', 'of', 'the', 'universe', 'such', 'theories', 'can', 'possess', 'an', 'adiabatic', 'regime', 'in', 'which', '... | [-0.17901242796589686, 0.23335699154800738, -0.09236611339566149, 0.1244170613984346, -0.0635435894116089, -0.1258736369066581, -0.03265061321264952, 0.26530455777297024, -0.26804008265470813, -0.3180695157423971, 0.06291908204220353, -0.2192534756117091, -0.09468835081525478, 0.16408981067116615, 0.03069536488467626, ... |
709.1129 | Analysis on disconnected sets | Some aspects of analysis on disconnected sets are briefly discussed, more
along the lines of regions with infinitely many components than Cantor sets.
| math.CA | some aspects of analysis on disconnected sets are briefly discussed more along the lines of regions with infinitely many components than cantor sets | [['some', 'aspects', 'of', 'analysis', 'on', 'disconnected', 'sets', 'are', 'briefly', 'discussed', 'more', 'along', 'the', 'lines', 'of', 'regions', 'with', 'infinitely', 'many', 'components', 'than', 'cantor', 'sets']] | [-0.16779848355698682, 0.16523268106191055, -0.004592863599891248, 0.11910206111876862, 0.013238716951530912, -0.09769151072301295, 0.02546630637801212, 0.39116720110177994, -0.15874515635811765, -0.13541967903628296, 0.1757366866602198, -0.43770617534123035, -0.10785274470791868, 0.34192492529425933, -0.04441800980788... |
709.113 | Properties of charge density waves in La$_{2-x}$Ba$_{x}$CuO$_4$ | We report a comprehensive x-ray scattering study of charge density wave
(stripe) ordering in $\rm La_{2-x}Ba_xCuO_4 (x \approx 1/8)$, for which the
superconducting $T_c$ is greatly suppressed. Strong superlattice reflections
corresponding to static ordering of charge stripes were observed in this
sample. The structur... | cond-mat.supr-con cond-mat.str-el | we report a comprehensive xray scattering study of charge density wave stripe ordering in rm la_2xba_xcuo_4 x approx 18 for which the superconducting t_c is greatly suppressed strong superlattice reflections corresponding to static ordering of charge stripes were observed in this sample the structural modulation at the... | [['we', 'report', 'a', 'comprehensive', 'xray', 'scattering', 'study', 'of', 'charge', 'density', 'wave', 'stripe', 'ordering', 'in', 'rm', 'la_2xba_xcuo_4', 'x', 'approx', '18', 'for', 'which', 'the', 'superconducting', 't_c', 'is', 'greatly', 'suppressed', 'strong', 'superlattice', 'reflections', 'corresponding', 'to... | [-0.20551207373276925, 0.25793022156762124, 0.008880641321641403, 0.04861146350810816, -0.030642870104881925, -0.07127943722426298, 0.0907101708842994, 0.3787752048823737, -0.24392894669282403, -0.3246268525330739, 0.024101503766819854, -0.3557508804344132, -0.04487393371719908, 0.08856126179683257, 0.09197663353336463... |
709.1131 | New UltraCool and Halo White Dwarf Candidates in SDSS Stripe 82 | A 2.5 x 100 degree region along the celestial equator (Stripe 82) has been
imaged repeatedly from 1998 to 2005 by the Sloan Digital Sky Survey. A new
catalogue of ~4 million light-motion curves, together with over 200 derived
statistical quantities, for objects in Stripe 82 brighter than r~21.5 has been
constructed b... | astro-ph | a 25 x 100 degree region along the celestial equator stripe 82 has been imaged repeatedly from 1998 to 2005 by the sloan digital sky survey a new catalogue of 4 million lightmotion curves together with over 200 derived statistical quantities for objects in stripe 82 brighter than r215 has been constructed by combining ... | [['a', '25', 'x', '100', 'degree', 'region', 'along', 'the', 'celestial', 'equator', 'stripe', '82', 'has', 'been', 'imaged', 'repeatedly', 'from', '1998', 'to', '2005', 'by', 'the', 'sloan', 'digital', 'sky', 'survey', 'a', 'new', 'catalogue', 'of', '4', 'million', 'lightmotion', 'curves', 'together', 'with', 'over', ... | [-0.026099711683544715, 0.11231248753099907, -0.06367965728589674, 0.06374589804909192, -0.18749377117832985, -0.030631740645664495, 0.13340131882450362, 0.39739922737339284, -0.12919303247983363, -0.42810552396311813, 0.052331291271157834, -0.3851106180809438, -0.010685806589984767, 0.24028512240506755, -0.12335050699... |
709.1132 | Study of time lags in HETE-2 Gamma-Ray Bursts with redshift: search for
astrophysical effects and Quantum Gravity signature | The study of time lags between spikes in Gamma-Ray Bursts light curves in
different energy bands as a function of redshift may lead to the detection of
effects due to Quantum Gravity. We present an analysis of 15 Gamma-Ray Bursts
with measured redshift, detected by the HETE-2 mission between 2001 and 2006 in
order to... | astro-ph | the study of time lags between spikes in gammaray bursts light curves in different energy bands as a function of redshift may lead to the detection of effects due to quantum gravity we present an analysis of 15 gammaray bursts with measured redshift detected by the hete2 mission between 2001 and 2006 in order to measur... | [['the', 'study', 'of', 'time', 'lags', 'between', 'spikes', 'in', 'gammaray', 'bursts', 'light', 'curves', 'in', 'different', 'energy', 'bands', 'as', 'a', 'function', 'of', 'redshift', 'may', 'lead', 'to', 'the', 'detection', 'of', 'effects', 'due', 'to', 'quantum', 'gravity', 'we', 'present', 'an', 'analysis', 'of',... | [-0.10769878248825218, 0.14815999475015842, -0.10246919290952836, 0.14470502393581255, -0.07015999847543285, -0.09685639566283277, 0.08292145258923428, 0.3531049082733013, -0.19388938377078652, -0.382028801592462, 0.04169641598304169, -0.3119959493475714, -0.048962956576636345, 0.2325769289375537, -0.03142478810905507,... |
709.1133 | The Role of Solvent Fluctuations in Hydrophobic Assembly | We use a coarse grained solvent model to study the self assembly of two
nano-scale hydrophobic particles in water. We show how solvent degrees of
freedom are involved in the process. By using tools of transition path
sampling, we elucidate the reaction coordinates describing the assembly. In
accord with earlier expec... | cond-mat.stat-mech | we use a coarse grained solvent model to study the self assembly of two nanoscale hydrophobic particles in water we show how solvent degrees of freedom are involved in the process by using tools of transition path sampling we elucidate the reaction coordinates describing the assembly in accord with earlier expectations... | [['we', 'use', 'a', 'coarse', 'grained', 'solvent', 'model', 'to', 'study', 'the', 'self', 'assembly', 'of', 'two', 'nanoscale', 'hydrophobic', 'particles', 'in', 'water', 'we', 'show', 'how', 'solvent', 'degrees', 'of', 'freedom', 'are', 'involved', 'in', 'the', 'process', 'by', 'using', 'tools', 'of', 'transition', '... | [-0.12353051446682524, 0.16767080958545355, -0.0877911746066806, 0.043288802668786666, 0.010414978579184648, -0.10269680932754337, 0.018956380004137015, 0.39589121856606835, -0.24420351076336339, -0.3215044849819624, -0.0063162844277697035, -0.2515779719641893, -0.170325283323055, 0.10968184185739939, -0.01568172371365... |
709.1134 | Almost solutions of equations in permutations | We will say that the permutations f_1,...,f_n is an e-solution of an equation
if the normalized Hamming distance between its l.h.p. and r.h.p. is less than
e. We give a sufficient conditions when near to an e-solution exists an exact
solution and some examples when there does not exist such a solution.
| math.GR | we will say that the permutations f_1f_n is an esolution of an equation if the normalized hamming distance between its lhp and rhp is less than e we give a sufficient conditions when near to an esolution exists an exact solution and some examples when there does not exist such a solution | [['we', 'will', 'say', 'that', 'the', 'permutations', 'f_1f_n', 'is', 'an', 'esolution', 'of', 'an', 'equation', 'if', 'the', 'normalized', 'hamming', 'distance', 'between', 'its', 'lhp', 'and', 'rhp', 'is', 'less', 'than', 'e', 'we', 'give', 'a', 'sufficient', 'conditions', 'when', 'near', 'to', 'an', 'esolution', 'ex... | [-0.16760234758616066, 0.09018668944582504, -0.09323200608532016, 0.07372178060736936, -0.07476484172093478, -0.1602245129806061, 0.004935241743134191, 0.39390326807132137, -0.293418120377912, -0.19667420577640699, 0.11526773527909356, -0.3443482369900896, -0.16163424570829824, 0.1984129728247913, -0.11872706572131182,... |
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