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 |
|---|---|---|---|---|---|---|
706.2314 | Hypersurfaces in H^{n+1} and conformally invariant equations: the
generalized Christoffel and Nirenberg problems | Our first objective in this paper is to give a natural formulation of the
Christoffel problem for hypersurfaces in $H^{n+1}$, by means of the hyperbolic
Gauss map and the notion of hyperbolic curvature radii for hypersurfaces. Our
second objective is to provide an explicit equivalence of this Christoffel
problem with... | math.DG math.AP | our first objective in this paper is to give a natural formulation of the christoffel problem for hypersurfaces in hn1 by means of the hyperbolic gauss map and the notion of hyperbolic curvature radii for hypersurfaces our second objective is to provide an explicit equivalence of this christoffel problem with the famou... | [['our', 'first', 'objective', 'in', 'this', 'paper', 'is', 'to', 'give', 'a', 'natural', 'formulation', 'of', 'the', 'christoffel', 'problem', 'for', 'hypersurfaces', 'in', 'hn1', 'by', 'means', 'of', 'the', 'hyperbolic', 'gauss', 'map', 'and', 'the', 'notion', 'of', 'hyperbolic', 'curvature', 'radii', 'for', 'hypersu... | [-0.14687702840561934, 0.03883662744424691, -0.08100653058049125, 0.07787711125964675, -0.12511854725474483, -0.11372923722027194, -0.0439114889325115, 0.3231731283439087, -0.270952707318318, -0.25900240810019587, 0.08699548858471495, -0.2964651472101364, -0.18924913895228973, 0.19889179338862847, -0.1437727205582103, ... |
706.2315 | Spin Polarized Transport Through a Single-Molecule Magnet:
Current-Induced Magnetic Switching | Magnetic switching of a single-molecule magnet (SMM) due to spin-polarized
current is investigated theoretically. The charge transfer between the
electrodes takes place via the lowest unoccupied molecular orbital (LUMO) of
the SMM. Generally, the double occupancy of the LUMO level, and a finite
on-site Coulomb repuls... | cond-mat.mes-hall | magnetic switching of a singlemolecule magnet smm due to spinpolarized current is investigated theoretically the charge transfer between the electrodes takes place via the lowest unoccupied molecular orbital lumo of the smm generally the double occupancy of the lumo level and a finite onsite coulomb repulsion is taken ... | [['magnetic', 'switching', 'of', 'a', 'singlemolecule', 'magnet', 'smm', 'due', 'to', 'spinpolarized', 'current', 'is', 'investigated', 'theoretically', 'the', 'charge', 'transfer', 'between', 'the', 'electrodes', 'takes', 'place', 'via', 'the', 'lowest', 'unoccupied', 'molecular', 'orbital', 'lumo', 'of', 'the', 'smm'... | [-0.1846733643559422, 0.15419401639596897, -0.03086313205842979, 0.12082256662403992, -0.006044966015132501, -0.166157400542672, 0.10894579494352195, 0.3769563574225028, -0.30152567574120265, -0.2689615385606885, -0.09136811794064185, -0.27130378241789466, -0.08401620023428126, 0.12582459351285658, 0.09041783950747327,... |
706.2316 | Stable Border Bases for Ideals of Points | Let $X$ be a set of points whose coordinates are known with limited accuracy;
our aim is to give a characterization of the vanishing ideal $I(X)$ independent
of the data uncertainty. We present a method to compute a polynomial basis $B$
of $I(X)$ which exhibits structural stability, that is, if $\widetilde X$ is
any ... | math.AC math.NA | let x be a set of points whose coordinates are known with limited accuracy our aim is to give a characterization of the vanishing ideal ix independent of the data uncertainty we present a method to compute a polynomial basis b of ix which exhibits structural stability that is if widetilde x is any set of points differi... | [['let', 'x', 'be', 'a', 'set', 'of', 'points', 'whose', 'coordinates', 'are', 'known', 'with', 'limited', 'accuracy', 'our', 'aim', 'is', 'to', 'give', 'a', 'characterization', 'of', 'the', 'vanishing', 'ideal', 'ix', 'independent', 'of', 'the', 'data', 'uncertainty', 'we', 'present', 'a', 'method', 'to', 'compute', '... | [-0.19080780239821207, 0.057630905540796314, -0.10007605663069137, -0.0320311913148943, -0.06708160174510829, -0.1733033187323954, 0.07175812102916719, 0.3310625903853556, -0.2980539945022362, -0.21612550173999695, 0.09806277843691953, -0.2675234366935201, -0.07499739196060634, 0.17284979611044612, -0.04922623733603736... |
706.2317 | Study of Di-Pion Transitions Among Upsilon(3S), Upsilon(2S), and
Upsilon(1S) States | We present measurements of decay matrix elements for hadronic transitions of
the form Upsilon(nS) -> pi pi Upsilon(mS) where (n, m) = (3, 1), (2, 1), and
(3, 2). We reconstruct charged and neutral pion modes with the final state
Upsilon decaying to either mu+mu- or e+e-. Dalitz plot distributions for the
twelve decay... | hep-ex | we present measurements of decay matrix elements for hadronic transitions of the form upsilonns pi pi upsilonms where n m 3 1 2 1 and 3 2 we reconstruct charged and neutral pion modes with the final state upsilon decaying to either mumu or ee dalitz plot distributions for the twelve decay modes are fit individually as ... | [['we', 'present', 'measurements', 'of', 'decay', 'matrix', 'elements', 'for', 'hadronic', 'transitions', 'of', 'the', 'form', 'upsilonns', 'pi', 'pi', 'upsilonms', 'where', 'n', 'm', '3', '1', '2', '1', 'and', '3', '2', 'we', 'reconstruct', 'charged', 'and', 'neutral', 'pion', 'modes', 'with', 'the', 'final', 'state',... | [-0.07534985711875682, 0.2588618963610572, -0.07785312571221044, 0.13133032242349613, 0.003421221104546044, -0.14167163470604768, 0.07330369303385034, 0.288219870826325, -0.18412956096103583, -0.2486312681188186, -0.024317146787861697, -0.36816207266066414, -0.01504476837372073, 0.08238291704597381, 0.14473515330479506... |
706.2318 | The Geometry of Regular Shear-Free Null Geodesic Congruences, CR
functions and their Application to the Flat-Space Maxwell Equations | We describe here what appears to be a new structure that is hidden in all
asymptotically vanishing Maxwell fields possessing a non-vanishing total
charge. Though we are dealing with real Maxwell fields on real Minkowski space
nevertheless, directly from the asymptotic field one can extract a complex
analytic world-li... | gr-qc | we describe here what appears to be a new structure that is hidden in all asymptotically vanishing maxwell fields possessing a nonvanishing total charge though we are dealing with real maxwell fields on real minkowski space nevertheless directly from the asymptotic field one can extract a complex analytic worldline def... | [['we', 'describe', 'here', 'what', 'appears', 'to', 'be', 'a', 'new', 'structure', 'that', 'is', 'hidden', 'in', 'all', 'asymptotically', 'vanishing', 'maxwell', 'fields', 'possessing', 'a', 'nonvanishing', 'total', 'charge', 'though', 'we', 'are', 'dealing', 'with', 'real', 'maxwell', 'fields', 'on', 'real', 'minkows... | [-0.15752665089486642, 0.12604213542586495, -0.06718753977397153, 0.10221643599594922, -0.13555966270437766, -0.08437341736889509, -0.04288738968587199, 0.34092273875139656, -0.25294661278684816, -0.2513697809474759, 0.06487460305026277, -0.25773855490436737, -0.18170766071687172, 0.1537239214719468, -0.037389888309028... |
706.2319 | Analysing the elasticity difference tensor of general relativity | The elasticity difference tensor, used in [1] to describe elasticity
properties of a continuous medium filling a space-time, is here analysed from
the point of view of the space-time connection. Principal directions associated
with this tensor are compared with eigendirections of the material metric.
Examples concern... | gr-qc | the elasticity difference tensor used in 1 to describe elasticity properties of a continuous medium filling a spacetime is here analysed from the point of view of the spacetime connection principal directions associated with this tensor are compared with eigendirections of the material metric examples concerning spheri... | [['the', 'elasticity', 'difference', 'tensor', 'used', 'in', '1', 'to', 'describe', 'elasticity', 'properties', 'of', 'a', 'continuous', 'medium', 'filling', 'a', 'spacetime', 'is', 'here', 'analysed', 'from', 'the', 'point', 'of', 'view', 'of', 'the', 'spacetime', 'connection', 'principal', 'directions', 'associated',... | [-0.13731570084663955, 0.0946719228671017, -0.07045832039280371, 0.023775389324873684, -0.06877845618873835, -0.12346374133432453, -0.0880619691176848, 0.4041418888352134, -0.2559402527456934, -0.1663375042209571, 0.15259728083514015, -0.2958283146673983, -0.17224972627379678, 0.09166734807870605, -0.028616658251055263... |
706.232 | On large automorphism groups of algebraic curves in positive
characteristic | In his investigation on large $K$-automorphism groups of an algebraic curve,
Stichtenoth obtained an upper bound on the order of the first ramification
group of an algebraic curve $\cX$ defined over an algebraically closed field of
characteristic $p$. Stichtenoth's bound has raised the problem of classifying
all $\K$... | math.AG | in his investigation on large kautomorphism groups of an algebraic curve stichtenoth obtained an upper bound on the order of the first ramification group of an algebraic curve cx defined over an algebraically closed field of characteristic p stichtenoths bound has raised the problem of classifying all kautomorphism gro... | [['in', 'his', 'investigation', 'on', 'large', 'kautomorphism', 'groups', 'of', 'an', 'algebraic', 'curve', 'stichtenoth', 'obtained', 'an', 'upper', 'bound', 'on', 'the', 'order', 'of', 'the', 'first', 'ramification', 'group', 'of', 'an', 'algebraic', 'curve', 'cx', 'defined', 'over', 'an', 'algebraically', 'closed', ... | [-0.24457629351566235, 0.05494976102141663, -0.12277523099755247, 0.010042565221277376, -0.048012866557886204, -0.14487014873574178, 0.03260004958758751, 0.2901828003053864, -0.34388568190236884, -0.24285053943594298, 0.08824986255882929, -0.2739187690926095, -0.0796594451740384, 0.2830700981120268, -0.1260939143598079... |
706.2321 | Lower bounds for moments of zeta prime rho | Assuming the Riemann Hypothesis, we establish lower bounds for moments of the
derivative of the Riemann zeta-function averaged over the non-trivial zeros of
$\zeta(s)$. Our proof is based upon a recent method of Rudnick and
Soundararajan that provides analogous bounds for moments of $L$-functions at
the central point... | math.NT | assuming the riemann hypothesis we establish lower bounds for moments of the derivative of the riemann zetafunction averaged over the nontrivial zeros of zetas our proof is based upon a recent method of rudnick and soundararajan that provides analogous bounds for moments of lfunctions at the central point averaged over... | [['assuming', 'the', 'riemann', 'hypothesis', 'we', 'establish', 'lower', 'bounds', 'for', 'moments', 'of', 'the', 'derivative', 'of', 'the', 'riemann', 'zetafunction', 'averaged', 'over', 'the', 'nontrivial', 'zeros', 'of', 'zetas', 'our', 'proof', 'is', 'based', 'upon', 'a', 'recent', 'method', 'of', 'rudnick', 'and'... | [-0.214524944513744, 0.006243030504122668, -0.19495874637619173, 0.1116956334821332, -0.04355750178151271, -0.04036242601589537, 0.09039722039711241, 0.2180778298563525, -0.16136924133581274, -0.24519849101118013, 0.09134460573869885, -0.266827932175468, -0.08846672076512785, 0.3046031139571877, -0.009798287304446977, ... |
706.2322 | Materials with a desired refraction coefficient can be made by embedding
small particles | A method is proposed to create materials with a desired refraction
coefficient, possibly negative one. The method consists of embedding into a
given material small particles. Given $n_0(x)$, the refraction coefficient of
the original material in a bounded domain $D \subset \R^3$, and a desired
refraction coefficient ... | math-ph math.MP | a method is proposed to create materials with a desired refraction coefficient possibly negative one the method consists of embedding into a given material small particles given n_0x the refraction coefficient of the original material in a bounded domain d subset r3 and a desired refraction coefficient nx one calculate... | [['a', 'method', 'is', 'proposed', 'to', 'create', 'materials', 'with', 'a', 'desired', 'refraction', 'coefficient', 'possibly', 'negative', 'one', 'the', 'method', 'consists', 'of', 'embedding', 'into', 'a', 'given', 'material', 'small', 'particles', 'given', 'n_0x', 'the', 'refraction', 'coefficient', 'of', 'the', 'o... | [-0.1734864247917402, 0.14127407608008602, -0.046380462959726775, -0.07703126691389693, -0.07140927019858415, -0.1779297108125941, 0.031028012018196466, 0.3422119561582804, -0.29709174109213965, -0.28124051476351736, 0.035201137720766225, -0.34747627295735406, -0.12322261734161435, 0.13077478791677916, -0.0454938584007... |
706.2323 | A sample of mJy radio sources at 1.4 GHz in the Lynx and Hercules fields
- I. Radio imaging, multicolour photometry and spectroscopy | With the goal of identifying high redshift radio galaxies with FRI
classification, here are presented high resolution, wide-field radio
observations, near infra-red and optical imaging and multi-object spectroscopy
of two fields of the Leiden-Berkeley Deep Survey. These fields, Hercules.1 and
Lynx.2, contain a comple... | astro-ph | with the goal of identifying high redshift radio galaxies with fri classification here are presented high resolution widefield radio observations near infrared and optical imaging and multiobject spectroscopy of two fields of the leidenberkeley deep survey these fields hercules1 and lynx2 contain a complete sample of 8... | [['with', 'the', 'goal', 'of', 'identifying', 'high', 'redshift', 'radio', 'galaxies', 'with', 'fri', 'classification', 'here', 'are', 'presented', 'high', 'resolution', 'widefield', 'radio', 'observations', 'near', 'infrared', 'and', 'optical', 'imaging', 'and', 'multiobject', 'spectroscopy', 'of', 'two', 'fields', 'o... | [-0.07574964547860073, 0.09863844027178005, -0.022002849883089464, 0.03527565888981236, -0.08490352873716847, -0.08042195188013691, 0.08213419910497197, 0.4552465042640977, -0.11352021090937316, -0.401306413649086, 0.13151142755385029, -0.3441952800787721, 0.018224447024391688, 0.18783433604258912, 0.004487042019724952... |
706.2324 | Special isogenies and tensor product multiplicities | We show that any bijection between two root systems that preserves angles
(but not necessarily lengths) gives rise to inequalities relating tensor
product multiplicities for the corresponding complex semisimple Lie groups (or
Lie algebras). We explain the inequalities in two ways: combinatorially, using
Littelmann's ... | math.RT math.AG | we show that any bijection between two root systems that preserves angles but not necessarily lengths gives rise to inequalities relating tensor product multiplicities for the corresponding complex semisimple lie groups or lie algebras we explain the inequalities in two ways combinatorially using littelmanns path model... | [['we', 'show', 'that', 'any', 'bijection', 'between', 'two', 'root', 'systems', 'that', 'preserves', 'angles', 'but', 'not', 'necessarily', 'lengths', 'gives', 'rise', 'to', 'inequalities', 'relating', 'tensor', 'product', 'multiplicities', 'for', 'the', 'corresponding', 'complex', 'semisimple', 'lie', 'groups', 'or',... | [-0.2189877037402062, 0.1377869821906995, -0.09981951589185384, 0.09252631886591835, -0.12155083785464446, -0.1930771021608023, -0.049391160592354176, 0.4140980819901151, -0.3587969118248551, -0.23588449378768284, 0.02639595906422924, -0.2228676634465134, -0.1758918817072446, 0.25840469972688646, -0.09466201896148344, ... |
706.2325 | The Monitor project: JW 380 -- a 0.26, 0.15 Msol pre main sequence
eclipsing binary in the Orion Nebula Cluster | We report the discovery of a low-mass (0.26 +/- 0.02, 0.15 +/- 0.01 Msol)
pre-main-sequence eclipsing binary with a 5.3 day orbital period. JW 380 was
detected as part of a high-cadence time-resolved photometric survey (the
Monitor project) using the 2.5m Isaac Newton Telescope and Wide Field Camera
for a survey of a... | astro-ph | we report the discovery of a lowmass 026 002 015 001 msol premainsequence eclipsing binary with a 53 day orbital period jw 380 was detected as part of a highcadence timeresolved photometric survey the monitor project using the 25m isaac newton telescope and wide field camera for a survey of a single field in the orion ... | [['we', 'report', 'the', 'discovery', 'of', 'a', 'lowmass', '026', '002', '015', '001', 'msol', 'premainsequence', 'eclipsing', 'binary', 'with', 'a', '53', 'day', 'orbital', 'period', 'jw', '380', 'was', 'detected', 'as', 'part', 'of', 'a', 'highcadence', 'timeresolved', 'photometric', 'survey', 'the', 'monitor', 'pro... | [-0.10509958887583952, 0.11745276942767205, -0.07985878499474988, 0.03550863846793623, -0.09977329041187961, -0.11199291462115758, 0.11020867168250036, 0.38270920662403995, -0.1685001637383517, -0.4002734563216122, 0.08317018654058451, -0.3051873278197142, -0.005381692716659543, 0.22266224077300387, -0.0708899248755694... |
706.2326 | The Cosmic Horseshoe: Discovery of an Einstein Ring around a Giant
Luminous Red Galaxy | We report the discovery of an almost complete Einstein ring of diameter 10"
in Sloan Digital Sky Survey (SDSS) Data Release 5 (DR5). Spectroscopic data
from the 6m telescope of the Special Astrophysical Observatory reveals that the
deflecting galaxy has a line-of-sight velocity dispersion in excess of 400 km/s
and a ... | astro-ph | we report the discovery of an almost complete einstein ring of diameter 10 in sloan digital sky survey sdss data release 5 dr5 spectroscopic data from the 6m telescope of the special astrophysical observatory reveals that the deflecting galaxy has a lineofsight velocity dispersion in excess of 400 kms and a redshift of... | [['we', 'report', 'the', 'discovery', 'of', 'an', 'almost', 'complete', 'einstein', 'ring', 'of', 'diameter', '10', 'in', 'sloan', 'digital', 'sky', 'survey', 'sdss', 'data', 'release', '5', 'dr5', 'spectroscopic', 'data', 'from', 'the', '6m', 'telescope', 'of', 'the', 'special', 'astrophysical', 'observatory', 'reveal... | [-0.10746510113464801, 0.0774149423060429, -0.08821448276376748, 0.07348336210918033, -0.13449712196712413, -0.01435141652954493, 0.008530058868698717, 0.41593757095768696, -0.07801523933179794, -0.3635608999307935, 0.027491206395821133, -0.3573115054301654, 0.018833330267761635, 0.21975694616816413, -0.001223161033772... |
706.2327 | A Robust Atom-Photon Entanglement Source for Quantum Repeaters | We demonstrate a novel way to efficiently and very robust create an
entanglement between an atomic and a photonic qubit. A single laser beam is
used to excite one atomic ensemble and two different spatial modes of scattered
Raman fields are collected to generate the atom-photon entanglement. With the
help of build-in... | quant-ph | we demonstrate a novel way to efficiently and very robust create an entanglement between an atomic and a photonic qubit a single laser beam is used to excite one atomic ensemble and two different spatial modes of scattered raman fields are collected to generate the atomphoton entanglement with the help of buildin quant... | [['we', 'demonstrate', 'a', 'novel', 'way', 'to', 'efficiently', 'and', 'very', 'robust', 'create', 'an', 'entanglement', 'between', 'an', 'atomic', 'and', 'a', 'photonic', 'qubit', 'a', 'single', 'laser', 'beam', 'is', 'used', 'to', 'excite', 'one', 'atomic', 'ensemble', 'and', 'two', 'different', 'spatial', 'modes', ... | [-0.09335702285170555, 0.17587654380873904, -0.06788285648958249, -0.019650668546091765, -0.03845919508021325, -0.2495021736757322, 0.06612322729673575, 0.3927959815218029, -0.22760355475316332, -0.3316607524725524, -0.02606142499399456, -0.23865481260317292, -0.10235129420391538, 0.22705513533543456, -0.08857225604693... |
706.2328 | Unique mechanisms from finite two-state trajectories | Single molecule data made of on and off events are ubiquitous. Famous
examples include enzyme turnover, probed via fluorescence, and opening and
closing of ion-channel, probed via the flux of ions. The data reflects the
dynamics in the underlying multi-substate on-off kinetic scheme (KS) of the
process, but the deter... | q-bio.QM cond-mat.other q-bio.OT | single molecule data made of on and off events are ubiquitous famous examples include enzyme turnover probed via fluorescence and opening and closing of ionchannel probed via the flux of ions the data reflects the dynamics in the underlying multisubstate onoff kinetic scheme ks of the process but the determination of t... | [['single', 'molecule', 'data', 'made', 'of', 'on', 'and', 'off', 'events', 'are', 'ubiquitous', 'famous', 'examples', 'include', 'enzyme', 'turnover', 'probed', 'via', 'fluorescence', 'and', 'opening', 'and', 'closing', 'of', 'ionchannel', 'probed', 'via', 'the', 'flux', 'of', 'ions', 'the', 'data', 'reflects', 'the',... | [-0.10894410371883241, 0.11997409222407932, -0.08226302375822711, 0.09877788465214256, -0.05430099760050788, -0.15094716554976131, 0.06071189155179344, 0.30543649523444705, -0.2843083457369929, -0.292835922334686, 0.06535980718044644, -0.2644186927594153, -0.11397382214756831, 0.20334173839373593, -0.013666469383087763... |
706.2329 | Numerical Kaehler-Ricci soliton on the second del Pezzo | The second del Pezzo surface is known by work of Tian-Zhu and Wang-Zhu to
admit a unique Kaehler-Ricci soliton. Applying a method described in
hep-th/0703057, we use Ricci flow to numerically compute that soliton metric.
We numerically compute the value of its Perelman entropy (or Gaussian density).
| math.DG gr-qc hep-th | the second del pezzo surface is known by work of tianzhu and wangzhu to admit a unique kaehlerricci soliton applying a method described in hepth0703057 we use ricci flow to numerically compute that soliton metric we numerically compute the value of its perelman entropy or gaussian density | [['the', 'second', 'del', 'pezzo', 'surface', 'is', 'known', 'by', 'work', 'of', 'tianzhu', 'and', 'wangzhu', 'to', 'admit', 'a', 'unique', 'kaehlerricci', 'soliton', 'applying', 'a', 'method', 'described', 'in', 'hepth0703057', 'we', 'use', 'ricci', 'flow', 'to', 'numerically', 'compute', 'that', 'soliton', 'metric', ... | [-0.15249591130439355, 0.01843869724088227, -0.1674682863826013, 0.09225508703536395, -0.087948946909898, -0.18084269155667204, -0.03179648316100887, 0.33865698424937285, -0.23826290437263314, -0.2288364179270423, 0.10834869026312725, -0.28202951699495316, -0.172054316144963, 0.16639426637582644, -0.10159648975114459, ... |
706.233 | Three body resonances in two meson-one baryon systems | We report four $\Sigma$'s and three $\Lambda$'s, in the 1500 - 1800 MeV
region, as two meson - one baryon S-wave $(1/2)^+$ resonances. We solve Faddeev
equations in the coupled channel approach. The invariant mass of one of the
meson-baryon pairs and that of the three particles have been varied and peaks
in the squar... | nucl-th | we report four sigmas and three lambdas in the 1500 1800 mev region as two meson one baryon swave 12 resonances we solve faddeev equations in the coupled channel approach the invariant mass of one of the mesonbaryon pairs and that of the three particles have been varied and peaks in the squared three body tmatrix have ... | [['we', 'report', 'four', 'sigmas', 'and', 'three', 'lambdas', 'in', 'the', '1500', '1800', 'mev', 'region', 'as', 'two', 'meson', 'one', 'baryon', 'swave', '12', 'resonances', 'we', 'solve', 'faddeev', 'equations', 'in', 'the', 'coupled', 'channel', 'approach', 'the', 'invariant', 'mass', 'of', 'one', 'of', 'the', 'me... | [-0.13376747066872574, 0.21212211743054188, -0.06375711083374157, 0.10186144082369852, -0.010609196196369618, -0.1632056998193492, 0.005747653596217231, 0.3293194242239911, -0.16311104324342188, -0.31020240267092475, -0.04599253258819939, -0.37587997343923363, -0.04134564668092192, 0.07127324951698585, 0.14188521094495... |
706.2331 | Pricing American Options for Jump Diffusions by Iterating Optimal
Stopping Problems for Diffusions | We approximate the price of the American put for jump diffusions by a
sequence of functions, which are computed iteratively. This sequence converges
to the price function uniformly and exponentially fast. Each element of the
approximating sequence solves an optimal stopping problem for geometric
Brownian motion, and ... | cs.CE | we approximate the price of the american put for jump diffusions by a sequence of functions which are computed iteratively this sequence converges to the price function uniformly and exponentially fast each element of the approximating sequence solves an optimal stopping problem for geometric brownian motion and can be... | [['we', 'approximate', 'the', 'price', 'of', 'the', 'american', 'put', 'for', 'jump', 'diffusions', 'by', 'a', 'sequence', 'of', 'functions', 'which', 'are', 'computed', 'iteratively', 'this', 'sequence', 'converges', 'to', 'the', 'price', 'function', 'uniformly', 'and', 'exponentially', 'fast', 'each', 'element', 'of'... | [-0.06563132821530518, 0.05963725192628368, -0.1285478025286769, 0.09117371582154495, -0.04679459046262006, -0.1097673839604896, 0.07953541927498817, 0.41855446378596955, -0.38414323600914535, -0.23035615941302645, 0.16066522176616774, -0.23881841850622246, -0.12086409418326285, 0.1992744090449479, -0.10328811177492349... |
706.2332 | Predictions from non trivial Quark-Lepton complementarity | The complementarity between the quark and lepton mixing matrices is shown to
provide robust predictions. We obtain these predictions by first showing that
the matrix V_M, product of the quark (CKM) and lepton (PMNS) mixing matrices,
may have a zero (1,3) entry which is favored by experimental data.
We obtain that a... | hep-ph | the complementarity between the quark and lepton mixing matrices is shown to provide robust predictions we obtain these predictions by first showing that the matrix v_m product of the quark ckm and lepton pmns mixing matrices may have a zero 13 entry which is favored by experimental data we obtain that any theoretical ... | [['the', 'complementarity', 'between', 'the', 'quark', 'and', 'lepton', 'mixing', 'matrices', 'is', 'shown', 'to', 'provide', 'robust', 'predictions', 'we', 'obtain', 'these', 'predictions', 'by', 'first', 'showing', 'that', 'the', 'matrix', 'v_m', 'product', 'of', 'the', 'quark', 'ckm', 'and', 'lepton', 'pmns', 'mixin... | [-0.1114050796558068, 0.2877366134575617, -0.01868423827897874, 0.12894823606562467, -0.05585931949739309, -0.18140527358577174, 0.07091786523750344, 0.2999957712522938, -0.2297536796322928, -0.2605971603229226, 0.05402116322133833, -0.3222543533148328, -0.04858195057012245, 0.11524199478763061, 0.06192870878205612, 0.... |
706.2333 | Loschmidt echo and stochastic-like quantum dynamics of nano-particles | We investigate time evolution of prepared vibrational state (system) coupled
to a reservoir with dense spectrum of its vibrational states. We assume that
the reservoir has an equidistant spectrum, and the system - reservoir coupling
matrix elements are independent of the reservoir states. The analytical
solution mani... | cond-mat.stat-mech cond-mat.mes-hall | we investigate time evolution of prepared vibrational state system coupled to a reservoir with dense spectrum of its vibrational states we assume that the reservoir has an equidistant spectrum and the system reservoir coupling matrix elements are independent of the reservoir states the analytical solution manifests thr... | [['we', 'investigate', 'time', 'evolution', 'of', 'prepared', 'vibrational', 'state', 'system', 'coupled', 'to', 'a', 'reservoir', 'with', 'dense', 'spectrum', 'of', 'its', 'vibrational', 'states', 'we', 'assume', 'that', 'the', 'reservoir', 'has', 'an', 'equidistant', 'spectrum', 'and', 'the', 'system', 'reservoir', '... | [-0.211738001782861, 0.17754780154565297, -0.07727489499375224, 0.05325736526606811, 0.04246821782931134, -0.17611779964494484, 0.038336051769416644, 0.3317023454061537, -0.2868964899158864, -0.2674087532278564, 0.08695960950399577, -0.25601946183100893, -0.10307545967882982, 0.16597948706432902, 0.029739610530022116, ... |
706.2334 | MadGraph/MadEvent v4: The New Web Generation | We present the latest developments of the MadGraph/MadEvent Monte Carlo event
generator and several applications to hadron collider physics. In the current
version events at the parton, hadron and detector level can be generated
directly from a web interface, for arbitrary processes in the Standard Model
and in sever... | hep-ph | we present the latest developments of the madgraphmadevent monte carlo event generator and several applications to hadron collider physics in the current version events at the parton hadron and detector level can be generated directly from a web interface for arbitrary processes in the standard model and in several phy... | [['we', 'present', 'the', 'latest', 'developments', 'of', 'the', 'madgraphmadevent', 'monte', 'carlo', 'event', 'generator', 'and', 'several', 'applications', 'to', 'hadron', 'collider', 'physics', 'in', 'the', 'current', 'version', 'events', 'at', 'the', 'parton', 'hadron', 'and', 'detector', 'level', 'can', 'be', 'ge... | [-0.021846477697859062, 0.18725059624686016, -0.06855750357156948, 0.17682084933325065, -0.06344981045649369, -0.158485771812825, -0.016680646791606777, 0.3341071074029577, -0.2131695775092607, -0.32231204179298206, 0.043687223047063704, -0.3574728138799615, 0.019107749356943017, 0.1843190458888535, 0.08194953062846645... |
706.2335 | Lateral Effects in Fermion Antibunching | Lateral effects are analyzed in the antibunching of a beam of free
non-interacting fermions. The emission of particles from a source is
dynamically described in a 3D full quantum field-theoretical framework. The
size of the source and the detectors, as well as the temperature of the source
are taken into account and ... | quant-ph | lateral effects are analyzed in the antibunching of a beam of free noninteracting fermions the emission of particles from a source is dynamically described in a 3d full quantum fieldtheoretical framework the size of the source and the detectors as well as the temperature of the source are taken into account and the beh... | [['lateral', 'effects', 'are', 'analyzed', 'in', 'the', 'antibunching', 'of', 'a', 'beam', 'of', 'free', 'noninteracting', 'fermions', 'the', 'emission', 'of', 'particles', 'from', 'a', 'source', 'is', 'dynamically', 'described', 'in', 'a', '3d', 'full', 'quantum', 'fieldtheoretical', 'framework', 'the', 'size', 'of', ... | [-0.10102327635081915, 0.18281513690375364, -0.10724913619028834, 0.07547868477682082, 0.010530985254221237, -0.09672970564032976, 0.007025941414758563, 0.36747278404923583, -0.2416222419159917, -0.3132652434851759, 0.05620080615537098, -0.30273647411511495, -0.047854166477918625, 0.18732577408305728, 0.025514758507219... |
706.2336 | Testing AdS/CFT Deviations from pQCD Heavy Quark Energy Loss with Pb+Pb
at LHC | Heavy quark jet quenching in nuclear collisions at LHC is predicted and
compared using the classical gravity AdS/CFT correspondence and Standard Model
perturbative QCD. The momentum independence and inverse quark mass dependence
of the drag coefficient in AdS/CFT differs substantially from the
characteristic log(pT/M... | nucl-th | heavy quark jet quenching in nuclear collisions at lhc is predicted and compared using the classical gravity adscft correspondence and standard model perturbative qcd the momentum independence and inverse quark mass dependence of the drag coefficient in adscft differs substantially from the characteristic logptmpt vari... | [['heavy', 'quark', 'jet', 'quenching', 'in', 'nuclear', 'collisions', 'at', 'lhc', 'is', 'predicted', 'and', 'compared', 'using', 'the', 'classical', 'gravity', 'adscft', 'correspondence', 'and', 'standard', 'model', 'perturbative', 'qcd', 'the', 'momentum', 'independence', 'and', 'inverse', 'quark', 'mass', 'dependen... | [-0.04728949676371283, 0.2185210293262369, -0.18561587514252298, 0.14641353069131988, -0.06561590439846945, -0.09469836192309028, 0.017729206991821733, 0.29469363532132575, -0.2452582329718603, -0.2633711026981473, -0.029160420449140172, -0.3027470342659702, 0.027428716390083232, 0.12704888538250492, 0.0391691269249551... |
706.2337 | The extended structure of the remote cluster B514 in M31. Detection of
extra-tidal stars | We present a study of the density profile of the remote M31 globular cluster
B514, obtained from HST/ACS observations. Coupling the analysis of the
distribution of the integrated light with star counts we can reliably follow
the profile of the cluster out to r~35", corresponding to ~130pc. The profile
is well fitted,... | astro-ph | we present a study of the density profile of the remote m31 globular cluster b514 obtained from hstacs observations coupling the analysis of the distribution of the integrated light with star counts we can reliably follow the profile of the cluster out to r35 corresponding to 130pc the profile is well fitted out to 15 ... | [['we', 'present', 'a', 'study', 'of', 'the', 'density', 'profile', 'of', 'the', 'remote', 'm31', 'globular', 'cluster', 'b514', 'obtained', 'from', 'hstacs', 'observations', 'coupling', 'the', 'analysis', 'of', 'the', 'distribution', 'of', 'the', 'integrated', 'light', 'with', 'star', 'counts', 'we', 'can', 'reliably'... | [-0.057247915637104754, 0.0420620078964814, -0.14130865212807314, 0.11208064205686938, -0.06936220464574054, -0.053574662318730606, 0.0627956294462065, 0.37933492238454997, -0.16482069535150584, -0.39665161987687364, 0.03278605848398466, -0.31751580584913175, -0.04012059338113412, 0.17790585665336928, -0.03997169236514... |
706.2338 | The light variability of the helium strong star HD 37776 as a result of
its inhomogeneous elemental surface distribution | We simulate light curves of the helium strong chemically peculiar star HD
37776 assuming that the observed periodic light variations originate as a
result of inhomogeneous horizontal distribution of chemical elements on the
surface of a rotating star. We show that chemical peculiarity influences the
monochromatic rad... | astro-ph | we simulate light curves of the helium strong chemically peculiar star hd 37776 assuming that the observed periodic light variations originate as a result of inhomogeneous horizontal distribution of chemical elements on the surface of a rotating star we show that chemical peculiarity influences the monochromatic radiat... | [['we', 'simulate', 'light', 'curves', 'of', 'the', 'helium', 'strong', 'chemically', 'peculiar', 'star', 'hd', '37776', 'assuming', 'that', 'the', 'observed', 'periodic', 'light', 'variations', 'originate', 'as', 'a', 'result', 'of', 'inhomogeneous', 'horizontal', 'distribution', 'of', 'chemical', 'elements', 'on', 't... | [-0.08633173693043109, 0.16010020164629588, -0.11395911575796512, 0.054861817421176684, -0.04830078442509358, -0.08608183266523366, 0.08181510261582355, 0.392172725040179, -0.24843650008193574, -0.321860034770977, 0.0073490879050670905, -0.2712341325894858, -0.1054877955421174, 0.20903712838413552, -0.07470988852616686... |
706.2339 | Low-Scale Technicolor at the Tevatron and LHC | The Tevatron experiments CDF and DO are close to making definitive statements
about the technicolor discovery mode rho_T -> W pi_T for M(rho_T) <~ 230 GeV
and M(pi_T) <~ 125 GeV. We propose new incisive tests for this mode and
searches for others that may be feasible at the Tevatron and certainly are at
the LHC. The ... | hep-ph hep-ex | the tevatron experiments cdf and do are close to making definitive statements about the technicolor discovery mode rho_t w pi_t for mrho_t 230 gev and mpi_t 125 gev we propose new incisive tests for this mode and searches for others that may be feasible at the tevatron and certainly are at the lhc the other searches in... | [['the', 'tevatron', 'experiments', 'cdf', 'and', 'do', 'are', 'close', 'to', 'making', 'definitive', 'statements', 'about', 'the', 'technicolor', 'discovery', 'mode', 'rho_t', 'w', 'pi_t', 'for', 'mrho_t', '230', 'gev', 'and', 'mpi_t', '125', 'gev', 'we', 'propose', 'new', 'incisive', 'tests', 'for', 'this', 'mode', '... | [-0.06006674676596091, 0.2502758565106403, -0.07041434020622173, 0.1515168703659481, -0.11515063367714391, -0.23862345777364952, 0.07063050051198001, 0.32200659908980966, -0.22853502074134685, -0.25175030477275356, 0.1000600725534224, -0.3512216756102916, 0.03990022362608062, 0.15981759127581963, 0.05608800339303632, 0... |
706.234 | Hodge-Stickelberger polygons for L-functions of exponential sums of
P(x^s) | Let P(x) be a one-variable Laurent polynomial of degree (d_1,d_2) over a
finite field of characteristic p. For any fixed positive integer s not
divisible by p, we prove that the (normalized) p-adic Newton polygon of the
L-functions of exponential sums of P(x^s) has a tight lower bound which we call
`Hodge-Stickelberg... | math.NT math.AG | let px be a onevariable laurent polynomial of degree d_1d_2 over a finite field of characteristic p for any fixed positive integer s not divisible by p we prove that the normalized padic newton polygon of the lfunctions of exponential sums of pxs has a tight lower bound which we call hodgestickelberger polygon dependin... | [['let', 'px', 'be', 'a', 'onevariable', 'laurent', 'polynomial', 'of', 'degree', 'd_1d_2', 'over', 'a', 'finite', 'field', 'of', 'characteristic', 'p', 'for', 'any', 'fixed', 'positive', 'integer', 's', 'not', 'divisible', 'by', 'p', 'we', 'prove', 'that', 'the', 'normalized', 'padic', 'newton', 'polygon', 'of', 'the'... | [-0.22416841313877905, 0.049394007099401664, -0.1749869076972545, 0.05192039747877667, -0.08636952624620983, -0.20148562786705565, 0.062289221441570786, 0.2490551485150883, -0.3314718292376986, -0.18125934067718458, 0.046421677525910185, -0.22503586214698965, -0.1540443787428861, 0.18948631856421178, -0.148695517384277... |
706.2341 | Tri-Bimaximal Neutrino Mixing and the Family Symmetry Z_7 x Z_3 | The Non-Abelian finite group PSL_2(7) is the only simple subgroup of SU(3)
with a complex three-dimensional irreducible representation. It has two maximal
subgroups, S_4 which, along with its own A_4 subgroup, has been successfully
applied in numerous models of flavor, as well as the 21 element Frobenius group
Z_7 x ... | hep-ph hep-th | the nonabelian finite group psl_27 is the only simple subgroup of su3 with a complex threedimensional irreducible representation it has two maximal subgroups s_4 which along with its own a_4 subgroup has been successfully applied in numerous models of flavor as well as the 21 element frobenius group z_7 x z_3 which has... | [['the', 'nonabelian', 'finite', 'group', 'psl_27', 'is', 'the', 'only', 'simple', 'subgroup', 'of', 'su3', 'with', 'a', 'complex', 'threedimensional', 'irreducible', 'representation', 'it', 'has', 'two', 'maximal', 'subgroups', 's_4', 'which', 'along', 'with', 'its', 'own', 'a_4', 'subgroup', 'has', 'been', 'successfu... | [-0.0741441285231921, 0.20946839596662256, -0.07456125089047867, 0.10201676586142706, -0.15561761337700358, -0.17898957395673165, 0.005106530692658306, 0.421356853534594, -0.25889555307358136, -0.2595910342168753, 0.14096200663055994, -0.2501539115184619, -0.06464223708256067, 0.12612570220903482, -0.03988139464715381,... |
706.2342 | Gravitational Wilson Loop and Large Scale Curvature | In a quantum theory of gravity the gravitational Wilson loop, defined as a
suitable quantum average of a parallel transport operator around a large
near-planar loop, provides important information about the large-scale
curvature properties of the geometry. Here we shows that such properties can be
systematically comp... | hep-th gr-qc | in a quantum theory of gravity the gravitational wilson loop defined as a suitable quantum average of a parallel transport operator around a large nearplanar loop provides important information about the largescale curvature properties of the geometry here we shows that such properties can be systematically computed in... | [['in', 'a', 'quantum', 'theory', 'of', 'gravity', 'the', 'gravitational', 'wilson', 'loop', 'defined', 'as', 'a', 'suitable', 'quantum', 'average', 'of', 'a', 'parallel', 'transport', 'operator', 'around', 'a', 'large', 'nearplanar', 'loop', 'provides', 'important', 'information', 'about', 'the', 'largescale', 'curvat... | [-0.1867138977377995, 0.18143153383870914, -0.10771154023971019, 0.08235902932373487, -0.03775004404527483, -0.12017977206425658, -0.017758799252037737, 0.3216899033364798, -0.2529659167543721, -0.2628478259612709, 0.0485272708682538, -0.23956352912511594, -0.14509368284758348, 0.19314335712662606, -0.0332014976145783,... |
706.2343 | Nonlinear perturbations of Fuchsian systems: corrections and
linearization, normal forms | Nonlinear perturbation of Fuchsian systems are studied in a region including
two singularities. It is proved that such systems are generally not
analytically equivalent to their linear part (they are not linearizable) and
the obstructions are found constructively, as a countable set of numbers.
Furthermore, assuming ... | math.CA | nonlinear perturbation of fuchsian systems are studied in a region including two singularities it is proved that such systems are generally not analytically equivalent to their linear part they are not linearizable and the obstructions are found constructively as a countable set of numbers furthermore assuming a polyno... | [['nonlinear', 'perturbation', 'of', 'fuchsian', 'systems', 'are', 'studied', 'in', 'a', 'region', 'including', 'two', 'singularities', 'it', 'is', 'proved', 'that', 'such', 'systems', 'are', 'generally', 'not', 'analytically', 'equivalent', 'to', 'their', 'linear', 'part', 'they', 'are', 'not', 'linearizable', 'and', ... | [-0.1995930499491975, 0.058319021038018, -0.08529995039625224, 0.116535080100009, -0.08714322496725377, -0.16335111480682743, -0.041711110415933436, 0.3688975475771829, -0.32418658892992275, -0.2143209340419014, 0.15689272878943336, -0.29084671105036164, -0.2243494484357016, 0.2371960409414727, -0.04875722361578292, 0.... |
706.2344 | Detectors for the James Webb Space Telescope Near-Infrared Spectrograph
I: Readout Mode, Noise Model, and Calibration Considerations | We describe how the James Webb Space Telescope (JWST) Near-Infrared
Spectrograph's (NIRSpec's) detectors will be read out, and present a model of
how noise scales with the number of multiple non-destructive reads
sampling-up-the-ramp. We believe that this noise model, which is validated
using real and simulated test ... | astro-ph | we describe how the james webb space telescope jwst nearinfrared spectrographs nirspecs detectors will be read out and present a model of how noise scales with the number of multiple nondestructive reads samplinguptheramp we believe that this noise model which is validated using real and simulated test data is applicab... | [['we', 'describe', 'how', 'the', 'james', 'webb', 'space', 'telescope', 'jwst', 'nearinfrared', 'spectrographs', 'nirspecs', 'detectors', 'will', 'be', 'read', 'out', 'and', 'present', 'a', 'model', 'of', 'how', 'noise', 'scales', 'with', 'the', 'number', 'of', 'multiple', 'nondestructive', 'reads', 'samplinguptheramp... | [-0.07698023801656079, 0.15477535805979864, -0.0907163750870227, 0.07998725401552514, -0.08914825460444734, -0.19824877658041476, 0.006651908730444827, 0.4423878019769415, -0.2270951356258069, -0.3205739329334536, 0.16017428624339858, -0.29044405963216263, -0.16878363240607377, 0.2524761957193477, -0.10817572742486171,... |
706.2345 | Phenomenology from a U(1) gauged hidden sector | We consider the phenomenological consequences of a hidden Higgs sector
extending the Standard Model (SM), in which the matter content are uncharged
under the SM gauge groups. We consider a simple case where the hidden sector is
gauged under a U(1) with one Higgs singlet. The only couplings between SM and
the hidden s... | hep-ph | we consider the phenomenological consequences of a hidden higgs sector extending the standard model sm in which the matter content are uncharged under the sm gauge groups we consider a simple case where the hidden sector is gauged under a u1 with one higgs singlet the only couplings between sm and the hidden sector are... | [['we', 'consider', 'the', 'phenomenological', 'consequences', 'of', 'a', 'hidden', 'higgs', 'sector', 'extending', 'the', 'standard', 'model', 'sm', 'in', 'which', 'the', 'matter', 'content', 'are', 'uncharged', 'under', 'the', 'sm', 'gauge', 'groups', 'we', 'consider', 'a', 'simple', 'case', 'where', 'the', 'hidden',... | [-0.12208607255628234, 0.2859744932747593, -0.03453545989468694, 0.16062832483163986, -0.10231460461785134, -0.21538927715859915, 0.04002434148600227, 0.30010396459777106, -0.22855333607447775, -0.2670753743695585, 0.037448482871006585, -0.30827273728424, -0.08982274787635297, 0.055007481837253035, 0.07959640833402151,... |
706.2346 | Non-Gaussianity analysis on local morphological measures of WMAP data | The decomposition of a signal on the sphere with the steerable wavelet
constructed from the second Gaussian derivative gives access to the
orientation, signed-intensity, and elongation of the signal's local features.
In the present work, the non-Gaussianity of the WMAP temperature data of the
cosmic microwave backgro... | astro-ph | the decomposition of a signal on the sphere with the steerable wavelet constructed from the second gaussian derivative gives access to the orientation signedintensity and elongation of the signals local features in the present work the nongaussianity of the wmap temperature data of the cosmic microwave background cmb i... | [['the', 'decomposition', 'of', 'a', 'signal', 'on', 'the', 'sphere', 'with', 'the', 'steerable', 'wavelet', 'constructed', 'from', 'the', 'second', 'gaussian', 'derivative', 'gives', 'access', 'to', 'the', 'orientation', 'signedintensity', 'and', 'elongation', 'of', 'the', 'signals', 'local', 'features', 'in', 'the', ... | [-0.11278795193777316, 0.09798082104443219, -0.09775620028333462, 0.06446924701427903, -0.08322335516050872, -0.04713224495881824, -0.009094701233078484, 0.3417412813373462, -0.2469484240454794, -0.3016716801457935, 0.09206389136164, -0.3198510643804049, -0.05768026846150557, 0.18026616414405267, -0.005778491647948546,... |
706.2347 | On the cyclicity of weight-homogeneous centers | Let W be a weight-homogeneous planar polynomial differential system with a
center. We find an upper bound of the number of limit cycles which bifurcate
from the period annulus of W under a generic polynomial perturbation. We apply
this result to a particular family of planar polynomial systems having a
nilpotent cent... | math.DS | let w be a weighthomogeneous planar polynomial differential system with a center we find an upper bound of the number of limit cycles which bifurcate from the period annulus of w under a generic polynomial perturbation we apply this result to a particular family of planar polynomial systems having a nilpotent center wi... | [['let', 'w', 'be', 'a', 'weighthomogeneous', 'planar', 'polynomial', 'differential', 'system', 'with', 'a', 'center', 'we', 'find', 'an', 'upper', 'bound', 'of', 'the', 'number', 'of', 'limit', 'cycles', 'which', 'bifurcate', 'from', 'the', 'period', 'annulus', 'of', 'w', 'under', 'a', 'generic', 'polynomial', 'pertur... | [-0.23202735345278466, 0.06965694429553489, -0.10292451505249899, -0.03326702117296269, -0.08989896731717247, -0.1393986092131984, 0.03665544644796422, 0.25905930284144624, -0.3098133520023631, -0.256561042325172, 0.11508756574143522, -0.2345938241175775, -0.13478883119699145, 0.22806095820851624, -0.0658487358180407, ... |
706.2348 | Analytic linearization of nonlinear perturbations of Fuchsian systems | Nonlinear perturbation of Fuchsian systems are studied in regions including
two singularities. Such systems are not necessarily analytically equivalent to
their linear part (they are not linearizable). Nevertheless, it is shown that
in the case when the linear part has commuting monodromy, and the eigenvalues
have po... | math.CA | nonlinear perturbation of fuchsian systems are studied in regions including two singularities such systems are not necessarily analytically equivalent to their linear part they are not linearizable nevertheless it is shown that in the case when the linear part has commuting monodromy and the eigenvalues have positive r... | [['nonlinear', 'perturbation', 'of', 'fuchsian', 'systems', 'are', 'studied', 'in', 'regions', 'including', 'two', 'singularities', 'such', 'systems', 'are', 'not', 'necessarily', 'analytically', 'equivalent', 'to', 'their', 'linear', 'part', 'they', 'are', 'not', 'linearizable', 'nevertheless', 'it', 'is', 'shown', 't... | [-0.18176186368140435, 0.06393949594348669, -0.0533297996022808, 0.08581625627277335, -0.06760529726187685, -0.18349304702827957, -0.09197661072821982, 0.3683603819348474, -0.2991644563848403, -0.1793492041986936, 0.16944819268572436, -0.3373973814513423, -0.2423673402518034, 0.1971828729581477, -0.052778638906276494, ... |
706.2349 | The $^{15}$O($\alpha$,$\gamma$)$^{19}$Ne Breakout Reaction and Impact on
X-Ray Bursts | The breakout reaction $^{15}$O($\alpha,\gamma$)$^{19}$Ne, which regulates the
flow between the hot CNO cycle and the rp-process, is critical for the
explanation of the burst amplitude and periodicity of X-ray bursters. We report
on the first successful measurement of the critical $\alpha$-decay branching
ratios of re... | nucl-ex astro-ph | the breakout reaction 15oalphagamma19ne which regulates the flow between the hot cno cycle and the rpprocess is critical for the explanation of the burst amplitude and periodicity of xray bursters we report on the first successful measurement of the critical alphadecay branching ratios of relevant states in 19ne popula... | [['the', 'breakout', 'reaction', '15oalphagamma19ne', 'which', 'regulates', 'the', 'flow', 'between', 'the', 'hot', 'cno', 'cycle', 'and', 'the', 'rpprocess', 'is', 'critical', 'for', 'the', 'explanation', 'of', 'the', 'burst', 'amplitude', 'and', 'periodicity', 'of', 'xray', 'bursters', 'we', 'report', 'on', 'the', 'f... | [-0.12753618223423077, 0.170492650884072, -0.04402190791322779, 0.06156112876487896, 0.00762295745232183, -0.03121541469843815, 0.14689132032672997, 0.3635130297473591, -0.17058738569840384, -0.28206797098012076, 0.08325032582987384, -0.2778009387624005, -0.0805678866226631, 0.27742011139786843, 0.012780542437331345, 0... |
706.235 | Kummer subfields of tame division algebras over Henselian valued fields | By generalizing the method used by Tignol and Amitsur in [TA85], we determine
necessary and sufficient conditions for an arbitrary tame central division
algebra D over a Henselian valued field E to have Kummer subfields [Corollary
2.11 and Corollary 2.12]. We prove also that if D is a tame semiramified
division algeb... | math.RA | by generalizing the method used by tignol and amitsur in ta85 we determine necessary and sufficient conditions for an arbitrary tame central division algebra d over a henselian valued field e to have kummer subfields corollary 211 and corollary 212 we prove also that if d is a tame semiramified division algebra of prim... | [['by', 'generalizing', 'the', 'method', 'used', 'by', 'tignol', 'and', 'amitsur', 'in', 'ta85', 'we', 'determine', 'necessary', 'and', 'sufficient', 'conditions', 'for', 'an', 'arbitrary', 'tame', 'central', 'division', 'algebra', 'd', 'over', 'a', 'henselian', 'valued', 'field', 'e', 'to', 'have', 'kummer', 'subfield... | [-0.20015125723785898, 0.08889858259621934, -0.09507084053972464, 0.039141092866690555, -0.0486301323058858, -0.21704707165991657, -0.028301668151941024, 0.3298540506093355, -0.3086194521590565, -0.21730370688764902, 0.04979069752153009, -0.17891313863939115, -0.12520653165398124, 0.1971103807994991, -0.120104286087195... |
706.2351 | Probing the Relation Between X-ray-Derived and Weak-Lensing-Derived
Masses for Shear-Selected Galaxy Clusters: I. A781 | We compare X-ray and weak-lensing masses for four galaxy clusters that
comprise the top-ranked shear-selected cluster system in the Deep Lens Survey.
The weak-lensing observations of this system, which is associated with A781,
are from the Kitt Peak Mayall 4-m telescope, and the X-ray observations are
from both Chand... | astro-ph | we compare xray and weaklensing masses for four galaxy clusters that comprise the topranked shearselected cluster system in the deep lens survey the weaklensing observations of this system which is associated with a781 are from the kitt peak mayall 4m telescope and the xray observations are from both chandra and xmmnew... | [['we', 'compare', 'xray', 'and', 'weaklensing', 'masses', 'for', 'four', 'galaxy', 'clusters', 'that', 'comprise', 'the', 'topranked', 'shearselected', 'cluster', 'system', 'in', 'the', 'deep', 'lens', 'survey', 'the', 'weaklensing', 'observations', 'of', 'this', 'system', 'which', 'is', 'associated', 'with', 'a781', ... | [-0.03088108910086714, 0.0686145447191103, -0.12444799759429055, 0.12304367225783888, -0.09555790052507762, -0.060624433726401916, 0.007466265705601914, 0.43185344498811495, -0.1813758417960149, -0.3597032731195812, 0.10302393616190555, -0.3196679952098325, -0.03802625274471556, 0.22387704140805628, 0.01344238540304602... |
706.2352 | Electron-acoustic-phonon scattering and electron relaxation in
two-coupled quantum rings | Electron relaxation, induced by acoustic phonons, is studied for coupled
quantum rings in the presence of external fields, both electric and magnetic.
We address the problem of a single electron in vertically coupled GaAs quantum
rings. Electron-phonon interaction is accounted for both deformation potential
and piezo... | cond-mat.other cond-mat.mtrl-sci | electron relaxation induced by acoustic phonons is studied for coupled quantum rings in the presence of external fields both electric and magnetic we address the problem of a single electron in vertically coupled gaas quantum rings electronphonon interaction is accounted for both deformation potential and piezoelectric... | [['electron', 'relaxation', 'induced', 'by', 'acoustic', 'phonons', 'is', 'studied', 'for', 'coupled', 'quantum', 'rings', 'in', 'the', 'presence', 'of', 'external', 'fields', 'both', 'electric', 'and', 'magnetic', 'we', 'address', 'the', 'problem', 'of', 'a', 'single', 'electron', 'in', 'vertically', 'coupled', 'gaas'... | [-0.21704691833860817, 0.2074298341359411, -0.0012579387319939478, 0.053222053810688, 0.007612992219981693, -0.13804918525829202, -0.021301530128610986, 0.38233943590450853, -0.2987310005795388, -0.28534253397513004, 0.02678599835351287, -0.28433475363999605, -0.08969666615261564, 0.19191418160418314, 0.078274190106562... |
706.2353 | Modeling partitioning of Min proteins between daughter cells after
septation in Escherichia coli | Ongoing sub-cellular oscillation of Min proteins is required to block
minicelling in E. coli. Experimentally, Min oscillations are seen in newly
divided cells and no minicells are produced. In model Min systems many daughter
cells do not oscillate following septation because of unequal partitioning of
Min proteins be... | q-bio.SC | ongoing subcellular oscillation of min proteins is required to block minicelling in e coli experimentally min oscillations are seen in newly divided cells and no minicells are produced in model min systems many daughter cells do not oscillate following septation because of unequal partitioning of min proteins between t... | [['ongoing', 'subcellular', 'oscillation', 'of', 'min', 'proteins', 'is', 'required', 'to', 'block', 'minicelling', 'in', 'e', 'coli', 'experimentally', 'min', 'oscillations', 'are', 'seen', 'in', 'newly', 'divided', 'cells', 'and', 'no', 'minicells', 'are', 'produced', 'in', 'model', 'min', 'systems', 'many', 'daughte... | [-0.12996458525166793, 0.2173132070723702, 0.01712155261210522, 0.07300667347860915, -0.0070766765514717386, -0.14626346423071535, 0.08124854936100104, 0.3723283748690258, -0.2783746573012596, -0.2975751113574541, 0.027140028223477525, -0.2912665907485301, -0.15989733722184182, 0.14613148789537853, -0.10554019709610764... |
706.2354 | FPTAS for optimizing polynomials over the mixed-integer points of
polytopes in fixed dimension | We show the existence of a fully polynomial-time approximation scheme (FPTAS)
for the problem of maximizing a non-negative polynomial over mixed-integer sets
in convex polytopes, when the number of variables is fixed. Moreover, using a
weaker notion of approximation, we show the existence of a fully
polynomial-time a... | math.OC | we show the existence of a fully polynomialtime approximation scheme fptas for the problem of maximizing a nonnegative polynomial over mixedinteger sets in convex polytopes when the number of variables is fixed moreover using a weaker notion of approximation we show the existence of a fully polynomialtime approximation... | [['we', 'show', 'the', 'existence', 'of', 'a', 'fully', 'polynomialtime', 'approximation', 'scheme', 'fptas', 'for', 'the', 'problem', 'of', 'maximizing', 'a', 'nonnegative', 'polynomial', 'over', 'mixedinteger', 'sets', 'in', 'convex', 'polytopes', 'when', 'the', 'number', 'of', 'variables', 'is', 'fixed', 'moreover',... | [-0.19093563218808007, 0.0024958715029141684, -0.0745978337039964, 0.06425863617267977, -0.052583704204557255, -0.13948669685568246, 0.10132185054115123, 0.3416814119555056, -0.38397560778280926, -0.25107729833366144, 0.09972578700722402, -0.2505151628025083, -0.14650689847702678, 0.1693637900332558, -0.085283042423220... |
706.2355 | Supergravity origin of the MSSM inflation | We consider the supergravity origin of the recently proposed MSSM
inflationary model, which relies on the existence of a saddle point along a
dimension six flat direction. We derive the conditions that the Kahler
potential has to satisfy for the saddle point to exist irrespective of the
hidden sector vevs. We show th... | hep-th astro-ph hep-ph | we consider the supergravity origin of the recently proposed mssm inflationary model which relies on the existence of a saddle point along a dimension six flat direction we derive the conditions that the kahler potential has to satisfy for the saddle point to exist irrespective of the hidden sector vevs we show that th... | [['we', 'consider', 'the', 'supergravity', 'origin', 'of', 'the', 'recently', 'proposed', 'mssm', 'inflationary', 'model', 'which', 'relies', 'on', 'the', 'existence', 'of', 'a', 'saddle', 'point', 'along', 'a', 'dimension', 'six', 'flat', 'direction', 'we', 'derive', 'the', 'conditions', 'that', 'the', 'kahler', 'pote... | [-0.1801109703306697, 0.13456278474217181, -0.06967863271895208, 0.12291788725476516, -0.12010430633825692, -0.18663930632174014, 0.011339511539738037, 0.36151160305169855, -0.20078927635117189, -0.2625674585407404, 0.09696275933130988, -0.19527268419532398, -0.16003555239815462, 0.1295184244916431, -0.0493446921145445... |
706.2356 | Anonymous quantum communication | We present the first protocol for the anonymous transmission of a quantum
state that is information-theoretically secure against an active adversary,
without any assumption on the number of corrupt participants. The anonymity of
the sender and receiver is perfectly preserved, and the privacy of the quantum
state is p... | quant-ph | we present the first protocol for the anonymous transmission of a quantum state that is informationtheoretically secure against an active adversary without any assumption on the number of corrupt participants the anonymity of the sender and receiver is perfectly preserved and the privacy of the quantum state is protect... | [['we', 'present', 'the', 'first', 'protocol', 'for', 'the', 'anonymous', 'transmission', 'of', 'a', 'quantum', 'state', 'that', 'is', 'informationtheoretically', 'secure', 'against', 'an', 'active', 'adversary', 'without', 'any', 'assumption', 'on', 'the', 'number', 'of', 'corrupt', 'participants', 'the', 'anonymity',... | [-0.24416886865911844, 0.14469291698043482, -0.08667920287517668, 0.034188331993188235, -0.017793120337125747, -0.3373778792532179, 0.13350037657158467, 0.3479463907808644, -0.28969091238472067, -0.2758314933049158, 0.10553170147112309, -0.2989667624470244, -0.06761158566958117, 0.12291665911421325, -0.1371540800867222... |
706.2357 | Charm-quark fragmentation with an effective coupling constant | We use a recently proposed non-perturbative model, based on an effective
strong coupling constant and free from tunable parameters, to study c-flavoured
hadron production in e+e- annihilation. Charm-quark production is described in
the framework of perturbative fragmentation functions, with NLO coefficient
functions,... | hep-ph | we use a recently proposed nonperturbative model based on an effective strong coupling constant and free from tunable parameters to study cflavoured hadron production in ee annihilation charmquark production is described in the framework of perturbative fragmentation functions with nlo coefficient functions nll nonsing... | [['we', 'use', 'a', 'recently', 'proposed', 'nonperturbative', 'model', 'based', 'on', 'an', 'effective', 'strong', 'coupling', 'constant', 'and', 'free', 'from', 'tunable', 'parameters', 'to', 'study', 'cflavoured', 'hadron', 'production', 'in', 'ee', 'annihilation', 'charmquark', 'production', 'is', 'described', 'in'... | [-0.04095458033370027, 0.09645445961947328, -0.12452535861088201, 0.13867047532291438, -0.042950520157599106, -0.08098820152129822, 0.04022949294318469, 0.34671072135321224, -0.15671571034144086, -0.2660488987443013, -0.0009292389090077426, -0.34959189793190515, -0.019462834398906965, 0.16515518059858528, 0.05959354825... |
706.2358 | Measurement of the Lambda_b lifetime using semileptonic decays | We report a measurement of the Lambda_b lifetime using a sample corresponding
to 1.3 fb$^{-1}$ of data collected by the D0 experiment in 2002--2006 during
Run II of the Fermilab Tevatron collider. The Lambda_b baryon is reconstructed
via the decay Lambda_b -> mu nu Lambda_c X. Using $4437 \pm 329$ signal
candidates, ... | hep-ex | we report a measurement of the lambda_b lifetime using a sample corresponding to 13 fb1 of data collected by the d0 experiment in 20022006 during run ii of the fermilab tevatron collider the lambda_b baryon is reconstructed via the decay lambda_b mu nu lambda_c x using 4437 pm 329 signal candidates we measure the lambd... | [['we', 'report', 'a', 'measurement', 'of', 'the', 'lambda_b', 'lifetime', 'using', 'a', 'sample', 'corresponding', 'to', '13', 'fb1', 'of', 'data', 'collected', 'by', 'the', 'd0', 'experiment', 'in', '20022006', 'during', 'run', 'ii', 'of', 'the', 'fermilab', 'tevatron', 'collider', 'the', 'lambda_b', 'baryon', 'is', ... | [-0.05431088901697153, 0.19221017099440052, -0.09445232112544129, 0.06316263405101216, -0.04876305711320994, -0.11162133714610553, 0.08911684477359551, 0.28425571699458435, -0.17775039049566735, -0.28470778180263845, -0.027130986694302636, -0.4271776619400964, 0.1216752910425505, 0.1253940146079803, 0.10190699907533084... |
706.2359 | Electronic compressibility of a graphene bilayer | We calculate the electronic compressibility arising from electron-electron
interactions for a graphene bilayer within the Hartree-Fock approximation. We
show that, due to the chiral nature of the particles in this system, the
compressibility is rather different from those of either the two-dimensional
electron gas or... | cond-mat.str-el | we calculate the electronic compressibility arising from electronelectron interactions for a graphene bilayer within the hartreefock approximation we show that due to the chiral nature of the particles in this system the compressibility is rather different from those of either the twodimensional electron gas or ordinar... | [['we', 'calculate', 'the', 'electronic', 'compressibility', 'arising', 'from', 'electronelectron', 'interactions', 'for', 'a', 'graphene', 'bilayer', 'within', 'the', 'hartreefock', 'approximation', 'we', 'show', 'that', 'due', 'to', 'the', 'chiral', 'nature', 'of', 'the', 'particles', 'in', 'this', 'system', 'the', '... | [-0.15965384307796635, 0.19748172298940792, -0.06370593491754885, 0.08296020516346014, 0.017596413649423697, -0.09419486412323665, 0.06644552639214495, 0.31480360975445704, -0.30964452606560877, -0.26502678110155947, -0.0594979002868735, -0.3645513472905339, -0.13997906862574003, 0.1145148971524133, 0.0942197838381236,... |
706.236 | Magnetorotational collapse of very massive stars to black holes in full
general relativity | We perform axisymmetric simulations of the magnetorotational collapse of very
massive stars in full general relativity. Our simulations are applicable to the
collapse of supermassive stars (M > 10^3M_sun) and to very massive Pop III
stars. We model our initial configurations by n=3 polytropes. The ratio of
magnetic t... | astro-ph gr-qc | we perform axisymmetric simulations of the magnetorotational collapse of very massive stars in full general relativity our simulations are applicable to the collapse of supermassive stars m 103m_sun and to very massive pop iii stars we model our initial configurations by n3 polytropes the ratio of magnetic to rotationa... | [['we', 'perform', 'axisymmetric', 'simulations', 'of', 'the', 'magnetorotational', 'collapse', 'of', 'very', 'massive', 'stars', 'in', 'full', 'general', 'relativity', 'our', 'simulations', 'are', 'applicable', 'to', 'the', 'collapse', 'of', 'supermassive', 'stars', 'm', '103m_sun', 'and', 'to', 'very', 'massive', 'po... | [-0.1646608307694802, 0.16674178370715928, -0.04111434117069903, 0.13771125721868505, -0.08429062053135833, -0.08657179513008363, 0.006955883382147873, 0.32965472996565887, -0.1970949433679053, -0.30662263481543506, 0.09729221752294719, -0.2452831925379716, 0.003666720797635537, 0.19958299602088211, -0.0026893938943510... |
706.2361 | A Parallactic Distance of 389 +24/-21 parsecs to the Orion Nebula
Cluster from Very Long Baseline Array Observations | We determine the parallax and proper motion of the flaring, non-thermal radio
star GMR A, a member of the Orion Nebula Cluster, using Very Long Baseline
Array observations. Based on the parallax, we measure a distance of 389 +24/-21
parsecs to the source. Our measurement places the Orion Nebula Cluster
considerably c... | astro-ph | we determine the parallax and proper motion of the flaring nonthermal radio star gmr a a member of the orion nebula cluster using very long baseline array observations based on the parallax we measure a distance of 389 2421 parsecs to the source our measurement places the orion nebula cluster considerably closer than t... | [['we', 'determine', 'the', 'parallax', 'and', 'proper', 'motion', 'of', 'the', 'flaring', 'nonthermal', 'radio', 'star', 'gmr', 'a', 'a', 'member', 'of', 'the', 'orion', 'nebula', 'cluster', 'using', 'very', 'long', 'baseline', 'array', 'observations', 'based', 'on', 'the', 'parallax', 'we', 'measure', 'a', 'distance'... | [-0.06158963547816046, 0.11276593171999234, -0.07330717109613308, 0.07343176348299227, -0.1046232550538012, -0.002461768579160591, 0.13741982160938293, 0.40254764913135216, -0.15974841424177924, -0.3838138349917756, 0.01408333276073691, -0.2717112303641038, 0.021018462384730076, 0.1974897142617079, -0.07291518197763719... |
706.2362 | Magnetization plateaus and sublattice ordering in easy axis Kagome
lattice antiferromagnets | We study kagome lattice antiferromagnets where the effects of easy axis
single-ion anisotropy ($D$) dominates over the Heisenberg exchange $J$. For $S
\ge 3/2$, virtual quantum fluctuations help lift the extensive classical
degeneracy. We demonstrate the presence of a one-third magnetization plateau
for a broad range... | cond-mat.str-el | we study kagome lattice antiferromagnets where the effects of easy axis singleion anisotropy d dominates over the heisenberg exchange j for s ge 32 virtual quantum fluctuations help lift the extensive classical degeneracy we demonstrate the presence of a onethird magnetization plateau for a broad range of magnetic fiel... | [['we', 'study', 'kagome', 'lattice', 'antiferromagnets', 'where', 'the', 'effects', 'of', 'easy', 'axis', 'singleion', 'anisotropy', 'd', 'dominates', 'over', 'the', 'heisenberg', 'exchange', 'j', 'for', 's', 'ge', '32', 'virtual', 'quantum', 'fluctuations', 'help', 'lift', 'the', 'extensive', 'classical', 'degeneracy... | [-0.24288781741311274, 0.2432844152152227, -0.021266765602043654, 0.056392786533647855, -0.1048017074607571, -0.15507089324055776, 0.04762338574210385, 0.3852223715189346, -0.2904954800695771, -0.28909822223283865, 0.05898043525631143, -0.2591793710033935, -0.04812332559469165, 0.14109250291027037, 0.058672428209482146... |
706.2363 | Dying Dyons Don't Count | The dyonic 1/4-BPS states in 4D string theory with N=4 spacetime
supersymmetry are counted by a Siegel modular form. The pole structure of the
modular form leads to a contour dependence in the counting formula obscuring
its duality invariance. We exhibit the relation between this ambiguity and the
(dis-)appearance of... | hep-th | the dyonic 14bps states in 4d string theory with n4 spacetime supersymmetry are counted by a siegel modular form the pole structure of the modular form leads to a contour dependence in the counting formula obscuring its duality invariance we exhibit the relation between this ambiguity and the disappearance of bound sta... | [['the', 'dyonic', '14bps', 'states', 'in', '4d', 'string', 'theory', 'with', 'n4', 'spacetime', 'supersymmetry', 'are', 'counted', 'by', 'a', 'siegel', 'modular', 'form', 'the', 'pole', 'structure', 'of', 'the', 'modular', 'form', 'leads', 'to', 'a', 'contour', 'dependence', 'in', 'the', 'counting', 'formula', 'obscur... | [-0.1682249437706073, 0.13841688679859146, -0.1142060036400438, 0.1576857173653044, -0.0699143952142421, -0.11707130867928843, 0.06292863613860288, 0.2905856064671624, -0.17752113057838254, -0.3057207349281181, 0.072593672531991, -0.28858078552514943, -0.17524194274701074, 0.12919548464755357, -0.052771454801599324, 0.... |
706.2364 | Super Star Cluster NGC1705-1: A Local Analogue to the Birthsite of
Long-duration Gamma-ray Bursts | Recent observations suggest that global properties of the host galaxies for
long-duration gamma-ray bursts (GRBs) are particularly well-suited for creating
the massive star progenitors of these GRBs. Motivated by the hypothesis that
massive young star clusters located in metal-poor, low-metallicity galaxies are
a nat... | astro-ph | recent observations suggest that global properties of the host galaxies for longduration gammaray bursts grbs are particularly wellsuited for creating the massive star progenitors of these grbs motivated by the hypothesis that massive young star clusters located in metalpoor lowmetallicity galaxies are a natural births... | [['recent', 'observations', 'suggest', 'that', 'global', 'properties', 'of', 'the', 'host', 'galaxies', 'for', 'longduration', 'gammaray', 'bursts', 'grbs', 'are', 'particularly', 'wellsuited', 'for', 'creating', 'the', 'massive', 'star', 'progenitors', 'of', 'these', 'grbs', 'motivated', 'by', 'the', 'hypothesis', 'th... | [-0.044091542124152484, 0.1248478383553565, -0.012312897143561227, 0.15842910322713238, -0.07772805988373846, -0.06941412283137803, 0.06739184302504095, 0.47278290320383876, -0.11951601834111585, -0.30196674374735305, -0.030997326622079862, -0.294752466528175, -0.000843313066401945, 0.18153302729278728, -0.015256971150... |
706.2365 | Chain motifs: The tails and handles of complex networks | Great part of the interest in complex networks has been motivated by the
presence of structured, frequently non-uniform, connectivity. Because diverse
connectivity patterns tend to result in distinct network dynamics, and also
because they provide the means to identify and classify several types of
complex networks, ... | cond-mat.dis-nn cond-mat.stat-mech | great part of the interest in complex networks has been motivated by the presence of structured frequently nonuniform connectivity because diverse connectivity patterns tend to result in distinct network dynamics and also because they provide the means to identify and classify several types of complex networks it becom... | [['great', 'part', 'of', 'the', 'interest', 'in', 'complex', 'networks', 'has', 'been', 'motivated', 'by', 'the', 'presence', 'of', 'structured', 'frequently', 'nonuniform', 'connectivity', 'because', 'diverse', 'connectivity', 'patterns', 'tend', 'to', 'result', 'in', 'distinct', 'network', 'dynamics', 'and', 'also', ... | [-0.15954190833224557, 0.06473412040944507, -0.018343195663637495, 0.06562708462343964, -0.04113483870057517, -0.13785917595875147, 0.00897023750077848, 0.414160038918665, -0.2792917497589765, -0.3156140451843119, 0.11337662805307691, -0.28124676606528565, -0.21062882844949796, 0.18498240123485898, -0.04442916583422929... |
706.2366 | Theoretical study of ferroelectric potassium nitrate | We present a detailed study of the structural behavior and polarization
reversal mechanism in phase III of KNO$_3$, an unusual ferroelectric material
in which the nitrate groups rotate during polarization reversal. This material
was one of several studied in a previous work [O. Di\'eguez and D. Vanderbilt,
Phys. Rev.... | cond-mat.mtrl-sci | we present a detailed study of the structural behavior and polarization reversal mechanism in phase iii of kno_3 an unusual ferroelectric material in which the nitrate groups rotate during polarization reversal this material was one of several studied in a previous work o dieguez and d vanderbilt phys rev lett bf 96 05... | [['we', 'present', 'a', 'detailed', 'study', 'of', 'the', 'structural', 'behavior', 'and', 'polarization', 'reversal', 'mechanism', 'in', 'phase', 'iii', 'of', 'kno_3', 'an', 'unusual', 'ferroelectric', 'material', 'in', 'which', 'the', 'nitrate', 'groups', 'rotate', 'during', 'polarization', 'reversal', 'this', 'mater... | [-0.1410420494124053, 0.09624927248589829, -0.07852655692747043, -0.02558482502692289, -0.03729348957178093, -0.07808316122259824, 0.08977921386249363, 0.38819720230155413, -0.20349920492153614, -0.3096086879050539, 0.01686953717707506, -0.25929927918158713, -0.18519691323500967, 0.16465371358658998, -0.030643147392378... |
706.2367 | Weyssenhoff fluid dynamics in general relativity using a 1+3 covariant
approach | The Weyssenhoff fluid is a perfect fluid with spin where the spin of the
matter fields is the source of torsion in an Einstein-Cartan framework. Obukhov
and Korotky showed that this fluid can be described as an effective fluid with
spin in general relativity. A dynamical analysis of such a fluid is performed
in a gau... | gr-qc astro-ph | the weyssenhoff fluid is a perfect fluid with spin where the spin of the matter fields is the source of torsion in an einsteincartan framework obukhov and korotky showed that this fluid can be described as an effective fluid with spin in general relativity a dynamical analysis of such a fluid is performed in a gauge in... | [['the', 'weyssenhoff', 'fluid', 'is', 'a', 'perfect', 'fluid', 'with', 'spin', 'where', 'the', 'spin', 'of', 'the', 'matter', 'fields', 'is', 'the', 'source', 'of', 'torsion', 'in', 'an', 'einsteincartan', 'framework', 'obukhov', 'and', 'korotky', 'showed', 'that', 'this', 'fluid', 'can', 'be', 'described', 'as', 'an'... | [-0.1885859314352274, 0.16329284019308576, -0.15108666903118498, 0.008170970914808591, -0.06752335817370679, -0.1159645055886358, -0.07611703552958585, 0.2574198630004737, -0.25247518437885746, -0.3244853374961111, 0.05804218714888755, -0.22582922188670748, -0.09825674921859862, 0.14602764387682235, -0.0108473790646290... |
706.2368 | A Note on Carleman's Inequality | We study a weighted version of Carleman's inequality via Carleman's original
approach. As an application of our result, we prove a conjecture of Bennett.
| math.CA | we study a weighted version of carlemans inequality via carlemans original approach as an application of our result we prove a conjecture of bennett | [['we', 'study', 'a', 'weighted', 'version', 'of', 'carlemans', 'inequality', 'via', 'carlemans', 'original', 'approach', 'as', 'an', 'application', 'of', 'our', 'result', 'we', 'prove', 'a', 'conjecture', 'of', 'bennett']] | [-0.09139263924832146, -0.05870824712170967, -0.16735371543715397, 0.09886202221969143, -0.01161051339780291, -0.09778396664963414, 0.10348286076138417, 0.2414865454969307, -0.2798020144691691, -0.2949132702002923, 0.115844593810228, -0.20348693631240167, -0.24020359758287668, 0.27282836474478245, -0.19438557346196225,... |
706.2369 | Surface Operators and Knot Homologies | Topological gauge theories in four dimensions which admit surface operators
provide a natural framework for realizing homological knot invariants. Every
such theory leads to an action of the braid group on branes on the
corresponding moduli space. This action plays a key role in the construction of
homological knot i... | hep-th math.GT math.QA | topological gauge theories in four dimensions which admit surface operators provide a natural framework for realizing homological knot invariants every such theory leads to an action of the braid group on branes on the corresponding moduli space this action plays a key role in the construction of homological knot invar... | [['topological', 'gauge', 'theories', 'in', 'four', 'dimensions', 'which', 'admit', 'surface', 'operators', 'provide', 'a', 'natural', 'framework', 'for', 'realizing', 'homological', 'knot', 'invariants', 'every', 'such', 'theory', 'leads', 'to', 'an', 'action', 'of', 'the', 'braid', 'group', 'on', 'branes', 'on', 'the... | [-0.1667383724451882, 0.12218148024406043, -0.15736487491072662, 0.06658508771879337, -0.09788061265875544, -0.14748194712835053, -0.047028075498242845, 0.23821298391333567, -0.2181885979697925, -0.317706797611001, 0.10870348993921652, -0.22872829320840538, -0.2351628300476525, 0.17086567435609668, -0.1722765323223971,... |
706.237 | Strange attractors in periodically-kicked degenerate Hopf bifurcations | We prove that spiral sinks (stable foci of vector fields) can be transformed
into strange attractors exhibiting sustained, observable chaos if subjected to
periodic pulsatile forcing. We show that this phenomenon occurs in the context
of periodically-kicked degenerate supercritical Hopf bifurcations. The results
and ... | math.DS math-ph math.MP | we prove that spiral sinks stable foci of vector fields can be transformed into strange attractors exhibiting sustained observable chaos if subjected to periodic pulsatile forcing we show that this phenomenon occurs in the context of periodicallykicked degenerate supercritical hopf bifurcations the results and their pr... | [['we', 'prove', 'that', 'spiral', 'sinks', 'stable', 'foci', 'of', 'vector', 'fields', 'can', 'be', 'transformed', 'into', 'strange', 'attractors', 'exhibiting', 'sustained', 'observable', 'chaos', 'if', 'subjected', 'to', 'periodic', 'pulsatile', 'forcing', 'we', 'show', 'that', 'this', 'phenomenon', 'occurs', 'in', ... | [-0.17861421087022442, 0.1933246841869102, -0.10523452804638789, 0.09246976542322395, -0.06287412081773465, -0.15041404881586248, 0.03573950295014164, 0.30590553945646837, -0.32065624984411095, -0.16228271026450855, 0.12665394675523903, -0.19259761847363105, -0.22591168963565275, 0.20980722536691107, -0.075911788850163... |
706.2371 | The rotating Morse potential model for diatomic molecules in the
tridiagonal J-matrix representation: I. Bound states | This is the first in a series of articles in which we study the rotating
Morse potential model for diatomic molecules in the tridiagonal J-matrix
representation. Here, we compute the bound states energy spectrum by
diagonalizing the finite dimensional Hamiltonian matrix of H2, LiH, HCl and CO
molecules for arbitrary ... | physics.chem-ph physics.atom-ph | this is the first in a series of articles in which we study the rotating morse potential model for diatomic molecules in the tridiagonal jmatrix representation here we compute the bound states energy spectrum by diagonalizing the finite dimensional hamiltonian matrix of h2 lih hcl and co molecules for arbitrary angular... | [['this', 'is', 'the', 'first', 'in', 'a', 'series', 'of', 'articles', 'in', 'which', 'we', 'study', 'the', 'rotating', 'morse', 'potential', 'model', 'for', 'diatomic', 'molecules', 'in', 'the', 'tridiagonal', 'jmatrix', 'representation', 'here', 'we', 'compute', 'the', 'bound', 'states', 'energy', 'spectrum', 'by', '... | [-0.07323345028848019, 0.0593834805174924, -0.06365834385209349, 0.03126765271969456, -0.0018472709991740732, -0.1336859094532523, 0.03738035199332341, 0.3984687901189867, -0.20154112626640303, -0.2450178453241879, 0.028441906960479, -0.27921536601728425, -0.1288550160869183, 0.1692914614774603, 0.05172315262310769, 0.... |
706.2372 | Prym varieties and applications | The classical definition of Prym varieties deals with the unramified covers
of curves. The aim of the present paper is to give explicit algebraic
descriptions of the Prym varieties associated to ramified double covers of
algebraic curves. We make a careful study of the connection with the concept of
algebraic complet... | math.AG math-ph math.MP | the classical definition of prym varieties deals with the unramified covers of curves the aim of the present paper is to give explicit algebraic descriptions of the prym varieties associated to ramified double covers of algebraic curves we make a careful study of the connection with the concept of algebraic completely ... | [['the', 'classical', 'definition', 'of', 'prym', 'varieties', 'deals', 'with', 'the', 'unramified', 'covers', 'of', 'curves', 'the', 'aim', 'of', 'the', 'present', 'paper', 'is', 'to', 'give', 'explicit', 'algebraic', 'descriptions', 'of', 'the', 'prym', 'varieties', 'associated', 'to', 'ramified', 'double', 'covers',... | [-0.2076658649602905, -0.010462332051247358, -0.15979234817496035, 0.1047054804603249, -0.15175448586523999, -0.13013131618936313, 0.020498911528193275, 0.2614859450404765, -0.3190417262085248, -0.20912240367761115, 0.09694021430368593, -0.24286242037487682, -0.1660693472076673, 0.2556667812168598, -0.20866524284065235... |
706.2373 | A widely tunable parametric amplifier based on a SQUID array resonator | We create a Josephson parametric amplifier from a transmission line resonator
whose inner conductor is made from a series SQUID array. By changing the
magnetic flux through the SQUID loops, we are able to adjust the circuit's
resonance frequency and, consenquently, the center of the amplified band,
between 4 and 7.8 ... | cond-mat.supr-con cond-mat.mes-hall | we create a josephson parametric amplifier from a transmission line resonator whose inner conductor is made from a series squid array by changing the magnetic flux through the squid loops we are able to adjust the circuits resonance frequency and consenquently the center of the amplified band between 4 and 78 ghz we ob... | [['we', 'create', 'a', 'josephson', 'parametric', 'amplifier', 'from', 'a', 'transmission', 'line', 'resonator', 'whose', 'inner', 'conductor', 'is', 'made', 'from', 'a', 'series', 'squid', 'array', 'by', 'changing', 'the', 'magnetic', 'flux', 'through', 'the', 'squid', 'loops', 'we', 'are', 'able', 'to', 'adjust', 'th... | [-0.15867357367028792, 0.132542245828857, 0.007019869480282068, -0.014051230144686996, -0.06528269668420156, -0.19603800416613618, 0.1106312263244763, 0.4311349351207415, -0.20901604392876227, -0.3428042200518151, 0.0993481898245712, -0.2874382301171621, -0.12312703204651673, 0.2620528218243271, -0.012435848950408399, ... |
706.2374 | Line and Mean Opacities for Ultracool Dwarfs and Extrasolar Planets | Opacities and chemical abundance data are crucial ingredients of ultracool
dwarf and extrasolar giant planet atmosphere models. We report here on the
detailed sources of molecular opacity data employed by our group for this
application. We also present tables of Rosseland and Planck mean opacities
which are of use in... | astro-ph | opacities and chemical abundance data are crucial ingredients of ultracool dwarf and extrasolar giant planet atmosphere models we report here on the detailed sources of molecular opacity data employed by our group for this application we also present tables of rosseland and planck mean opacities which are of use in som... | [['opacities', 'and', 'chemical', 'abundance', 'data', 'are', 'crucial', 'ingredients', 'of', 'ultracool', 'dwarf', 'and', 'extrasolar', 'giant', 'planet', 'atmosphere', 'models', 'we', 'report', 'here', 'on', 'the', 'detailed', 'sources', 'of', 'molecular', 'opacity', 'data', 'employed', 'by', 'our', 'group', 'for', '... | [-0.022757807726182654, 0.14937381558449922, -0.04471601175960252, 0.08562582224016119, -0.06939426090195364, -0.025143047677254123, 0.10969346344977848, 0.40858262449305144, -0.15254068933427334, -0.342198261006249, 0.04399872997124572, -0.2920791750085598, -0.05545151396139434, 0.19320004347884878, -0.026290361740651... |
706.2375 | Connecting LHC, ILC, and Quintessence | If the cold dark matter consists of weakly interacting massive particles
(WIMPs), anticipated measurements of the WIMP properties at the Large Hadron
Collider (LHC) and the International Linear Collider (ILC) will provide an
unprecedented experimental probe of cosmology at temperatures of order 1 GeV.
It is worth emp... | hep-ph astro-ph hep-th | if the cold dark matter consists of weakly interacting massive particles wimps anticipated measurements of the wimp properties at the large hadron collider lhc and the international linear collider ilc will provide an unprecedented experimental probe of cosmology at temperatures of order 1 gev it is worth emphasizing t... | [['if', 'the', 'cold', 'dark', 'matter', 'consists', 'of', 'weakly', 'interacting', 'massive', 'particles', 'wimps', 'anticipated', 'measurements', 'of', 'the', 'wimp', 'properties', 'at', 'the', 'large', 'hadron', 'collider', 'lhc', 'and', 'the', 'international', 'linear', 'collider', 'ilc', 'will', 'provide', 'an', '... | [-0.08574117238085772, 0.19275543775573845, -0.1506595552428602, 0.15556495115874644, -0.08632347199026888, -0.1526052860575892, -0.04836073519437382, 0.31405816439670237, -0.21676419468493618, -0.3606740429239282, 0.04698011751026945, -0.3050694012705555, 0.022351636753731113, 0.18624384321117932, 0.0635059235790679, ... |
706.2376 | Dynamical Masses for Pre-Main Sequence Stars: A Preliminary Physical
Orbit for V773 Tau A | We report on interferometric and radial-velocity observations of the
double-lined 51-d period binary (A) component of the quadruple pre-main
sequence (PMS) system V773 Tau. With these observations we have estimated
preliminary visual and physical orbits of the V773 Tau A subsystem. Among other
parameters, our orbit m... | astro-ph | we report on interferometric and radialvelocity observations of the doublelined 51d period binary a component of the quadruple premain sequence pms system v773 tau with these observations we have estimated preliminary visual and physical orbits of the v773 tau a subsystem among other parameters our orbit model includes... | [['we', 'report', 'on', 'interferometric', 'and', 'radialvelocity', 'observations', 'of', 'the', 'doublelined', '51d', 'period', 'binary', 'a', 'component', 'of', 'the', 'quadruple', 'premain', 'sequence', 'pms', 'system', 'v773', 'tau', 'with', 'these', 'observations', 'we', 'have', 'estimated', 'preliminary', 'visual... | [-0.10971753384163378, 0.13657896774507153, -0.061114394975579286, 0.042752715655187346, -0.055064107033323095, -0.11581341909309176, 0.0591840997390191, 0.4136718046873898, -0.14980961060353432, -0.37859009361141416, 0.055431178187480175, -0.3119884884990934, 0.01663511312645243, 0.21529787580667803, -0.03466071593764... |
706.2377 | Collisional parton energy loss in a finite size QCD medium revisited:
Off mass-shell effects | We study the collisional energy loss mechanism for particles produced off
mass-shell in a finite size QCD medium. The off mass-shell effects introduced
are to consider particles produced in wave packets instead of plane waves and
the length scale associated to an in-medium particles' life-time. We show that
these eff... | hep-ph | we study the collisional energy loss mechanism for particles produced off massshell in a finite size qcd medium the off massshell effects introduced are to consider particles produced in wave packets instead of plane waves and the length scale associated to an inmedium particles lifetime we show that these effects redu... | [['we', 'study', 'the', 'collisional', 'energy', 'loss', 'mechanism', 'for', 'particles', 'produced', 'off', 'massshell', 'in', 'a', 'finite', 'size', 'qcd', 'medium', 'the', 'off', 'massshell', 'effects', 'introduced', 'are', 'to', 'consider', 'particles', 'produced', 'in', 'wave', 'packets', 'instead', 'of', 'plane',... | [-0.12201525109845239, 0.2318380858534412, -0.06577722296152297, 0.13836258269177118, -0.03014290290842722, -0.027600129210465663, 0.009721760000395882, 0.358734507281501, -0.2774897135567625, -0.2829734733378565, 0.03379504030742389, -0.310395837740486, -0.02929498023890496, 0.14768171102974798, 0.02659667733855344, 0... |
706.2378 | Geysers in the Lagoon: new Herbig-Haro objects in M8 | Aims: We search for direct evidence of ongoing star formation by accretion in
the Lagoon Nebula (M8), using optical wide-field narrow-band imaging obtained
at La Silla Observatory.
Methods: We examine [SII] and Halpha images for line-emission features that
could be interpreted as signatures of outflow activity of t... | astro-ph | aims we search for direct evidence of ongoing star formation by accretion in the lagoon nebula m8 using optical widefield narrowband imaging obtained at la silla observatory methods we examine sii and halpha images for lineemission features that could be interpreted as signatures of outflow activity of the exciting sou... | [['aims', 'we', 'search', 'for', 'direct', 'evidence', 'of', 'ongoing', 'star', 'formation', 'by', 'accretion', 'in', 'the', 'lagoon', 'nebula', 'm8', 'using', 'optical', 'widefield', 'narrowband', 'imaging', 'obtained', 'at', 'la', 'silla', 'observatory', 'methods', 'we', 'examine', 'sii', 'and', 'halpha', 'images', '... | [-0.06551220314133735, 0.06747398085093924, -0.055128180577109255, 0.1229597294703126, -0.11893911116889545, -0.0666829332177128, 0.09003475486533716, 0.47107639023590653, -0.16606724386413893, -0.3568744233321576, 0.08837817990708918, -0.29687708834452287, -0.09937073928082273, 0.20553097253709676, -0.0244474475296945... |
706.2379 | The Derivative Expansion of the Effective Action and the Renormalization
Group Equation | The perturbative evaluation of the effective action can be expanded in powers
of derivatives of the external field. We apply the renormalization group
equation to the term in the effective action that is second order in the
derivatives of the external field and all orders in a constant external field,
considering bot... | hep-th | the perturbative evaluation of the effective action can be expanded in powers of derivatives of the external field we apply the renormalization group equation to the term in the effective action that is second order in the derivatives of the external field and all orders in a constant external field considering both ma... | [['the', 'perturbative', 'evaluation', 'of', 'the', 'effective', 'action', 'can', 'be', 'expanded', 'in', 'powers', 'of', 'derivatives', 'of', 'the', 'external', 'field', 'we', 'apply', 'the', 'renormalization', 'group', 'equation', 'to', 'the', 'term', 'in', 'the', 'effective', 'action', 'that', 'is', 'second', 'order... | [-0.19733044594599336, 0.15274087472261824, -0.09627816007089089, 0.07700963873831629, -0.10681922755240664, -0.079694869292343, -0.003212527947171646, 0.3426073405699914, -0.23476791155396723, -0.294181733451528, 0.07214104001040515, -0.25156966384555046, -0.13258572193045243, 0.13027353681322626, 0.011929928722298321... |
706.238 | Tightening of knots in proteins | We perform theoretical studies of stretching of 20 proteins with knots within
a coarse grained model. The knot's ends are found to jump to well defined
sequential locations that are associated with sharp turns whereas in
homopolymers they diffuse around and eventually slide off. The waiting times of
the jumps are inc... | q-bio.BM cond-mat.soft | we perform theoretical studies of stretching of 20 proteins with knots within a coarse grained model the knots ends are found to jump to well defined sequential locations that are associated with sharp turns whereas in homopolymers they diffuse around and eventually slide off the waiting times of the jumps are increasi... | [['we', 'perform', 'theoretical', 'studies', 'of', 'stretching', 'of', '20', 'proteins', 'with', 'knots', 'within', 'a', 'coarse', 'grained', 'model', 'the', 'knots', 'ends', 'are', 'found', 'to', 'jump', 'to', 'well', 'defined', 'sequential', 'locations', 'that', 'are', 'associated', 'with', 'sharp', 'turns', 'whereas... | [-0.13507443759905025, 0.1991409065730467, -0.07958616165922501, 0.09082331710079736, -0.0355017780187867, -0.16999511663625771, 0.060058769124962795, 0.4688264549382635, -0.2754432630750376, -0.2913866511410782, 0.09861796104972176, -0.27741503139101975, -0.06940237680651448, 0.1707940152201273, -0.04248797472226559, ... |
706.2381 | Koszul duality in deformation quantization, I | Let $\alpha$ be a polynomial Poisson bivector on a finite-dimensional vector
space $V$ over $\mathbb{C}$. Then Kontsevich [K97] gives a formula for a
quantization $f\star g$ of the algebra $S(V)^*$. We give a construction of an
algebra with the PBW property defined from $\alpha$ by generators and
relations. Namely, w... | math.QA | let alpha be a polynomial poisson bivector on a finitedimensional vector space v over mathbbc then kontsevich k97 gives a formula for a quantization fstar g of the algebra sv we give a construction of an algebra with the pbw property defined from alpha by generators and relations namely we define an algebra as the quot... | [['let', 'alpha', 'be', 'a', 'polynomial', 'poisson', 'bivector', 'on', 'a', 'finitedimensional', 'vector', 'space', 'v', 'over', 'mathbbc', 'then', 'kontsevich', 'k97', 'gives', 'a', 'formula', 'for', 'a', 'quantization', 'fstar', 'g', 'of', 'the', 'algebra', 'sv', 'we', 'give', 'a', 'construction', 'of', 'an', 'algeb... | [-0.1354972804852639, 0.05387897655481404, -0.1169303380329985, 0.049796377931138794, -0.13417816015413347, -0.13277117523766768, -0.024249465893088875, 0.32850085196843565, -0.39960859255875397, -0.19393240841731552, 0.08487766417369369, -0.2173346282616563, -0.1509113119217908, 0.19177211995129703, -0.136143272874948... |
706.2382 | A characteristic observable signature of preferred frame effects in
relativistic binary pulsars | In this paper we develop a consistent, phenomenological methodology to
measure preferred-frame effects (PFEs) in binary pulsars that exhibit a high
rate of periastron advance. We show that in these systems the existence of a
preferred frame for gravity leads to an observable characteristic `signature'
in the timing d... | astro-ph | in this paper we develop a consistent phenomenological methodology to measure preferredframe effects pfes in binary pulsars that exhibit a high rate of periastron advance we show that in these systems the existence of a preferred frame for gravity leads to an observable characteristic signature in the timing data which... | [['in', 'this', 'paper', 'we', 'develop', 'a', 'consistent', 'phenomenological', 'methodology', 'to', 'measure', 'preferredframe', 'effects', 'pfes', 'in', 'binary', 'pulsars', 'that', 'exhibit', 'a', 'high', 'rate', 'of', 'periastron', 'advance', 'we', 'show', 'that', 'in', 'these', 'systems', 'the', 'existence', 'of'... | [-0.1287895673355104, 0.07998731839893801, -0.09460161489305008, 0.0865970276842143, -0.12736449725302854, -0.10808159723307308, 0.07179610367596287, 0.3561136238998405, -0.2589347274698527, -0.31110297845271545, 0.08560932309917686, -0.2225841916532401, -0.10100962538813228, 0.24192286317374453, -0.04997126624220982, ... |
706.2383 | Allovalency revisited: an analysis of multisite phosphorylation and
substrate rebinding | The utilization of multiple phosphorylation sites in regulating a biological
response is ubiquitous in cell signaling. If each site contributes an
additional, equivalent binding site, then one consequence of an increase in the
number of phosphorylations may be to increase the probability that, upon
disassociation, a ... | q-bio.SC q-bio.MN | the utilization of multiple phosphorylation sites in regulating a biological response is ubiquitous in cell signaling if each site contributes an additional equivalent binding site then one consequence of an increase in the number of phosphorylations may be to increase the probability that upon disassociation a ligand ... | [['the', 'utilization', 'of', 'multiple', 'phosphorylation', 'sites', 'in', 'regulating', 'a', 'biological', 'response', 'is', 'ubiquitous', 'in', 'cell', 'signaling', 'if', 'each', 'site', 'contributes', 'an', 'additional', 'equivalent', 'binding', 'site', 'then', 'one', 'consequence', 'of', 'an', 'increase', 'in', 't... | [-0.08736744412029816, 0.17043115009437315, -0.03099568569354269, 0.112320204914566, -0.028182002140628482, -0.15678309393886303, 0.0884268544429284, 0.37095814592988285, -0.2790846670576871, -0.2644067732247197, -0.012390038976908371, -0.27967361442201977, -0.221571925850986, 0.1454639114880478, -0.044980102280364524,... |
706.2384 | Galois theory of iterated endomorphisms | Given an abelian algebraic group $A$ over a global field $F$, $\alpha \in
A(F)$, and a prime $\ell$, the set of all preimages of $\alpha$ under some
iterate of $[\ell]$ generates an extension of $F$ that contains all
$\ell$-power torsion points as well as a Kummer-type extension. We analyze the
Galois group of this e... | math.NT | given an abelian algebraic group a over a global field f alpha in af and a prime ell the set of all preimages of alpha under some iterate of ell generates an extension of f that contains all ellpower torsion points as well as a kummertype extension we analyze the galois group of this extension and for several classes o... | [['given', 'an', 'abelian', 'algebraic', 'group', 'a', 'over', 'a', 'global', 'field', 'f', 'alpha', 'in', 'af', 'and', 'a', 'prime', 'ell', 'the', 'set', 'of', 'all', 'preimages', 'of', 'alpha', 'under', 'some', 'iterate', 'of', 'ell', 'generates', 'an', 'extension', 'of', 'f', 'that', 'contains', 'all', 'ellpower', '... | [-0.2504410923787021, 0.090611013675945, -0.09669455176359312, 0.037808542442642624, -0.08001314624713335, -0.13297316680710786, -0.01761083614021927, 0.30601274253359073, -0.3342164384222702, -0.2515957413854971, 0.06354009826005452, -0.2794808169040894, -0.09899024976245155, 0.21479137849487967, -0.06247542555460093,... |
706.2385 | Dynamical ultrafast all-optical switching of planar GaAs/AlAs photonic
microcavities | The authors study the ultrafast switching-on and -off of planar GaAs/AlAs
microcavities. Up to 0.8% refractive index changes are achieved by optically
exciting free carriers at 1720 nm and a pulse energy of 1.8 micro Joules. The
cavity resonance is dynamically tracked by measuring reflectivity versus time
delay with ... | physics.optics | the authors study the ultrafast switchingon and off of planar gaasalas microcavities up to 08 refractive index changes are achieved by optically exciting free carriers at 1720 nm and a pulse energy of 18 micro joules the cavity resonance is dynamically tracked by measuring reflectivity versus time delay with tunable la... | [['the', 'authors', 'study', 'the', 'ultrafast', 'switchingon', 'and', 'off', 'of', 'planar', 'gaasalas', 'microcavities', 'up', 'to', '08', 'refractive', 'index', 'changes', 'are', 'achieved', 'by', 'optically', 'exciting', 'free', 'carriers', 'at', '1720', 'nm', 'and', 'a', 'pulse', 'energy', 'of', '18', 'micro', 'jo... | [-0.1282602837183387, 0.2540409959777183, -0.019085838396504923, -0.013827987667592662, 0.00850587215291353, -0.15764000213144952, 0.09530099859222065, 0.47479277719567353, -0.23821451337714386, -0.40950953629002107, 0.0775519497844659, -0.25080893294642437, -0.039908015351692167, 0.21689324472141494, 0.000721192555837... |
706.2386 | The Scattering Polarization of the Sr I 4607 \AA Line at the Diffraction
Limit Resolution of a 1-m Telescope | One of the greatest challenges in solar and stellar physics in coming years
will be to observe the Second Solar Spectrum with a spatial resolution
significantly better than 1 arcsec. This type of scattering polarization
observations would probably allow us to discover hitherto unknown aspects of
the Sun's hidden magn... | astro-ph | one of the greatest challenges in solar and stellar physics in coming years will be to observe the second solar spectrum with a spatial resolution significantly better than 1 arcsec this type of scattering polarization observations would probably allow us to discover hitherto unknown aspects of the suns hidden magnetis... | [['one', 'of', 'the', 'greatest', 'challenges', 'in', 'solar', 'and', 'stellar', 'physics', 'in', 'coming', 'years', 'will', 'be', 'to', 'observe', 'the', 'second', 'solar', 'spectrum', 'with', 'a', 'spatial', 'resolution', 'significantly', 'better', 'than', '1', 'arcsec', 'this', 'type', 'of', 'scattering', 'polarizat... | [-0.0884581010459977, 0.15221311005118948, -0.0376195155960672, 0.08139674910144012, -0.09275548609723737, -0.12078944620638411, 0.005784888212923045, 0.38692915126074495, -0.25383323339146996, -0.35149676695980164, 0.07098746456614616, -0.26143515264779765, -0.10706093219188947, 0.18803608716082046, -0.006620403336007... |
706.2387 | Fermi surface of CeIn3 above the Neel critical field | We report measurements of the de Haas-van Alphen effect in CeIn3 in magnetic
fields extending to ~90 T, well above the Ne'el critical field of Hc ~61 T. The
unreconstructed Fermi surface a-sheet is observed in the high magnetic field
polarized paramagnetic limit, but with its effective mass and Fermi surface
volume s... | cond-mat.str-el cond-mat.mtrl-sci | we report measurements of the de haasvan alphen effect in cein3 in magnetic fields extending to 90 t well above the neel critical field of hc 61 t the unreconstructed fermi surface asheet is observed in the high magnetic field polarized paramagnetic limit but with its effective mass and fermi surface volume strongly re... | [['we', 'report', 'measurements', 'of', 'the', 'de', 'haasvan', 'alphen', 'effect', 'in', 'cein3', 'in', 'magnetic', 'fields', 'extending', 'to', '90', 't', 'well', 'above', 'the', 'neel', 'critical', 'field', 'of', 'hc', '61', 't', 'the', 'unreconstructed', 'fermi', 'surface', 'asheet', 'is', 'observed', 'in', 'the', ... | [-0.20713382508521053, 0.2608787325186469, -0.038059160499033906, 0.05440981900131311, -0.0490197584414008, -0.09439601064800765, 0.08713481467537056, 0.31454813762596157, -0.22521815983333973, -0.3352905960207937, -0.016423869691083604, -0.3024750394803105, -0.06319719349325757, 0.21606039442121983, 0.0149168155457109... |
706.2388 | Longitudinal Spin Measurements with Inclusive Hadrons in Polarized p+p
Collisions at 200 GeV | We present measurements of the double longitudinal spin asymmetries for
inclusive pi0 and pi+(-) production in polarized p+p collisions at sqrt(s) =
200 GeV at mid-rapidity with the STAR detector from the 2005 RHIC run. These
measurements are used to access Delta G/G, the gluon polarization in the
proton. The observe... | hep-ex | we present measurements of the double longitudinal spin asymmetries for inclusive pi0 and pi production in polarized pp collisions at sqrts 200 gev at midrapidity with the star detector from the 2005 rhic run these measurements are used to access delta gg the gluon polarization in the proton the observed unpolarized in... | [['we', 'present', 'measurements', 'of', 'the', 'double', 'longitudinal', 'spin', 'asymmetries', 'for', 'inclusive', 'pi0', 'and', 'pi', 'production', 'in', 'polarized', 'pp', 'collisions', 'at', 'sqrts', '200', 'gev', 'at', 'midrapidity', 'with', 'the', 'star', 'detector', 'from', 'the', '2005', 'rhic', 'run', 'these'... | [-0.03473224331433552, 0.22649933566987915, -0.15123712039452844, 0.1500939166372908, -0.014268808016952659, -0.117749141069258, -0.019355822874266387, 0.37376216245840105, -0.17470576216666295, -0.23400021916521446, -0.10747393921961443, -0.3851462675125471, 0.11967081252285945, 0.16877526254601044, 0.1279700689317126... |
706.2389 | Models for microquasars | I review current models used to interpret the spectra and variability of
microquasars. Among other things, I discuss the structure of the accretion flow
and its dependence on mass accretion rate, the intrinsic connection between hot
comptonizing corona and compact radio jet in the hard state, as well as
possible mode... | astro-ph | i review current models used to interpret the spectra and variability of microquasars among other things i discuss the structure of the accretion flow and its dependence on mass accretion rate the intrinsic connection between hot comptonizing corona and compact radio jet in the hard state as well as possible models for... | [['i', 'review', 'current', 'models', 'used', 'to', 'interpret', 'the', 'spectra', 'and', 'variability', 'of', 'microquasars', 'among', 'other', 'things', 'i', 'discuss', 'the', 'structure', 'of', 'the', 'accretion', 'flow', 'and', 'its', 'dependence', 'on', 'mass', 'accretion', 'rate', 'the', 'intrinsic', 'connection'... | [-0.07465533896819833, 0.10393491125732814, -0.02737440096848097, 0.1619585480639404, -0.11103643291658655, -0.12316012973465103, 0.037846997706699616, 0.44208779587343183, -0.2241867753417836, -0.3248990585225798, 0.12403200944218323, -0.3071144575291534, -0.06674245216874118, 0.24332003678031958, -0.04599946366920683... |
706.239 | Stochastic Parabolic Equations of Full Second Order | A procedure is described for defining a generalized solution for stochastic
differential equations using the Cameron-Martin version of the Wiener Chaos
expansion. Existence and uniqueness of this Wiener Chaos solution is
established for parabolic stochastic PDEs such that both the drift and the
diffusion operators ar... | math.PR math.AP | a procedure is described for defining a generalized solution for stochastic differential equations using the cameronmartin version of the wiener chaos expansion existence and uniqueness of this wiener chaos solution is established for parabolic stochastic pdes such that both the drift and the diffusion operators are of... | [['a', 'procedure', 'is', 'described', 'for', 'defining', 'a', 'generalized', 'solution', 'for', 'stochastic', 'differential', 'equations', 'using', 'the', 'cameronmartin', 'version', 'of', 'the', 'wiener', 'chaos', 'expansion', 'existence', 'and', 'uniqueness', 'of', 'this', 'wiener', 'chaos', 'solution', 'is', 'estab... | [-0.14785265860147775, 0.04276595055125654, -0.0956593712978065, 0.09339739720104262, -0.10539456412661821, -0.08051608392968773, -0.04663014555349946, 0.23689208345487714, -0.37327690437436106, -0.1686203695833683, 0.20977405942045152, -0.264320422206074, -0.1909644104540348, 0.18730736574158072, -0.05529087743721903,... |
706.2391 | From Random Processes to Generalized Fields: A Unified Approach to
Stochastic Integration | The paper studies stochastic integration with respect to Gaussian processes
and fields. It is more convenient to work with a field than a process: by
definition, a field is a collection of stochastic integrals for a class of
deterministic integrands. The problem is then to extend the definition to
random integrands. ... | math.PR | the paper studies stochastic integration with respect to gaussian processes and fields it is more convenient to work with a field than a process by definition a field is a collection of stochastic integrals for a class of deterministic integrands the problem is then to extend the definition to random integrands an orth... | [['the', 'paper', 'studies', 'stochastic', 'integration', 'with', 'respect', 'to', 'gaussian', 'processes', 'and', 'fields', 'it', 'is', 'more', 'convenient', 'to', 'work', 'with', 'a', 'field', 'than', 'a', 'process', 'by', 'definition', 'a', 'field', 'is', 'a', 'collection', 'of', 'stochastic', 'integrals', 'for', 'a... | [-0.1142211555207551, 0.11202096836017403, -0.11572749245920227, 0.07723883351092546, -0.10949039210456314, -0.06946265266637679, 0.04400821266955956, 0.3610510106559272, -0.29309190644857447, -0.21864571210745773, 0.10369635784478339, -0.22473811371742772, -0.19819627145120688, 0.22756918049878902, -0.0620908706348288... |
706.2392 | New interpretation for energy gap $\Delta$ of the cut-off approximation
in the BCS theory of superconductivity | This paper concerns the solution of the self-consistency equation for energy
gap parameter $\Delta_{\bf k}$ in the BCS theory of superconductivity. We show
that there exists a well-defined relation between the solution for energy gap
parameter amplitude $|\Delta_{\bf k}|$ for a general interaction $V_{{\bf
k},{\bf k}... | cond-mat.supr-con | this paper concerns the solution of the selfconsistency equation for energy gap parameter delta_bf k in the bcs theory of superconductivity we show that there exists a welldefined relation between the solution for energy gap parameter amplitude delta_bf k for a general interaction v_bf kbf k and energy gap delta obtain... | [['this', 'paper', 'concerns', 'the', 'solution', 'of', 'the', 'selfconsistency', 'equation', 'for', 'energy', 'gap', 'parameter', 'delta_bf', 'k', 'in', 'the', 'bcs', 'theory', 'of', 'superconductivity', 'we', 'show', 'that', 'there', 'exists', 'a', 'welldefined', 'relation', 'between', 'the', 'solution', 'for', 'ener... | [-0.19074700856058396, 0.1605403372628196, -0.07463733865356541, 0.08049871048760565, -0.036683573253094195, -0.13857466102712215, 0.11749780275746881, 0.35532617584906795, -0.24681681871693084, -0.31569760485009396, 0.0007248755487150208, -0.3047094825296638, -0.05762222557475561, 0.15552489860431556, 0.03713749014625... |
706.2393 | Consequences Of Fully Dressing Quark-Gluon Vertex Function With
Two-Point Gluon Lines | We extend recent studies of the effects of quark-gluon vertex dressing upon
the solutions of the Dyson-Schwinger equation for the quark propagator. A
momentum delta function is used to represent the dominant infrared strength of
the effective gluon propagator so that the resulting integral equations become
algebraic.... | nucl-th | we extend recent studies of the effects of quarkgluon vertex dressing upon the solutions of the dysonschwinger equation for the quark propagator a momentum delta function is used to represent the dominant infrared strength of the effective gluon propagator so that the resulting integral equations become algebraic the q... | [['we', 'extend', 'recent', 'studies', 'of', 'the', 'effects', 'of', 'quarkgluon', 'vertex', 'dressing', 'upon', 'the', 'solutions', 'of', 'the', 'dysonschwinger', 'equation', 'for', 'the', 'quark', 'propagator', 'a', 'momentum', 'delta', 'function', 'is', 'used', 'to', 'represent', 'the', 'dominant', 'infrared', 'stre... | [-0.09259534533019177, 0.1820617979731469, -0.13897370820865035, 0.10489479603478685, -0.13128090768586845, -0.0303890153253451, 0.026506902342662217, 0.34255350969266146, -0.2090923473238945, -0.20531741400714965, 0.027775067439069972, -0.30601474730297923, -0.08045310286805034, 0.1238450822676532, 0.03355044482275843... |
706.2394 | Theory for superconductivity in a magnetic field: A local approximation
approach | We present a microscopic theory for superconductivity in a magnetic field
based on a local approximation approach. We derive an expression for free
energy density $F$ as a function of temperature $T$ and vector potential {\bf
a}, and two basic equations of the theory: the first is an implicit solution
for energy gap ... | cond-mat.supr-con | we present a microscopic theory for superconductivity in a magnetic field based on a local approximation approach we derive an expression for free energy density f as a function of temperature t and vector potential bf a and two basic equations of the theory the first is an implicit solution for energy gap parameter am... | [['we', 'present', 'a', 'microscopic', 'theory', 'for', 'superconductivity', 'in', 'a', 'magnetic', 'field', 'based', 'on', 'a', 'local', 'approximation', 'approach', 'we', 'derive', 'an', 'expression', 'for', 'free', 'energy', 'density', 'f', 'as', 'a', 'function', 'of', 'temperature', 't', 'and', 'vector', 'potential... | [-0.1911408198779843, 0.19086513239845726, -0.04647170563388181, 0.02906765884092676, -0.04404293458031858, -0.13410020377962803, 0.08432349935513887, 0.32773013766447123, -0.2282624862379442, -0.266081024816151, 0.005579955344356896, -0.27628542439685794, -0.08029776148542245, 0.16585517129232005, 0.045295326881294215... |
706.2395 | Combining Weak Lensing Tomography with Halo Clustering to Probe Dark
Energy | Two methods of constraining the properties of dark energy are weak lensing
tomography and cluster counting. Uncertainties in mass calibration of clusters
can be reduced by using the properties of halo clustering (the clustering of
clusters). However, within a single survey, weak lensing and halo clustering
probe the ... | astro-ph | two methods of constraining the properties of dark energy are weak lensing tomography and cluster counting uncertainties in mass calibration of clusters can be reduced by using the properties of halo clustering the clustering of clusters however within a single survey weak lensing and halo clustering probe the same den... | [['two', 'methods', 'of', 'constraining', 'the', 'properties', 'of', 'dark', 'energy', 'are', 'weak', 'lensing', 'tomography', 'and', 'cluster', 'counting', 'uncertainties', 'in', 'mass', 'calibration', 'of', 'clusters', 'can', 'be', 'reduced', 'by', 'using', 'the', 'properties', 'of', 'halo', 'clustering', 'the', 'clu... | [-0.09261642829308589, 0.09902002791566729, -0.1296903190875123, 0.18714850625651774, -0.10931616493505357, -0.07544018476834438, 0.008171835635545585, 0.35357948944312084, -0.22795428971076392, -0.39557353318141303, 0.05898248745410088, -0.2989782450417873, -0.007854304784505165, 0.19588044544411226, 0.028686605045214... |
706.2396 | Model of embedded spaces: the field equations | A study of the Model of Embedded Spaces (MES) with a relativistic version of
Finslerian geometry is continued. The field equations of the MES (Einstein and
Maxwell types) are derived, and this formally completes geometrization of
classical electrodynamics. The minimal action principle leads to geometrization
of the f... | gr-qc | a study of the model of embedded spaces mes with a relativistic version of finslerian geometry is continued the field equations of the mes einstein and maxwell types are derived and this formally completes geometrization of classical electrodynamics the minimal action principle leads to geometrization of the field sour... | [['a', 'study', 'of', 'the', 'model', 'of', 'embedded', 'spaces', 'mes', 'with', 'a', 'relativistic', 'version', 'of', 'finslerian', 'geometry', 'is', 'continued', 'the', 'field', 'equations', 'of', 'the', 'mes', 'einstein', 'and', 'maxwell', 'types', 'are', 'derived', 'and', 'this', 'formally', 'completes', 'geometriz... | [-0.19153144060530597, 0.07379106980644995, -0.11560814380128351, 0.07519783519415392, -0.11994913623978694, -0.1013117220136337, -0.015099344585905783, 0.21940958792887008, -0.23930848855525255, -0.29395615713049966, 0.10402572162921489, -0.2244032093634208, -0.11157250406944917, 0.19074646827519043, -0.06708297130858... |
706.2397 | Inversely Unstable Solutions of Two-Dimensional Systems on Genus-p
Surfaces and the Topology of Knotted Attractors | In this paper, we will show that a periodic nonlinear, time-varying
dissipative system that is defined on a genus-p surface contains one or more
invariant sets which act as attractors. Moreover, we shall generalize a result
in [Martins, 2004] and give conditions under which these invariant sets are not
homeomorphic t... | math.DS | in this paper we will show that a periodic nonlinear timevarying dissipative system that is defined on a genusp surface contains one or more invariant sets which act as attractors moreover we shall generalize a result in martins 2004 and give conditions under which these invariant sets are not homeomorphic to a circle ... | [['in', 'this', 'paper', 'we', 'will', 'show', 'that', 'a', 'periodic', 'nonlinear', 'timevarying', 'dissipative', 'system', 'that', 'is', 'defined', 'on', 'a', 'genusp', 'surface', 'contains', 'one', 'or', 'more', 'invariant', 'sets', 'which', 'act', 'as', 'attractors', 'moreover', 'we', 'shall', 'generalize', 'a', 'r... | [-0.20612095954983184, 0.14678763601540898, -0.1164170758190024, 0.0762410357563446, -0.04567042167919377, -0.14851299135635296, -3.844504089405139e-05, 0.3183661907662948, -0.27040030382573604, -0.22171932076724868, 0.14042695936126012, -0.24314663832386335, -0.21252004259886842, 0.19817708298253517, -0.12872463977895... |
706.2398 | Toy models of a non-associative quantum mechanics | Toy models of a non-associative quantum mechanics are presented. The
Heisenberg equation of motion is modified using a non-associative commutator.
Possible physical applications of a non-associative quantum mechanics are
considered. The idea is discussed that a non-associative algebra could be the
operator language f... | quant-ph hep-ph hep-th math.RA | toy models of a nonassociative quantum mechanics are presented the heisenberg equation of motion is modified using a nonassociative commutator possible physical applications of a nonassociative quantum mechanics are considered the idea is discussed that a nonassociative algebra could be the operator language for the no... | [['toy', 'models', 'of', 'a', 'nonassociative', 'quantum', 'mechanics', 'are', 'presented', 'the', 'heisenberg', 'equation', 'of', 'motion', 'is', 'modified', 'using', 'a', 'nonassociative', 'commutator', 'possible', 'physical', 'applications', 'of', 'a', 'nonassociative', 'quantum', 'mechanics', 'are', 'considered', '... | [-0.13073233044706284, 0.18737168779286245, -0.15754152107983826, 0.14960753124129647, -0.12823021278406183, -0.1861622901322941, -0.08690741509587194, 0.3007794017903507, -0.3121261129776637, -0.18339692614972591, 0.05478641693674338, -0.24735532385918002, -0.20293208036649352, 0.24274704821097354, -0.1038067656491572... |
706.2399 | Cosmological Constraints on f(R) Acceleration Models | Models which accelerate the expansion of the universe through the addition of
a function of the Ricci scalar f(R) leave a characteristic signature in the
large-scale structure of the universe at the Compton wavelength scale of the
extra scalar degree of freedom. We search for such a signature in current
cosmological ... | astro-ph gr-qc | models which accelerate the expansion of the universe through the addition of a function of the ricci scalar fr leave a characteristic signature in the largescale structure of the universe at the compton wavelength scale of the extra scalar degree of freedom we search for such a signature in current cosmological data s... | [['models', 'which', 'accelerate', 'the', 'expansion', 'of', 'the', 'universe', 'through', 'the', 'addition', 'of', 'a', 'function', 'of', 'the', 'ricci', 'scalar', 'fr', 'leave', 'a', 'characteristic', 'signature', 'in', 'the', 'largescale', 'structure', 'of', 'the', 'universe', 'at', 'the', 'compton', 'wavelength', '... | [-0.12584834012456916, 0.1079349381510507, -0.08916871761638587, 0.1294521220115712, -0.12371879464824981, -0.048825530655449256, -0.04546272786286532, 0.31439530533812515, -0.24054997333918104, -0.310315264105818, 0.03547803430278278, -0.3114766241537423, -0.0263573221944336, 0.2175842032227551, 0.06509510738194214, -... |
706.24 | Causality and Unitarity Are Not Violated in Space-Times with an
Additional Compact Time-like Dimension | The hypothesis that the causal properties of space-time, as well as other
properties of physical systems like unitarity, charge conservation, etc., might
be decided by the higher dimensional structure (in particular,
higher-dimensional physical laws), rather than by the four-dimensional one, is
explored in order to e... | hep-ph gr-qc | the hypothesis that the causal properties of spacetime as well as other properties of physical systems like unitarity charge conservation etc might be decided by the higher dimensional structure in particular higherdimensional physical laws rather than by the fourdimensional one is explored in order to evade the most a... | [['the', 'hypothesis', 'that', 'the', 'causal', 'properties', 'of', 'spacetime', 'as', 'well', 'as', 'other', 'properties', 'of', 'physical', 'systems', 'like', 'unitarity', 'charge', 'conservation', 'etc', 'might', 'be', 'decided', 'by', 'the', 'higher', 'dimensional', 'structure', 'in', 'particular', 'higherdimension... | [-0.12469445414899383, 0.18060361118114088, -0.061426201049471274, 0.14736275380164443, -0.12882834416814148, -0.19846923378645442, 0.004892600933089852, 0.23769623383122962, -0.2185748404244805, -0.2910700598076801, 0.13103530359148863, -0.2571818069263827, -0.12426448860787787, 0.15378130137105472, -0.052496348333079... |
706.2401 | Leptogenesis and dark matter unified in a non-SUSY model for neutrino
masses | We propose a unified explanation for the origin of dark matter and baryon
number asymmetry on the basis of a non-supersymmetric model for neutrino
masses. Neutrino masses are generated in two distinct ways, that is, a
tree-level seesaw mechanism with a single right-handed neutrino, and one-loop
radiative effects by a... | hep-ph | we propose a unified explanation for the origin of dark matter and baryon number asymmetry on the basis of a nonsupersymmetric model for neutrino masses neutrino masses are generated in two distinct ways that is a treelevel seesaw mechanism with a single righthanded neutrino and oneloop radiative effects by a new addit... | [['we', 'propose', 'a', 'unified', 'explanation', 'for', 'the', 'origin', 'of', 'dark', 'matter', 'and', 'baryon', 'number', 'asymmetry', 'on', 'the', 'basis', 'of', 'a', 'nonsupersymmetric', 'model', 'for', 'neutrino', 'masses', 'neutrino', 'masses', 'are', 'generated', 'in', 'two', 'distinct', 'ways', 'that', 'is', '... | [-0.14710472963685006, 0.29996991976932214, -0.036985232490686734, 0.23417168419416012, -0.1436950177885592, -0.19656397686993474, 0.06419143239199593, 0.29971330563880894, -0.20488652635953927, -0.2978768465629975, -0.01266541659909611, -0.24730530719419844, -0.052864145116856026, 0.0982117868710734, 0.074062580904482... |
706.2402 | Realizable spin models and entanglement dynamics in superconducting flux
qubit systems | Realizable spin models are investigated in a two superconducting flux qubit
system. It is shown that a specific adjustment of system parameters in the two
flux qubit system makes it possible to realize an artificial two-spin system
that cannot be found naturally. For the artificial two-spin systems, time
evolution of... | cond-mat.mes-hall | realizable spin models are investigated in a two superconducting flux qubit system it is shown that a specific adjustment of system parameters in the two flux qubit system makes it possible to realize an artificial twospin system that cannot be found naturally for the artificial twospin systems time evolution of a prep... | [['realizable', 'spin', 'models', 'are', 'investigated', 'in', 'a', 'two', 'superconducting', 'flux', 'qubit', 'system', 'it', 'is', 'shown', 'that', 'a', 'specific', 'adjustment', 'of', 'system', 'parameters', 'in', 'the', 'two', 'flux', 'qubit', 'system', 'makes', 'it', 'possible', 'to', 'realize', 'an', 'artificial'... | [-0.21620815770984336, 0.25333791580953857, -0.04303520559778917, 0.07525793144213822, 0.04643429713360092, -0.2305266827243031, 0.007729035489319358, 0.39688360847685544, -0.28217171564756427, -0.28900669041468063, 0.03210893421601213, -0.24559670066446415, -0.11902631691191345, 0.22787810473164427, 0.0110315463680308... |
706.2403 | Existence and non-existence results for quasilinear elliptic exterior
problems with nonlinear boundary conditions | Existence and non-existence results are established for quasilinear elliptic
problems with nonlinear boundary conditions and lack of compactness. The proofs
combine variational methods with the geometrical feature, due to the
competition between the different growths of the non-linearities.
| math.AP | existence and nonexistence results are established for quasilinear elliptic problems with nonlinear boundary conditions and lack of compactness the proofs combine variational methods with the geometrical feature due to the competition between the different growths of the nonlinearities | [['existence', 'and', 'nonexistence', 'results', 'are', 'established', 'for', 'quasilinear', 'elliptic', 'problems', 'with', 'nonlinear', 'boundary', 'conditions', 'and', 'lack', 'of', 'compactness', 'the', 'proofs', 'combine', 'variational', 'methods', 'with', 'the', 'geometrical', 'feature', 'due', 'to', 'the', 'comp... | [-0.10984991183718912, 0.027903266275595678, -0.08021378639693323, 0.08455225995031039, -0.1338926218878968, -0.13047515885218194, -0.07476224524802283, 0.2977720460315284, -0.3117675100404181, -0.3150152135150213, 0.17077758501430876, -0.28759748714142724, -0.10385063190723916, 0.21653711094864106, -0.0716935581938167... |
706.2404 | Commuting linear operators and algebraic decompositions | For commuting linear operators $P_0,P_1,..., P_\ell$ we describe a range of
conditions which are weaker than invertibility. When any of these conditions
hold we may study the composition $P=P_0P_1... P_\ell$ in terms of the
component operators or combinations thereof. In particular the general
inhomogeneous problem $... | math.OA math.AP | for commuting linear operators p_0p_1 p_ell we describe a range of conditions which are weaker than invertibility when any of these conditions hold we may study the composition pp_0p_1 p_ell in terms of the component operators or combinations thereof in particular the general inhomogeneous problem puf reduces to a syst... | [['for', 'commuting', 'linear', 'operators', 'p_0p_1', 'p_ell', 'we', 'describe', 'a', 'range', 'of', 'conditions', 'which', 'are', 'weaker', 'than', 'invertibility', 'when', 'any', 'of', 'these', 'conditions', 'hold', 'we', 'may', 'study', 'the', 'composition', 'pp_0p_1', 'p_ell', 'in', 'terms', 'of', 'the', 'componen... | [-0.1396951865948116, 0.11017925752591205, -0.052983954859276615, 0.086257569991479, -0.0555201935795291, -0.09805331608901421, -0.015256446236404979, 0.3123563229824261, -0.31452783807180823, -0.2678201399510726, 0.13207810244348367, -0.2609768260968849, -0.11968191079213283, 0.2003301073234373, -0.06647895077864328, ... |
706.2405 | Dispersion Relation for Alfven Waves in a Viscous, Diffusive Plasma | Propagation of Alfven waves in the solar plasma has been a topic of
scientific interest for a long time. We have derived a dispersion relation for
shear Alfven waves in a viscous and diffusive plasma.
| astro-ph | propagation of alfven waves in the solar plasma has been a topic of scientific interest for a long time we have derived a dispersion relation for shear alfven waves in a viscous and diffusive plasma | [['propagation', 'of', 'alfven', 'waves', 'in', 'the', 'solar', 'plasma', 'has', 'been', 'a', 'topic', 'of', 'scientific', 'interest', 'for', 'a', 'long', 'time', 'we', 'have', 'derived', 'a', 'dispersion', 'relation', 'for', 'shear', 'alfven', 'waves', 'in', 'a', 'viscous', 'and', 'diffusive', 'plasma']] | [-0.2160170650508787, 0.27194783235234876, -0.08854903030608381, 0.0787739383322852, -0.1033638492758785, -0.01393350213766098, -0.06895887018846614, 0.36246185818953175, -0.2400735661919628, -0.23950710424355098, 0.03682562289094286, -0.2502731204032898, -0.06475322438137872, 0.2722690261368241, 0.06597043169396265, 0... |
706.2406 | Collective motion in quantum diffusive environment | The general problem of dissipation in macroscopic large-amplitude collective
motion and its relation to energy diffusion of intrinsic degrees of freedom of
a nucleus is studied. By applying the cranking approach to the nuclear
many-body system, a set of coupled dynamical equations for the collective
classical variabl... | nucl-th | the general problem of dissipation in macroscopic largeamplitude collective motion and its relation to energy diffusion of intrinsic degrees of freedom of a nucleus is studied by applying the cranking approach to the nuclear manybody system a set of coupled dynamical equations for the collective classical variable and ... | [['the', 'general', 'problem', 'of', 'dissipation', 'in', 'macroscopic', 'largeamplitude', 'collective', 'motion', 'and', 'its', 'relation', 'to', 'energy', 'diffusion', 'of', 'intrinsic', 'degrees', 'of', 'freedom', 'of', 'a', 'nucleus', 'is', 'studied', 'by', 'applying', 'the', 'cranking', 'approach', 'to', 'the', 'n... | [-0.16286412779934323, 0.18291598885582808, -0.12239916676965852, 0.07224352006466152, -0.027923618300029866, -0.07156397960184571, 0.015035004295313206, 0.2846793685323344, -0.32694140730951077, -0.26757910537223023, 0.035254764424350396, -0.25506669420769285, -0.10680109687531605, 0.16444681064249614, 0.0007710777438... |
706.2407 | Parity violation in hydrogen revisited | We reconsider parity violation experiments in atomic hydrogen and deuterium
in the light of existing tests of the Electroweak interactions, and assess
whether new experiments, using improved experimental techniques, could make
useful contributions to testing the Standard Model (SM). We find that, if
parity experiment... | hep-ph | we reconsider parity violation experiments in atomic hydrogen and deuterium in the light of existing tests of the electroweak interactions and assess whether new experiments using improved experimental techniques could make useful contributions to testing the standard model sm we find that if parity experiments in hydr... | [['we', 'reconsider', 'parity', 'violation', 'experiments', 'in', 'atomic', 'hydrogen', 'and', 'deuterium', 'in', 'the', 'light', 'of', 'existing', 'tests', 'of', 'the', 'electroweak', 'interactions', 'and', 'assess', 'whether', 'new', 'experiments', 'using', 'improved', 'experimental', 'techniques', 'could', 'make', '... | [-0.08489045160099214, 0.2157466443067923, -0.046117896432264986, 0.08322780600577159, -0.029827355676176913, -0.1870611437717317, 0.07423420630581055, 0.34679396177904265, -0.21038281783524865, -0.32366442040639737, 0.040855266174439395, -0.2938212513363043, 0.008718768348188357, 0.2050782637026396, 0.0367949097281665... |
706.2408 | A New Type of Two-photon Forward Radiation in Pure Liquids | Unexpected spectral features are observed in the two photon spectrum of the
pure water in the forward direction when an 80 femtosecond laser pulse is
focused at 10^10Wcm-2 or less. Such intensity is much lower than the breakdown
or stimulated threshold of the liquid water. The two broad features are about
2700cm-1 an... | physics.chem-ph physics.optics | unexpected spectral features are observed in the two photon spectrum of the pure water in the forward direction when an 80 femtosecond laser pulse is focused at 1010wcm2 or less such intensity is much lower than the breakdown or stimulated threshold of the liquid water the two broad features are about 2700cm1 and 5000c... | [['unexpected', 'spectral', 'features', 'are', 'observed', 'in', 'the', 'two', 'photon', 'spectrum', 'of', 'the', 'pure', 'water', 'in', 'the', 'forward', 'direction', 'when', 'an', '80', 'femtosecond', 'laser', 'pulse', 'is', 'focused', 'at', '1010wcm2', 'or', 'less', 'such', 'intensity', 'is', 'much', 'lower', 'than'... | [-0.07593304658697429, 0.19324919278182437, -0.07216344781907148, 0.06950792301563745, -0.043899185675223475, -0.17115277431236164, 0.025614684522242366, 0.5084124912770049, -0.2510105775741553, -0.29219393616596473, 0.08970120662791672, -0.32400894971808547, -0.056331933751810816, 0.2236123869175236, 0.002013003223042... |
706.2409 | On the Number of Nodal Domains of Random Spherical Harmonics | Let N(f) be a number of nodal domains of a random Gaussian spherical harmonic
f of degree n. We prove that as n grows to infinity, the mean of N(f)/n^2 tends
to a positive constant, and that N(f)/n^2 exponentially concentrates around
that constant.
This result is consistent with predictions made by Bogomolny and Sc... | math-ph math.MP math.PR | let nf be a number of nodal domains of a random gaussian spherical harmonic f of degree n we prove that as n grows to infinity the mean of nfn2 tends to a positive constant and that nfn2 exponentially concentrates around that constant this result is consistent with predictions made by bogomolny and schmit using a perco... | [['let', 'nf', 'be', 'a', 'number', 'of', 'nodal', 'domains', 'of', 'a', 'random', 'gaussian', 'spherical', 'harmonic', 'f', 'of', 'degree', 'n', 'we', 'prove', 'that', 'as', 'n', 'grows', 'to', 'infinity', 'the', 'mean', 'of', 'nfn2', 'tends', 'to', 'a', 'positive', 'constant', 'and', 'that', 'nfn2', 'exponentially', ... | [-0.19424047620850615, 0.20103567822661716, -0.05284532287623733, 0.005098576250020415, -0.05272209414397366, -0.18083880643825978, 0.06373488128883764, 0.3010335043545638, -0.23230110520671587, -0.2155518937688612, 0.05686714635157841, -0.30654147116001695, -0.12294688292604405, 0.1609461964944785, -0.0144977373938672... |
706.241 | On the Supergravity Description of Wilson Loop in Non-commutative Dipole
Field Theory | The Wilson loop in the non-commutative dipole field theory is re-examined
within the framework of dual gravity description. In contrast to the previous
investigations, we let the dual string be moving along the deformed $S^5$ and
find the exact expression of the interquark potential. The potential shows a
Coulomb beh... | hep-th | the wilson loop in the noncommutative dipole field theory is reexamined within the framework of dual gravity description in contrast to the previous investigations we let the dual string be moving along the deformed s5 and find the exact expression of the interquark potential the potential shows a coulomb behavior at a... | [['the', 'wilson', 'loop', 'in', 'the', 'noncommutative', 'dipole', 'field', 'theory', 'is', 'reexamined', 'within', 'the', 'framework', 'of', 'dual', 'gravity', 'description', 'in', 'contrast', 'to', 'the', 'previous', 'investigations', 'we', 'let', 'the', 'dual', 'string', 'be', 'moving', 'along', 'the', 'deformed', ... | [-0.14469756668660086, 0.12446222678104155, -0.12194879738632841, 0.07581189258269512, -0.029305574748463726, -0.13283694714521738, 0.027975768042213876, 0.38747782698624794, -0.2214443694542137, -0.2619829584727995, 0.018164711759734043, -0.2979083086011579, -0.1414962220792281, 0.12476758278805662, -0.019153217580547... |
706.2411 | Violation of the London Law and Onsager-Feynman quantization in
multicomponent superconductors | Non-classical response to rotation is a hallmark of quantum ordered states
such as superconductors and superfluids. The rotational responses of all
currently known single-component "super" states of matter (superconductors,
superfluids and supersolids) are largely described by two fundamental
principles and fall into... | cond-mat.supr-con astro-ph hep-ph | nonclassical response to rotation is a hallmark of quantum ordered states such as superconductors and superfluids the rotational responses of all currently known singlecomponent super states of matter superconductors superfluids and supersolids are largely described by two fundamental principles and fall into two categ... | [['nonclassical', 'response', 'to', 'rotation', 'is', 'a', 'hallmark', 'of', 'quantum', 'ordered', 'states', 'such', 'as', 'superconductors', 'and', 'superfluids', 'the', 'rotational', 'responses', 'of', 'all', 'currently', 'known', 'singlecomponent', 'super', 'states', 'of', 'matter', 'superconductors', 'superfluids',... | [-0.13247487251038678, 0.26996559795311914, -0.0728685771803191, 0.057166556477609244, -0.025254066331562266, -0.17854656015328174, 0.06720534645484885, 0.3198178948612133, -0.2556366910462949, -0.29441468171608537, 0.04066068655550619, -0.2838077062824324, -0.06938930453190496, 0.15105711608263317, 0.01982968725062517... |
706.2412 | Generalized gauge-invariance for gravitational waves | The aim of this paper is to show the gauge-invariance on the response of
interferometers to gravitational waves (GWs). In this process, after a review
of results on the Tranverse-Traceless (TT) gauge, where, in general, the
theoretical computations on GWs are performed, which is due for completness, we
analyse the ga... | gr-qc | the aim of this paper is to show the gaugeinvariance on the response of interferometers to gravitational waves gws in this process after a review of results on the tranversetraceless tt gauge where in general the theoretical computations on gws are performed which is due for completness we analyse the gauge of the loca... | [['the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'show', 'the', 'gaugeinvariance', 'on', 'the', 'response', 'of', 'interferometers', 'to', 'gravitational', 'waves', 'gws', 'in', 'this', 'process', 'after', 'a', 'review', 'of', 'results', 'on', 'the', 'tranversetraceless', 'tt', 'gauge', 'where', 'in', 'general', 'the... | [-0.17828976931648227, 0.11697167126977867, -0.0869871823972947, 0.061277219059394226, -0.06485795241472236, -0.029492123002136075, 0.003145007203440056, 0.3720079571562442, -0.21345027386387055, -0.2562917007272591, 0.0828770456978787, -0.2691424564030525, -0.1411855292610346, 0.18036806609047376, -0.0268371434262057,... |
706.2413 | Comparison of Theory and Direct Numerical Simulations of Drag Reduction
by Rodlike Polymers in Turbulent Channel Flows | Numerical simulations of turbulent channel flows, with or without additives,
are limited in the extent of the Reynolds number \Re and Deborah number \De.
The comparison of such simulations to theories of drag reduction, which are
usually derived for asymptotically high \Re and \De, calls for some care. In
this paper ... | nlin.CD | numerical simulations of turbulent channel flows with or without additives are limited in the extent of the reynolds number re and deborah number de the comparison of such simulations to theories of drag reduction which are usually derived for asymptotically high re and de calls for some care in this paper we present a... | [['numerical', 'simulations', 'of', 'turbulent', 'channel', 'flows', 'with', 'or', 'without', 'additives', 'are', 'limited', 'in', 'the', 'extent', 'of', 'the', 'reynolds', 'number', 're', 'and', 'deborah', 'number', 'de', 'the', 'comparison', 'of', 'such', 'simulations', 'to', 'theories', 'of', 'drag', 'reduction', 'w... | [-0.1459496794213053, 0.14413831563156454, -0.07366238394197785, 0.01429760892226893, -0.03676468690502502, -0.1003798547289556, 0.0017605492917244277, 0.2946933393499681, -0.2325164498428681, -0.3410106999799609, 0.12228856714292695, -0.25907254512865274, -0.14060806665691503, 0.23408016196307949, -0.0603701834999291,... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.